id stringlengths 19 42 | text stringlengths 0 4.51M | added stringlengths 24 24 | created stringlengths 20 24 | source stringclasses 4
values | original_shard_dir stringclasses 232
values | original_shard_idx int64 0 311k | num_tokens int64 1 885k |
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proofpile-arXiv_065-241 | \section{Motivation}
Chromium is considered as the archetypical itinerant antiferromagnet~\cite{1988_Fawcett_RevModPhys, 1994_Fawcett_RevModPhys}. Interestingly, it shares its body-centered cubic crystal structure $Im\overline{3}m$ with the archetypical itinerant ferromagnet $\alpha$-iron and, at melting temperature, ... | 2024-02-18T23:39:40.791Z | 2020-07-22T02:11:10.000Z | algebraic_stack_train_0000 | 45 | 9,343 | |
proofpile-arXiv_065-242 |
\section{Meta-Learning for Optimal Agent}
The trade-off described above begs the following question: How can it be managed in an environment with unknown properties? That is, how does an agent decide whether to pursue single-task or multitask training in a new environment so that it can learn the tasks most efficientl... | 2024-02-18T23:39:40.794Z | 2021-01-06T02:23:41.000Z | algebraic_stack_train_0000 | 46 | 7,720 | |
proofpile-arXiv_065-251 | \section{Introduction}
In recent years, advances in GPU technology and machine learning libraries enabled the trend towards deeper neural networks in Automatic Speech Recognition (ASR) systems.
End-to-end ASR systems transcribe speech features to letters or tokens without any intermediate representations.
There are two... | 2024-02-18T23:39:40.833Z | 2020-07-22T02:14:15.000Z | algebraic_stack_train_0000 | 48 | 3,987 | |
proofpile-arXiv_065-287 | "\\section{Data Specifications Table}\n\n\\begin{table}[htb]\n\\centering\n\\footnotesize\n\\label{D(...TRUNCATED) | 2024-02-18T23:39:40.960Z | 2021-05-31T02:02:16.000Z | algebraic_stack_train_0000 | 55 | 17,146 | |
proofpile-arXiv_065-341 | "\\section{INTRODUCTION}\n\n\n\n\n\nThe study of the elementary excitations of ultrarelativistic pl(...TRUNCATED) | 2024-02-18T23:39:41.191Z | 1996-09-02T12:52:05.000Z | algebraic_stack_train_0000 | 68 | 3,609 | |
proofpile-arXiv_065-405 | "\\section{Dynamics and time orientation}\n\nWe introduce a treatment of dynamics which may be readi(...TRUNCATED) | 2024-02-18T23:39:41.360Z | 1996-09-18T21:55:10.000Z | algebraic_stack_train_0000 | 79 | 4,776 | |
proofpile-arXiv_065-507 | "\\section{Introduction}\n\nSupersymmetry (SUSY) predicts the existence of a spin 1/2 partner\nof t(...TRUNCATED) | 2024-02-18T23:39:41.742Z | 1997-09-18T00:18:33.000Z | algebraic_stack_train_0000 | 95 | 7,943 | |
proofpile-arXiv_065-516 | "\\section{INTRODUCTION}\nSimulations of full QCD with Wilson fermions at zero temperature so\nfar h(...TRUNCATED) | 2024-02-18T23:39:41.762Z | 1996-09-12T18:46:32.000Z | algebraic_stack_train_0000 | 98 | 1,400 | |
proofpile-arXiv_065-592 | "\\section{Introduction}\n\nThe environment at the centers of galaxy cluster cooling flows is exotic(...TRUNCATED) | 2024-02-18T23:39:41.975Z | 1996-09-25T00:50:31.000Z | algebraic_stack_train_0000 | 112 | 3,767 | |
proofpile-arXiv_065-794 | "\\section{Introduction}\n\nSince the very moment when one is introduced to the quantum formalism {\(...TRUNCATED) | 2024-02-18T23:39:42.619Z | 1996-09-04T21:25:10.000Z | algebraic_stack_train_0000 | 154 | 2,611 |
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