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01744818 | The problem of electrical injection into 2D semiconductors like MoS 2, MoSe2, WSe2, or WS2 is thus a new challenge in this field, after the recent exploration of electrical spin injection into tridimensional (3D) semiconductors such as GaAs [9,10,11], Si [12], Ge [13], and in 2D Graphene [14]. The first experimental proof of electrical spin injection in 2D semiconductors has just been reported very recently: Ye et al. | 2017 | [
"phys"
] | [
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] | 01744818 | VI. CHARGE TRANSFER AT THE Co(0001)/MoS2 INTERFACE
To calculate the charge transfer between atoms induced by covalent bonding at the Co(0001)/MoS2 interface, we proceeded as follows: first, we calculated the majority spin electron density ( )
VIII. | 2017 | [
"phys"
] | [
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)
With the identity (39) the expression (38) becomes
p (1) = ik T k T k α Ro U u (0) + e z × u (0) + ρ (0) α 2 e z - iRo k T k α dk dt • u (0) . (40)
Re-writing (40) by means of the phase equation ( 35), we further obtain
p (1) = ik T β 2 e z × u (0) + ρ (0) α 2 e z + 2iRo k T U β 2 u (0) , (41)
where
β 2 = k T k α = k 2 r + k 2 θ + k 2 z /α 2 . | 2021 | [
"phys"
] | [
"336598",
"196526",
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] | [
"1094933",
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01744818 | 5 as belonging to the valence and conduction bands of the isolated MoS2 layer: The DOS curves of the isolated MoS2 sheet has also been represented in Fig. 5, where it has been shifted to coincide to the main DOS peaks of MoS2 at the Co/MoS2 interface. | 2017 | [
"phys"
] | [
"519179",
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] | [
"18552",
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] | 01744818 | Unfortunately, this ferromagnetic material has a Curie temperature near 200K, far below room temperature. An alternative way consists in using ferromagnetic metals (FM) like Cobalt, Iron or Nickel, with Curie temperatures well above room temperature. | 2017 | [
"phys"
] | [
"519179",
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] | [
"18552",
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] | 04235306 | To generate a 3D forest model, a CSV file containing the x 1 , x 2 coordinates of the trees and their diameter at breast height (DBH) is read and processed using Python scripts. The FreeCAD API is used to generate a triangular surface mesh representing the scene and containing data about the boundary materials. | 2023 | [
"phys"
] | [
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01744818 | The minority spin charge transfer is similarly given by 7 shows a top and a side view (the direction of observation corresponds to the blue arrow in Fig. 3) of the calculated three-dimensional majority and minority spin charge transfers interface is due to an excess of minority spin electrons, concomitant with a lack of majority spin electrons on interface Co atoms. | 2017 | [
"phys"
] | [
"519179",
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] | [
"18552",
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] | 01744818 | CONCLUSIONS
In this paper we have investigated the electronic structure of a single low-strained hcp Co(0001)/MoS2 interface, using first-principles calculations based on the functional density theory, in order to estimate the potentiality of a cobalt injector for electrical spin injection into a MoS2 monolayer, in view of spintronic devices as spin-FET. We first described the lowest energy atomic structure and show that interface S atoms are covalently bound to one, two or three interface Co atoms. | 2017 | [
"phys"
] | [
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] | [
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] | 03020547 | 2. Faster heating generated a more extensive range of heat flow and increasing cure rate. | 2020 | [
"phys"
] | [
"866",
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] | [
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] |
01744818 | Figure 7 :
7 Figure 7: (a): Top view and (b): side view of the majority spin charge transfer
Figure 8 :
8 Figure 8: Sketch representing (a): the bottom view (below the Co contact) and (b): the side view of the physical area involving the Co(0001) contact, (MoS2)*, the Schottky barrier (MoS2)*/ MoS2 obtained by suitable doping and the MoS2 channel. The one-dimensional border which should be designed to lower the exponential decay of wave functions in the Schottky barrier is indicated by red a dashed line in (a), together with the (ΓK) direction of MoS2 (red arrow). | 2017 | [
"phys"
] | [
"519179",
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] | [
"18552",
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] | 01744818 | It has been realized successfully in Fe/GaAs system [10] where GaAs was gradually n-doped up to 10 19 cm -3 at the interface, resulting in a very efficient electrical spin injection from Fe into GaAs in tunnel regime. In the context of TMDCs, the general problem of electrical contacts on TMDCs for transport in a two-dimensionnal channel is a challenging task (tackled for example by phase engineering techniques [31,32], as well as using contacts based on heterostructures involving graphene [22]. | 2017 | [
"phys"
] | [
"519179",
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] | [
"18552",
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] | 01494656 | R Lozada Garcia
N Nieuwjaer
C Desfrançois
F Lecomte
S D Leite
B Manil
M Broquier
G Grégoire
Vibronic spectra of protonated hydroxypyridines: contributions of prefulvenic and planar structures
Various hydroxypyridine derivatives are endogenous or synthetic photosensitizers which could contribute to solar radiation damages. The study of their excited states could lead to a better understanding of their action mechanisms. | 2017 | [
"phys"
] | [
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01744818 | 5 The estimation of the spin polarization at the Fermi level for Co/MoS2 interface is of importance for spin injection. As pointed out by Mazin [30], an accurate determination of the electric current spin polarization would however require complementary DFT-based calculations (including the transmittance of the whole complex structure and the effects of the bias voltage). | 2017 | [
"phys"
] | [
"519179",
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] | [
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] | 01744818 | The lattice parameter that we chose for the Co(5x5)/MoS2(4x4) unit cell corresponds to four times the lattice parameter calculated for MoS2 (0.319 nm). The atomic structure of all the different MoS2/Co(5MLs)/MoS2 supercells that we have considered has been obtained by minimizing the forces acting on the different atoms. | 2017 | [
"phys"
] | [
"519179",
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"519179"
] | [
"18552",
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] | 04308317 | To attenuate signal contributions of DC offsets, non-linearities and signal components situated at twice the demodulation frequency, a sinc-filter is applied. The combination of the low time constant with the sinc-filter results in higher measurement noise compared to the detection with the boxcar filter. | 2023 | [
"phys"
] | [
"497162"
] | [
"184739"
] |
01744818 | As pointed out by Mazin [30], an accurate determination of the electric current spin polarization would however require complementary DFT-based calculations (including the transmittance of the whole complex structure and the effects of the bias voltage). V. SPIN MAGNETIC MOMENTS AT THE Co(0001)/MoS2 INTERFACE
The spin magnetic moment of Co atoms is on average 8% lower at the Co(0001)/MoS2 interface than in bulk hcp Co (1.69 µB), with values that depend on the kind of interface S atom to which they are covalently bound: The interface Co atoms that show the highest spin magnetic moment (1.66 µB and 1.63 µB) are the 4 atoms which are not bound to S atoms, followed by Co3 (1.62 µB) and Co2 atoms (1.57 µB). | 2017 | [
"phys"
] | [
"519179",
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"519179"
] | [
"18552",
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"171543",
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] | 01744818 | have shown that spin polarized holes can be injected in WSe2 from the ferromagnetic semiconductor GaMnAs that acts as a spin aligner [15]. Unfortunately, this ferromagnetic material has a Curie temperature near 200K, far below room temperature. | 2017 | [
"phys"
] | [
"519179",
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"116255",
"43574",
"519179"
] | [
"18552",
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] | 03604636 | The results suggested that this force (of order 400 pN) is an intrinsic quantity, independent of the number of fibrin layers involved in the adhesive contact. (1), and platelets form anchoring points for fibrin fiber formation (2). | 2001 | [
"phys"
] | [
"690",
"690",
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"23430"
] | [
"891744"
] |
01744818 | CHARGE TRANSFER AT THE Co(0001)/MoS2 INTERFACE
To calculate the charge transfer between atoms induced by covalent bonding at the Co(0001)/MoS2 interface, we proceeded as follows: first, we calculated the majority spin electron density ( )
VIII. CONCLUSIONS
In this paper we have investigated the electronic structure of a single low-strained hcp Co(0001)/MoS2 interface, using first-principles calculations based on the functional density theory, in order to estimate the potentiality of a cobalt injector for electrical spin injection into a MoS2 monolayer, in view of spintronic devices as spin-FET. | 2017 | [
"phys"
] | [
"519179",
"519179",
"116255",
"43574",
"519179"
] | [
"18552",
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"171543",
"18553"
] | 01744818 | This band is more clearly visible for minority spin (Fig. 4b) than for majority spin electrons for which it is located in the continuum of Co d-bands (Fig. | 2017 | [
"phys"
] | [
"519179",
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] | [
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] | 04396278 | Figure 1 :
1 Figure 1: Schematic drawing of the discharge cell a) detailed view b) view through quartz barThe plasma is generated in the gas gap by applying a sinusoidal high voltage (HV) to the upper
The surface and cross section morphology of TiO 2 NPs plasma thin film are investigated by scanning electron microscopy (SEM Hitachi S-4500). The images are acquired in the high resolution mode with an extraction voltage of 5 kV and a magnification from x10 K to x100 K.The chemical composition of the coating is analyzed by X-ray photoelectron spectroscopy (VG Escalab 220i XL) using a 1486.6 eV, Al -ray source. | 2017 | [
"phys"
] | [
"92448",
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01744818 | This is performed within the second-order perturbation theory, for which we chose to include unoccupied electron states up to the maximum energy of 48 eV above the Fermi level, the magnetization being oriented along the Co(0001) axis. III. | 2017 | [
"phys"
] | [
"519179",
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] | [
"18552",
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] | 01744818 | The distance between interface S and Co atoms is of 0.236 nm between S3 and Co3, 0.234 nm between S2 and Co2, and of 0.221 or 0.222 nm between the 12
. Red and green areas respectively correspond to a local excess and a local lack of electrons. | 2017 | [
"phys"
] | [
"519179",
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"43574",
"519179"
] | [
"18552",
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] | 03113407 | [START_REF] Lee | The relation of education and income to cognitive function among professional women[END_REF] Overall, these findings suggest that females under the age of 71 with a mid-to-high income may be better protected from the negative outcomes in memory performance associated with insomnia disorder, and that other clinical or lifestyle factors do not appear to significantly further predict memory performance within insomnia disorder. The identification of declarative memory impairment independently associated with insomnia in older adults is particularly important in the context of cognitive decline. | 2019 | [
"phys"
] | [
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01744818 | Figure 7 :
7 Figure 7: (a): Top view and (b): side view of the majority spin charge transfer
Figure 8 :
8 Figure 8: Sketch representing (a): the bottom view (below the Co contact) and (b): the side view of the physical area involving the Co(0001) contact, (MoS2)*, the Schottky barrier (MoS2)*/ MoS2 obtained by suitable doping and the MoS2 channel. The one-dimensional border which should be designed to lower the exponential decay of wave functions in the Schottky barrier is indicated by red a dashed line in (a), together with the (ΓK) direction of MoS2 (red arrow). | 2017 | [
"phys"
] | [
"519179",
"519179",
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"519179"
] | [
"18552",
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] | 01744818 | have shown that spin polarized holes can be injected in WSe2 from the ferromagnetic semiconductor GaMnAs that acts as a spin aligner [15]. Unfortunately, this ferromagnetic material has a Curie temperature near 200K, far below room temperature. | 2017 | [
"phys"
] | [
"519179",
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"519179"
] | [
"18552",
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] | 01473661 | These remarks on the pressure were regardless the connement. In fact, reducing it was only responsible of a decrease in the electric eld at a given current. | 2017 | [
"phys"
] | [
"214579",
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] | [
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01744818 | Some of these interface bands have a non-negligible dispersion near the Fermi level (electrons in the metallic phase of MoS2 at the Co/MoS2 interface will not have a high effective mass). Each energy band in Figs. | 2017 | [
"phys"
] | [
"519179",
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] | [
"18552",
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] | 01744818 | For this metallic phase of MoS2, a spin polarization at the Fermi level of 16 % in absolute value is calculated, that could allow spin injection into the semiconducting MoS2 monolayer channel. Finally, the symmetry of the majority and minority spin electron wave functions at the Fermi level in the Co-bound metallic phase of MoS2 and the orientation of the border between the metallic and semiconducting phases of MoS2 are investigated, and their impact on spin injection into the MoS2 channel is discussed. | 2017 | [
"phys"
] | [
"519179",
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] | [
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] | 01332808 | The parameters are chosen in the three non trivial phases, the CDW, the SCDW and the PMD. For each of them, the SDCI clearly improves the GS energies, hence showing that correlations have been incorporated. | 2014 | [
"phys"
] | [
"446814",
"446814"
] | [
"767034"
] |
01744818 | Band structure and density of states of the hybrid system are calculated for minority and majority spin electrons, taking into account spin-orbit coupling. We demonstrate that MoS2 bound to the Co contact becomes metallic due to hybridization between Co d and S p orbitals. | 2017 | [
"phys"
] | [
"519179",
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"519179"
] | [
"18552",
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] | 01744818 | A lower spin magnetic moment is observed for Co atoms at the interface, together with a small magnetization of S atoms. Mo atoms also hold small magnetic moments which can takes positive as well as negative values. | 2017 | [
