task stringclasses 2
values | instruction stringclasses 2
values | input stringlengths 461 1.8k | draft_output stringlengths 44 774 | review_status stringclasses 1
value | notes stringclasses 1
value |
|---|---|---|---|---|---|
keywords | Extract the 8 most important technical keywords from the passage. | uorescence at the specific lines highlighted in (b).(d) Histograms of the EMCCD photoelectron
counts from individual Cs and Rb sites over 5000 loading shots. The individual Cs and Rb sites are highlighted
in (c). The two peaks correspond to the measured intensity from sites with zero atoms, and sites with one atom.
Ato... | atoms, fluorescence, sites, light, emccd, two, one, atom | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | in sustaining coherent behavior, they are as long as 25 mm but have an inner diameter less than 20 nm, with
separations between tubules on the order of 20 nm. Unlike isolated atomic systems, it is difficult to justify the
Markovian approximations under these circumstances. The Born approximations assume the system-
... | in sustaining coherent behavior, they are as long as 25 mm but have an inner diameter less than 20 nm, with
separations between tubules on the order of 20 nm. Unlike isolated atomic systems, it is difficult to justify the
Markovian approximations under these circumstances. The Born approximations assume the system-
... | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 7
2.2 Elementary lemmas . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 8
2.3 Main ideas . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 9
3 Trotter type algorithms and error representations 10
3.1 The standard and gen... | 9
3 Trotter type algorithms and error representations 10
3.1 The standard and generalized Trotter formulae . 10
3.2 Error representations . 10
4 Operator norm error bounds 12
5 Vector norm error bounds 14
6 Application to Schr¨ odinger equation with time-dependent effective mass and fre-
quency 19
Accepted in Quantum 20... | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | ve broadcast and other fundamental problems, such as spanning tree
construction, MST, and BFS, with significantly less communication cost (com-
pared tom, the number of edges) inarbitrary networksusing the power ofquan-
tum communication?
Quantum communication advantage.The recent work of [DMP25] gave a partial answer ... | message, complexity, communication, quantum, they, leader, bound, election | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | usly , they were tackled by means of SOS
matrices and Lemma 4.37. In the dual approach, write the matrix𝐺 ∈ ℝ 𝑚×𝑚[𝒙]in
the matrix constraint𝐺 ⪰ 0 in terms of a finite family{𝛤𝒌}𝒌 ⊂ ℝ 𝑚×𝑚 of symmetric
matrices:𝐺 = ∑𝒌 𝛤𝒌𝒙𝒌. The corresponding localizing (block) matrix𝑀𝑑(𝐺𝒚)is then
𝑀𝑑(𝐺𝒚)𝒊,𝒋 ≔ ∑
�... | matrix, matrices, complex-valued, one, moment, lemma, localizing, problems | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | e target cell must be moved W horizontal
cells and H vertical cells. Then, the total steps are roughly
W + H + 6min(W, H) + 5 |W − H| beats ignoring a small
constant. This takes 7√n beats in the worst case, i.e., W =√n, H = √n/2.
When one logical cell is loaded from the point SAM, there
are two empty cells in the SAM r... | e target cell must be moved W horizontal
cells and H vertical cells. Then, the total steps are roughly
W + H + 6min(W, H) + 5 |W − H| beats ignoring a small
constant. This takes 7√n beats in the worst case, i.e., W =√n, H = √n/2. | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | ∼
1/Q(v/c)2, whereQ∼ω 0/δωis the Q-factor of ring res-
onators.
To implement parallel optical computations in fre-
quency band, the width of the involved spectral lines
should be much less than the distance between them in
the frequency band. Thus, the value ofQis restricted
by the conditionδω≪∆ω=ω 02v/c. Letv/c∼10 −5.... | ∼
1/Q(v/c)2, whereQ∼ω 0/δωis the Q-factor of ring res-
onators. To implement parallel optical computations in fre-
quency band, the width of the involved spectral lines
should be much less than the distance between them in
the frequency band. Thus, the value ofQis restricted
by the conditionδω≪∆ω=ω 02v/c. | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | finite dimensions, the left action l(a) = a⊗ IB and the right action is r(b) = IA⊗ b. We
have a cyclic and separating vector |ΩΦ⟩ forA∨B and
⟨ΩΦ|l(a)|ΩΦ⟩ = ρB◦ Φ(a), ⟨ΩΦ|r(b)|ΩΦ⟩ = ρB(b) . (B.70)
Here, ρB is the state before the quantum channel and ρB◦ Φ is the state after the channel
[44]. Modular theory can be general... | map, state, hilbert, decodable, action, cyclic, separating, quantum | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | nes
show the analytical approximation of the minimum energy
gap derived in Eq.(D63). The green dotted lines show the
analytic approximation E±
n − E±
n+1 = 4ϵ2.
5. Minimum energy gap
We can approximate the minimum energy gap by
differentiating the approximate quantization condition
Eq. (D45) with respect to n at a = 0.... | energy, minimum, gap, show, approximation, d63, approximate, gives | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | elderly care systems, and smart technology
for healthy longevity. Dr. Chen is a Board Member of the Taiwan Association
of Integrated Care and Chair of the Asia Working Group for Sarcopenia. He
was an Advisor to various committees in central and local governments and
contributed to global forums on age-friendly policy a... | optical, taiwan, national, university, care, medicine, degree, biomedical | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | uorescence at the specific lines highlighted in (b).(d) Histograms of the EMCCD photoelectron
counts from individual Cs and Rb sites over 5000 loading shots. The individual Cs and Rb sites are highlighted
in (c). The two peaks correspond to the measured intensity from sites with zero atoms, and sites with one atom.
