REVIEW 3 major objections 6 minor 95 references
Language Model for Large-Text Transmission in Noisy Quantum Communications
T0 review · 3 major / 6 minor · reviewed 2026-08-16 · deepseek-v4-flash
Pith's one-line read A language model plugged in after the decoder cuts noisy-quantum sentence errors from 76% to 24%.
desk verdict A real but modest error-reduction result for BERT-corrected superdense coding, undercut by an unfair classical baseline that makes entanglement look more helpful than it is. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The load-bearing object is PQC-BERT, a two-module post-decoding pipeline. The word-level repairing module compares each decoded word against a dictionary and replaces it with the dictionary word whose ASCII bit string is closest in Hamming distance; the sentence-level repairing module then passes the repaired text through a BERT-based correction network that proposes context-appropriate words, and an evaluation network trained with focal loss decides whether each proposal should be accepted or the dictionary repair kept. The mechanism works because natural language is statistically redundant: even when individual bits are corrupted, the surrounding words strongly constrain what the damaged word must be, so a bidirectional Transformer can infer the intended text. The paper's additional claim that quantum resources improve the pipeline rests on comparing error rates after the same post-processor for classical bits, qubit superdense coding, and qudit superdense coding.
What would settle it
Send one half of a Bell state through an experimentally realized amplitude-damping channel, perform a complete two-qubit Bell measurement, and compare the outcome distribution with the one produced by the paper's Appendix C simulation of the same channel at the same noise strength; if the two distributions differ substantially, the reported gains for amplitude damping are an artifact of the simplified noise model.
Extended reading notes
Core claim
The central claim is that a classical NLP post-decoder, PQC-BERT, successfully corrects nearly all of the semantically relevant errors in text transmitted by noisy superdense coding, reducing sentence error rates from roughly 76% to below 26% at a 1% bit-flip noise level, and that it does so without the extra qubits of quantum error correction or the repeated rounds of quantum error mitigation. A further claim is that entanglement itself helps the language model: under identical bit-flip noise and noise strength, quantum superdense coding with PQC-BERT outperforms a classical bit channel with the same post-processor, and qudit superdense coding with d = 4 outperforms qubit superdense coding. The paper interprets this as showing that increased entanglement improves transmission performance even though PQC-BERT never interacts with the quantum states directly.
Load-bearing premise
The reported error reductions rest on simulating noisy channels as probabilistic bit and phase flips on randomly chosen qubits rather than as full quantum-channel evolution; if that simplified model does not reproduce the measurement statistics of real amplitude damping or depolarizing channels, the corresponding error-rate numbers would change.
Editorial extensions
If this is right
- If the central claim holds, a noisy quantum channel can carry intelligible prose at useful rates without the physical-qubit overhead of quantum error correction or the sample overhead of quantum error mitigation.
- Because PQC-BERT is trained without noise-model labels, a single deployment could be dropped into channels whose noise is unknown or time-varying, removing a separate noise-characterization step.
- The reported qudit advantage implies that moving from qubits to higher-dimensional entangled systems improves not only capacity but also the effectiveness of the language-model cleanup, which would make qudit superdense coding an attractive target for implementation.
- The 5 to 16 word optimal range suggests a concrete transmission protocol design: split long text into units of at most 16 words before sending, so that each unit is corrected in the regime where the model works best.
- The reported error-detection accuracy suggests PQC-BERT could be used as a context-sensitive pre-screen that flags likely error locations before a conventional quantum error correction code acts on them.
Reading between the lines
- A natural extension the paper leaves implicit is to test whether the same post-decoding cleanup transfers to other redundant data types, such as speech phonemes, images with spatial autocorrelation, or protocol headers, where a learned prior could substitute for the language prior used here.
- If the entanglement advantage observed in simulation is real, the mechanism is worth isolating: it may come from the specific error patterns superdense coding produces rather than from an intrinsic quantum benefit, and a controlled experiment varying only the channel use under the same noise floor could separate those effects.
- The numerical setup as described suggests a cheap additional test: feed the same corrupted bit strings through a strong neural decoder without any quantum protocol to see how much of the reported gain is linguistic redundancy alone and how much is specific to entanglement-assisted error patterns.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper proposes PQC-BERT, a post-decoding language-model module for noisy quantum superdense coding. Text is converted to ASCII, encoded into Bell states, transmitted through noisy quantum channels (bit-flip, phase-flip, depolarizing, amplitude damping), and then repaired by a word-level dictionary module and a BERT-based sentence-level correction/evaluation network. The authors report numerical experiments on two text datasets showing that PQC-BERT substantially reduces bit, word, and sentence error rates after transmission, and they claim that entanglement-assisted (quantum) communication improves PQC-BERT's correction performance compared with a classical channel at the same noise strength.