"phys"
] | [
"519179",
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] | [
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] | 04077162 | This clearly illustrates the notable differences in the physical behaviour of the cavity model with a completely positive Liouvillian and the friction model which is manifestly not completely positive. V. EFFECTIVE MEAN-FIELD THEORIES
Mean-field descriptions [START_REF] Nishimori | Elements of phase transitions and critical phenomena[END_REF] of phase transitions often provide a first qualitative appreciation of cooperative effects in manybody systems. | 2023 | [
"phys"
] | [
"525770",
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01744818 | PERSPECTIVES: TOWARDS ELECTRICAL SPIN INJECTION IN MoS2
In the context of spin injection into bulk semiconductor materials, it has been established that the so-called conductivity mismatch [16] between the ferromagnetic metal injector and the semiconductor constitutes a fundamental obstacle for efficient spin injection at the ferromagnetic metal/semiconductor interface in the diffusive regime. To circumvent this problem, it has been shown that a thin tunnel barrier must be introduced between FM and SC, inducing an effective spin dependent resistance [17]. | 2017 | [
"phys"
] | [
"519179",
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] | [
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] | 01744818 | We finally discuss the physical properties of the Co(0001)/MoS2 interface in the perspective of spin injection in the 2D semiconductor MoS2, and give insights on the possible utilization of the low strained Co/MoS2 contact for in plane spin transport in lateral channels [17]. II.FIRST-PRINCIPLES METHODS
The ground state energy, the charge and the spin densities of all the supercells have been calculated self-consistently using the full-potential augmented plane waves + local orbitals (APW+lo) method implemented in the code WIEN2k [START_REF] Blaha | WIEN2k, an augmented plane wave+local orbitals program for calculating crystal properties[END_REF]. | 2017 | [
"phys"
] | [
"519179",
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] | [
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] | 01068649 | An MKS 999 Quattro multi-sensor transducer is used to monitor the pressure in the chamber. The argon and xenon flow into the thruster is regulated with a Bronkhorst El-flow and Brooks 5850E series mass flow controllers. | 2014 | [
"phys"
] | [
"252027",
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] | [
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01744818 | The lattice parameter that we chose for the Co(5x5)/MoS2(4x4) unit cell corresponds to four times the lattice parameter calculated for MoS2 (0.319 nm). The atomic structure of all the different MoS2/Co(5MLs)/MoS2 supercells that we have considered has been obtained by minimizing the forces acting on the different atoms. | 2017 | [
"phys"
] | [
"519179",
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"519179"
] | [
"18552",
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] | 01744818 | This holds for majority as well as for minority spin electrons. Despite the strong modification of the electronic structure of MoS2, important DOS peaks can be identified in Fig. | 2017 | [
"phys"
] | [
"519179",
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] | [
"18552",
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] | 01265015 | Thus, the thermodynamic limit
ρ (∞) B (A) = lim L→∞ tr ρ (L) B A = lim L→∞ tr ρ (L) BAB * tr(ρ (L) BB * ) = ρ (∞) (BAB * ) ρ (∞) (BB * )
also exists and defines a local perturbation ρ
(∞) B
of the state ρ (∞) . Assume that the sequence of Hamiltonians {H (L) } L≥0 defines a dynamics
ρ (∞) B,t (A) = lim L→∞ ρ (L) B e itH (L) Ae -itH (L)
on these states. | 2017 | [
"phys"
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01744818 | These new bands correspond to interface Bloch states involving covalently bound Co and S atoms. They strongly modify the physical properties of MoS2, giving a metallic behavior to this layer, induced by interface covalent bonding. | 2017 | [
"phys"
] | [
"519179",
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] | [
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] | 01744818 | Each of the interface Co atoms are bound to a single S atom, except the four ones marked by a star in Fig. 3. | 2017 | [
"phys"
] | [
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] | 02050889 | Figure 6. Temperature dependence of the shear modulus G and Poisson's ratio 𝜈 of the (a) as-prepared C1-SiOC-1600 SiOC glass-ceramic and (b) after a thermal treatment for 6 days at 1100 °C. | 2019 | [
"phys"
] | [
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01744818 | After all the atoms have reached their equilibrium position, we observed that the ground state energy is the lowest for Supercell1, and respectively 0.0827 eV and 0.813 eV higher for Supercell2 and Supercell3. These energy differences correspond to the whole supercells, which all contain 2 MoS 2/Co interfaces with 16 MoS2 formula units in the 4x4 MoS2 cell. | 2017 | [
"phys"
] | [
"519179",
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] | 01744818 | The problem of electrical injection into 2D semiconductors like MoS 2, MoSe2, WSe2, or WS2 is thus a new challenge in this field, after the recent exploration of electrical spin injection into tridimensional (3D) semiconductors such as GaAs [9,10,11], Si [12], Ge [13], and in 2D Graphene [14]. The first experimental proof of electrical spin injection in 2D semiconductors has just been reported very recently: Ye et al. | 2017 | [
"phys"
] | [
"519179",
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] | [
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] | 00592348 | [END_REF]. The stated aim of [START_REF] Barbour | The nature of time[END_REF] is to "persuade you that time as an independent concept has no place in physics", as seen in its introduction. | 2011 | [
"phys"
] | [
"203264"
] | [
"874996"
] |
01744818 | FIGURE CAPTIONS
have studied the Ni(111)/MoS2 interface, but they mostly focus their study on the consequences of the insertion of a graphene layer between Ni and MoS2, than on a detailed description of the Ni(111)/MoS2 interface [22]. Finally, Yin et al. | 2017 | [
"phys"
] | [
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] | [
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] | 01744818 | These new bands correspond to interface Bloch states involving covalently bound Co and S atoms. They strongly modify the physical properties of MoS2, giving a metallic behavior to this layer, induced by interface covalent bonding. | 2017 | [
"phys"
] | [
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] | [
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] | 00143680 | The calculations here have been made with a salt containing 80 mole% of LiF completed with BeF 2 but some other possible components (CaF 2 for example) are under study. INITIAL FISSILE CHOICE AND INVENTORIES TMSR Started with 233 U
The 233 U initial inventory ranges from 2550 kg for a HN proportion in the salt of 7.5 mole % to 6180 kg for a HN proportion of 27.5 mole % (see Table 1). | 2007 | [
"phys"
] | [
"126",
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] | [
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01744818 | This work
indicates if a spin-polarized current can be injected through the Co/MoS2 interface to a MoS2 channel. DOS curves shown in Fig. | 2017 | [
"phys"
] | [
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] | [
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] | 01744818 | This holds for majority as well as for minority spin electrons. Despite the strong modification of the electronic structure of MoS2, important DOS peaks can be identified in Fig. | 2017 | [
"phys"
] | [
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] | 03360800 | 2 /
2 FeCoB (1.6) FeCoB (1.2)/Ta0.2 Please do not adjust margins Please do not adjust margins
Fig. 4 a
4 Fig.4 a) Resistance variation with the pulse duration for different pulse amplitudes. | 2021 | [
"phys"
] | [
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] | [
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] |
01744818 | For all these reasons, the genuine atomic structure of the Co/MoS2 interface may probably be different from that used by these authors. In the present paper, we considered supercells built from 5x5 Co(0001) atomic layers with the hcp stacking and a 4x4 MoS2 single layer. | 2017 | [
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] | [
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] | [
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] | 01744818 | Leong et al. and Co/MoS2 interfaces [23]. | 2017 | [
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] | [
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] | [
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] | 02433902 | 3: some views of equipments
Next important milestones will be the installation of main circuits components (for the reactor building), and the completion of the hot cells complex structure (for the nuclear auxiliaries building). Fig. | 2017 | [
"phys"
] | [
"92792",
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] | [
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01744818 | The radius of the red circles in panels (b) and (c) is proportional to the MoS2 contribution to the electron states. The blue arrow in panel (a) indicates the minimum of the conduction band in MoS2; its corresponding position in the band structure of the Co/MoS2 slab is also shown with a blue arrow in panel (b), where it corresponds to the height of the Schottky barrier. | 2017 | [
"phys"
] | [
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] | [
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] | 01744818 | The distance between interface S and Co atoms is of 0.236 nm between S3 and Co3, 0.234 nm between S2 and Co2, and of 0.221 or 0.222 nm between the 12
. Red and green areas respectively correspond to a local excess and a local lack of electrons. | 2017 | [
"phys"
] | [
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] | [
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] | 04067221 | Fig 1 presents an example of a two stages cable, a triplet of triplets (3x3 multiplicity). We check the values of the magnetic coefficients (n and through the penetration steps to assess the results of the study. | 2022 | [
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] | [
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01744818 | After all the atoms have reached their equilibrium position, we observed that the ground state energy is the lowest for Supercell1, and respectively 0.0827 eV and 0.813 eV higher for Supercell2 and Supercell3. These energy differences correspond to the whole supercells, which all contain 2 MoS 2/Co interfaces with 16 MoS2 formula units in the 4x4 MoS2 cell. | 2017 | [
"phys"
] | [
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] | [
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] | 01744818 | Leong et al. and Co/MoS2 interfaces [23]. | 2017 | [
"phys"
] | [
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] | [
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] | 00951772 | 66 MC(%) F 6 kHz 1.0 (0) 1.9 (2.0) 10.1 (9.9) 19.6 (19.9)
SNR 1 (1) 1.9 (2.2) 10.1 (10.8) 19.6 (21.7)
Table 2 . Modulation contrast (MC) and signal to noise ratio (SNR) of the LOFI images (Figs. | 2010 | [
"phys"
] | [
"392407",
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] | [
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] |
01744818 | As discussed by Zhong et al. [27], this seems to give results in a better agreement with experimental ones than those computed with the GW method, probably due to the fact that many-electron effects are greatly depressed by the charge transfer at the MoS2/metal interface, which significantly screens electron-electron interaction [27]. | 2017 | [
"phys"
] | [
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"519179"
] | [
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] | 01744818 | 7d). ( ) ( ) ( ) ( ) { } r r r r 2 , , MoS Co n n n n ↓ ↓ ↓ ↓ + - = ∆ . | 2017 | [
"phys"
] | [
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"519179"
] | [
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] | 02635273 | One would expect the voltage performance to be determined by the bandgap of the QW material. The the most challenging situation is to compare samples with the same effective threshold, as in this set of samples. | 2006 | [
"phys"
] | [
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01744818 | 3. The atomic layers present a small warping near the Co/MoS2 interface, due to the different numbers of chemical bounds formed by the non-equivalent interface S atoms. | 2017 | [
"phys"
] | [
"519179",
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"519179"
] | [
"18552",
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] | 01744818 | 5 as belonging to the valence and conduction bands of the isolated MoS2 layer: The DOS curves of the isolated MoS2 sheet has also been represented in Fig. 5, where it has been shifted to coincide to the main DOS peaks of MoS2 at the Co/MoS2 interface. | 2017 | [
"phys"
] | [
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"519179"
] | [
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] | 02464478 | k 0 coth 0 @ ~! ! | 2020 | [
"phys"
] | [
"70384"
] | [
"19133"
] |
01744818 | The largest wave vector Kmax used for expanding the Kohn-Sham wave functions in the interstitial area between atomic spheres is given by the dimensionless parameter RminKmax=6.0, where Rmin is the smallest atomic sphere radius of the supercell; this corresponds to an energy cut-off of 151 eV. The irreducible wedge of the Co/MoS2 supercell two-dimensional Brillouin zone was sampled with a k-mesh of typically 24 different k-vectors, generated with a special k-grid used to perform Brillouin zone integrations with the modified tetrahedron integration method. | 2017 | [
"phys"
] | [
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"519179"
] | [
"18552",
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] | 01744818 | This estimation of the Schottky barrier height is larger than the values measured experimentally (between 60 meV in [28] and 121 meV [29]). These measurements are however performed on exfoliated MoS2 flakes. | 2017 | [
"phys"
] | [
"519179",
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] | [
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] | 01926640 | Although ACL injury does not often occurs during the push-off phase of vertical jumping, the investigation of the push-off during maximal single leg jump makes it possible to compare a standardized multi-joint movement (i.e. only one aim which is jumping as high as possible) between ACL-R and healthy people. | 2017 | [
"phys"
] | [
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] | [
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01744818 | Leong et al. and Co/MoS2 interfaces [23]. | 2017 | [
"phys"
] | [
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"519179"
] | [
"18552",
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] | 01744818 | The conduction electron wavefunctions in the isolated MoS2 channel exhibit a strong Mo dz 2 character (as well as a smaller Mo s character), and a S (px+py) character. The DOS at the Fermi level calculated for (MoS2)* is qualitatively different from the DOS at the bottom of the conduction band of MoS2. | 2017 | [
"phys"
] | [
"519179",
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] | [