Ato... | atoms, fluorescence, sites, light, emccd, two, one, atom | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | in sustaining coherent behavior, they are as long as 25 mm but have an inner diameter less than 20 nm, with
separations between tubules on the order of 20 nm. Unlike isolated atomic systems, it is difficult to justify the
Markovian approximations under these circumstances. The Born approximations assume the system-
... | in sustaining coherent behavior, they are as long as 25 mm but have an inner diameter less than 20 nm, with
separations between tubules on the order of 20 nm. Unlike isolated atomic systems, it is difficult to justify the
Markovian approximations under these circumstances. The Born approximations assume the system-
... | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 7
2.2 Elementary lemmas . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 8
2.3 Main ideas . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 9
3 Trotter type algorithms and error representations 10
3.1 The standard and gen... | 9
3 Trotter type algorithms and error representations 10
3.1 The standard and generalized Trotter formulae . 10
3.2 Error representations . 10
4 Operator norm error bounds 12
5 Vector norm error bounds 14
6 Application to Schr¨ odinger equation with time-dependent effective mass and fre-
quency 19
Accepted in Quantum 20... | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | ve broadcast and other fundamental problems, such as spanning tree
construction, MST, and BFS, with significantly less communication cost (com-
pared tom, the number of edges) inarbitrary networksusing the power ofquan-
tum communication?
Quantum communication advantage.The recent work of [DMP25] gave a partial answer ... | message, complexity, communication, quantum, they, leader, bound, election | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | usly , they were tackled by means of SOS
matrices and Lemma 4.37. In the dual approach, write the matrix𝐺 ∈ ℝ 𝑚×𝑚[𝒙]in
the matrix constraint𝐺 ⪰ 0 in terms of a finite family{𝛤𝒌}𝒌 ⊂ ℝ 𝑚×𝑚 of symmetric
matrices:𝐺 = ∑𝒌 𝛤𝒌𝒙𝒌. The corresponding localizing (block) matrix𝑀𝑑(𝐺𝒚)is then
𝑀𝑑(𝐺𝒚)𝒊,𝒋 ≔ ∑
�... | matrix, matrices, complex-valued, one, moment, lemma, localizing, problems | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | e target cell must be moved W horizontal
cells and H vertical cells. Then, the total steps are roughly
W + H + 6min(W, H) + 5 |W − H| beats ignoring a small
constant. This takes 7√n beats in the worst case, i.e., W =√n, H = √n/2.
When one logical cell is loaded from the point SAM, there
are two empty cells in the SAM r... | e target cell must be moved W horizontal
cells and H vertical cells. Then, the total steps are roughly
W + H + 6min(W, H) + 5 |W − H| beats ignoring a small
constant. This takes 7√n beats in the worst case, i.e., W =√n, H = √n/2. | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | ∼
1/Q(v/c)2, whereQ∼ω 0/δωis the Q-factor of ring res-
onators.
To implement parallel optical computations in fre-
quency band, the width of the involved spectral lines
should be much less than the distance between them in
the frequency band. Thus, the value ofQis restricted
by the conditionδω≪∆ω=ω 02v/c. Letv/c∼10 −5.... | ∼
1/Q(v/c)2, whereQ∼ω 0/δωis the Q-factor of ring res-
onators. To implement parallel optical computations in fre-
quency band, the width of the involved spectral lines
should be much less than the distance between them in
the frequency band. Thus, the value ofQis restricted
by the conditionδω≪∆ω=ω 02v/c. | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | finite dimensions, the left action l(a) = a⊗ IB and the right action is r(b) = IA⊗ b. We
have a cyclic and separating vector |ΩΦ⟩ forA∨B and
⟨ΩΦ|l(a)|ΩΦ⟩ = ρB◦ Φ(a), ⟨ΩΦ|r(b)|ΩΦ⟩ = ρB(b) . (B.70)
Here, ρB is the state before the quantum channel and ρB◦ Φ is the state after the channel
[44]. Modular theory can be general... | map, state, hilbert, decodable, action, cyclic, separating, quantum | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | nes
show the analytical approximation of the minimum energy
gap derived in Eq.(D63). The green dotted lines show the
analytic approximation E±
n − E±
n+1 = 4ϵ2.
5. Minimum energy gap
We can approximate the minimum energy gap by
differentiating the approximate quantization condition
Eq. (D45) with respect to n at a = 0.... | energy, minimum, gap, show, approximation, d63, approximate, gives | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | elderly care systems, and smart technology
for healthy longevity. Dr. Chen is a Board Member of the Taiwan Association
of Integrated Care and Chair of the Asia Working Group for Sarcopenia. He
was an Advisor to various committees in central and local governments and
contributed to global forums on age-friendly policy a... | optical, taiwan, national, university, care, medicine, degree, biomedical | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | ach
could potentially allow for multiple uses (recycling) of the
single-issued quantum token, while still benefiting from
the information-theoretic protection provided by quan-
tum mechanics.
In the existing literature, the concept of quantum
tokens appears under different names, such as quan-
tum money [1, 19, 20], qu... | quantum, quan-, tum, classical, relies, s-money, token, tokens | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | n photon number ns is ϕ Kerr = 2 χtn s = 0 . 16.
(a) ns = 4 (low energy, strong nonlinearity χt = 0 . 02). (b) ns = 20 (higher energy,
weaker nonlinearity χt = 0 . 004). (c) Wigner negativity volume versus loss after the
Kerr interaction: orange curve for case (a), blue curve for case (b).
state with higher non-lineari... | n photon number ns is ϕ Kerr = 2 χtn s = 0 . (a) ns = 4 (low energy, strong nonlinearity χt = 0 . (b) ns = 20 (higher energy,
weaker nonlinearity χt = 0 . | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | points represent simulations for idealπpulses, while the red points show
simulated results obtained using the realisticπpulses employed in our experiment. The black dashed lines indicate linear fits,
with the scaling exponents being 1.00 (a), 2.00 (b), 1.00 (c), and 2.00 (d), respectively.
which yield
(OB − ⟨OB⟩)|ψ 0⟩=... | points represent simulations for idealπpulses, while the red points show
simulated results obtained using the realisticπpulses employed in our experiment. The black dashed lines indicate linear fits,
with the scaling exponents being 1.00 (a), 2.00 (b), 1.00 (c), and 2.00 (d), respectively. which yield
(OB − ⟨OB⟩)|ψ 0⟩=... | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | riments, and point out key differences with
respect to the non-interacting case. The momentum dis-
tribution Πt(k) of the system is the Fourier transform of
the one-body reduced density matrix (OBRDM) ρt(x, y),
Πt(k) = 1
2π
∫ 2π
0
dx
∫ 2π
0
dy eik(x−y)ρt(x, y), (8)
with the momentum (in unit of ¯ k) k ∈ Z due to the
per... | momentum, distribution, non-interacting, case, system, obrdm, reads, localized | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | sion has been quantified by exact
complementarity relations, which we have derived both for specific and general initial states. These relations establish
that initial coherence is not merely beneficial but is a necessary resource for entanglement generation; its absence
in any subsystem yields zero entanglement. Furth... | entanglement, quantum, coherence, initial, gravity, phys, relations, degree | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | le
the latter does not. Surprisingly, this is false. The following
theorem, proven in App. F, holds instead.