Significance. If the results hold, the paper demonstrates a potentially useful hybrid classical-quantum approach: using a pretrained language model as a software-only postprocessor to repair text corrupted by quantum channel noise, without the qubit overhead of quantum error correction or the sampling overhead of quantum error mitigation. The core before/after error reduction is supported by held-out test data and replicated experiments, and the protocol is simple to describe. However, the headline claim that quantum entanglement improves PQC-BERT's error mitigation is undermined by an apples-to-oranges comparison, and the amplitude-damping simulation is not faithful to the stated channel. These issues are load-bearing for the paper's central message, so the results as presented cannot be accepted at face value.
major comments (3)
- [Sec. III.B, Table I] The classical-vs-quantum comparison is not normalized to the same per-information-bit error rate. In qubit superdense coding, a bit-flip error on the transmitted qubit acts as X⊗I on the encoded Bell state |Φ_zx⟩; since X Z^z X^x = (-1)^z Z^z X^{x⊕1}, the z bit never flips and only the x bit flips with probability λ. The effective per-bit error rate for the quantum channel is therefore λ/2, while the classical baseline has per-bit error rate λ. At λ=0.01, the quantum text entering PQC-BERT is already half as noisy as the classical text, so the higher Accuracy/F1 in Table I and the lower SER in Fig. 7 are the expected consequence of sending two bits per channel use, not evidence that entanglement improves PQC-BERT. To support the claim that 'entanglement does indeed improve PQC-BERT's performance', the comparison must be repeated with a classical baseline set to the same effective per-bit error rate (e.g., λ/2) or with an explicit resource-normalized analysis.
- [Appendix C and Fig. 4] The simulation of amplitude damping is described only as 'applying probabilistic noise to randomly selected qubits'. The amplitude-damping channel defined in Table II has Kraus operators K0 = diag(1, sqrt(1-λ)) and K1 = [[0, sqrt(λ)], [0,0]], which is not a Pauli channel. A random bit/phase flip does not reproduce the correct action on Bell states (for instance, K1 maps |1⟩ to |0⟩, changing the population and producing correlated errors that differ from Pauli flips). Without a faithful CPTP-map simulation or an explicit demonstration that the Bell-measurement error statistics coincide with those of the simplified model, the amplitude-damping entries in Fig. 4 and the claim of robustness across 'four distinct quantum noise models' are not supported. Please either implement the correct channel for all four models or restrict the claims to the channels actually simulated.
- [Sec. III.C, Fig. 7 and Appendix E] The qubit-vs-qudit comparison likewise lacks per-information-bit normalization. A qudit of dimension d = 4 transmits log2(4^2)=4 classical bits per channel use, twice as many as a qubit, and the qudit bit-flip noise defined in Table II has a different effect per encoded bit than either the qubit or the classical baseline. Without normalizing the noise strength to the probability of error per transmitted information bit (or specifying a fair cost per channel use), the conclusion that 'increased entanglement leads to improved transmission performance' is not established. The authors should re-analyze the data under a matched per-bit error rate, or clearly state that the advantage is only in raw channel-use efficiency, not in per-bit error resilience.
minor comments (6)
- [Sec. II.C.1] The subsection heading reads 'Word-Level Repairing Module (SLRM)', but the acronym defined and used elsewhere is WLRM; please correct the heading.
- [Abstract and Sec. III.C] The phrase 'successfully corrects nearly all of the errors' overstates the numerical results: after PQC-BERT, the sentence error rate remains around 24% at λ=0.01 (Sec. III.C and Fig. 4). Please align the wording with the reported SER values.
- [Sec. III.D] The claim that PQC-BERT operates 'without prior knowledge of the noise model or parameters' is only partially demonstrated. The training data are corrupted by the same noise models and apparently the same parameter range used in testing; please clarify what variation of noise parameters and models appears in the training set to justify the 'arbitrary noise conditions' wording.
- [Table I and Appendix D] The metrics Accuracy, Precision, Recall, and F1 are defined at the sentence level, while Sec. III.B discusses word-level correction. Please clarify the evaluation granularity to avoid confusion when interpreting Table I.
- [Fig. 8 / Appendix F] The explanation that the character 'x' in the decoded text is a generic placeholder for any non-alphabetic error character is important for interpreting the example; consider moving it to the main text near the figure instead of only in Appendix F.
- [References] Reference [46] (an integrated space-to-ground quantum communication network) appears in the list of sentiment-analysis BERT works; please verify that all citations in Sec. I are placed under the correct claims.