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] | 01386365 | The holographic images of these two datasets were then demodulated spatially [31], to yield 661 × 661 complex-valued time traces X(t) of 128 elements each, cropped from the 2048 × 2048 calculation array, over an off-axis spatial region of interest where the image was expected. We then compared two types of signal demodulation procedures to assess the magnitude of the oscillating signal at the frequency ∆ω in X(t) at each pixel : Fourier analysis, and singular value analysis of temporal fluctuations. | 2015 | [
"phys"
] | [
"250059",
"1004908"
] | [
"1300"
] |
01744818 | FIGURE CAPTIONS
have studied the Ni(111)/MoS2 interface, but they mostly focus their study on the consequences of the insertion of a graphene layer between Ni and MoS2, than on a detailed description of the Ni(111)/MoS2 interface [22]. Finally, Yin et al. | 2017 | [
"phys"
] | [
"519179",
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"519179"
] | [
"18552",
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] | 01744818 | Each of the interface Co atoms are bound to a single S atom, except the four ones marked by a star in Fig. 3. | 2017 | [
"phys"
] | [
"519179",
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"519179"
] | [
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] | 00149105 | Second, we report the charge ordering on the oxygen in La 7 8 Sr 1 8 MnO 3 ; our observations confirm the stacking of alternate hole-rich and hole-poor planes. In both cases, the O states are directly related to the Mn states, emphasizing the hybridized nature of the active states involved in the electronic orderings. | 2007 | [
"phys"
] | [
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01744852 | Hence we can use the VARPRO approach to solve for {p, α} [START_REF] Golub | Separable nonlinear least squares: the variable projection method and its applications[END_REF]. The unknown α is substituted by Λ (p)
+ Y, where Λ (p) + is the Moore-Penrose generalized inverse of Λ (p). | 2018 | [
"info"
] | [
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] | [
"1010653",
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] | 01744852 | The experiments are carried out for SNR values ranging from 5 to 100 in steps of 5. We simulated T 2 relaxometry data with the following parameters: first echo (TE 0 ) is at 9ms; TE= 9ms; 32 echoes, 100 signal averages. | 2018 | [
"info"
] | [
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] | [
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] | 04172460 | . . | 2023 | [
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] | [
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] | [
"1273324"
] |
01744852 | These may be distinguished based on their transverse relaxation times which can be measured using T 2 relaxometry MRI. However, due to physical limitations on achievable resolution, each voxel contains a combination of these tissues, rendering the estimation complex. | 2018 | [
"info"
] | [
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"81450",
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] | [
"1010653",
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] | 01744852 | The stimulated echoes are thus obtained using the EPG algorithm [START_REF] Prasloski | Applications of stimulated echo correction to multicomponent T2 analysis[END_REF]. EPG(•) is the stimulated echo computed at t i = i ∆TE where i = {1, . | 2018 | [
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
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] | 01379683 | By the minimality assumption, if v k contains a restricted term, then it must be equal to some t l 0 < l ≤ n and therefore, that t l t j , which contradicts the local restriction. Therefore, since t j is a restricted term, k = 0. | 2016 | [
"info"
] | [
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] | [
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01744852 | 1 . 1 Fig. | 2018 | [
"info"
] | [
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"491318"
] | [
"1010653",
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] | 01744852 | Here we propose an estimation framework to obtain brain microstructure information using a multi-compartment tissue model from T 2 relaxometry MRI data. The T 2 space is modeled as a weighted mixture of three continuous probability density functions (PDF), each representing the tissues with short, medium and high T 2 relaxation times. | 2018 | [
"info"
] | [
"491318",
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] | [
"1010653",
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] | 01930460 | Figure 8 . 8 Figure 8. | 2016 | [
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] | [
"214",
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01744852 | 1). High w s values in the genu of the CC of healthy volunteer data (refer Fig. | 2018 | [
"info"
] | [
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] | [
"1010653",
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] | 01744852 | 1 . 1 Fig. | 2018 | [
"info"
] | [
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"491318"
] | [
"1010653",
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] | 03866767 | 16 seems to be richer than the TM models are (e.g., destination, origin, and victim). The TM modeling is precise in terms of clear separation of events from the static description. | 2022 | [
"info"
] | [
"1062838"
] | [
"1069014"
] |
01744852 | The increment in µ m values in lesion-1 as we approach the lesion core from the lesion boundary might also indicate a reduction in axon density. This is in accordance with the pathology of MS lesion evolution [10][11]. | 2018 | [
"info"
] | [
"491318",
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"81450",
"491318"
] | [
"1010653",
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] | 01744852 | EPG(•) is the stimulated echo computed at t i = i ∆TE where i = {1, . . | 2018 | [
"info"
] | [
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] | [
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] | 04086455 | Recent surveys, as the one offered by [START_REF] Xie | Explainable deep learning: A field guide for the uninitiated[END_REF], suggest that explainability can be decomposed by the methods used to evaluate it. A brief description of the main families found in literature is provided below. | 2023 | [
"info"
] | [
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] | [
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01744852 | ( 4) for p, the values of α are obtained as Λ (p) + Y. The optimization for {α, p} and B 1 is performed alternatively until convergence. | 2018 | [
"info"
] | [
"491318",
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"81450",
"491318"
] | [
"1010653",
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] | 01830532 | Due to higher TEs in dMRI, the myelin information is not present in the dMRI signals. However, myelin information can be obtained by estimating the myelin water fraction (MWF) from T2 relaxometry MRI signal [START_REF] Laule | Magnetic resonance imaging of myelin[END_REF][START_REF] Mackay | Magnetic resonance of myelin water: An in vivo marker for myelin[END_REF]. | 2018 | [
"sdv",
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] | [
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] | [
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] | 03789133 | Methodology for the creation of integrated design and analysis framework pertaining to safety and security. Fundamental well-defined notions that are the building blocks upon which high-level requirements can be decomposed and characterized. | 2021 | [
"info"
] | [
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] | [
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01744852 | The weights chosen for each compartment were, {w s , w m , w h } = {0.2, 0.7, 0.1}. The B 1 , M 0 and T 1 values considered for this simulation were 1.3, 950 and 1000 respectively. | 2018 | [
"info"
] | [
"491318",
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"81450",
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] | [
"1010653",
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] | 01830532 | We used the 2D multislice Carr-Purcell-Meiboom-Gill (CPMG) sequence to acquire T2 relaxometry data. CPMG sequences suffer from the effect of the stimulated echoes due to imperfect refocusing. | 2018 | [
"sdv",
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] | [
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"81450",
"491318"
] | [
"1010653",
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] | 03332510 | A semantics σ satisfies compensation iff, there exists a WAG
G = A , w, R such that for two arguments a, b ∈ A , • w(a) = w(b), • σ G (a) > 0, • |{x ∈ Att G (a) | σ G (x) > 0}| > |{y ∈ Att G (b) | σ G (y) > 0}| • ∃y ∈ Att G (b) s.t. ∀x ∈ Att G (a), σ G (y) > σ G (x) and σ G (a) = σ G (b). | 2021 | [
"info"
] | [
"90448"
] | [
"740997"
] |
01744852 | The minimization problem in Eq. ( 4) is solved for µ m using the analytically obtained derivative in Eq. | 2018 | [
"info"
] | [
"491318",
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"81450",
"491318"
] | [
"1010653",
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] | 01830532 | 2. This MS patient had 18 MS lesions out of which 3 of them had Gd enhancing regions. | 2018 | [
"sdv",
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] | [
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] | [
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] | 01216165 | Using a cognitive model means to define what it wants (e.g. to find fire, to extinguish a specific fire, to get water) and how to do it (e.g. | 2015 | [
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01744852 | Sudhanya Chatterjee
Olivier Commowick
Onur Afacan
Simon K Warfield
Christian Barillot
MULTI-COMPARTMENT MODEL OF BRAIN TISSUES FROM T2 RELAXOMETRY MRI USING GAMMA DISTRIBUTION
Keywords: T 2 relaxometry, microstructure, brain
The brain microstructure, especially myelinated axons and free fluids, may provide useful insight into brain neurodegenerative diseases such as multiple sclerosis (MS). These may be distinguished based on their transverse relaxation times which can be measured using T 2 relaxometry MRI. | 2018 | [
"info"
] | [
"491318",
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"81450",
"491318"
] | [
"1010653",
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] | 01830532 | Demyelination marks the onset of MS [START_REF] Lassmann | Heterogeneity of multiple sclerosis pathogenesis: Implications for diagnosis and therapy[END_REF]. Myelin has a very short T2 relaxation time (<50ms) due to its tightly wrapped structure [START_REF] Lancaster | Three-pool model of white matter[END_REF]. | 2018 | [
"sdv",
"info"
] | [
"491318",
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] | [
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] | 00797367 | It seeks the linear subspace that captures the maximal variance from the data. Its good interpretability taken aside, this method tends to compress the elements in the projection space (i.e. | 2013 | [
"info"
] | [
"214267",
"214267"
] | [
"932607",
"932608"
] |
01744852 | ( 4) for p, the values of α are obtained as Λ (p) + Y. The optimization for {α, p} and B 1 is performed alternatively until convergence. | 2018 | [
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
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] | 01830532 | The medium-T2 compartment is a mixed pool and conveys information on intracellular matter (such as unmyelinated axons and glia), intra and extracellular fluids [START_REF] Lancaster | Three-pool model of white matter[END_REF]. The T2 space is modeled as a weighted mixture of the three compartments, where each compartment is represented by a continuous probability density function (PDF). | 2018 | [
"sdv",
"info"
] | [
"491318",
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] | [
"1010653",
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] | 01764197 | The absolute error is taken from the computer tools or the measurement methods. For the calculi and the similarities, we will use partial differential method and weighted mean absolute error. | 2017 | [
"info"
] | [
"136804",
"136804"
] | [
"1030707",
"861738"
] |
01744852 | Multi-compartment model using gamma PDF The previous estimation framework is generic as it does not depend on the chosen PDF. We choose here to use gamma PDF for f j (•) for j = {1, 2 ,3} since their non-negativity and skewed nature are well suited to describe the compartments used to model the T 2 space. | 2018 | [
"info"
] | [
"491318",
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"81450",
"491318"
] | [
"1010653",
"14904",
"1245"
] | 01744852 | Since p ∈ R k , the Jacobian matrix J ∈ R k×m and its columns are computed as shown in [START_REF] Golub | Separable nonlinear least squares: the variable projection method and its applications[END_REF]. To compute the elements of J, we need to obtain ∂Λ/∂p ji , ∀i, j [START_REF] Golub | Separable nonlinear least squares: the variable projection method and its applications[END_REF]. | 2018 | [
"info"
] | [
"491318",
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"81450",
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] | [
"1010653",
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] | 01832930 | • Visual (C)oncepts: concept of governor, concept of dependent, concepts of both
• Visual (S)patial: the normalized distance between the top-left and bottom-right corners of the governor and dependent bounding boxes, the areas of those boxes, and the ratio between the areas of the governor and dependent boxes. It is important to notice that the visual features in our study are limited to spatial information about bounding boxes and visual concepts. | 2018 | [
"info"
] | [
"527033",
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"530703"
] | [
"12660",
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] |
01744852 | , m} and m is the number of echoes. Optimization M 0 and w j can be combined into a single term α j ∈ R + without any loss of generality. | 2018 | [
"info"
] | [
"491318",
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"81450",
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] | [
"1010653",
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"1245"
] | 01744852 | Hence, we opt for an alternate optimization scheme where we iterate between optimization of {p, α} with a fixed value of B 1 and optimization for B 1 using the obtained {p, α} values. The terms Λ (p, B 1 ) and α in Eq. | 2018 | [
"info"
] | [
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] | [
"1010653",
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"1245"
] | 01184194 | The Sphinx3 tools [START_REF] Placeway | The 1996 Hub-4 Sphinx-3 system[END_REF] were used to train the phonetic acoustic models and to decode the audio signals. The MFCC (Mel Frequency Cepstral Coefficients) acoustic analysis gives 12 MFCC parameters and a logarithmic energy per frame (window of 32 ms, 10 ms shift). | 2015 | [
"info"
] | [
"420403",
"420403"
] | [
"15904"
] |
01744852 | We present a novel multi-compartment T 2 (MCT2) estimation based on variable projection, applicable to any MCT2 microstructure model. We derive this estimation for a three-gamma distribution model. | 2018 | [
"info"
] | [
"491318",
"491318",
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"81450",
"491318"
] | [
"1010653",
"14904",
"1245"
] | 01744852 | The method was finally tested on T 2 relaxometry MRI data of a MS patient. The observations from our estimation maps were compared with the pathological findings on MS lesion reported in the literature [START_REF] Lassmann | Heterogeneity of multiple sclerosis pathogenesis: Implications for diagnosis and therapy[END_REF][START_REF] Cr Guttmann | The evolution of multiple sclerosis lesions on serial MR[END_REF]. | 2018 | [