Theorem 2 (Rni(Q) = Rni(QI)). For every quantum in-
strumental assemblage, there exists a Q assemblage with the
same non-instrumentality robustness.
From a practical viewpoint, the theorem provides a signifi-
can... | The following
theorem, proven in App. For every quantum in-
strumental assemblage, there exists a Q assemblage with the
same non-instrumentality robustness. From a practical viewpoint, the theorem provides a signifi-
cant computational shortcut in the task of, given a fixed value
ofRni, finding an assemblage with that rob... | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | ˆa†
k↑
ˆa†
k+q↓
!
U †
R = 1√
2
1e iφ
−e−iφ 1
ˆa†
k↑
ˆa†
k+q↓
!
UR,q=0
ˆa†
x↑
ˆa†
x↓
!
U †
R,q=0 = 1√
2
1e iφ
−e−iφ 1
ˆa†
x↑
ˆa†
x↓
!
.
The time evolutions of operators in the Heisenberg pic-
ture are the inverses of this, i.e. we make use of
U †
MaWˆa†
k↑/↓UMaW = ˆa†
−x↑/↓
U †
MaWˆa†
x↑/↓UMaW = ˆa†
k↑/↓
U †... | operators, initial, steps, fig, heisenberg, maw, umaw, then | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | a fermionic environment [42]. Using notation
based on the more recent formulation by Gough and James [26], we can define the most general type of
quantum white noise dynamics as follows. (This theory is rather specialized, and most readers would do
well to take this definition, and the remainder of this section, on trust... | Using notation
based on the more recent formulation by Gough and James [26], we can define the most general type of
quantum white noise dynamics as follows. (This theory is rather specialized, and most readers would do
well to take this definition, and the remainder of this section, on trust, rather than trying to unders... | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | ix A: Generation of comb from MPS
Let us consider a three dimensional functionf(x, y, z)
which is encoded into an MPS of three tensors per di-
mension,
f(x, y, z) =
X
λ
Aσ1
1,λ1
Aσ2
λ1,λ2
Aσ3
λ2,λ3
Bσ4
λ3,λ4
Bσ5
λ4,λ5
Bσ6
λ5,λ6
C σ7
λ6,λ7
C σ8
λ7,λ8
C σ9
λ8,1 ,(A1)
whereλ j denotes the bond indices and sites 1−3 encode... | comb, tensor, mps, bond, three, encode, thexdimension, thea | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | + ˆσz
2 ˆσz
3 ˆσz
4 + ˆσz
1 ˆσz
3 ˆσz
4
−ˆσz
3 −ˆσz
4 −ˆσz
1 ˆσz
2 ˆσz
3 −ˆσz
1 ˆσz
2 ˆσz
4).(19)
In practice, after the VQE optimisation concludes and
the optimal parameters(θ⋆,φ ⋆)are found, they are used
to evaluate the expectation values of the observablesˆχˆK
and ˆKon the quantum hardware. Since both observables
a... | + ˆσz
2 ˆσz
3 ˆσz
4 + ˆσz
1 ˆσz
3 ˆσz
4
−ˆσz
3 −ˆσz
4 −ˆσz
1 ˆσz
2 ˆσz
3 −ˆσz
1 ˆσz
2 ˆσz
4).(19)
In practice, after the VQE optimisation concludes and
the optimal parameters(θ⋆,φ ⋆)are found, they are used
to evaluate the expectation values of the observablesˆχˆK
and ˆKon the quantum hardware. Since both observables
a... | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | due to their dependence on the respective cosmo-
logical constants, Λ f(R)
m and Λ RI
m . These findings highlight the potential for testing quantum gravitational
theories through observations of black hole radiation spectra, bridging the gap between theoretical predictions
and experimental constraints.
Finally, we wan... | gup, black, gravity, zero, hawking, temperature, constants, quantum | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | ntage in combinatorial optimization
as quantum hardware matures.
VIII. ACKNOWLEDGEMENTS
G.E., R.C., and M.A.M.-D. acknowledge the sup-
port from grants MINECO/FEDER Projects, PID2021-
122547NB-I00 FIS2021, MADQuantumCM project
funded by Comunidad de Madrid, the Recovery, Trans-
formation, and Resilience Plan, NextGener... | ntage in combinatorial optimization
as quantum hardware matures. ACKNOWLEDGEMENTS
G.E., R.C., and M.A.M.-D. acknowledge the sup-
port from grants MINECO/FEDER Projects, PID2021-
122547NB-I00 FIS2021, MADQuantumCM project
funded by Comunidad de Madrid, the Recovery, Trans-
formation, and Resilience Plan, NextGenerationE... | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | ez. The one-body density matrix,ρ(z, z ′) =⟨ ˆΨ†(z) ˆΨ(z′)⟩50 is obtained
from TWA simulations as
ρ(z, z′) = ψ∗(z)ψ(z ′)− 1
2 δ(z, z ′)(7)
whereδ(z, z ′)is the delta function, subtracted due to the symmetrically ordered calculation of the correlation
in Wigner function theory, and· · ·denotes the stochastic average. Di... | The one-body density matrix,ρ(z, z ′) =⟨ ˆΨ†(z) ˆΨ(z′)⟩50 is obtained
from TWA simulations as
ρ(z, z′) = ψ∗(z)ψ(z ′)− 1
2 δ(z, z ′)(7)
whereδ(z, z ′)is the delta function, subtracted due to the symmetrically ordered calculation of the correlation
in Wigner function theory, and· · ·denotes the stochastic average. Diagon... | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | U [α(t), β(t)] whose as-
sociated time-dependent Hamiltonian H(t) has the Lie
algebra su(2) ⊕ su(2) as its dynamical symmetry. In
general this time-dependent Hamiltonian H(t) is a lin-
ear combination of all angular momenta of this Lie al-
gebra. In the Hilbert space of the two pseudospins any
pure quantum state, say |... | U [α(t), β(t)] whose as-
sociated time-dependent Hamiltonian H(t) has the Lie
algebra su(2) ⊕ su(2) as its dynamical symmetry. In
general this time-dependent Hamiltonian H(t) is a lin-
ear combination of all angular momenta of this Lie al-
gebra. In the Hilbert space of the two pseudospins any
pure quantum state, say |... | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | ions inaug urated one of
the most outstanding revolutionary periods in western thou ght. One of its
results was the creation of two physical theories: QM and Rel ativity. But,
as Constantin Piron has remarked, these were in the end “two f ailed rev-
olutions” [41] for, up to the present, none of these theories has been... | ions inaug urated one of
the most outstanding revolutionary periods in western thou ght. One of its
results was the creation of two physical theories: QM and Rel ativity. But,
as Constantin Piron has remarked, these were in the end “two f ailed rev-
olutions” [41] for, up to the present, none of these theories has been... | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | ial time diminished as power la w with the characteristic
exponent 2/α 0 if the perturbation surpasses σh.
