Recent comments from SciRate

Kishor Bharti Mar 31 2025 05:17 UTC

Congratulations! Just wanted to mention that we had proposed the weight-5 [[30,4,5]] code and several other such codes in https://arxiv.org/abs/2406.19151 (Page 3, Table 1 and the supplementary material.)

Konstantinos Meichanetzidis Mar 28 2025 17:59 UTC

Reminds me of a Nirvana song called "Smells like Quantum Advantage".

somearbitraryresearcher Mar 27 2025 21:42 UTC

How can emerging physical-layer security strategies be systematically integrated into 6G ISAC networks to simultaneously safeguard both communication data and sensing information, while preserving the ultra-low latency and dual functionality that define ISAC’s commercial appeal?

somearbitraryresearcher Mar 27 2025 21:42 UTC

How can the 6GStarLab mission, envisioned as an open, flexible in-orbit platform, enable experimentation of future 3GPP NTN standards across multiple frequency bands and optical links while ensuring reliability, scalability, and adaptability for diverse use cases in dynamic orbital environments?

somearbitraryresearcher Mar 27 2025 21:41 UTC

How can a networked ecosystem of autonomous and embodied AI agents, each potentially possessing distinct goals, learning algorithms, and generative foundation models, maintain consistent, coherent, and up-to-date shared knowledge while operating under dynamic network conditions and diverse task requ

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Bartosz Regula Mar 27 2025 10:10 UTC

Ludovico didn't let me do this :(

Gerardo Adesso Mar 27 2025 10:08 UTC

Shouldn't it actually be denoted by Ü, or would that be the umlaut umlaut information?

Arpit Dua Mar 27 2025 01:20 UTC

No problem, thank you!

Nouédyn Baspin Mar 26 2025 08:03 UTC

Oh that's so cool! Sorry I missed it. I'll add a reference to your work in a future update :)

Arpit Dua Mar 25 2025 21:25 UTC

Hi Nouédyn,

Congrats on your result! With regards to the open question that you stated about self-correcting memories in dimensions less than 4D, we wanted to share our [work which discusses self-correcting memories on fractal lattices][1] with Hausdorff dimension $D_H=4-\epsilon$, obtained by punc

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Ryan Babbush Mar 25 2025 20:46 UTC

Thanks to both of you for your explanations. All this makes sense except that I am not fully convinced that we even know for which instance *sizes* quantum advantage is expected. It is plausible to me that at the sizes where random instances become classically intractable, all instances either conce

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Zhiyuan Wang Mar 25 2025 12:17 UTC

Dear Markus,

Thank you for your explanations. I haven't yet read the full details of your paper, but I'm curious if it is possible to generalize your results from the symmetric group S_N to the braid group B_N, and also "rule out" non-Abelian anyons in 2D? Does it make sense to talk about "invar

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Craig Gidney Mar 25 2025 06:43 UTC

Ah, duh, it's not a 1d stabilizer code. It's local at each level, using only adjacent logical qubits, but each level is zoomed out so the global picture is not made up of local stabilizers.

Craig Gidney Mar 25 2025 06:36 UTC

Doesn't Jones et al's concatenated 1D construction from https://journals.aps.org/prx/pdf/10.1103/PhysRevX.8.021058 have a growing distance?

somearbitraryresearcher Mar 24 2025 09:49 UTC

The paper reads well but it is missing relevant secure ISAC works such as [R1]

=====

References

[R1] A. Bazzi and M. Chafii, “Secure Full Duplex Integrated Sensing and Communications,” in IEEE Transactions on Information Forensics and Security, vol. 19, pp. 2082-2097, 2024, doi: 10.1109/TIFS.2023

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somearbitraryresearcher Mar 24 2025 09:47 UTC

The paper introduces a dynamic array partitioning framework for monostatic ISAC systems to enhance sensing performance while supporting communication requirements. In particular, the paper formulates a joint optimization of transmit beamforming and array partitioning to minimize Bayesian Cramér-Rao

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somearbitraryresearcher Mar 24 2025 09:14 UTC

Indeed, such methods are especially crucial in 6G networks, where the importance of achieving high bandwidth efficiency and sustaining the connection in adverse conditions is significan. A significant adversity can come from satellite incumbents [R1] and coexistence which is of paramount importance