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
"14904",
"1245"
] | 01304022 | The number of a vertex v is obtained by computing the number of visited vertices during the tree traversal before the first or the second visit to v. More precisely: the vertex numbered k is the k th visited vertex such that an even number of vertices have been visited before it; it is denoted v k . An example of a run of Trav and the numbering of vertices is given in Fig. | 2016 | [
"info"
] | [
"3102",
"3102",
"3102"
] | [
"857979",
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] |
01744852 | The terms Λ (p, B 1 ) and α in Eq. ( 2) are linearly separable. | 2018 | [
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
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"1245"
] | 01744852 | The T 2 relaxation values between those of myelin and myelinated axons and the free fluids correspond to the glial cells and extracellular tissues [START_REF] Lancaster | Three-pool model of white matter[END_REF]. An ability to obtain the condition of these tissues can help us gain better insights into the onset and progress of neurodegenerative diseases such as multiple sclerosis (MS). | 2018 | [
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
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] | 01152120 | This representation using darts and pointers describes the cells of an object as well as all the incidence and adjacency relationships. If two i-cells share a common (i -1)-cell, they are adjacent (for example two volumes sharing a common face). | 2015 | [
"info"
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] | [
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01744852 | We validate our framework on synthetic data and illustrate its potential on healthy volunteer and MS patient data. INTRODUCTION
MRI voxels of the human brain are heterogeneous in terms of tissue types due to the limited imaging resolution and physical constraints. | 2018 | [
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
"14904",
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] | 01744852 | The ventricles and other regions with free fluids have a higher µ m compared to the normal appearing white matter (NAWM) tissues. This is relevant as free fluids have a higher T 2 value compared to the relatively tightly bound tissues present in NAWM. | 2018 | [
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
"14904",
"1245"
] | 00707939 | The second objective is one in which method engineering is used to produce method "on-the-fly". Situational method engineering is the construction of methods which are tuned to specific situations of development projects. | 1998 | [
"info"
] | [
"74131"
] | [
"864300"
] |
01744852 | data. The results of the synthetic data simulation are shown in Fig 1. | 2018 | [
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
"14904",
"1245"
] | 01830532 | ( 1), f j (T 2 ; p) is the chosen PDF to represent the j-th compartment with parameters p j = {p j1 , p j2 , . . | 2018 | [
"sdv",
"info"
] | [
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"81450",
"81450",
"491318"
] | [
"1010653",
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] | 01188258 | For further information, the reader is referred to the DMTF Base Metric Profile [START_REF] Merkin | Base metrics profile[END_REF]. Examples. | 2014 | [
"info"
] | [
"394761",
"394761",
"217752",
"394761"
] | [
"994068",
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] |
01744852 | EPG(•) is the stimulated echo computed at t i = i ∆TE where i = {1, . . | 2018 | [
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
"14904",
"1245"
] | 01830532 | In addition to those maps, the weight of isotropic free water (f w ) is a crucial one that could identify edema or other free water related phenomena and we therefore included it in the parameters as well. Data
All acquisitions were made on a 3T MRI scanner. | 2018 | [
"sdv",
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
"14904",
"1245"
] | 03318017 | p p , ext + (p) = ext + (p ). Algorithm 1
1 MonteCloPi algorithm 1: function MO N T ECL OPI(timeBudget) 2:
function BESTCHILD(p) 50: return argmax p ∈C(p) U CB(p, p ) C(p) is the set of children of p 51: end function
Fig. | 2021 | [
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] | [
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"413086",
"1074546",
"413086"
] | [
"182635",
"8911",
"7269",
"3878"
] |
01744852 | Most of these methods primarily focus on the MWF estimation. However, MWF alone might not be able to convey the en-tire information since it is a relative measurement. | 2018 | [
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
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"1245"
] | 01830532 | Higher number of echoes and shorter echo times for the T2 relaxometry data will facilitate MCT2 models. However, this study illustrates that even with clinical protocols, we have good detection of enhanced lesion regions using only MCT2 and MCDiff features. | 2018 | [
"sdv",
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
"14904",
"1245"
] | 04398273 | We evaluated the GEMM compiled with NVCC 10.2 and 11.3 with different levels of optimizations (O0, O1, O3, and MinRF, see Section 3.2). In fact, even for a simple code like GEMM, compiler optimizations can considerably impact the execution of the dynamic instructions. | 2024 | [
"info"
] | [
"1071247",
"43688",
"304024",
"304024"
] | [
"754557"
] |
01744852 | , m} and m is the number of echoes. Optimization M 0 and w j can be combined into a single term α j ∈ R + without any loss of generality. | 2018 | [
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
"14904",
"1245"
] | 01830532 | In the early stages, the MS lesions undergo active blood brain barrier (BBB) breakdown [START_REF] Guttmann | The evolution of multiple sclerosis lesions on serial mr[END_REF][START_REF] Lassmann | Heterogeneity of multiple sclerosis pathogenesis: Implications for diagnosis and therapy[END_REF]. Lesions in this stage are referred to as enhancing lesions and the clinical significance of its identification is well established. | 2018 | [
"sdv",
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
"14904",
"1245"
] | 01386495 | 9.Head-Gasket Seal Tester (S.Ohkawa et al. 1993 [3])
seals to verify seal strength of improved Rubber-S. | 2014 | [
"info"
] | [
"232340",
"232340",
"232340"
] | [
"991280"
] |
01744852 | , p jn } ∈ R n are the PDF parameters. In Eq. | 2018 | [
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
"14904",
"1245"
] | 01830532 | Regions of lesion undergoing active BBB breakdown has a higher water content owing to the undergoing tissue damages such as functional impairment of the morphologically intact endothelial cells [START_REF] Guttmann | The evolution of multiple sclerosis lesions on serial mr[END_REF]. Hence by the virtue of the brain tissue microstructure characteristics of MS lesions, we may identify enhancing regions in the lesion (if any). | 2018 | [
"sdv",
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
"14904",
"1245"
] | 01219317 | The chemical species dynamic transport is defined by both advection and diffusion processes, whereas the term R includes interspecies chemical reactions and emissions or absorption from sources. For more information concerning the components and the discretization of the system the reader can refer, for example to [START_REF] Bahi | Synchronous and asynchronous solution of a 3D transport model in a grid computing environment[END_REF] in which a third dimension is added to the problem, however, in this paper the 2D variant of the problem is solved. | 2012 | [
"info"
] | [
"866",
"866",
"866"
] | [
"740228"
] |
01744852 | To compute the elements of J, we need to obtain ∂Λ/∂p ji , ∀i, j [START_REF] Golub | Separable nonlinear least squares: the variable projection method and its applications[END_REF]. After solving Eq. | 2018 | [
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
"14904",
"1245"
] | 01830532 | This method is repeated 100 times to avoid any bias in sampling the data set for model training. The accuracy statistics are recorded for every repetition. | 2018 | [
"sdv",
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
"14904",
"1245"
] | 00744059 | This services table stores only the adjoining node to be contacted to reach the service. We ensure, at each instant, that there is exactly one token per connected component. | 2012 | [
"info"
] | [
"3102",
"3102",
"3102"
] | [
"4685",
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] |
01744852 | Fig. 3 . | 2018 | [
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
"14904",
"1245"
] | 01830532 | In addition to those maps, the weight of isotropic free water (f w ) is a crucial one that could identify edema or other free water related phenomena and we therefore included it in the parameters as well. Data
All acquisitions were made on a 3T MRI scanner. | 2018 | [
"sdv",
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
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] | 02987433 | METHOD
The approach we used here consists in first generating a set of Pareto-optimal points. These points are particular in the sense that they share a common specificity: they are all optimal relative to some (antagonistic) user-defined objectives. | 2009 | [
"info"
] | [
"96164"
] | [
"3909"
] |
01744852 | For example, every square millimeter of the corpus callosum in a human brain has more than 100,000 fibers (myelinated and non-myelinated) of varying diameters [START_REF] Tomasch | Size, distribution, and number of fibres in the human corpus callosum[END_REF]. These tissues can be distinguished based on their T 2 relaxation times. | 2018 | [
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
"14904",
"1245"
] | 01830532 | . }. | 2018 | [
"sdv",
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
"14904",
"1245"
] | 00643774 | A special evaluation code is an evaluation code as defined in Def. 2 where the expression mapping "ex" is realized as follows. | 2011 | [
"info"
] | [
"1150306",
"56056",
"2071",
"2438",
"88963"
] | [
"833459",
"935330"
] |
01744852 | The unknown α is substituted by Λ (p)
+ Y, where Λ (p) + is the Moore-Penrose generalized inverse of Λ (p). The VARPRO cost function is computed as:
arg min p I -Λ (p) Λ (p) + Y 2 2 (4)
where, I -Λ (p) Λ (p) + is the projector on the orthogonal complement of the column space of Λ (p). | 2018 | [
"info"
] | [
"491318",
"491318",
"81450",
"81450",
"491318"
] | [
"1010653",
"14904",
"1245"
] | 01830532 | However, this study illustrates that even with clinical protocols, we have good detection of enhanced lesion regions using only MCT2 and MCDiff features. Conclusion
We proposed a method to identify MS lesion voxels in which the brain tissues are undergoing active BBB breakdown using brain tissue microstructure information derived from advanced MRI techniques. | 2018 | [
"sdv",
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] | [
"491318",
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] | [
"1010653",
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] | 00498484 | This is particularly complicated since an element can belong to several cycles which do not have the same length. It is difficult to show the length of cycles to which belongs an element. | 2008 | [
"info"
] | [
"12959",
"82140",
"82140",
"82140"
] | [
"939",
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] |
01744852 | f (T 2 ; µ j , v j ) = T (µ 2 j /vj )-1 2 Γ µ 2 j /v j (v j /µ j ) µ 2 j v j exp -T 2 v j /µ j (5)
Hence we have, There are almost no echoes available which correspond to the high-T 2 compartment. The robustness and accuracy of the implementations to simultaneously estimate the weights and all the PDF parameters has been found to be not reliable [START_REF] Kj Layton | Modelling and estimation of multicomponent T 2 distributions[END_REF]. | 2018 | [
"info"
] | [
"491318",
"491318",
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"81450",
"491318"
] | [
"1010653",
"14904",
"1245"
] | 01830532 | The remaining (L-) and (E+) voxels are then used to evaluate the classifier performance. This method is repeated 100 times to avoid any bias in sampling the data set for model training. | 2018 | [
"sdv",
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] | [
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"491318"
] | [
"1010653",
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] | 02495231 | The 2019 revision of the World Population Prospects from the United Nations (UN) [START_REF]World population prospects 2019[END_REF] estimates that there are 7.7 billion people worldwide and that this number could grow to around 8.5 billion in 2030, 9.7 billion in 2050, and 10.9 billion in 2100. This phenomenon deserves great attention from the government as well as the general population. | 2020 | [
"info"
] | [
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] | [
"946035",
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01744885 | Valentin Laurent
email: valentin.laurent@univ-orleans.fr
Pierre Lanari
Inès Naïr
Romain Augier
Abdeltif Lahfid
Laurent Jolivet
Exhumation of eclogite and blueschist (Cyclades, Greece):Pressure-temperature evolution determined by thermobarometry and garnet quilibrium modelling
Keywords: Subduction zone, Exhumation of eclogite and blueschist, Garnet equilibrium modelling, XMAPTOOLS, Slab rollback
High-pressure rocks such as eclogite and blueschist are metamorphic markers of paleosubduction zones, and their formation at high-pressure and low-temperature conditions is relatively well understood since it has been the focus of numerous petrological investigations in the past 40 years. The tectonic mechanisms controlling their exhumation back to the surface are, however, diverse, complex and still actively debated. | 2018 | [
"sdu"
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] | [
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] | 01744885 | When considering MnO,
Accepted Article
This article is protected by copyright. All rights reserved. | 2018 | [
"sdu"
] | [
"82342",
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"524367",
"18404",
"541927"
] | [
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] | 03429159 | The observations obtained from the ceilometer show a light occurrence of cumulus above the R/V Revelle, which is consistent with the low values of simulated cloud fraction (below 5%). Over the periods of highest cloud cover i.e. | 2021 | [
"sdu"
] | [
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] | [
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01744885 | Textural analysis shows that this sample is formed by a matrix of fine-grained glaucophane and omphacite with minor rutile, Fe-oxide, white mica, epidote and albite hosting porphyroblasts of garnet, glaucophane, quartz, calcite and chlorite (Figures 4 and12). Pressure shadows are composed of quartz, phengite, epidote and glaucophane with minor albite and represent 10 vol% of the sample (Figure 12). | 2018 | [
"sdu"
] | [
"82342",