Then secondly we use a flexible method to get t2 and t3 and the key point is to use fitted local α in terms of some
fixed time interval to find typical transitive time,here we use the nam e as local α to distinguish i... | time, local, perturbation, transitive, get, xed, smoothing, then | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | CONCLUSION AND OUTLOOK
Various exactly solvable models of chaotic quantum many-
body dynamics have appeared in the literature in the past
years, each with a characteristic shape of information spread-
ing and varying degrees of solvability. This research was
kickstarted by dual-unitary circuits, in which space-time du-... | CONCLUSION AND OUTLOOK
Various exactly solvable models of chaotic quantum many-
body dynamics have appeared in the literature in the past
years, each with a characteristic shape of information spread-
ing and varying degrees of solvability. This research was
kickstarted by dual-unitary circuits, in which space-time du-... | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | nsider the Pearson correlation coefficient to quantify
spatial correlations and conclude, that in agreement with
a casual inspection of Fig. 6 (a, d) there are no significant
spatial trends.
Using finite element simulations of the qubit geometry
we are able to infer T1 times limited by the loss tan-
gents of the aluminium ... | times, qubit, qubits, loss, fig, materials, coherence, spatial | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | al. [2020], He et al. [2021], and variational quantum algorithm
Rakyta and Zimborás [2022a,b], He et al. [2023].
Depending on their performance, various approaches might yield different results, resulting in the
need to check the equivalence between their outputs. There are numerous algorithms that can do this,
such as... | quantum, algorithm, circuits, classical, simulation, eq-gan, performance, might | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | g on the inside glass
surface and subsequent surface chemistry that eliminates
metallic Rb adsorbed on the glass. Loss of a thin layer
of Rb adsorbate on the glass is believed to be the cause
for Rb pressure loss at higher rf powers.
EIT-based plasma diagnostics are performed with cas-
cade EIT from the Rb ground state... | eit, probe, mhz, glass, transition, state, through, coupler | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | ed as σ:=ρ⊕0∈B(H (s)
d ⊕H (a)
d )
and a time t> 0. The simulation steps are as follows:
12
1. The agent calculates ηsatisfying the quasi-
Hermiticity conditionH†
PT =ηHPTη−1 with∥η∥=
1.
2. The agent implements the procedure described
above to simulate Gηby setting ˜η= ηand for a
single copy of σ(Eq. (F1)).
3. The agen... | agent, hpt, procedure, prover, implements, upt, probability, scheme | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | tant already in
the acceleration experiments due to so-called spin-rotation couplin g [51]. In these applications a better understanding
of spinning particle at the classical level may be very useful.
There are a lot of operators proposed for the position and spin of r elativistic electron, see [4, 34–36, 45, 52].
Whic... | spin, operators, position, classical, pryce, model, electron, conventional | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | ve a simple alternative argument which makes
use of the R´enyi entropy S∞(λ1, . . . , λN) =− log maxi λi and the inequality S2≥ S∞ [C4]. Namely,
deff = exp(S2(λ1, . . . , λN))≥ exp(S∞(λ1, . . . , λN)) =
(
max
i
λi
)−1 n→∞
−→ ∞
according to Lemma 41 above, applied to the sequence of states ¯ρ(n)
0 = ∑
i π(n)
i ρ(n)
0 π(n... | ve a simple alternative argument which makes
use of the R´enyi entropy S∞(λ1, . , λN) =− log maxi λi and the inequality S2≥ S∞ [C4]. , λN)) =
(
max
i
λi
)−1 n→∞
−→ ∞
according to Lemma 41 above, applied to the sequence of states ¯ρ(n)
0 = ∑
i π(n)
i ρ(n)
0 π(n)
i . | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | bservables of
the system, in particular, the covariance matrix elements, will become time-independent, but the cor-
responding density matrix operator does not take on the thermal form unless γ approaches zero. We
expect the effective temperature defined in (2.7) to have similar dynamical features as any other system
obs... | system, temperature, bath, thermal, ective, state, zero, equilibrium | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | SciPost Physics Submission
Quantum Walks on Graphs of the Ordered Hamming Scheme
and Spin Networks
Hiroshi Miki1*, Satoshi Tsujimoto 2, Luc Vinet 3
1 Meteorological College, Asahi-Cho, Kashiwa 277 0852, Japan
2 Department of Applied Mathematics and Physics, Graduate School of Informatics, Kyoto
University, Sakyo-Ku, Ky... | SciPost Physics Submission
Quantum Walks on Graphs of the Ordered Hamming Scheme
and Spin Networks
Hiroshi Miki1*, Satoshi Tsujimoto 2, Luc Vinet 3
1 Meteorological College, Asahi-Cho, Kashiwa 277 0852, Japan
2 Department of Applied Mathematics and Physics, Graduate School of Informatics, Kyoto
University, Sakyo-Ku, Ky... | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | be the vacuum |0⟩ instead of the two-photon state |ψin⟩. This is done
by replacing the field operators { ˆA1, ˆB1, ˆA2, ˆB2, ˆC2, ˆD2} in the decomposition of ˆUJK with the
single photon modes ˆA′
1, ˆB′
1, etc, as given by the expression (4.83) in Sec 4.4. One could then
use the identities (4.67) to obtain the same res... | vacuum, state, bob, bogolyubov, operators, single, transformation, photon | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | -3
10 -2
10 -1
10 0
d
(a)
(b)
FIG. 6. The parametric functiondillustrates fluctuations in
the height of the central phase-space features of the compass
states under decoherence: (a)p=q= 0, and (b)X 0 = 1.5.
curve, which corresponds to a higher number of pho-
ton subtractions, decays more slowly than the red curve.