Circularity Check
No significant circularity: the SER-reduction claim is a supervised held-out evaluation, not a fit to its own inputs.
full rationale
The paper's central claim is that PQC-BERT, a BERT-based post-decoding module with a word-level dictionary corrector and a sentence-level correction/evaluation network, lowers sentence error rates on text corrupted by simulated quantum noise. This is an empirical machine-learning claim, not a derivation from first principles. The training pipeline is explicit: during training, WLRM-corrected text Tw is the input and the original text T is the target (Algorithm 1, Appendix C); the data is split 80:10:10 and metrics are computed on held-out test text. Thus the reported error reduction is not equivalent to a fitted parameter or to a self-definitional quantity. The protocol does not rely on any uniqueness theorem or ansatz imported from the authors' prior work; self-citations such as refs. [4], [7], [19], [31], and [79] are background or future-direction citations and are not load-bearing. Two weaknesses exist but they are correctness issues rather than circularity. First, the classical-vs-quantum comparison in Sec. III.B and Table I fixes the same bit-flip rate lambda on the classical bit channel and on the transmitted qubit; for superdense coding a single-qubit bit-flip changes the Bell outcome zx to z(x XOR 1) with probability lambda, leaving the z bit untouched, so the per-information-bit error rate is lambda/2 for the quantum path and lambda for the classical path. The higher quantum F1 and lower SER therefore reflect an unnormalized baseline, not a demonstrated entanglement-assisted enhancement of PQC-BERT; this is a benchmark-validity problem, not a circular derivation. Second, the Appendix C amplitude-damping simulation is described as probabilistic flips on randomly selected qubits rather than the CPTP map in Table II, which undermines trust in that channel's numbers but is again a modeling and credibility issue. The paper's own Discussion limits the results to simulated noise, saying the datasets are 'masked with simulated quantum noise,' which is consistent with a non-circular but simulation-only claim.
Assumptions & free parameters
free parameters (4)
- Focal loss alpha =
not reported
- Focal loss gamma =
not reported
- Loss combination weight theta =
not reported
- BERT fine-tuning learning rate =
based on prior work [85]
assumptions (3)
- domain assumption Natural language text has sufficient statistical redundancy for a pre-trained language model to predict and correct corrupted words.
- ad hoc to paper The noise simulation, which applies probabilistic bit/phase flips to randomly selected qubits, faithfully reproduces the four quantum channels (bit-flip, phase-flip, depolarizing, amplitude damping) defined in Appendix A.
- ad hoc to paper The classical communication baseline is an independent per-bit bit-flip channel with the same noise probability as the per-qubit channel.
Cite this review
Pith. "Pith review of Language Model for Large-Text Transmission in Noisy Quantum Communications." pith.science (2026). https://pith.science/paper/W3THB3DJ
@misc{pith2026250420842,
author = {Pith},
title = {Pith review of: Language Model for Large-Text Transmission in Noisy Quantum Communications},
year = {2026},
howpublished = {\url{https://pith.science/paper/W3THB3DJ}},
note = {Machine review of arXiv:2504.20842}
}
read the original abstract
Quantum communication has the potential to revolutionize information processing, providing unparalleled security and increased capacity compared to its classical counterpart by using the principles of quantum mechanics. However, the presence of noise remains a major barrier to realizing these advantages. While strategies like quantum error correction and mitigation have been developed to address this challenge, they often come with substantial overhead in physical qubits or sample complexity, limiting their practicality for large-scale information transfer. Here, we present an alternative approach: applying machine learning frameworks from natural language processing to enhance the performance of noisy quantum communications, focusing on superdense coding. By employing bidirectional encoder representations from transformers (BERT), a model known for its capabilities in natural language processing, we demonstrate improvements in information transfer efficiency without resorting to conventional error correction or mitigation techniques. These results mark a step toward the practical realization of a scalable and resilient quantum internet.
Figures
Figures from the paper (5 more)
Reference graph
Works this paper leans on
-
[1]
Athirdpartypreparedthe maximallyentangledstate |Φ00⟩anddistributedittothe sender, Alice, and the receiver, Bob
EntanglementDistribution. Athirdpartypreparedthe maximallyentangledstate |Φ00⟩anddistributedittothe sender, Alice, and the receiver, Bob
-
[2]
Alice encodes two bits of classical informa- tion zx∈{ 0, 1}2 into one of the Bell states|Φzx⟩ by applying Pauli operationsZ(z)X(x) to her qubit
Encoding. Alice encodes two bits of classical informa- tion zx∈{ 0, 1}2 into one of the Bell states|Φzx⟩ by applying Pauli operationsZ(z)X(x) to her qubit
-
[3]
Alice then sends her qubit to Bob through the noisy quantum channelE
Noisy Communication. Alice then sends her qubit to Bob through the noisy quantum channelE
-
[4]
ASCII encoding
Decoding. Upon receiving the qubit from Alice, Bob performs a Bell measurement. Based on the measure- mentoutcome,Bobdecodestheclassicalinformation zx that Alice encoded. A schematic representation of the superdense coding proto- colisprovidedinFig.1(b). BysubstitutingthePauligateswith Heisenberg-Weyloperators,wecanreadilyextendtheprotocol fromthequbitcas...
