Dataset Viewer
Auto-converted to Parquet Duplicate
id
stringlengths
9
10
abstract
stringlengths
13
3.93k
embedding
sequence
1001.0001
The Krotov combining construction of perfect 1-error-correcting binary codes from 2000 and a theorem of Heden saying that every non-full-rank perfect 1-error-correcting binary code can be constructed by this combining construction is generalized to the $q$-ary case. Simply, every non-full-rank perfect code $C$ is the union of a well-defined family of $\mu$-components $K_\mu$, where $\mu$ belongs to an "outer" perfect code $C^*$, and these components are at distance three from each other. Components from distinct codes can thus freely be combined to obtain new perfect codes. The Phelps general product construction of perfect binary code from 1984 is generalized to obtain $\mu$-components, and new lower bounds on the number of perfect 1-error-correcting $q$-ary codes are presented.
[ -0.015585657209157002, 0.016744695603847, -0.014822055585682002, -0.021612657234072002, -0.025117043405771002, 0.007990547455847001, -0.0015007843030610001, -0.033080320805311, -0.025062501430511003, -0.027816921472549, -0.0014505024300880002, 0.039052776992321, -0.016867417842149002, 0.00...
1001.0002
Logarithmic conformal field theories with vanishing central charge describe systems with quenched disorder, percolation or dilute self-avoiding polymers. In these theories the energy momentum tensor acquires a logarithmic partner. In this talk we address the construction of possible gravity duals for these logarithmic conformal field theories and present two viable candidates for such duals, namely theories of massive gravity in three dimensions at a chiral point.
[ 0.004695892333984, 0.01996518112719, 0.0027995395939790003, -0.007442802656441001, 0.0007342636818060001, 0.030124336481094003, -0.020399797707796003, -0.030395971611142002, -0.010919732041656001, -0.014288007281720002, 0.027733946219086, 0.029798373579978003, -0.009059031493961001, 0.0201...
1001.0003
We construct new families of non-supersymmetric sourceless type IIA AdS4 vacua on those coset manifolds that also admit supersymmetric solutions. We investigate the spectrum of left-invariant modes and find that most, but not all, of the vacua are stable under these fluctuations. Generically, there are also no massless moduli.
[ -0.0005790717550550001, 0.004832370672374, -0.009515740908682001, -0.008235687389969, -0.027199441567063002, 0.023162869736552003, -0.028228901326656, -0.012360303662717, 0.0037588868290180004, -0.017351834103465, 0.021754134446382002, 0.013775812461972, -0.010924476198852002, 0.0290687251...
1001.0004
Examples of symmetric informationally complete positive operator valued measures (SIC-POVMs) have been constructed in every dimension less than or equal to 67. However, it remains an open question whether they exist in all finite dimensions. A SIC-POVM is usually thought of as a highly symmetric structure in quantum state space. However, its elements can equally well be regarded as a basis for the Lie algebra gl(d,C). In this paper we examine the resulting structure constants, which are calculated from the traces of the triple products of the SIC-POVM elements and which, it turns out, characterize the SIC-POVM up to unitary equivalence. We show that the structure constants have numerous remarkable properties. In particular we show that the existence of a SIC-POVM in dimension d is equivalent to the existence of a certain structure in the adjoint representation of gl(d,C). We hope that transforming the problem in this way, from a question about quantum state space to a question about Lie algebras, may help to make the existence problem tractable.
[ 0.023628670722246004, 0.00021616531012100002, 0.022768700495362, -0.037319920957088006, -0.033497836440801, 0.030003359541296, -0.024311184883117003, -0.024201981723308, -0.015056281350553001, -0.029457347467541, 0.026891091838479, 0.017390482127666, -0.011534503661096, 0.02154017426073500...
1001.0005