Th... | wigner, decoherence, negativity, temporal, fig, states, evolution, features | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | ion as in Definition 14.
In Ref. [13] this is also called the GKSL theorem, since the derivation is based on the pioneering works
by Gorini, Kossakowski and Sudarshan in Ref. [113], and Lindblad in Ref. [116], which studied the time-
independent case in detail. For proofs of the time-dependent case see Refs [22, 121, 15... | [13] this is also called the GKSL theorem, since the derivation is based on the pioneering works
by Gorini, Kossakowski and Sudarshan in Ref. [116], which studied the time-
independent case in detail. For proofs of the time-dependent case see Refs [22, 121, 153]. | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | l descrip-
tion of the potential outside the active dipole is
analogous to how a scalar magnetic potential is
a useful quantity to describe the magnetic field
outside a permanent magnet, highlighting that
either a magnetic scalar or vector potential can
be used.
Now by substituting the fields given in eqns.
(12) and (15)... | magnetic, obtain, vector, substituting, law, potential, potentials, impressed | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | ) When
E′ = {e1, e2, e3, e4}, with c(e1) = c(e2) = c(e3) = c(e4) = 1, after t = 50 time steps. Two
of the elementary links have success probability p1 with cutoffs 5, 15, and the other two
links have success probability p2 with cutoffs 10, 20.
where E′ ⊆ E and G = (V, E, c) is a graph corresponding to the physical (ele... | elementary, links, link, obtain, expression, success, corresponding, then | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | uantum oracle circuits 𝒜𝜆 with 𝒜𝜆 accepting advice of length 𝑡(𝜆)and an advice family
{adv𝜆}𝜆≥1 where |adv𝜆| = 𝑡(𝜆), such that for every input 𝑥 of length 𝜆 = |𝑥|,
• 𝑥 ∈ ℒ yes ⟹ Pr[𝒜𝒪
𝜆 (𝑥,adv𝜆) = 1] ≥2
3 ,
• 𝑥 ∈ ℒ no ⟹ Pr[𝒜𝒪
𝜆 (𝑥,adv𝜆) = 1] ≤1
3 .
If 𝑡(𝜆) = 0then we say ℒ𝒪 ∈ BQP𝒪.
Definit... | uantum oracle circuits 𝒜𝜆 with 𝒜𝜆 accepting advice of length 𝑡(𝜆)and an advice family
{adv𝜆}𝜆≥1 where |adv𝜆| = 𝑡(𝜆), such that for every input 𝑥 of length 𝜆 = |𝑥|,
• 𝑥 ∈ ℒ yes ⟹ Pr[𝒜𝒪
𝜆 (𝑥,adv𝜆) = 1] ≥2
3 ,
• 𝑥 ∈ ℒ no ⟹ Pr[𝒜𝒪
𝜆 (𝑥,adv𝜆) = 1] ≤1
3 . If 𝑡(𝜆) = 0then we say ℒ𝒪 ∈ BQP𝒪. Definit... | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | 1 (2005).
[9] C. Zhang, H. Yuan, Z. Tang, W. Quan, and J. C. Fang,
Inertial rotation measurement with atomic spins: From
angular momentum conservation to quantum phase the-
ory, Appl. Phys. Rev. 3, 041305 (2016).
[10] X. Wu, Z. Pagel, B. S. Malek, T. H. Nguyen, F. Zi, D. S.
Scheirer, and H. M¨ uller, Gravity surveys us... | phys, rev, zhang, atomic, uller, sci, adv, scanning | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | tive laboratories at distant locations, but have set up all kinds of practical
arrangements in advance. In particular, they are at rest with respect to the same inertial frame of reference
and they have set up accordingly synchronised clocks. They both possess some kind of random number
generators and are able to simul... | they, random, chosen, angle, output, settings, outcomes, laboratories | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | pect to the working distribution in the
deterministic context (AB).
Let C,D ∈ { 0, 1}. Irrespective of the current context (AB), define 4 new observables,
i.e., 4 Hermitian operators derived from S as
SCD = U− 1
CD S U CD.
From Eq. ( 100) we have
⟨S⟩AB = Tr(ρABS) = Tr(UABρ00U− 1
ABS) = Tr(ρ00SAB) = ⟨SAB⟩00 =
{
− 1 if A ... | sab, chsh, because, classical, context, state, quantum, new | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | 0.15 0.20
E/c
0.2
0.4
0.6
0.8
1.0
1.2
1.4
S/c=ln(ρ)/c
Figure 3 . Full density of states of the averaged Narain theory –U(1) gravity. Blue lines:
S1/c and S2/c as functions of e = E/c, where the full density of states (entropy) ofU(1)
gravity is S = max( S1, S2). S1 dominates for E < 0 and S2 for E > 0. Brown line: the
... | 0.15 0.20
E/c
0.2
0.4
0.6
0.8
1.0
1.2
1.4
S/c=ln(ρ)/c
Figure 3 . Full density of states of the averaged Narain theory –U(1) gravity. Blue lines:
S1/c and S2/c as functions of e = E/c, where the full density of states (entropy) ofU(1)
gravity is S = max( S1, S2). | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | ed on exact diagonalization
and are performed at half filling. We setJ= 1,V= 0.25,
β= (
√
5−1)/2 and varyδto drive the localization phase
transition. Panel (a-c) are the three different type of localiza-
tion tensor discussed in the main text, and Panle (d) shows
the scaling behavior to confirm the convergence of the n... | ed on exact diagonalization
and are performed at half filling. We setJ= 1,V= 0.25,
β= (
√
5−1)/2 and varyδto drive the localization phase
transition. Panel (a-c) are the three different type of localiza-
tion tensor discussed in the main text, and Panle (d) shows
the scaling behavior to confirm the convergence of the n... | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | ition along a physically real wave spread
out in space, for example. We consider the wavenumber k a classical ob-
servable since the wavelength is in principle classically measurable. The
eigenvalues of the classical Hermitian operators are experimentally verifi-
able quantities.