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"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01744885 | Consequently, this island has been the focus of petrological, structural and geochronological studies aimed at constraining the tectonometamorphic evolution of the CBU subduction complex (e.g. [START_REF] Cliff | Geochronological challenges posed by continuously developing tectonometamorphic systems: insights from Rb-Sr mica ages from the Cycladic Blueschist Belt, Syros (Greece)[END_REF][START_REF] Keiter | A new geological map of the Island of Syros (Aegean Sea, Greece): Implications for lithostratigraphy and structural history of the Cycladic Blueschist Unit[END_REF][START_REF] Keiter | Structural development of high-pressure metamorphic rocks on Syros island (Cyclades, Greece)[END_REF][START_REF] Lagos | High precision Lu-Hf geochronology of Eocene eclogite-facies rocks from Syros, Cyclades, Greece[END_REF][START_REF] Laurent | Strain localization in a fossilized subduction channel: Insights from the Cycladic Blueschist Unit (Syros, Greece)[END_REF][START_REF] Laurent | Extraneous argon in high-pressure metamorphic rocks: Distribution, origin and transport in the Cycladic Blueschist Unit (Greece)[END_REF][START_REF] Lister | White mica 40 Ar/ 39 Ar age spectra and the timing of multiple episodes of high-P metamorphic mineral growth in the Cycladic eclogite-blueschist belt, Syros, Aegean Sea, Greece[END_REF][START_REF] Philippon | Tectonics of the Syros blueschists (Cyclades, Greece): From subduction to Aegean extension[END_REF][START_REF] Schumacher | Glaucophane-bearing marbles on Syros, Greece[END_REF]Soukis & Stöckli, 2013;[START_REF] Tomaschek | Zircons from Syros, Cyclades, Greece -recrystallization and mobilization of zircon during high-pressure metamorphism[END_REF]Trotet, Jolivet, & Vidal, 2001a;[START_REF] Trotet | Exhumation of Syros and Sifnos metamorphic rocks (Cyclades, Greece). | 2018 | [
"sdu"
] | [
"82342",
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] | [
"773731",
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] | 03066191 | Therefore, the paired magnetic lineations (N1 and N2) reflect spatial variations in crustal magnetization associated with the record of magnetic field reversals within the oceanic crust. Two pairs of magnetic anomalies are not sufficient for a unique, unambiguous correlation with the geomagnetic polarity time scale (GPTS). | 2019 | [
"sdu"
] | [
"1005035"
] | [
"765013",
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] |
01744885 | Fast extension but little exhumation: the Vari detachment in the Cyclades, Greece. Geological Magazine,140,[245][246][247][248][249][250][251][252]. | 2018 | [
"sdu"
] | [
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] | [
"773731",
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] | 01744885 | | Geology of Syros
Located in the Cycladic Archipelago (Figure 2), Syros is mainly composed of metasedimentary and metabasite from the CBU. To the SE of the island, a large-scale klippe of Pelagonian affinity, locally referred as the Vari Unit, is also exposed, limited by the Vari detachment (Figure 3; e.g. | 2018 | [
"sdu"
] | [
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] | [
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] | 00700820 | This particular climatic regime coupled with an exceptional heavy rainfall could possibly have increased the sediment load over the minimum threshold to produce a hyperpycnite in the deep sea. We believe that the two hyperpycnites dated at 11,544±184 and 10,882±255 cal. | 2012 | [
"sdu"
] | [
"179899",
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"57190",
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] | [
"180232"
] |
01744885 | | Petrographic interpretations
Omphacite compositions suggest that this sample has reached eclogite-facies conditions. Then, it has recorded a strong retrogression as attested by the practically complete destabilisation of omphacite (+quartz) into albite. | 2018 | [
"sdu"
] | [
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] | [
"773731",
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] | 01744885 | SUPPORTING INFORMATION
Additional Supporting Information may be found online in the supporting information tab for this article. Figure S1. | 2018 | [
"sdu"
] | [
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] | [
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] | 02483085 | Current modelling was performed according to the equation ( 2) and without taking into account the effect of presence of CO 2 . The overall olivine reaction rate in the model is as follows:
R d = r A 0 V m m 0 n (4)
where R d signifies the overall reaction rate (mol.l -1 .s -1 ), r is the specific dissolution rate (mol.m -2 .s -1 ) extracted from equation ( 2), A 0 refers to
A C C E P T E D M A N U S C R I P T ACCEPTED MANUSCRIPT
the initial surface area of the solid (m 2 ), V designates the volume of solution (l), m 0 represents the initial moles of solid, and m is the moles of solid at given time. | 2017 | [
"sdu"
] | [
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] | [
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01744885 | RSCM-T are determined with a calibration-attached accuracy of 50 °C in the range 330-640 °C (Beyssac et al., 2002a). Relative uncertainties on RSCM-T obtained from samples selected within the same section are however much smaller and bracketed to 10-15 °C (e.g. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
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] | 01744885 | | Garnet equilibrium modelling
GRTMOD computations were performed on samples SY1401, SY1460, SY1407 and SY1418 using several compositions (WR and LB, Table 1) including or excluding MnO and using the JUN92.bs thermodynamic database (see the methods, section 3.3.2). The results are reported in P-T diagrams (Figure 15) with error bars that represent the uncertainty in the optimal P-T conditions resulting from the uncertainties in chemical analyses, taken as the spacing between the garnet isopleths (see Lanari et al., 2017). | 2018 | [
"sdu"
] | [
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] | [
"773731",
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] | 01054338 | Petrographic descriptions and mineral chemistry
Tidéridjaouine
Ten eclogites/garnet amphibolites were sampled and 4 were selected for detailed mineralogical and geochemical investigations. The eclogite TINZ 3 (Fig. | 2014 | [
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01744885 | Figure 17 :
17 Figure 17: P-T path of the Cycladic Blueschist Unit on Syros. a) RSCM peak temperatures and results of empirical thermobarometry. | 2018 | [
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] | [
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"176806",
"862863"
] | 01744885 | Such shape of the P-T path for early exhumation following peak P-T conditions is also retrieved on Sifnos Island [START_REF] Groppo | Glaucophane schists and associated rocks from Sifnos (Cyclades, Greece): New constraints on the P-T evolution from oxidized systems[END_REF]. Moreover, this retrograde evolution of the CBU on Syros is close to that proposed by [START_REF] Lister | White mica 40 Ar/ 39 Ar age spectra and the timing of multiple episodes of high-P metamorphic mineral growth in the Cycladic eclogite-blueschist belt, Syros, Aegean Sea, Greece[END_REF], except for their unconstrained retrograde P-T loops (Figures 1 and17). | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01427249 | f represent the remaining fraction of the initial content of vapor in the air-mass (Rayleigh distillation model) B. Same processes represented in the δ 18 O vs δ 2 H domain. | 2017 | [
"sdu"
] | [
"221836",
"477685",
"221836",
"18404",
"18404",
"179899",
"179899",
"221836",
"221836",
"79849",
"221836",
"477683",
"57629"
] | [
"765555",
"735144",
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"738286",
"831382",
"736826",
"10029"
] |
01744885 | The main structure accommodating this top-to-the NE deformation is the Vari Detachment described on Syros and Tinos and located at the roof of the CBU. [START_REF] Ring | The Hellenic subduction system: high-pressure metamorphism, exhumation, normal faulting, and large-scale extension. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01744885 | Moreover, this work highlights the powerful use of LB composition calculated from the composition of local assemblages identified on compositional maps as an approximation of reactive bulk compositions for thermodynamic modelling. Because of the local heterogeneities of metamorphic rocks and the compositional zoning of the rock-forming minerals, the measured wholerock composition is not always adapted for modelling (e.g. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 00932790 | A pseudo-depth (λ/2.5) velocity model is shown on the bottom left (Figure 5.9). This profile is used as initial model for fundamental mode inversion. | 2013 | [
"sdu"
] | [
"43221"
] | [
"770513"
] |
01744885 | The composition of white mica shows a more complex pattern with four distinct compositional groups based on the Si and Na contents (Figure 7). Within the omphacitic matrix and in the pressure-shadow, phengite shows a strong increase in celadonite from core to rim and at the contact with the garnet porphyroblast (Figure 7; phengite 1: XCel =0.35-0.45 and phengite 2: XCel =0.45- 0.65 ). | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01744885 | Local bulk compositions were generated from the oxide weight-percentage maps by averaging pixels with a density correction (Lanari & Engi, 2017). Finally, the structural formula was calculated for each pixel of the mapped area on the basis of 12 anhydrous oxygen for garnet, 11 for white mica, 12.5 for epidote, 6 for clinopyroxene, 14 for chlorite and 8 for feldspar. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01148223 | Here, soil-gas is typically sampled at the surface or in shallow depths down to 2 m. The concentration of radon gas ( 222 Rn), as a product of the radioactive decay of uranium ( 238 U) with a half-life of 3.8 days, is determined by the abundance of its mother nuclide 226 Ra, by migration and decay rate. The presence of carrier gases (CO 2 , CH 4 ) exhaled by deeper reservoirs may play a dominant role in controlling transport and redistribution of radon towards the earth's surface [START_REF] Ciotoli | The detection of concealed faults in the Ofanto Basin using the correlation between soil-gas fracture surveys[END_REF][START_REF] Etiope | Evidence for radon transport by carrier gas through faulted clays in Italy[END_REF][START_REF] Etiope | Carbon dioxide and radon geohazards over a gas-bearing fault in the Siena Graben (Central Italy)[END_REF][START_REF] Walia | Soil-gas monitoring: a tool for fault delineation studies along Hsinhua Fault (Tainan), Southern Taiwan[END_REF][START_REF] Yang | Exhalation of radon and its carrier gases in SW Taiwan[END_REF][START_REF] Yang | Variations of soil radon and thoron concentrations in a fault zone and prospective earthquakes in SW Taiwan[END_REF]. | 2012 | [
"sdu"
] | [
"234416",
"234416",
"234416",
"234416",
"109490",
"119591"
] | [
"866123",
"8354"
] |
01744885 | Annual Review[END_REF]. First, the late Cretaceous-Eocene convergence between Africa and Eurasia plates led to the formation of the Hellenides-Taurides belt. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01744885 | | METHODS
| EPMA compositional mapping
X-ray maps have been acquired to measure the compositional variability of the studied minerals at the local scale (from half a mm to a few µm) and to investigate the relationships between compositional zoning and microstructures. This technique has proved to be efficient in the characterization of compositional zoning related to P-T changes [START_REF] Kohn | Retrograde net transfer reaction insurance for pressure-temperature estimates[END_REF][START_REF] Lanari | Diachronous evolution of the alpine continental subduction wedge: evidence from P-T estimates in the Briançonnais Zone houillère (France-Western Alps)[END_REF][START_REF] Lanari | Deciphering high-pressure metamorphism in collisional context using microprobe mapping methods: Application to the Stak eclogitic massif (northwest Himalaya)[END_REF][START_REF] Loury | Late Paleozoic evolution of the South Tien Shan: Insights from P-T estimates and allanite geochronology on retrogressed eclogites (Chatkal range, Kyrgyzstan)[END_REF]. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 03181956 | The dehydration temperatures observed for a suite of amphiboles that are likely to be stable in different lithologies in the Earth's mantle ranges between 1200 to 1300 K [START_REF] Mandler | Controls on the stability and composition of amphibole in the Earth's mantle[END_REF]. We note the enhancement in the electrical conductivity is in good agreement with the dehydration-induced melting observed in amphibolites [START_REF] Wyllie | Amphibolite dehydration-melting: Sorting out the solidus[END_REF]. | 2021 | [
"sdu"
] | [
"1063727",
"1063727",
"1057450",
"1057450"
] | [
"739158",
"12848"
] |
01744885 | Figure 4 :
4 Figure 4: Thin-section pictures of typical textures and mineralogical assemblages of analysed samples for thermobarometry and thermodynamic modelling. Figure 5 :
5 Figure 5: Outcrop and sample description of SY1401 (Kampos Subunit). | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01744885 | Fast extension but little exhumation: the Vari detachment in the Cyclades, Greece. Geological Magazine,140,[245][246][247][248][249][250][251][252]. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 03276307 | Figure 3 . 3 Figure 3.13: Quito Fault recurrence models based either on seismicity (red line) or on total geodetic moment rates (black dashed lines), with a b-value=0.81 (Beauval et al. | 2020 | [
"sdu"
] | [
"1043225"
] | [
"807917"
] |
01744885 | Recently proposed (but not constrained) for the CBU on Syros by [START_REF] Lister | White mica 40 Ar/ 39 Ar age spectra and the timing of multiple episodes of high-P metamorphic mineral growth in the Cycladic eclogite-blueschist belt, Syros, Aegean Sea, Greece[END_REF], this heating phase was previously retrieved on Tinos and Andros islands [START_REF] Huet | Coupled phengite 40 Ar-39 Ar geochronology and thermobarometry: P-T-t evolution of Andros Island (Cyclades, Greece)[END_REF][START_REF] Parra | Relation between the intensity of deformation and retrogression in blueschist metapelites of Tinos Island (Greece) evidenced by chlorite-mica local equilibria[END_REF]. On Tinos, this phase was estimated at 9-10 kbar and between 400 and 550 °C, while on Andros, it was estimated at lower conditions of 7 kbar and 300-420 °C [START_REF] Huet | Coupled phengite 40 Ar-39 Ar geochronology and thermobarometry: P-T-t evolution of Andros Island (Cyclades, Greece)[END_REF][START_REF] Parra | Relation between the intensity of deformation and retrogression in blueschist metapelites of Tinos Island (Greece) evidenced by chlorite-mica local equilibria[END_REF]. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01744885 | Such variations are generally explained by the presence of an inherited component of CM (Beyssac et al., 2002a) or to the concentration of structural defects caused by pervasive deformation (see [START_REF] Aoya | Extending the applicability of the Raman carbonaceous-material geothermometer using data from contact metamorphic rocks[END_REF] for further discussions). | Empirical thermobarometry
The garnet-omphacite thermometer of [START_REF] Ravna | The garnet-clinopyroxene Fe 2+ -Mg geothermometer: an updated calibration[END_REF] was used to estimate the temperature of garnet and co-existing omphacite, whereas the pressure information was extracted from the assemblage garnet-omphacite-phengite (Waters & Martin, 1996). | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 00546961 | Figure 6 :
6 Figure 6: Results obtained from Scenario 1B -Variation in mineral concentrations around the injection well after a 300-day period of supercritical CO 2 injection (flow rate = 1 kg s -1 and T = 40 °C): (a) 10 m; (b) 1 m. Negative values correspond to dissolution and positive values to precipitation. Figure 7 :
7 Figure 7: Variation in dolomite (a) and siderite (b) concentrations 1 m from the injection well at mid-depth in the reservoir for Scenarios 1A and 1B. | 2010 | [
"sdu"
] | [
"18404",
"18404",
"18404"