We aim to reveal environmental dependence of infrared luminosity functions (IR LFs) of galaxies at z~0.8 using the AKARI satellite. We construct restframe 8um IR LFs in the cluster region RXJ1716.4+6708 at z=0.81, and compare them with a blank field using the AKARI North Ecliptic Pole deep field data at the same redshift. AKARI's wide field of view (10'x10') is suitable to investigate wide range of galaxy environments. AKARI's 15um filter is advantageous here since it directly probes restframe 8um at z~0.8, without relying on a large extrapolation based on a SED fit, which was the largest uncertainty in previous work. We have found that cluster IR LFs at restframe 8um have a factor of 2.4 smaller L^* and a steeper faint-end slope than that of the field. Confirming this trend, we also found that faint-end slopes of the cluster LFs becomes flatter and flatter with decreasing local galaxy density. These changes in LFs cannot be explained by a simple infall of field galaxy population into a cluster. Physics that can preferentially suppress IR luminous galaxies in high density regions is required to explain the observed results.
[ 0.021031482145190003, 0.007450645789504001, -0.011589893139898002, -0.006280709523707, -0.011152022518217002, 0.027407977730035, -0.035467535257339006, -0.002709325635805, -0.01588650047779, -0.027572179213166, 0.0015334030613300001, 0.007861149497330001, 0.01052258349955, 0.00342086586169...
1001.0006
We present the first comparison of virial masses of galaxy clusters with their Sunyaev-Zel'dovich Effect (SZE) signals. We study 15 clusters from the Hectospec Cluster Survey (HeCS) with MMT/Hectospec spectroscopy and published SZE signals. We measure virial masses of these clusters from an average of 90 member redshifts inside the radius $r_{100}$. The virial masses of the clusters are strongly correlated with their SZE signals (at the 99% confidence level using a Spearman rank-sum test). This correlation suggests that $Y_{SZ}$ can be used as a measure of virial mass. Simulations predict a powerlaw scaling of $Y_{SZ}\propto M_{200}^\alpha$ with $\alpha\approx$1.6. Observationally, we find $\alpha$=1.11$\pm$0.16, significantly shallower (given the formal uncertainty) than the theoretical prediction. However, the selection function of our sample is unknown and a bias against less massive clusters cannot be excluded (such a selection bias could artificially flatten the slope). Moreover, our sample indicates that the relation between velocity dispersion (or virial mass estimate) and SZE signal has significant intrinsic scatter, comparable to the range of our current sample. More detailed studies of scaling relations are therefore needed to derive a robust determination of the relation between cluster mass and SZE.
[ -0.009176731109619, -0.007445912342518001, 0.0035939933732150003, -0.025887612253427002, -0.017552534118294, 0.040154986083507004, -0.023118302226066003, 0.010194859467446001, -0.028263244777917, -0.049304563552141, -0.0037263499107210002, 0.042326990514993, 0.0016985775437200002, 0.018027...
1001.0007
"We reveal cosmic star-formation history obscured by dust using deep infrared observation with the A(...TRUNCATED)
[0.019308622926473,-0.0065242024138560005,-0.018979499116539,-0.018019553273916,-0.002357009565457,0(...TRUNCATED)
1001.0008
"In this Letter, we briefly review the multi-stream inflation scenario, and discuss its implications(...TRUNCATED)
[-0.020563460886478,-0.0077112978324290005,-0.003916688263416001,-0.013286219909787001,-0.0020278610(...TRUNCATED)
1001.0009
"Theoretical studies of stretching proteins with slipknots reveal a surprising growth of their unfol(...TRUNCATED)
[-0.018460078164935,-0.012798245996236001,0.010370752774178002,-0.026737205684185004,-0.013959825970(...TRUNCATED)
1001.0011
"Spatial separation of electrons and holes in graphene gives rise to existence of plasmon waves conf(...TRUNCATED)
[-0.008414856158196002,0.022923229262232003,0.011329719796776001,-0.001989955315366,-0.0028159432113(...TRUNCATED)
End of preview. Expand in Data Studio

Dataset Card for "arxiv_embeddings_480k"

More Information needed

Downloads last month
3