3. The state space of a composite syste... | ition along a physically real wave spread
out in space, for example. We consider the wavenumber k a classical ob-
servable since the wavelength is in principle classically measurable. The
eigenvalues of the classical Hermitian operators are experimentally verifi-
able quantities. | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | e issue arises
that the initial states of trajectories|ψ z(0)⟩are noise de-
pendent. Thus, we introduce a normalized trajectory
|φz⟩, defined as
|φz⟩ ≡ |ψz⟩
Q
k
1√coshr k
e
−tanhr k
2 (z∗
k)2
,(F3)
to satisfy the coincidence of the initial condition
|φz(0)⟩=|ψ A(0)⟩. Consequently, we obtain
∂
∂z ∗
k
|ψz⟩=
Y
k′
1q
coshr... | tanhr, initial, two, coshr, equation, stochastic, case, normalized | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | ng time T(S; n, ·, ·, ·, ·, ·);
– the running time T(A; n, ·, ·).
Moreover ,DeTypeh calculates the description of A′ in polynomial time in that of S and A; in particular , |A′|=
polyh(|S|, |A|).
• (Linear constraints processor properties) The ouput linea r constraints processor TM L′(n, ·, ·, ·, ·) runs in time poly-
n... | ng time T(S; n, ·, ·, ·, ·, ·);
– the running time T(A; n, ·, ·). Moreover ,DeTypeh calculates the description of A′ in polynomial time in that of S and A; in particular , |A′|=
polyh(|S|, |A|). • (Linear constraints processor properties) The ouput linea r constraints processor TM L′(n, ·, ·, ·, ·) runs in time poly-
n... | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | hows the gain distri-
bution for the three different angles atδ/2π∼5.5 MHz,
along with the respective transverse profile in the inset.
Figures 3 (a-c) show the gain distribution forθ eff= 3,4.8
and 6 mrad, respectively. Figure (a) shows a gain distri-
bution in the probe channel that spreads over modes up
ton= 8, going... | hows the gain distri-
bution for the three different angles atδ/2π∼5.5 MHz,
along with the respective transverse profile in the inset. Figures 3 (a-c) show the gain distribution forθ eff= 3,4.8
and 6 mrad, respectively. Figure (a) shows a gain distri-
bution in the probe channel that spreads over modes up
ton= 8, going... | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | on. For instance,
:ˆϕ(x)2: =
XZ
k,k′
:
uk(x)uk′(x)ˆakˆak′ +u ∗
k(x)uk′(x)ˆa†
kˆak′ +u k(x)u∗
k′(x)ˆakˆa†
k′ +u ∗
k(x)u∗
k′(x)ˆa†
kˆa†
k′
:
=
XZ
k,k′
uk(x)uk′(x)ˆakˆak′ +u ∗
k(x)uk′(x)ˆa†
kˆak′ +u k(x)u∗
k′(x)ˆa†
k′ˆak +u ∗
k(x)u∗
k′(x)ˆa†
kˆa†
k′
46
= ˆϕ2(x)−
XZ
k
uk(x)u∗
k(x),(1.141)
where in the first equali... | For instance,
:ˆϕ(x)2: =
XZ
k,k′
:
uk(x)uk′(x)ˆakˆak′ +u ∗
k(x)uk′(x)ˆa†
kˆak′ +u k(x)u∗
k′(x)ˆakˆa†
k′ +u ∗
k(x)u∗
k′(x)ˆa†
kˆa†
k′
:
=
XZ
k,k′
uk(x)uk′(x)ˆakˆak′ +u ∗
k(x)uk′(x)ˆa†
kˆak′ +u k(x)u∗
k′(x)ˆa†
k′ˆak +u ∗
k(x)u∗
k′(x)ˆa†
kˆa†
k′
46
= ˆϕ2(x)−
XZ
k
uk(x)u∗
k(x),(1.141)
where in the first equality, ... | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | .37 ns,
(c)t= 0.5 ns, (d)t= 0.6 ns, and (e)t= 0.8 ns.
9
0 MaxMin
(a)
(b)
(c)
FIG. 5. Magnetic field distribution for magnetic flux excita-
tion at frequencyω m incident from the left, showing signifi-
cant frequency multiplication in the nonreciprocal supercon-
ducting frequency bus. The bus parameters are eΦdc = 0.7
... | flux, frequency, field, magnetic, distribution, array, fig, multiplication | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | the RF transition frequency). We present
3
a model to predict the observed behavior of the EIT sig-
nal in the presence of BLWGN, and show excellent agree-
ment between experimental and model results.
II. EXPERIMENT AL SETUP AND NOISE
SOURCE
A picture of the experimental setup and a block dia-
gram of the noise source... | laser, signal, noise, cell, probe, eit, fig, vapor | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | s
{(1, 0, 0), (0, 1, 0), (0, 0, 1), (−1, −1, −1)}. Other geometric arrangements [for which the last vector is diffeomorphic to
(1, 1, 1), (1, 1, 0), (−1, −1, 0), (0, 0, 1) or (0 , 0, −1)] imply different choices of καβγ, which will not be addressed here.
The first contribution to the right-hand side of Eq. (82) is
l
j1... | link, spin, network, grasps, spins, node, where, second | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | y of a quantum
phase to encode non-local information in terms of how
much spread the state becomes in stabilizer space when
perturbed by finite-depth non-Clifford circuits. This op-
erational concept captures how a phase can “host” dis-
tributed magic resources. While conventional phases
such as symmetry-broken or para... | y of a quantum
phase to encode non-local information in terms of how
much spread the state becomes in stabilizer space when
perturbed by finite-depth non-Clifford circuits. This op-
erational concept captures how a phase can “host” dis-
tributed magic resources. While conventional phases
such as symmetry-broken or para... | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | P)Λ− 1
s (p0), with the constant boost Λ− 1
s (p0) replaced
by Λ c(ki). This has the consequence that the constituent spins are defined so that the zero-momentum vector
of the many-body system is the standard vector.