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[5]
ASCII encoding
Word-Level Repairing Module (SLRM) We begin by introducing our word-level repairing module (WLRM).Foragivenword wq i, derivedfromsuperdensecod- ing and subsequently mapped through the inverse mapping A−1 of the “ASCII encoding”, we assess its validity against thepredefineddictionary Dict. Ifwq i isfoundin Dict,werede- finewq i asww i and proceed to the ne...
-
[6]
Thecorrection network utilizes BERT [34] to analyze the linguistic context effectively
Sentence-Level Repairing Module (SLRM) Oursentence-levelrepairingmodule(SLRM)isconstructed using BERT and comprises two interconnected networks: the correctionnetworkandtheevaluationnetwork. Thecorrection network utilizes BERT [34] to analyze the linguistic context effectively. However, we have observed that BERT tends to recommendchangesevenwhentheorigin...
-
[7]
Specifically, we consider the ideal text,T , a quote attributed to Albert Einstein: “Imagination is more FIG
Text Transmission through Noisy Channels Here,weemployPQC-BERTtotransmitatextandevaluate its performance. Specifically, we consider the ideal text,T , a quote attributed to Albert Einstein: “Imagination is more FIG. 2. Efficient Text Transmission with PQC-BERT.In each round of noisy communication, errors manifest in differ- entways. Wepresenttwoexamples,w...
-
[8]
Thismetricquantifiestheratioof erroneous bits to the total number of bits transmitted
BitErrorRate(BER). Thismetricquantifiestheratioof erroneous bits to the total number of bits transmitted. It is affected by the channel’s noise parameters, providing valuable insights into the system’s sensitivity to noise, its interference suppression capabilities, and its overall communication capacity – making it a crucial metric in information theory
Show all 95 references
-
[9]
Thismetricassessesthepro- portionoferrorswithintransmitteddatablocks, defined as the number of erroneous words divided by the total numberoftransmittedwords
WordErrorRate(WER). Thismetricassessesthepro- portionoferrorswithintransmitteddatablocks, defined as the number of erroneous words divided by the total numberoftransmittedwords. Iteffectivelyevaluatesthe quality of transmission at the word level
-
[10]
ASCII encoding
Sentence Error Rate (SER).This metric measures the performanceofourtextcommunicationprotocolbycal- culating the ratio of erroneous sentences to the total number of sentences transmitted. It provides valuable insightintotheprotocol’saccuracyatthesentencelevel. Figure 3 visualiz...
-
[11]
Bouwmeester, J
D. Bouwmeester, J. W. Pan, K. Mattle, and et al., Experimental quantum teleportation, Nature390, 575 (1997)
1997
-
[12]
Gisin and R
N. Gisin and R. Thew, Quantum communication, Nature Pho- tonics1, 165 (2007)
2007
-
[13]
Cozzolino, B
D. Cozzolino, B. Da Lio, D. Bacco, and L. K. Oxenløwe, High- dimensional quantum communication: Benefits, progress, and future challenges, Quantum Science and Technology5, 043001 (2019)
2019
-
[14]
J.Xing, Y.Li,D.Qu,L.Xiao,Z.Fan,H.Ma,P.Xue, K.Bharti, D.E.Koh,andY.Xiao,Teleportationwithembezzlingcatalysts, Communications Physics7, 357 (2024)
2024
-
[15]
Hu, C.-X
X.-M. Hu, C.-X. Huang, Y.-B. Sheng, L. Zhou, B.-H. Liu, Y. Guo, C. Zhang, W.-B. Xing, Y.-F. Huang, C.-F. Li, and G.- C. Guo, Long-distance entanglement purification for quantum communication, Phys. Rev. Lett.126, 010503 (2021)