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Konstantinos Meichanetzidis Mar 21 2025 17:25 UTC

Thank you Ryan for the comment. As Tuomas says, we do make it clear in Sec V that we have only identify the instance *sizes* for which advantage is expected. I still think this is cool, though, and takes a non-trivial amount of work to benchmark this end-to-end quantum algorithm. This project is mos

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Borivoje Dakic Mar 19 2025 22:36 UTC

Dear All,

I would like to call attention to our paper [https://arxiv.org/abs/2306.05919, also Ref. 11], which appeared slightly before Zhiyuan’s paper and presents a very similar classification of generalized statistics, termed transtatistics. I am still reviewing the work by Manuel, Thomas, and M

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Alexander Schmidhuber Mar 17 2025 21:59 UTC

sure!

Mark M. Wilde Mar 17 2025 20:44 UTC

The explicit expression appeared even earlier in Eq. (4) of

https://arxiv.org/abs/1310.7178

for the special case of α = z = 1/2 .

Oscar Higgott Mar 17 2025 16:26 UTC

Thanks for pointing this out, we’ll update the paper with this information in the next version. We used 30 iterations of parallel sum-product BP and OSD combination sweep with order 60 (all using the ldpc library).

qodesign Mar 17 2025 15:05 UTC

BP-OSD has a lot of parameters which can have a big affect on performance and complexity. It would help if you explicitly specify these parameters; otherwise it's hard to compare decoders.

Konstantinos Meichanetzidis Mar 17 2025 03:47 UTC

+1 !

Tuomas Laakkonen Mar 17 2025 00:30 UTC

Indeed, I agree. To be honest, when we started this project we thought there would be obvious instances that work this way, but it turned out there weren't. We discuss this more explicitly in section 5. Perhaps some of the confusing parts are leftover from earlier drafts and should be reworded, than

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Ryan Babbush Mar 16 2025 16:55 UTC

Thanks Tuomas. I don’t doubt that there exist classically intractable instances of the Jones polynomial problem (the worst case complexity results you mention are sufficient for establishing that). The trouble is actually finding those hard instances without requiring inordinate quantum resources to

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Tuomas Laakkonen Mar 16 2025 01:29 UTC

Thanks for the kind words! I am interested in adapting this kind of approach to the Khovanov homology, and I have some questions about your quantum algorithm for this (I might email you about it, if that's alright).

Tuomas Laakkonen Mar 16 2025 01:23 UTC

Hi Ryan - I'm not aware of any explicit instances of this type, except those arising from the BQP/DQC1-completeness proofs of the problem, which seems like 'cheating' to me. So they certainly exist, conditional on P != BQP, but I'm not sure they are natural or interesting. On the other hand, it migh

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Markus P. Müller Mar 15 2025 05:22 UTC

Dear Zhiyuan,

thank you so much for your interest and your explanations! We agree that a key distinction is whether one demands invariance of *all* observables or just the local ones, and your interesting results are not in contradiction to ours.

Let us add a few clarifications; we are still t

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Ryan Babbush Mar 14 2025 18:36 UTC

Very interesting paper. You discuss that for random instances of the problem the coefficients of the Jones polynomial will exponentially concentrate, which prevents the quantum computer from efficiently providing a non-trivial estimate of the Jones polynomial. You also discuss instances of the probl

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MariusK Mar 11 2025 15:49 UTC

Dear Zhiyuan,

Thanks a lot for the clarifications!

Best wishes,
Marius

Alexander Schmidhuber Mar 10 2025 15:28 UTC

Congratulations on this excellent paper! It’s exciting to see that quantum algorithms for knot invariants are a promising tool for benchmarking and potentially even for near-term quantum advantage.

Shoham Jacoby Mar 09 2025 06:26 UTC

Ok, Thank you for the reply!

Yunzhe Zheng Mar 07 2025 23:55 UTC

Thanks for the question. Weak physical measurement will become weaker logical measurement if the logical measurement is performed by destructive measurement of all supported physical qubits. We focused on the destructive case because in MSD the measured logical qubits should be discarded and only th

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Zhiyuan Wang Mar 07 2025 11:40 UTC

Dear Marius and Thomas,

I just briefly read the first few sections of this interesting paper, and let me share my thoughts on this. While this paper probably rules out parastatistics in all few body systems, it does not rule out the emergent R-matrix parastatistics in topologically ordered system

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Shoham Jacoby Mar 05 2025 13:37 UTC

Thank you for the interesting read.