] | [
"1762",
"185100"
] |
01744885 | Moreover, this work highlights the powerful use of LB composition calculated from the composition of local assemblages identified on compositional maps as an approximation of reactive bulk compositions for thermodynamic modelling. Because of the local heterogeneities of metamorphic rocks and the compositional zoning of the rock-forming minerals, the measured wholerock composition is not always adapted for modelling (e.g. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01744885 | Additionally, minimum peak metamorphic P-T conditions obtained with empirical thermobarometry (22-24 kbar for 500-560 °C and 19-21 kbar for 500-560 °C) fall in the same range of maximum P-T conditions calculated with GRTMOD (22-24 kbar and 550-580 °C, Figure 17). The retrograde path is constrained through an event of garnet growth occurring at 10-12 kbar and 500-570 °C that suggests a period of relatively isobaric heating. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 02391397 | The initial injectivity/productivity index, is far from the economically viable target. Under such conditions, several operations are considered to enhance the output of the wells, either by improving near-well permeability, or by opening hydrological connections to permeable zones not directly intersected by the well. | 2019 | [
"sdu"
] | [
"18404",
"18404",
"18404",
"18404",
"18404",
"18404",
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"18404"
] | [
"12888",
"184182",
"952004",
"3884",
"893206",
"746000",
"740603"
] |
01744885 | | Petrographic interpretations
The compositional zoning preserved in garnet, phengite and omphacite can be used in a qualitative way to reconstruct the P-T history of this sample. Several lines of evidence suggest the prograde growth of garnet under increasing pressure conditions, (1) plagioclase inclusions are only observed in the core of garnet, suggesting that the transformation of plagioclase into omphacite was not complete at the initiation of garnet growth, (2) the chemical composition of omphacite and phengite inclusions in the core of garnet have respectively lower XJd and XCel content than inclusions in the rim, which again suggests an increase in pressure during garnet growth, (3) the compositional zoning in both omphacite and phengite grains in the matrix shows a similar trend (e.g. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01744885 | In this model ~9 vol% of garnet is produced (2 vol% core and 7 vol% rim). In sample SY1407, the best defined models were obtained using the LB composition and suggest garnet growth for core, mantle and rim at lower pressure conditions of 10-12 kbar at 500-560 °C. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01281805 | The beam is discretised by a tetrahedral mesh containing 1146 nodes. The FEM calculations are performed directly on this mesh whereas Reed's computations are performed on a coarser mesh made of 288 cubic elements. | 2015 | [
"sdu"
] | [
"247127",
"247127",
"208812",
"151875"
] | [
"9211",
"9500",
"860335"
] |
01744885 | The multi-stage exhumation process of the CBU within the Hellenic subduction zone is strongly governed by slab rollback. Expanding to the general aspects of subduction zones, we suggest that such metamorphic evolution of HP-LT units, with two exhumation stages delimited by a phase of isobaric heating, should be regarded as a characteristic feature of exhumation driven by slab rollback. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01744885 | Metabasite appears pervasively retrograded under greenschist-facies conditions. However, [START_REF] Laurent | Strain localization in a fossilized subduction channel: Insights from the Cycladic Blueschist Unit (Syros, Greece)[END_REF] have shown that within metre-scale metabasite boudins, HP relicts are preserved with the occurrence of eclogite-and blueschist-facies parageneses. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 02351658 | Such observations likely indicate that the main deformation ended significantly before the synkinematic magmas reached the solid-state; i.e., before ~550 Ma. The viscosity increase during cooling in a hot orogen may also lead to a progressive decrease of the contribution of gravity-driven forces to regional deformation, so the strain regime progressively becomes dependent on far-field forces only. | 2019 | [
"sdu"
] | [
"527120",
"7119",
"527120",
"7119",
"7119"
] | [
"987856",
"180272",
"865903"
] |
01744885 | Moreover, the P-T path proposed in this study for the CBU on Syros shows interesting similarities with those previously proposed for Tinos and Andros islands [START_REF] Huet | Coupled phengite 40 Ar-39 Ar geochronology and thermobarometry: P-T-t evolution of Andros Island (Cyclades, Greece)[END_REF][START_REF] Parra | Relation between the intensity of deformation and retrogression in blueschist metapelites of Tinos Island (Greece) evidenced by chlorite-mica local equilibria[END_REF]. The main characteristic of these paths is the two-step exhumation history delimited by an isobaric phase of heating (Figure 17). | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01744885 | Slab retreat then induced large-scale back-arc extension leading to thermal re-equilibration of the lithosphere from a cold syn-orogenic regime in the subduction zone to a
Accepted Article
This article is protected by copyright. All rights reserved. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 03684928 | In other words, the validation allows us to identify the products that better close the sea level budget, given the altimetric and gravimetric missions. The validation dataset is not strictly independent, as most of the products assimilate altimetric data. | 2017 | [
"sdu"
] | [
"430037",
"413764",
"413764",
"1044077",
"441569"
] | [
"758605",
"763028",
"769517"
] |
01744885 | Relative uncertainties on RSCM-T obtained from samples selected within the same section are however much smaller and bracketed to 10-15 °C (e.g. [START_REF] Augier | Exhumation kinematics of the Cycladic Blueschists unit and backarc extension, insight from the Southern Cyclades (Sikinos and Folegandros Islands, Greece)[END_REF][START_REF] Gabalda | Thermal structure of a fossil subduction wedge in the Western Alps[END_REF][START_REF] Brovarone | Stacking and metamorphism of continuous segments of subducted lithosphere in a highpressure wedge: the example of Alpine Corsica (France)[END_REF]. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01744885 | Extension in the back-arc domain was characterized by a distributed deformation oriented N-S over a wide region covering the entire Aegean Sea, part of western Anatolia and the Rhodope Massif in the north [START_REF] Gautier | Ductile crust exhumation and extensional detachments in the central Aegean (Cyclades and Evvia Islands)[END_REF][START_REF] Jolivet | Cenozoic geodynamic evolution of the Aegean[END_REF][START_REF] Jolivet | Ductile extension and the formation of the Aegean Sea[END_REF][START_REF] Ring | The Hellenic subduction system: high-pressure metamorphism, exhumation, normal faulting, and large-scale extension. Annual Review[END_REF][START_REF] Urai | Alpine deformation on Naxos (Greece)[END_REF]. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01668914 | (iii) V2-type fluid inclusions: these consist of two-phase fluid inclusions and contain a dominant vapour phase (>80%) with a minor liquid phase. They comprise irregularly shaped fluid inclusions and range from 12 to 24 µm in size. | 2017 | [
"sdu"
] | [
"154620",
"247127",
"247127",
"247127",
"247127",
"247127",
"300825",
"247127"
] | [
"1309193",
"738600"
] |
01744885 | A JEOL JXA-8230 instrument was used at ISTerre (University of Grenoble-Alpes, France) to acquire X-ray compositional maps and spot analyses required for the analytical standardization of the maps [START_REF] De Andrade | Quantification of electron microprobe compositional maps of rock thin sections: an optimized method and examples[END_REF]. Analytical conditions for mapping were 15 keV accelerating voltage, 100 nA specimen current and 15 keV accelerating voltage and 12 nA specimen current for spot analyses. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01744885 | The white arrow shows incipient top-to-the east shear deformation. b) BSE image of the mapped area. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 03455623 | Buccally, a short, arcuate but continuous paracristid runs from the protoconid to the paraconid. The distal margin of the trigonid lacks a distinct or markedly notched protocristid because the J o u r n a l P r e -p r o o f inflated protoconid and metaconid are almost fused at their bases. | 2021 | [
"sdu"
] | [
"87313",
"541953",
"301800",
"16829"
] | [
"791843",
"746033"
] |
01744885 | | P-T evolution of the CBU
In light of our results, the shape of the P-T path of the CBU on Syros is constrained by prograde, peak and retrograde garnet growth stages, maximum RSCM temperature and peak pressure crystallization of the garnet-omphacite-phengite assemblage (Figure 17). Preservation of prograde mineral parageneses constraining the burial P-T conditions of HP-LT metamorphic rocks is rare and often preserved only in garnet cores. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01744885 | The retrograde path is constrained through an event of garnet growth occurring at 10-12 kbar and 500-570 °C that suggests a period of relatively isobaric heating. This late event is only recorded in retrogressed samples from the basal and mid-part of the CBU on Syros. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 02174597 | 400 Ma to 330 Ma, which are characterized by high εNd values related to the lithosphere of the Rheic Ocean [START_REF] Murphy | Highly depleted oceanic lithosphere in the Rheic Ocean: implications for Paleozoic reconstructions[END_REF][START_REF] Murphy | Highly depleted isotopic compositions evident in Iapetus and Rheic Ocean basalts: implications for crustal generation and preservation[END_REF]. Conclusion
Detrital zircon ages of the clastic matrix in the S 2 and3. | 2019 | [
"sdu"
] | [
"447443",
"187882",
"524367",
"447443",
"557915"
] | [
"17239"
] |
01744885 | This post-orogenic phase of exhumation is mainly accommodated by opposing-sense sets of detachment such as the North Cycladic Detachment System (NCDS, Jolivet et al., 2010), associated with syn-greenschist top-to-the NE sense of shear, or the West Cycladic Detachment System (WCDS, [START_REF] Grasemann | Miocene bivergent crustal extension in the Aegean: Evidence from the western Cyclades (Greece)[END_REF], a syn-greenschist top-to-the SW system of detachments outcropping on Serifos, Kythnos and Kea islands. Then, final exhumation stages of the CBU toward the surface were accommodated by post-metamorphic brittle deformation through low-angle and steeply dipping normal faults (e.g. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01744885 | RSCM analyses were conducted on thin sections prepared on CM-rich metasedimentary rocks cut in the structural X-Z plane. To avoid defects on the CM related to thin-section preparation, analyses were all performed below the surface of the section by focusing the laser beam beneath dominantly quartz and calcite. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 02380710 | The evolution of the frequency content of the extracted waves can be appreciated from Figure 10, where we present the Stockwell transforms of the vertical component. On the top of the figures we have plotted (the black circles) the predominant frequency (the frequency of maximum amplitude of the Transform) at each station. | 2019 | [
"sdu"
] | [
"18404",
"229915",
"221994",
"160405",
"221992"
] | [
"1000587",
"760804",
"770243"
] |
01744885 | The timing of this early growth of garnet is well constrained at 53.4 2.6 Ma [START_REF] Dragovic | Pulsed dehydration and garnet growth during subduction revealed by zoned garnet geochronology and thermodynamic modeling, Sifnos, Greece[END_REF]. Accepted Article
This article is protected by copyright. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01744885 | e) Composition of white mica defines four distinct groups in the map. f) Composition of clinopyroxene. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 04442946 | We calculated the probability of chance association between the FRB and either of the merging galaxies by using a Bayesian framework called Probabilistic Association of Transients to their Hosts (PATH; Aggarwal et al. 2021). | 2023 | [
"sdu"
] | [
"27857",
"74662"
] | [
"1347986",
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"1348049",
"1348092",
"134... |
01744885 | Here, however, we show in addition that the evolutions of the three subunits were similar during the first part of exhumation, from 22 kbar to 10 kbar and that they diverged from that point, with the lower units being heated at constant pressure before their final exhumation, a precision not attained with the methods used by [START_REF] Trotet | Exhumation of Syros and Sifnos metamorphic rocks (Cyclades, Greece). New constraints on the PT paths[END_REF]. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01744885 | On average, RSCM-T are equivalent within error in each subunit with 537 ± 20 °C in the Posidonia Subunit, 540 ± 19 °C in the Chroussa Subunit and 530 ± 17 °C in the Kampos Subunit (Table 2). Moreover, the maximum RSCM-T measured in each subunit is also equivalent within error, showing that these three subunits have experienced quite similar peak temperatures during their metamorphic history. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01333950 | DISCUSSION
FACETS appears to have performed well to map explicitly the entire outcrop. A facet-by-facet check was undertaken, which showed good agreement to within 10° of both dip and strike of digital versus compass/clino mesurements. | 2016 | [
"sdu"
] | [
"18404",
"444932",
"18404",
"18404"
] | [
"183643",
"184459",
"183560"
] |
01744885 | As the diffusion rates of the major cations in the intergranular medium are largely unknown, a qualitative approximation of the size of the equilibration volume is required. In this study, all the equilibrium models involving Gibbs free energy minimizations were computed using as reference both (1) the bulk rock composition measured by ICP-OES and (2) a local bulk composition derived from thin-section analysis and compositional maps. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01744885 | | Garnet equilibrium modelling
GRTMOD computations were performed on samples SY1401, SY1460, SY1407 and SY1418 using several compositions (WR and LB, Table 1) including or excluding MnO and using the JUN92.bs thermodynamic database (see the methods, section 3.3.2). The results are reported in P-T diagrams (Figure 15) with error bars that represent the uncertainty in the optimal P-T conditions resulting from the uncertainties in chemical analyses, taken as the spacing between the garnet isopleths (see Lanari et al., 2017). | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 03044964 | In the present work, thermal dispersion is acknowledged via the Bear-Scheidegger model [START_REF] Bear | Introduction to Modeling of Transport Phenomena in Porous Media[END_REF][START_REF] Emami-Meybodi | Dispersion-driven instability of mixed convective flow in porous media[END_REF]. This model suggests that dispersion results in greater mixing in the direction of flow than in the transverse direction. | 2020 | [
"sdu"
] | [
"199013",
"85744",
"441569"
] | [
"1151621",
"800698",
"949945"
] |