2021
-
[16]
X.-M. Hu, C. Zhang, B.-H. Liu, et al. , Experimental high- dimensionalquantumteleportation,Phys.Rev.Lett. 125,230501 (2020)
2020
-
[17]
J. Xing, T. Feng, Z. Fan, H. Ma, K. Bharti, D. E. Koh, and Y.Xiao,Fundamentallimitationsoncommunicationoveraquan- tum network (2023), arXiv:2306.04983 [quant-ph]
2023 arXiv
-
[18]
J.-G. Ren, P. Xu, H.-L. Yong, L. Zhang, S.-K. Liao, J. Yin, W.-Y. Liu, W.-Q. Cai, M. Yang, L. Li,et al., Ground-to-satellite quantum teleportation, Nature549, 70 (2017)
2017
-
[19]
Liao, W.-Q
S.-K. Liao, W.-Q. Cai, W.-Y. Liu, L. Zhang, Y. Li, J.-G. Ren, et al.,Satellite-to-groundquantumkeydistribution,Nature 549, 43 (2017)
2017
-
[20]
C.-Y. Lu, Y. Cao, C.-Z. Peng, and J.-W. Pan, Micius quantum experiments in space, Rev. Mod. Phys.94, 035001 (2022)
2022
-
[21]
Li, W.-Q
Y. Li, W.-Q. Cai, J.-G. Ren, ,et al., Microsatellite-based real- time quantum key distribution, Nature640, 47 (2025)
2025
-
[22]
Yin, J.-G
J. Yin, J.-G. Ren, H. Lu,et al., Quantum teleportation and en- tanglementdistributionover100-kilometrefree-spacechannels, Nature488, 185 (2012)
2012
-
[23]
J. L. Liu, X. Y. Luo, Y. Yu, and et al., Creation of mem- ory–memory entanglement in a metropolitan quantum network, Nature629, 579 (2024)
2024
-
[24]
C. M. Knaut, A. Suleymanzade, Y. C. Wei, and et al., Entan- glement of nanophotonic quantum memory nodes in a telecom network, Nature629, 573 (2024)
2024
-
[25]
C. H. Bennett, P. W. Shor, J. A. Smolin, and A. V. Thapliyal, Entanglement-assistedclassicalcapacityofnoisyquantumchan- nels, Phys. Rev. Lett.83, 3081 (1999)
1999
-
[26]
Harrow, P
A. Harrow, P. Hayden, and D. Leung, Superdense coding of quantum states, Phys. Rev. Lett.92, 187901 (2004)
2004
-
[27]
J. T. Barreiro, T.-C. Wei, and P. G. Kwiat, Beating the chan- nel capacity limit for linear photonic superdense coding, Nature Physics4, 282 (2008)
2008
-
[28]
X.-M. Hu, Y. Guo, B.-H. Liu, Y.-F. Huang, C.-F. Li, and G.-C. Guo, Beating the channel capacity limit for superdense coding with entangled ququarts, Science Advances4, eaat9304 (2018)
2018
-
[29]
Y. Li, J. Xing, D. Qu, L. Xiao, Z. Fan, Z.-J. Zheng, H. Ma, P.Xue,K.Bharti,D.E.Koh,andY.Xiao,Communicationwith quantum catalysts (2024), arXiv:2406.14395 [quant-ph]
2024
-
[30]
Knill and R
E. Knill and R. Laflamme, Theory of quantum error-correcting codes, Phys. Rev. A55, 900 (1997)
1997
-
[31]
T. Aoki, G. Takahashi, T. Kajiya, and et al., Quantum error correction beyond qubits, Nature Physics5, 541 (2009)
2009
-
[32]
B. M. Terhal, Quantum error correction for quantum memories, Rev. Mod. Phys.87, 307 (2015)
2015
-
[33]
Krinner, N
S. Krinner, N. Lacroix, A. Remm, and et al., Realizing repeated quantumerrorcorrectioninadistance-threesurfacecode,Nature 605, 669 (2022)
2022
-
[34]
V. V. Sivak, A. Eickbusch, B. Royer, and et al., Real-time quan- tum error correction beyond break-even, Nature616, 50 (2023)
2023
-
[35]
Liu and S
Z.-W. Liu and S. Zhou, Approximate symmetries and quantum error correction, npj Quantum Information9, 119 (2023)
2023
-
[36]
Z.-W.LiuandS.Zhou,Ageneraltheoryofquantumcodescon- necting quantum computation, complexity and physics, Nature Physics20, 1708 (2024)
2024
-
[37]
S. Endo, S. C. Benjamin, and Y. Li, Practical quantum error mitigation for near-future applications, Phys. Rev. X8, 031027 (2018)