The constituent spin operators defined in ( 152) have the property that they can be added to the orbital
... | P)Λ− 1
s (p0), with the constant boost Λ− 1
s (p0) replaced
by Λ c(ki). This has the consequence that the constituent spins are defined so that the zero-momentum vector
of the many-body system is the standard vector. The constituent spin operators defined in ( 152) have the property that they can be added to the orbital
... | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | 81)
Hence, the fusion subcategoriesS(Mf2,Mf3, 1) andS(Mf3,Mf2, 1) can only have
Wilson lines as common elements. The trivial Wilson lineW1 is of course a common
element. As we saw in section 2.3, a Wilson line,Wπ, is a member of the fusion
subcategory,S(Mf2,Mf3, 1), only if the condition
χπ(h) :=B(e,h ) deg χπ = deg χπ... | 81)
Hence, the fusion subcategoriesS(Mf2,Mf3, 1) andS(Mf3,Mf2, 1) can only have
Wilson lines as common elements. The trivial Wilson lineW1 is of course a common
element. As we saw in section 2.3, a Wilson line,Wπ, is a member of the fusion
subcategory,S(Mf2,Mf3, 1), only if the condition
χπ(h) :=B(e,h ) deg χπ = deg χπ... | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | um is known.
5 Discussion and Conclusion
The quantum multinomial distribution expresses multiphoton transition probabilities as a
coherent average over routing matrices, weighted by the multivariate hypergeometric dis-
tribution. The same routing matrices, the same weights, and the same amplitudes appear
in the classic... | quantum, classical, multinomial, routing, hypergeometric, distribution, same, interference | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | 1,...,j −
√
M 2 − κ2
i
∪i=1,...,j
√
M 2 − κ2
i ∪ [M, ∞ ),
and the equations (7.75) define the occupation frac-
tion νk of the bound states of the central band in
the form
|Eb,j |=M sin
( πνj
2
)
, j = 1, · · ·,l. (7.77)
Note that for this type of condensates the occupa-
tion fractions are related by ν1 < ν2 < · · ·< νl.... | 1,...,j −
√
M 2 − κ2
i
∪i=1,...,j
√
M 2 − κ2
i ∪ [M, ∞ ),
and the equations (7.75) define the occupation frac-
tion νk of the bound states of the central band in
the form
|Eb,j |=M sin
( πνj
2
)
, j = 1, · · ·,l. (7.77)
Note that for this type of condensates the occupa-
tion fractions are related by ν1 < ν2 < · · ·< νl.... | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | VvJv7n9VIdXvkZE0mqqSCLRWHKkY7RLAU0YJISzSeGYCKZuRWRETYRaJNVyYTgLr+8StrnVbderd3VKo3rPI4iHMMJnIELl9CAW2hCCwik8Ayv8GY9WS/Wu/WxaC1Y+cwR/IH1+QNxDJL1</latexit>
⊋
1
3
Figure 1: The dynamics of our counterexample in phase space. Quantum and classical Gaussian states
are uniquely represented by their covariance ellipse. We assum... | classical, state, quantum, time, dynamics, gaussian, dimensions, step | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | and the impact of orbital in comparison
to the spin, we calculate the energy scales within the
constant interaction model. Zeeman energy,EZ, is given
by:
EZ =g ∗µBB=g ∗ eℏB
2me
where me is the electron mass. The orbital energy,Eorb
scale is given by:
Eorb =ℏω c = ℏeB
m∗
where m∗ = 0 .09 ± 0.002me [25] is the effective ... | and the impact of orbital in comparison
to the spin, we calculate the energy scales within the
constant interaction model. Zeeman energy,EZ, is given
by:
EZ =g ∗µBB=g ∗ eℏB
2me
where me is the electron mass. The orbital energy,Eorb
scale is given by:
Eorb =ℏω c = ℏeB
m∗
where m∗ = 0 .09 ± 0.002me [25] is the effective ... | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | tate as the coupling
increases. The off-diagonal elements indicate that the su-
perposition of eigenstates |e1⟩ and |e4⟩ grows rapidly and
thus decoherence does not fully take place in the energy
eigenbasis. Both the diagonal and off-diagonal elements
approach the pointer limit predicted by Eq. (8).
When the matrix eleme... | coupling, diagonal, elements, pointer, limit, state, steady, system | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | re these completeness results
have appeared, they were also included into each of the PhD theses of Vilmart, Ng and
Wang [100, 117, 121].
9.2 W-states and the ZW-calculus
The early completeness results of both Oxford and Nancy relied on a translation of the
ZX-calculus into the related ZW-calculus. Before we go into th... | re these completeness results
have appeared, they were also included into each of the PhD theses of Vilmart, Ng and
Wang [100, 117, 121]. 9.2 W-states and the ZW-calculus
The early completeness results of both Oxford and Nancy relied on a translation of the
ZX-calculus into the related ZW-calculus. Before we go into th... | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | nm,
which lines up well with the absorption/emission differ-
ence of the triplet. The triplet transition is also optically
brightest for F −
3 , with a TDM 2 of 7.9 Debye 2, and the
ground state triplet is ∼ 250 meV lower in energy than
the ground state singlet [62], suggesting this state may
be responsible for the exp... | nm,
which lines up well with the absorption/emission differ-
ence of the triplet. The triplet transition is also optically
brightest for F −
3 , with a TDM 2 of 7.9 Debye 2, and the
ground state triplet is ∼ 250 meV lower in energy than
the ground state singlet [62], suggesting this state may
be responsible for the exp... | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | d. However, the mod el can be motivated by
the interaction of nonrelativistic systems with the electromagnetic field [19, 39]. The form
of (43) then suggests a connection between the UDW defect and t he Wilson lines of the
underlying electromagnetic theory. To see this, let us begin by revis iting the origin of
the UDW ... | eld, interaction, udw, dipole, function, electromagnetic, atom, vector | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | +ωk
+ cosϑk−cos
(
(νl−ωk)T−ϑk
)
νl−ωk
]}
.(S6)
Appendix B: Optimization withπ-pulses
This appendix formulates the optimization problem of
combining globalπ-pulses with gradient–modulation seg-
ments in order to realize a target Ising interaction
∑
j,k
ΛjkZjZk .(S1)
Consider a sequence ofMgradient–modulation seg-
ments.... | pulses, matrix, diagonal, target, interaction, cos, appendix, optimization | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | ive gates of superconducting qubit architectures are provided in Fig. 4.