01744885 | New constraints on the PT paths[END_REF], who suggested that the P-T evolution was not the same throughout the nappe pile and that the best-preserved parts at the top had been exhumed along a colder path than the lower units. Here, however, we show in addition that the evolutions of the three subunits were similar during the first part of exhumation, from 22 kbar to 10 kbar and that they diverged from that point, with the lower units being heated at constant pressure before their final exhumation, a precision not attained with the methods used by [START_REF] Trotet | Exhumation of Syros and Sifnos metamorphic rocks (Cyclades, Greece). | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01744885 | Omphacite 1 has lower jadeite and higher diopside content (XJd =0.36-0.40 , XDi =0.35-0.38 ) than omphacite 2 (XJd =0.46-0.54 , XDi =0.27-0.32 ), and is observed in the core of the omphacite 2 in both matrix and garnet (Figure 9). The composition of glaucophane is homogeneous (XGln =0.95- 0.99 ) and only a few epidote grains are observed in the matrix with a few allanitic cores (Figure 8). | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 02106907 | (red, Andrault et al., 2011), peridotite (green, Fiquet et al., 2010;yellow, Stixrude et al., 2009), and Mg 2 SiO 4 (blue, [START_REF] Mosenfelder | Thermodynamic properties of Mg 2 SiO 4 liquid at ultra-high pressures from shock measurements to 200 GPa on forsterite and wadsleyite[END_REF]. [START_REF] Hirose | Subsolidus and melting phase relations of basaltic composition in the uppermost lower mantle[END_REF] and LH-DAC [START_REF] Andrault | Melting of subducted basalt at the core-mantle boundary[END_REF][START_REF] Hirose | The fate of subducted basaltic crust in the Earth's lower mantle[END_REF]. | 2018 | [
"sdu"
] | [
"247163"
] | [
"18141"
] |
01744885 | This late event is only recorded in retrogressed samples from the basal and mid-part of the CBU on Syros. RSCM-T estimates provide also an upper limit to the maximum amount of heating during this period. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01744885 | For the modified LB composition, the results show an excellent correlation between the predicted assemblage in equilibrium and petrographic observations with phengite, omphacite, epidote and quartz that are all observed as inclusions near the garnet rim and/or within the matrix (Figures 6 and7). Rutile is not present in the mapped area but is commonly observed as an inclusion in the rim of other porphyroblasts of the same sample. | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01427240 | Figure 8 . 8 Figure 8. | 2017 | [
"sdu"
] | [
"129675",
"129675",
"187882",
"524367",
"187882",
"524367",
"129675"
] | [
"17239"
] |
01744885 | On Syros, the timing of this first exhumation step, accommodated within the subduction channel while the overall regime was still under compression, is constrained between 50 and 35 Ma by 40 Ar/ 39 Ar and Rb/Sr ages [START_REF] Cliff | Geochronological challenges posed by continuously developing tectonometamorphic systems: insights from Rb-Sr mica ages from the Cycladic Blueschist Belt, Syros (Greece)[END_REF][START_REF] Laurent | Extraneous argon in high-pressure metamorphic rocks: Distribution, origin and transport in the Cycladic Blueschist Unit (Greece)[END_REF][START_REF] Lister | White mica 40 Ar/ 39 Ar age spectra and the timing of multiple episodes of high-P metamorphic mineral growth in the Cycladic eclogite-blueschist belt, Syros, Aegean Sea, Greece[END_REF]. Syn-orogenic exhumation kinematic indicators are well exposed on Syros, Sifnos and Tinos, showing a clear top-to-the E/NE sense of shear observed in preserved HP rocks [START_REF] Gautier | Ductile crust exhumation and extensional detachments in the central Aegean (Cyclades and Evvia Islands)[END_REF][START_REF] Jolivet | Ductile extension and the formation of the Aegean Sea[END_REF][START_REF] Laurent | Strain localization in a fossilized subduction channel: Insights from the Cycladic Blueschist Unit (Syros, Greece)[END_REF][START_REF] Philippon | Tectonics of the Syros blueschists (Cyclades, Greece): From subduction to Aegean extension[END_REF][START_REF] Roche | Anatomy of the Cycladic Blueschist Unit on Sifnos Island (Cyclades, Greece)[END_REF]Trotet et al., 2001a). | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01744885 | This outcrop corresponds to the contact zone between the Kampos and Chroussa subunits, which is interpreted as an extensional top-to-the east shear zone, namely the Kastri Shear Zone (see Laurent et al., 2016 for details). Well-preserved eclogite shows a weak deformation and still exhibits the original structure of a pillow-lava breccia (Figure 5b-d). | 2018 | [
"sdu"
] | [
"82342",
"187882",
"524367",
"18404",
"541927"
] | [
"773731",
"176806",
"862863"
] | 01677325 | It is convenient to express the weak-photon three-momentum in cylindrical coordinates x = (r, φ w , z). Then, only the distribution function f w depends on the angle φ w , which allows a direct integration defining the function ( see also (4.122))
F w (r, µ) = 2π φw=0 f w r, φ w , z(r 2 , µ) dφ w , (4.38)
where z(r 2 , µ) is defined in equation (4.119) by
z(r 2 , µ) = k 4 r 2 µk max -4µ max k . | 2017 | [
"sdu"
] | [
"157"
] | [
"17570"
] |
01744978 | By construction, since E 0 has no positive atoms in its body, I@p = ;. By transparency of P , ↵.e is also a minimum p-faithful run of P on ; in which all events but e are invisible at p, and ↵.e(;)@p = ↵.e(I)@p = E 0 (;). | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | However, we show how the violating runs can be filtered out. Definition 6.5. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01094051 | . . | 2014 | [
"info"
] | [
"162175",
"105160",
"56663",
"93591",
"81173"
] | [
"962307",
"4078",
"962308"
] |
01744978 | Blockchain technology provides an alternative to such a central authority. It is, in spirit, an excellent match with collaborative workflows. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | Now suppose a literal ¬R@q(x, u) occurs in the body of some rule r of P . First, an instantiation ⌫ of this rule may hold because ¬Key R@q (⌫(x)) holds. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01076465 | INTRODUCTION
Sixty years ago, Shannon [START_REF] Shannon | A Mathematical Theory of Communication[END_REF] provided a mathematical framework to analyze fundamental limits of information transfer in the case of single-input single-output channels. He introduced the channel capacity as the maximum rate at which information can be reliably transmitted. | 2008 | [
"info"
] | [
"123689",
"58436",
"2465"
] | [
"170874",
"960958",
"863308",
"960959"
] |
01744978 | We show that computing minimal scenarios for a peer is generally hard (coNP-complete). Moreover, despite being observationally equivalent to the original run, scenarios can be misleading by di↵ering considerably from what occurs in the actual run. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | It is adapted to our context to take into account the view relations for keys. A term is a variable or a constant. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01806054 | On the contrary, automatic evaluation is able to run continuously and can provide results when needed. We are aware that some important services or dependencies can be discovered only during exceptional operations or back-up servers become active only after failure of the main one. | 2017 | [
"info"
] | [
"412450",
"412450"
] | [
"1032616",
"994058"
] |
01744978 | Furthermore, we impose the following (losslessness) condition: For each
I 2 Inst K (D) and R 2 D, I(R) = chase K ⇣ [ {(I@p(R@p)) ? | p 2 P, R@p 2 D@p}
⌘
The losslessness property guarantees that for each tuple in I(R), and each A in R, the value of the tuple for A is visible at some peer. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | The operator T p (⇢, •) is additive: for all subsequences ↵ 1 , ↵ 2 of e(⇢), T p (⇢, ↵ 1 +↵ 2 ) = T p (⇢, ↵ 1 )+ T p (⇢, ↵ 2 ). We now turn to the proof of the theorem. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01587979 | 0 K n r , M dyn tot = M 1 r 0 . . | 2018 | [
"info"
] | [
"473973",
"481386",
"500495"
] | [
"16179",
"17099"
] |
01744978 | Since k 2 K 1,2 , t 00 2 I 0 2 (R) and so t 0 2 e 2 (I 0 2 )(R) and t 2 e 2 (I 0
2 )@p(R@p). We have shown that e 1 (I 0 1 )@p ✓ e 2 (I 0
2 )@p. The converse holds by symmetry, so e 1 (I 0 1 )@p = e 2 (I 0
2 )@p. Also, adom(e 2 (I 0 2 )) \ new(↵) = ;. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | It is easy to see that the program in the example is not transparent for Sue. Intuitively, this is because the relation cfoOK carries information that Sue does not see, yet it impacts Sue's view of the workflow. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01891764 | Grid reflectivity data is then transformed to a 2D intensity image to which a line detection using a Hough Transform [START_REF] Duda | Use of the Hough transformation to detect lines and curves in pictures[END_REF] is applied for lane markings detection. We chose the polar representation (r, θ) of lines as it is relevant for localization. | 2018 | [
"info"
] | [
"454685",
"133641",
"454685",
"133641",
"133641"
] | [
"20861"
] |
01744978 | As an added benefit, the view program rules provide provenance information for the updates observed by the peer. INTRODUCTION
Consider peers participating in a collaborative workflow. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | Definition 4.4. Let ⇢ = {(e i , I i )} 0in be a run of P and p a fixed peer. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01679828 | 4 Fig. 4. | 2017 | [
"info"
] | [
"32772",
"72398",
"32772"
] | [
"1026415",
"1026416",
"1026417"
] |
01744978 | Thus, E 0 (;) = I 0 . If E 0 is an event of p then the statment holds. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | ( †) For all instances I 1 , I 2 and events e 1 , e 2 such that e i is applicable at I i and visible at p (i = 1, 2) and e 1 (I 1 )@p = e 2 (I 2 )@p, and for each sequence ↵ of events such that adom(e 2 (I 2 )) \ new(↵) = ;, if ↵ is a minimum p-faithful run on e 1 (I 1 ) such that all its events but the last are silent at p, then the same holds on e 2 (I 2 ), and ↵(e 1 (I 1 ))@p = ↵(e 2 (I 2 ))@p. We show that ( † 0 ): ( †) holds i↵ it holds for all instances I 0 1 , I 0 2 such that, for each relation R, I 0 i (R) contains at most c|↵|+2 tuples. For suppose this holds. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 00795994 | add diversity) in the system, so it is harder for the attacker to understand typical behaviors. There has been a large body of research propose to introduce diversity in the form of randomization at different abstraction levels (in memory locations, compiler, program execution) [START_REF] Caballero | Would diversity really increase the robustness of the routing infrastructure against software defects? | 2009 | [
"info"
] | [
"17973",
"135817",
"135817",
"17973",
"135817",
"2466"
] | [
"5597"
] |
01744978 | The existence of counterexamples can be easily checked by a nondeterministic pspace algorithm. This completes the proof. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | This completes the base of the induction. For the induction step, let 0 < j < n suppose there is a run ⇢ j of P such that ⇢ j @p ⇠ ⇢ p | j . | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01367791 | First, we estimate the undressed human body shape in motion for the given sequence. This step reduces significantly the search space of the problem by providing a good First, a statistical model of undressed body shape is fitted to the frame (c). | 2016 | [
"info"
] | [
"1042488",
"467202",
"1042488",
"1042488",
"1042488",
"1042488"
] | [
"9473",
"554",
"4428",
"3317"
] |
01744978 | Observe also that a peer can delete only a tuple the peer sees, and that, if an insertion succeeds, the tuple the peer inserted is part of its view after the update (by (ii)). Some subtleties of updates are illustrated next. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | Consider the run ⇢ consisting of the following events: e: +ok@cto :f : ok@cto :g: +ok@ceo :h: +approval@assistant :-ok@assistant
The subrun e h is a scenario of ⇢ at peer applicant. It indicates that the applicant's request was approved because it was ok'd by the cto. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01785362 | This makes the process very time consuming and tedious to perform over the entire LOD. Therefore, as an illustration, we ran the instance matching tool on two flagship examples of false positive D T s:
Semantically Similar Labels: We choose education-data-gov-uk 17 as a D S and its corresponding false positive D T oxpoints 18 . | 2016 | [
"info"
] | [
"181"
] | [
"795352"
] |
01744978 | This completes the proof. 2
Proof of Theorem 5.11 Clearly, (ii) follows from (i) and Theorem 5.10. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | (This does not prevent them from performing arbitrarily long sequences of events irrelevant to that particular peer.) We show that one can decide whether, for a given h, a workflow program only produces transparent and hbounded runs for a particular peer. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 03976435 | Here, the Y axis gives us the information that statement 2 is inside an "else" branch, labelled by its condition [START_REF] Pea | Language-Independent Conceptual "Bugs" in Novice Programming[END_REF], which is in inside a while loop (1), itself inside the highest level "Repeat" loop. The X axis give a temporal information. | 2005 | [
"info"
] | [
"24191",
"24191",
"24191"
] | [
"829581",
"829582",
"957637"
] |
01744978 | An insertion atom at p is of the form +R@p(x) where R@p 2 D@p and x is a tuple of variables and constants, of appropriate arity. A deletion atom p is an expression Key R@p (x), where R@p 2 D@p and x is a variable or constant. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | It is transparent and, by h-boundedness, its length is less or equal to h. We can therefore extend the events of P to transparent events of P t to capture the events in ↵ 0 i . Because its length is less that h, we dispose of enough space in the B i . | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 00589734 | Fig. 1 Fig. | 2009 | [
"info"
] | [
"396897",
"396897"
] | [
"4158",
"9956"
] |
01744978 | , A = a and A = B are elementary conditions. A condition is a Boolean combination of elementary conditions. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | Now suppose that a new event e arrives. We need to compute the following (where ⇢.e denotes the concatenation of ⇢ and e):
(i) T ! | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 03445794 | Generic Bootloader
To realize the PoC, we decided to implement additional blocks over the base codes of FreeRTOS. Then, a simple and generic bootloader that manages also the firmware updates was implemented. | 2022 | [
"info"
] | [
"95837",
"204598"
] | [
"21917"
] |
01744978 | Intuitively, T ! p (⇢, f ) represents an "explanation" of the individual event f by a minimal boundary and modification pfaithful subrun of ⇢ containing f . | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | Note that, in order to enable powerful static analysis, the views in [START_REF] Abiteboul | Collaborative data-driven workflows: think global, act local[END_REF] did not use selections. The more powerful views used here better capture realistic peer views. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 02071914 | And quadgrams are four-term strings: "your destination is 3", "destination is 3 miles", and "is 3 miles away". In our experiment, we use unigrams, bigrams, trigrams, and quadgrams to calculate the correlated TF and TFIDF features. | 2019 | [
"info"
] | [
"556026",
"556027"
] | [
"1044253",
"1044254"
] |
01744978 | Proof. Straightforward induction on the length of ↵. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | It is easy to show: Theorem 5.9. It is undecidable, given a program P and peer p, (i) whether P is transparent for p, and (ii) whether there exists h such that P is h-bounded for p.