2018
-
[38]
Z. Cai, R. Babbush, S. C. Benjamin, S. Endo, W. J. Huggins, Y. Li, J. R. McClean, and T. E. O’Brien, Quantum error mitiga- tion, Rev. Mod. Phys.95, 045005 (2023)
2023
-
[39]
Takagi, H
R. Takagi, H. Tajima, and M. Gu, Universal sampling lower bounds for quantum error mitigation, Phys. Rev. Lett. 131, 210602 (2023)
2023
-
[40]
Takagi, S
R. Takagi, S. Endo, S. Minagawa, and M. Gu, Fundamental limits of quantum error mitigation, npj Quantum Information8, 11 (2022)
2022
-
[41]
Z. Liu, Y. Xiao, and Z. Cai, Non-markovian noise sup- pression simplified through channel representation (2024), arXiv:2412.11220 [quant-ph]
2024 arXiv
-
[42]
M. Liao, Y. Zhu, G. Chiribella, and Y. Yang, Noise-agnostic quantum error mitigation with data augmented neural models, npj Quantum Information11, 8 (2025)
2025
-
[43]
Gomez,L.u.Kaiser,andI.Polosukhin,Attentionisallyouneed, Advances in Neural Information Processing Systems30(2017)
A.Vaswani,N.Shazeer,N.Parmar,J.Uszkoreit,L.Jones,A.N. Gomez,L.u.Kaiser,andI.Polosukhin,Attentionisallyouneed, Advances in Neural Information Processing Systems30(2017)
2017
-
[44]
Devlin, M.-W
J. Devlin, M.-W. Chang, K. Lee, and K. Toutanova, BERT: Pre-training of deep bidirectional transformers for language un- derstanding, Proceedings of the 2019 Conference of the North American Chapter of the Association for Computational Lin- guistics: Human Language Technologie...
2019
-
[45]
Bello, S.-C
A. Bello, S.-C. Ng, and M.-F. Leung, A bert framework to sen- timent analysis of tweets, Sensors23, 506 (2023)
2023
-
[46]
Cao and C
J. Cao and C. Lai, A bilingual multi-type spam detection model based on m-bert, GLOBECOM 2020-2020 IEEE Global Com- munications Conference , 1 (2020)
2020
-
[47]
C.Oswald,S.E.Simon,andA.Bhattacharya,Spotspam: Inten- tionanalysis–drivensmsspamdetectionusingbertembeddings, ACM Transactions on the Web (TWEB)16, 1 (2022)
2022
-
[48]
Hakala and S
K. Hakala and S. Pyysalo, Biomedical named entity recogni- tion with multilingual bert, Proceedings of the 5th workshop on BioNLP open shared tasks , 56 (2019). 10
2019
-
[49]
Chang, L
Y. Chang, L. Kong, K. Jia, and Q. Meng, Chinese named entity recognitionmethodbasedonbert,2021IEEEinternationalcon- ference on data science and computer application (ICDSCA) , 294 (2021)
2021
-
[50]
Z. Yang, Z. Dai, Y. Yang, J. Carbonell, R. Salakhutdinov, and Q. V. Le, Xlnet: generalized autoregressive pretraining for lan- guageunderstanding,Proceedingsofthe33rdInternationalCon- ference on Neural Information Processing Systems (2019)
2019
-
[51]
Z.Liu,W.Lin,Y.Shi,andJ.Zhao,Arobustlyoptimizedbertpre- training approach with post-training, Chinese Computational LinguisticsLNCS 13175, 471 (2021)
2021
-
[52]
Z. Lan, M. Chen, S. Goodman, K. Gimpel, P. Sharma, and R. Soricut, Albert: A lite bert for self-supervised learning of language representations (2020), arXiv:1909.11942 [cs.CL]
2020 arXiv
-
[53]
M.Hoang,O.A.Bihorac,andJ.Rouces,Aspect-basedsentiment analysis using bert, Proceedings of the 22nd nordic conference on computational linguistics , 187 (2019)
2019
-
[54]
H. Xu, B. Liu, L. Shu, and S. Y. Philip, Bert post-training for reviewreadingcomprehensionandaspect-basedsentimentanal- ysis,Proceedingsofthe2019ConferenceoftheNorthAmerican Chapter of the Association for Computational Linguistics: Hu- manLanguageTechnologies,Volume1(LongandSh...