Note that above results are incomparable in the
sense that Result 2 cannot be decuced form 3 and
vice versa. This is because they make statements
about hardness of outcome probabilities for different
fractions of circuits. Formal versions of the ab... | ive gates of superconducting qubit architectures are provided in Fig. Note that above results are incomparable in the
sense that Result 2 cannot be decuced form 3 and
vice versa. This is because they make statements
about hardness of outcome probabilities for different
fractions of circuits. | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | n through random pulse-intensity variations, and was first successfully
demonstrated in [11]. However, while it improves performance, the decoy-state approach relies on conservative
assumptions for multi-photon pulses—assuming they are fully compromised—which forces conservative intensity
choices, limits maximum transm... | n through random pulse-intensity variations, and was first successfully
demonstrated in [11]. However, while it improves performance, the decoy-state approach relies on conservative
assumptions for multi-photon pulses—assuming they are fully compromised—which forces conservative intensity
choices, limits maximum transm... | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | 09).
[67] P . Wendenbaum, T. Platini, and D. Karevski, Phys. Rev.
A 91, 040303 (2015).
[68] S. Attal and Y. Pautrat, in Annales Henri Poincar ´e, Vol. 7
(Springer, 2006) pp. 59–104.
[69] A. Barchielli, Phys. Rev. A 34, 1642 (1986).
[70] A. Barchielli and V . Belavkin, Journal of Physics A: Math-
ematical and General 24... | Pautrat, in Annales Henri Poincar ´e, Vol. Belavkin, Journal of Physics A: Math-
ematical and General 24, 1495 (1991). Petruccione,The Theory of Open Quan-
tum Systems (Oxford University Press, 2007). | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | hin the currently probed
phase space, in agreement with the theoretical prediction. These results experimentally corroborate
the full hierarchy of quantum correlations in top quarks with discord being the most basic form of
quantum correlation, followed by entanglement, steering and Bell correlation. The significance o... | hin the currently probed
phase space, in agreement with the theoretical prediction. These results experimentally corroborate
the full hierarchy of quantum correlations in top quarks with discord being the most basic form of
quantum correlation, followed by entanglement, steering and Bell correlation. The significance o... | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | a real-linear
map, it has 1- and (−1)-eigenspacesV + andV −, which one thinks of as the “real”
and “imaginary” elements ofC n with respect toc. IfAis ann×ncomplex matrix
commuting withc, thenAV + =V +, and ifBis ann×nmatrix whose columns
form an orthonormal basis ofV +, thenB †ABis a real matrix.
Letι:C 2 →C 2 be the c... | a real-linear
map, it has 1- and (−1)-eigenspacesV + andV −, which one thinks of as the “real”
and “imaginary” elements ofC n with respect toc. IfAis ann×ncomplex matrix
commuting withc, thenAV + =V +, and ifBis ann×nmatrix whose columns
form an orthonormal basis ofV +, thenB †ABis a real matrix. Letι:C 2 →C 2 be the c... | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | ive using Theorem 4.6.2, and obtain
d
dt D(id ⊗Tt(ρAA′)|| id ⊗Rσ(ρAA′))
= d
dt H(A)ρA + d
dt tr
Tt(ρA′) log(Rσ(ρ′
A))
− d
dt H(AB)(id ⊗Tt)(ρAA′)
= − tr
(S − Rσ)(ρA′) log(Rσ(ρA′))
+ tr
(id ⊗(S − Rσ))(ρAA′) log((id⊗Tt)(ρAA′))
= tr
(id ⊗(S − Rσ))(ρAA′)
log((id ⊗Tt)(ρAA′)) − 1 ⊗ log(Rσ(ρA′))
= tr
(id ⊗... | log, dt2, quantum, second, derivative, mda, channel, expression | pending | |
summary | Summarize the following scientific passage in 2-4 sentences using clear academic language. | Hall Effect Gyrators and Circulators
Giovanni Viola 1 and David P. DiVincenzo 1, 2, 3
1Institute for Quantum Information, R WTH Aachen University, D-52056 Aachen, Germany
2Peter Gr¨ unberg Institute: Theoretical Nanoelectronics, Research Center J¨ ulich
3J¨ ulich-Aachen Research Alliance (JARA), Fundamentals of Future I... | Hall Effect Gyrators and Circulators
Giovanni Viola 1 and David P. DiVincenzo 1, 2, 3
1Institute for Quantum Information, R WTH Aachen University, D-52056 Aachen, Germany
2Peter Gr¨ unberg Institute: Theoretical Nanoelectronics, Research Center J¨ ulich
3J¨ ulich-Aachen Research Alliance (JARA), Fundamentals of Future I... | pending | |
keywords | Extract the 8 most important technical keywords from the passage. | Einstein’s Equivalence principle for superpositions of gravitational fields and
quantum reference frames
Flaminia Giacomini 1, 2, ∗ and ˇCaslav Brukner 3, 4
1Perimeter Institute for Theoretical Physics,
31 Caroline St. N, Waterloo, Ontario, N2L 2Y5, Canada
2Institute for Theoretical Physics, ETH Z ¨urich,
Wolfgang-Paul... | quantum, gravitational, eep, reference, physics, vienna, principle, frames | pending |
End of preview. Expand in Data Studio
Scientific Papers SFT Queue
Instruction-tuning style records derived from scientific paper passages for summarization and keyword extraction tasks.
Splits in this repo
pilot/sft_review_queue_10.jsonl: 10-item pilot split for quick validationsft_review_queue_500.jsonl: 500-item review queue
Schema
Each JSONL row has:
task:summaryorkeywordsinstruction: task instructioninput: source passagedraft_output: initial target outputreview_status: review state (pendingin current queue)notes: free-text reviewer notes
Data quality status
- All rows in the current uploads parse as valid JSONL
- Known issue: some rows contain encoding artifacts (for example
’,Â) - Recommended next step: text normalization before production fine-tuning
Intended use
- Pilot SFT experiments
- Human-in-the-loop review pipelines
- Dataset quality iteration before large-scale releases
Limitations
- Draft outputs are not fully human-validated
- Potential encoding artifacts can reduce model quality
- Domain coverage depends on source paper mix
Attribution
Maintainer: YanJo199
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