Proof. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01652785 | [x = l] l → v} GET {l → v} (get l) {λ x. [x = v] l → v} SET {l → v } (set (l, v)) {λ x. l → v}
Fig. | 2019 | [
"info"
] | [
"233382",
"2544",
"454413",
"568599"
] | [
"170232",
"878"
] |
01744978 | The pspace upper bound follows from the fact that ch+1 is polynomial in h and P , which yields a non-deterministic pspace test. This completes the proof. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | Let R@q(k, u) occur in the body of e i h+1 . Then i h belongs to an R-lifecycle of k in ⇢, and, by modification faithfulness, all prior events of the Rlifecycle that a↵ect attributes in att(R, q) of tuples with key k are included in ↵. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 02959460 | Table 3: PER/CER in the semi-supervised setting. A pretrained CPC system plus a linear classifier trained on limited amounts of labels compared to the same system trained from scratch (PER). | 2020 | [
"info"
] | [
"267305",
"267305",
"267305",
"267305",
"267305",
"267305",
"505215",
"1316",
"267305",
"267305",
"267305",
"267305",
"267305",
"267305",
"267305",
"505215",
"1316"
] | [
"1009057",
"915272",
"1027061",
"757939"
] |
01744978 | We denote the sequence of attributes of R by att(R). A database schema is a finite set of relation schemas. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | As discussed earlier, condition (C1) is meant to guarantee that a peer knows when it is performing an event visible at p, which enables maintaining the relation Stage. (C3') is a natural condition that essentially comes down to preventing the "reuse" of a key after it has been deleted. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 00564443 | There exist in the literature some works relating to the RCPSP/CPR. Among others, we can cite Neumann and Schwindt [START_REF] Neumann | Project scheduling with inventory constraints[END_REF] who formalize the problem of project scheduling with inventory constraints and generalized precedence constraints, including both renewable and storage resources. | 2013 | [
"info"
] | [
"95464",
"388570",
"388570",
"391256"
] | [
"15435",
"262",
"6370"
] |
01744978 | We next introduce the notion of "p-faithful subrun of ⇢", that prevents the kinds of anomalies previously illustrated. First, the definition is driven by the intuition that tuples in a given relation with a fixed key k represent evolving objects in the workflow. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | Proof of Theorem 3.4 Membership in coNP is immediate. For hardness, we reduce the problem of testing unsatisfiability of a Boolean formula to testing whether a scenario for some peer p is minimal. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 02182477 | 9. It is seen how the color diversity changes according to the number of GCL in the model. | 2019 | [
"info"
] | [
"206",
"206",
"27997",
"27997",
"206"
] | [
"4198",
"6956",
"858",
"6795"
] |
01744978 | Consider a run that derives OK. Suppose the run starts with V 1 @q :-; C 5 @q :-V 1 @q ; V 2 @q :-; C 5 @q :-V 2 @q. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | For (a), we need to show that e i h+1 is applicable in I 0 h . Let R@q(k, u) occur in the body of e i h+1 . | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01236355 | For a pair of events a, b ∈ E, the event a causally precedes the event b if the following condition is satisfied:
a → b if V C i (a) < V C j (b)
D. Immediate Dependency Relation (IDR)
The IDR is the transitive reduction of the HBR [START_REF] Pomares-Hernandez | The Immediate Dependency Relation: An Optimal Way to Ensure Causal Group Communication[END_REF]. It is denoted by "↓", and it is defined as follows:
Definition 5. | 2015 | [
"info"
] | [
"23285",
"388540",
"388967",
"23285"
] | [
"6138",
"921684"
] |
01744978 | In addition, there is a peer p that sees the projection of R on K with the selection p = (A q = 1) ^( _ ' ) where = ^x2X (A x = 1), and ' checks that the formula ' is true for the valuation ⌫ of X such that ⌫(x) = true i↵ A
x = 1. The program consists of all ground rules of the form r xi : +R@p xi (0, 1) :-(for each x i 2 X) e :
+R@q(0, 1) :-Consider the run ⇢ consisting of r x1 . | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | RELATED WORK
A survey on data-centric business process management is provided in [START_REF] Hull | Data management perspectives on business process management: tutorial overview[END_REF], and surveys on formal analysis of data centric workflows are presented in [START_REF] Calvanese | Foundations of data-aware process analysis: a database theory perspective[END_REF][START_REF] Deutsch | Automatic verification of database-centric systems[END_REF]. Although not focused explicitly on workflows, Dedalus [START_REF] Alvaro | Dedalus: Datalog in time and space[END_REF][START_REF] Hellerstein | The declarative imperative: experiences and conjectures in distributed logic[END_REF] and Webdamlog [START_REF] Abiteboul | A rule-based language for web data management[END_REF][START_REF] Abiteboul | Viewing the web as a distributed knowledge base[END_REF] are systems supporting distributed data processing based on condition/action rules. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01758206 | The classification results obtained with this framework were in line with the state of the art and highlighted that the atlases used for region-based approaches should be chosen with care. The code will be made publicly available at the time of the conference at https://github.com/aramis-lab/AD-ML . | 2018 | [
"info"
] | [
"542032",
"542032",
"542032",
"542032",
"542032",
"542029",
"542032",
"542032",
"353778",
"542032"
] | [
"1030165",
"1015113",
"18837",
"14646",
"739344",
"10949"
] |
01744978 | Suppose that p also sees the propositions
Definition 4 . 3 . | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | Condition (C1) is natural in many applications where peers are doing some computations about a peer p, for which transparency is desired. For instance, p may be a customer, a job applicant, a participant in a crowdsourcing application, etc. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 00374648 | A simulator that would use the semantics of time as described in Z.100, would not be able to make any assumption on the way time progresses, and therefore many unrealistic executions will be present in the resulting graph. As a result, the simulator would not guarantee elementary properties like when a timer expires, it will be consumed by the concerned process in a reasonable amount of time (whatever the notion of reasonable is). | 2001 | [
"info"
] | [
"194",
"194",
"194",
"91068",
"91068",
"2545"
] | [
"1084328",
"171281",
"735145"
] |
01744978 | The first essentially says that various properties of sequences of events are invariant under isomorphism. Lemma A.2. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | Each program obtained using the aforementioned guidelines is transparent and h-bounded for p.
Boundedness by acyclicity. We next show how to guarantee boundedness for a certain class of programs using an acyclicity condition. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01349524 | Finally, we showcase results through the example of embedding audio processing in the Antescofo score of Anthèmes 2. REAL-TIME COORDINATION OF MUSICAL EVENTS AND COMPUTING ACTIONS 2.1 A Paradigmatic Example
As an illustration, we showcase a mixed music piece that has entered the repertoire, Anthèmes 2 (1997) by Pierre Boulez for violin and live electronics. | 2016 | [
"info"
] | [
"247362",
"410617",
"454664",
"1374",
"410617",
"454664",
"1374",
"410617",
"454664",
"1374",
"252664",
"248359"
] | [
"4485",
"2943",
"6067",
"989897",
"882828"
] |
01744978 | When an update +Q(u, b 1 , ..., b h ) is performed, its set of non-? B i 's is set to the concatenation of all distinct non-? | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | that insert or delete up to M arbitrary tuples in relations of D@p, where M is the maximum number of updates in the head of a rule in P ). Clearly, these are of little interest. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 00591066 | This creates complicated debugging scenarios when problems, especially transient ones occur. Using the current approach, the time required to distribute a component will depend not on the size of the component, but on its structure. | 2011 | [
"info"
] | [
"24471",
"25697"
] | [
"16377",
"3314"
] |
01744978 | Acknowledgment. Serge Abiteboul and Pierre Bourhis are supported by the ANR Project Headwork, ANR-16-CE23-0015, 2016-2021. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | We will use the notion of step-provenance of a fact, i.e. the set of step ids in that stage that contribute to deriving the fact. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 00399472 | When the Viterbi state-space (L) is sufficient, the performance is optimum in the error rate sense. M c k (n) = Re d * k (n + ν k ) • 2ψ k (n + ν k ) - l d l (n + ν l ) • e j2π∆f kl (n+ν l )Ts s kl (ν k -ν l ) - (9) 2 l p p>0 d l (n + ν l -p) • e j2π∆f kl (n+ν l -p)Ts s kl (p + ν k -ν l ) 0 5 10 15 10 -4 10 -3 10 -2 10
Figure 4 shows the average BER versus the carrier spacing. | 2007 | [
"info"
] | [
"2372",
"2372",
"2372",
"2545",
"16294"
] | [
"933376",
"185026",
"2507",
"836659"
] |
01744978 | Scenarios are considered in Section 3, faithfulness in Section 4, transparency and view programs in Section 5, and design methodology for transparent and bounded programs in Section 6. Related work and conclusions are considered in two last sections. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | Otherwise,
T ! p (⇢.e, f ) = T ! | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 03008405 | The current results are still restrictive in the programs that can be expressed and the rigidity of its properties; however, we believe that we have a minimal and reliable basis for further studies. In the future, we plan to introduce more dynamic trees for example using linearity and borrowing types, but also primitive to attach and detach tree to the object dependence graph, in order to constantly ensure a tree structure, but allow the structure of the tree to evolve at runtime. | 2020 | [
"info"
] | [
"528454",
"50791",
"556832"
] | [
"595"
] |
01744978 | Achieving this requires a more careful approach, in which the "steps" in each stage are identified by ids consisting of fresh values. More precisely, each event within the stage ↵.e 0 is called a step, and is identified by a step id. | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01744978 | Now suppose there is a tuple t 00 with key k in I 2 (R). Since k 2 K 1,2 , t 00 2 I 0 2 (R) and so t 0 2 e 2 (I 0 2 )(R) and t 2 e 2 (I 0
2 )@p(R@p). | 2018 | [
"info"
] | [
"478610",
"432644",
"26818"
] | [
"749231",
"964789"
] | 01391281 | This would allow for richer interaction techniques leveraging the direct manipulation of many robots at once. Another technical limitation of our system is its use of an external projector for tracking. | 2016 | [
"info"
] | [
"92966",
"56039",
"42193",
"42193",
"56039",
"56039",
"42193"
] | [
"8723",
"10778"
] |
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