One thing that baffled me is the claim that weak physical measurement translates to weaker logical measurement. It sounds like this leads to quantum error correction becomes ineffective against weak physical measurements. How is this possible and what am I miss

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MariusK Mar 02 2025 18:01 UTC

Dear Manuel, Thomas, and Markus,

Thanks for the clarification! From just skimming through the paper superficially, I was indeed under the impression that Eq. (1) is a constant requirement.

Best wishes,
Marius

Thomas D. Galley Feb 27 2025 19:36 UTC

Dear Marius,

thanks very much for your interest and your thoughtful comments!
We agree that the paper by Wang and Hazzard is interesting. Indeed, we cite it and consider it as part of the motivation for our work. We think our results should apply there because all we assume is that there is *som

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Tzula Propp Feb 27 2025 12:31 UTC

This is a very nice overview, but it does QBism a bit of a disservice. Specifically, the motivation for QBism comes from interpreting quantum probabilities, not states, hence the connection to Bayes and a subsequent quantum Bayes theorem. The collapse problem as explained here doesn't distinguish cl

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MariusK Feb 26 2025 15:11 UTC

Great work!

There is one promising approach to parastatistics of which I am unsure whether it is covered by your framework. See e.g. this paper by Wang and Hazzard:

https://www.nature.com/articles/s41586-024-08262-7

They use the trick that guides us from Abelian gauge theories to non-Abelia

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Fernando Pastawski Feb 25 2025 19:49 UTC

Wow! This is quite the break though! Looking forward to reading it in detail!

Naibin Zhou Feb 23 2025 04:08 UTC

fantastic work!

Patricio Fuentes Feb 19 2025 17:45 UTC

Hi Anqi! Thank you for your comment. It's technically all-to-all, but with distributed entanglement systems as outlined in [Scalable Fault-Tolerant Quantum Technologies with Silicon Color Centers][1] it is possible to break the all-to-all scaling. Ultimately, there is a tradeoff between IO scaling a

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Lim Youngrong Feb 19 2025 14:55 UTC

Thanks for the second question. Corollary 2 applies to a general matrix with a norm greater than 1, resulting in an exponential additive error. However, in GBS cases, the norm of the corresponding matrix is strictly less than 1. For more details, please refer to S4 of the supplemental material.

Zhenghao Li Feb 19 2025 14:27 UTC

Thank you for your reply. Can you elaborate why your Hafnian approximation is efficient regardless of the matrix norm? I ask this, because in Corollary 2, the additive error does scale exponentially with the norm of the matrix. If I absorb this into the error epsilon, does the run-time then have an

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Lim Youngrong Feb 19 2025 14:04 UTC

Thank you for your interesting question! In general, the norm of a matrix is important, and approximating the hafnian of a matrix with a large norm naturally leads to a large additive error. However, specifically for a GBS circuit, we can efficiently approximate the corresponding hafnian regardless

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Zhenghao Li Feb 19 2025 10:50 UTC

Hi, exciting paper! In your Corollary 2, the efficiency of estimating the hafnian seems to also assume that the norm of the matrix needs to be inverse-polynomially bounded. Is that generally true for a GBS circuit that you propose to estimate the Hafnian with?

Guanyu Zhu Feb 17 2025 01:46 UTC

We have updated the manuscript to v2 (https://arxiv.org/abs/2501.19375). In particular, we have added a conjecture about the constant-depth equivalence between the skeleton and thickened qLDPC codes in Sec. VD, which will allow a direct implementation of a logical gate corresponding to a constant-d

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Anqi Gong Feb 12 2025 13:17 UTC

Congratulations on this wonderful result!!

Could you please comment on your depth-one assumption for implementing $\Pi_i CNOT_{i,\pi^{-1}(i)+n_r^2}$ for arbitrary permutation $\pi=\sigma_1\otimes \sigma_2$ (page 15)? For the physical implementation time to be independent of the size of the simplex

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Igor Sokolov Feb 11 2025 08:18 UTC

Super work! @Giulia Mazzola