2019
-
[55]
M. G. Sousa, K. Sakiyama, L. d. S. Rodrigues, P. H. Moraes, E. R. Fernandes, and E. T. Matsubara, Bert for stock market sentimentanalysis,2019IEEE31stInternationalConferenceon Tools with Artificial Intelligence (ICTAI) , 1597 (2019)
2019
-
[56]
Y. Cao, Q. Zhang, T.-Y. Chen,et al., An integrated space-to- groundquantumcommunicationnetworkover4,600kilometres, Nature589, 214 (2021)
2021
-
[57]
N. J. Prottasha, A. A. Sami, M. Kowsher, S. A. Murad, A. K. Bairagi,M.Masud,andM.Baz,Transferlearningforsentiment analysis using bert based supervised fine-tuning, Sensors22, 4157 (2022)
2022
-
[58]
Zhang, H
S. Zhang, H. Huang, J. Liu, and H. Li, Spelling error correction with soft-masked bert, Proceedings of the 58th Annual Meeting of the Association for Computational Linguistics , 882 (2020)
2020
-
[59]
M. Tan, D. Chen, Z. Li, and P. Wang, Spelling error correction with bert based on character-phonetic, 2020 IEEE 6th Interna- tional Conference on Computer and Communications (ICCC) , 1146 (2020)
2020
-
[60]
T. T. H. Nguyen, A. Jatowt, N.-V. Nguyen, M. Coustaty, and A. Doucet, Neural machine translation with bert for post-ocr error detection and correction, Proceedings of the ACM/IEEE joint conference on digital libraries in 2020 , 333 (2020)
2020
-
[61]
Horodecki, P
R. Horodecki, P. Horodecki, M. Horodecki, and K. Horodecki, Quantum entanglement, Rev. Mod. Phys.81, 865 (2009)
2009
-
[62]
Khatri and M
S. Khatri and M. M. Wilde, Principles of quantum communi- cation theory: A modern approach (2024), arXiv:2011.04672 [quant-ph]
2024 arXiv
-
[63]
96, 190501 (2006)
C.Schuck,G.Huber,C.Kurtsiefer,andH.Weinfurter,Complete deterministiclinearopticsbellstateanalysis,Phys.Rev.Lett. 96, 190501 (2006)
2006
-
[64]
Hodosh, P
M. Hodosh, P. Young, and J. Hockenmaier, Framing image de- scriptionasarankingtask: Data,modelsandevaluationmetrics, Journal of Artificial Intelligence Research47, 853 (2013)
2013
-
[65]
Warstadt, A
A. Warstadt, A. Singh, and S. R. Bowman, A corpus for mod- eling rich morphological agreement, Proceedings of the 2019 Conference of the North American Chapter of the Association forComputationalLinguistics: HumanLanguageTechnologies, Volume 1 (Long and Short Papers) , 4186 (2019)
2019
-
[66]
Beltagy, M
I. Beltagy, M. E. Peters, and A. Cohan, Longformer: The long- document transformer (2020), arXiv:2004.05150 [cs.CL]
2020 arXiv
-
[67]
Zaheer, G
M. Zaheer, G. Guruganesh, A. Dubey, J. Ainslie, C. Alberti, S. Ontanon, P. Pham, A. Ravula, Q. Wang, L. Yang, and A.Ahmed,Bigbird: Transformersforlongersequences(2021), arXiv:2007.14062 [cs.CL]
2021 arXiv
-
[68]
Chatterjee, K
A. Chatterjee, K. Phalak, and S. Ghosh, Quantum error cor- rection for dummies, 2023 IEEE International Conference on Quantum Computing and Engineering (QCE)01, 70 (2023)
2023
-
[69]
J.Carrasquilla,Machinelearningforquantummatter,Advances in Physics: X5, 1797528 (2020)
2020
-
[70]
R.G.Melko,G.Carleo,J.Carrasquilla,andJ.I.Cirac,Restricted boltzmannmachinesinquantumphysics,NaturePhysics 15,887 (2019)
2019
-
[71]
G.CarleoandM.Troyer,Solvingthequantummany-bodyprob- lem with artificial neural networks, Science355, 602 (2017)
2017
-
[72]
Carrasquilla and R
J. Carrasquilla and R. G. Melko, Machine learning phases of matter, Nature Physics13, 431 (2017)
2017
-
[73]
Wallnöfer, A
J. Wallnöfer, A. A. Melnikov, W. Dür, and H. J. Briegel, Ma- chine learning for long-distance quantum communication, PRX Quantum1, 010301 (2020)
2020
-
[74]
Lloyd, Quantum machine learning, Nature549, 195 (2017)
J.Biamonte,P.Wittek,N.Pancotti,P.Rebentrost,N.Wiebe,and S. Lloyd, Quantum machine learning, Nature549, 195 (2017)
2017
-
[75]
Dunjko and H
V. Dunjko and H. J. Briegel, Machine learning & artificial in- telligence in the quantum domain: a review of recent progress, Reports on Progress in Physics81, 074001 (2018)
2018
-
[76]
N. Guo, Z. Yu, M. Choi, A. Agrawal, K. Nakaji, A. Aspuru- Guzik,andP.Rebentrost,Quantumlinearalgebraisallyouneed for transformer architectures (2024), arXiv:2402.16714 [quant- ph]
2024
-
[77]
Z. Yu, Q. Chen, Y. Jiao, Y. Li, X. Lu, X. Wang, and J. Z. Yang, Non-asymptotic approximation error bounds of parameterized quantum circuits (2024), arXiv:2310.07528 [quant-ph]
2024 arXiv
-
[78]
E. A. Cherrat, I. Kerenidis, N. Mathur, J. Landman, M. Strahm, and Y. Y. Li, Quantum vision transformers, Quantum8, 1265 (2024)
2024
-
[79]
J. Tian, X. Sun, Y. Du, S. Zhao, Q. Liu, K. Zhang, W. Yi, W. Huang, C. Wang, X. Wu, M.-H. Hsieh, T. Liu, W. Yang, and D. Tao, Recent advances for quantum neural networks in generative learning, IEEE Transactions on Pattern Analysis and Machine Intelligence45, 12321 (2023)
2023
-
[80]
X. Wang, J. Liu, T. Liu, Y. Luo, Y. Du, and D. Tao, Symmetric pruning in quantum neural networks (2023), arXiv:2208.14057 [quant-ph]
2023 arXiv
-
[81]
Slussarenko and G
S. Slussarenko and G. J. Pryde, Photonic quantum informa- tion processing: A concise review, Applied Physics Reviews 6, 041303 (2019)
2019
-
[82]
C.FabreandN.Treps,Modesandstatesinquantumoptics,Rev. Mod. Phys.92, 035005 (2020)
2020
-
[83]
Y. Yuan, Y. Xiao, Z. Hou, S.-M. Fei, G. Gour, G.-Y. Xiang, C.- F. Li, and G.-C. Guo, Strong majorization uncertainty relations and experimental verifications, npj Quantum Information9, 65 (2023)
2023
-
[84]
Rivas and S
A. Rivas and S. F. Huelga,Open Quantum Systems: An Intro- duction (Springer, 2012)
2012
-
[85]
F. A. Pollock, C. Rodríguez-Rosario, T. Frauenheim, M. Pater- nostro,andK.Modi,Non-markovianquantumprocesses: Com- plete framework and efficient characterization, Phys. Rev. A97, 012127 (2018)
2018
-
[86]
D.A.Lidar,Lecturenotesonthetheoryofopenquantumsystems (2020), arXiv:1902.00967 [quant-ph]
2020 arXiv
-
[87]
S.MilzandK.Modi,Quantumstochasticprocessesandquantum non-markovian phenomena, PRX Quantum2, 030201 (2021)
2021
-
[88]
Y. Xiao, K. Sengupta, S. Yang, and G. Gour, Uncertainty prin- ciple of quantum processes, Phys. Rev. Res.3, 023077 (2021)
2021
-
[89]
Y. Xiao, Y. Yang, X. Wang, Q. Liu, and M. Gu, Quantum un- certainty principles for measurements with interventions, Phys. Rev. Lett.130, 240201 (2023)
2023
-
[90]
Taranto, S
P. Taranto, S. Milz, M. Murao, M. T. Quintino, and K. Modi, Higher-order quantum operations (2025), arXiv:2503.09693 [quant-ph]. 11
2025 arXiv
-
[91]
Gottesman, Theory of fault-tolerant quantum computation, Phys
D. Gottesman, Theory of fault-tolerant quantum computation, Phys. Rev. A57, 127 (1998)
1998
-
[92]
D. A. Lidar and T. A. Brun, eds.,Quantum Error Correction (Cambridge University Press, Cambridge, 2013)
2013
-
[93]
Gottesman, Surviving as a quantum computer in a classical world, Textbook manuscript preprint (2024)
D. Gottesman, Surviving as a quantum computer in a classical world, Textbook manuscript preprint (2024)
2024
-
[94]
Ross and G
T.-Y. Ross and G. Dollár, Focal loss for dense object detection, proceedings of the IEEE conference on computer vision and pattern recognition , 2980 (2017)
2017
-
[95]
x” in the decoded text serve as generic error indicators: they do not represent corrupted instances of the letter “x
A. J. Quijano, S. Nguyen, and J. Ordonez, Grid search hyperpa- rameter benchmarking of bert, albert, and longformer on duorc (2021), arXiv:2101.06326 [cs.CL]. Appendix A: Noise Models In a closed quantum system, the evolution of the quantum state is reversible and governed by u...
2021 arXiv
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