REVIEW 2 major objections 4 minor 54 references
Resource quantification for programming low-depth quantum circuits
T0 review · 2 major / 4 minor · reviewed 2026-08-04 · deepseek-v4-flash
Pith's one-line read Programming a low-depth brickwork quantum circuit on N qubits, with allowed error ~ 1/polylog N, requires Θ(N polylog N) qubits of program memory in the worst case.
desk verdict The upper bound is clean and the problem is well chosen, but the lower bound that gives the Θ(N polylog N) claim imports a lemma whose hypothesis is not met, so the tightness result is not established. 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 central object is the program cost, the base-2 logarithm of the dimension of the subspace spanned by the processor's program states. The lower-bound machinery is the measure-and-operate programming framework together with Holevo information: an approximate unitary n-design supplies a hard ensemble, and a continuity bound on von Neumann entropy forces any successful processor's program states to contain many bits. The upper-bound machinery is the covering number of the set of brickwork-circuit unitaries, with a postselected processor that stores the index of the closest net point. The light-cone argument—grouping local gates into larger blocks—is the tool used to test whether layout infor
What would settle it
Construct a family of N-qubit low-depth brickwork circuits and an explicit programming scheme with program dimension exp(o(N polylog N)) that achieves diamond-norm error O(1/polylog N) on every circuit in the family; this would refute the claimed Ω(N polylog N) lower bound. A narrower test is whether the imported lemma's bound ||P_U − (U⊗I)^{⊗n}||_⋄ ≤ 4n√(2ε) can fail when U is restricted to the brickwork family; if it fails, the lower-bound proof collapses.
Extended reading notes
Core claim
The paper's central claim is that the program cost cP = log2 dP of an N-qubit low-depth brickwork circuit obeys a tight worst-case bound cP = Θ(N polylog N) when the diamond-norm error is ε ~ 1/polylog N. The lower bound is information-theoretic: feeding states created by an approximate unitary n-design through any ε-universal processor forces the program states to carry Ω(n log(d/n)) bits of Holevo information, and optimizing n gives Ω(N polylog N). The upper bound is combinatorial: an ε-net of brickwork-circuit unitaries has size roughly [(eN/k)^k (12ℓ/ε)^{2^{2k+1}}]^ℓ, so storing the index of the nearest net point costs O(N polylog N) qubits. The paper further claims that generic universa
Load-bearing premise
The lower bound assumes that a lemma proved for processors approximating every unitary in U(d) still holds for a processor required only to program low-depth circuits; the paper does not justify that the diamond-norm closeness to U^{⊗n} survives this restriction, and it also uses a cited low-depth unitary-design construction without re-proving it at the needed parameters.
Editorial extensions
If this is right
- The worst-case program cost for low-depth brickwork circuits is exactly Θ(N polylog N) at error ε ~ 1/polylog N; no asymptotically smaller memory scheme exists.
- Generic universal programming of arbitrary N-qubit unitaries requires exponentially more memory and gates (poly(2^N, 1/√ε)), so restricting to low-depth circuits is essential for practical programmable NISQ processors.
- Programming each constant-size local gate separately achieves the optimal scaling; light-cone reduction does not improve the asymptotic cost for generic local gates.
- As the allowed error ε goes to 0, the program cost diverges whenever √ε 2^N > 1, recovering the no-programming theorem in the exact limit.
- Programming and learning separate for low-depth circuits: some low-depth brickwork unitaries are hard to learn but can be programmed efficiently.
Reading between the lines
- Editorial inference: The lower-bound proof imports a lemma proven for processors that are ε-universal over all of U(d) into the restricted low-depth setting; if that lemma cannot be re-proven under restricted universality, the Ω(N polylog N) worst-case bound may be unsupported even though the upper bound is concrete.
- Editorial inference: The upper-bound construction assumes the sender knows a classical description of the target circuit (to pick the nearest net point), so this is a model of programming a known circuit, not learning an unknown one; the tight cost can be read as the storage price of that description.
- Editorial inference: The same Holevo-information and covering-number techniques should extend to other constant-degree circuit families and to 2D brickwork layouts; a testable prediction is that Θ(N polylog N) persists, with the polylog exponent set by allowed depth and geometry.
- Editorial inference: The commuting-Pauli example suggests a broader criterion—light-cone reduction saves memory when the effective parameter count per light-cone grows more slowly than the number of local gates it contains; other structured families satisfying this criterion may yield further savings.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. This paper studies the resources required to approximately program low-depth brickwork quantum circuits on N qubits. The main formal result claims a tight worst-case program cost Θ(N polylog N) when the programming error is ε ∼ 1/polylog N: Theorem 18 gives an Ω(N polylog N) lower bound based on Holevo information of approximate unitary designs supported on low-depth circuits, and Theorem 23 gives a matching O(N polylog N) upper bound via a covering-net construction. The paper also analyzes the gate complexity of the measure-and-operate programming scheme and discusses a light-cone reduction trade-off.
Significance. If the lower bound were established for processors restricted to the low-depth family, the tight Θ(N polylog N) characterization would be a meaningful advance over prior program-cost bounds, which are non-trivial only for constant N. The upper bound is simple and robust. The lower-bound strategy—comparing the Holevo information of program states for an approximate design with the Haar ensemble—is conceptually appealing and could be of independent interest. However, the proof currently imports a lemma whose hypothesis is not satisfied by the restricted processors appearing in the main claim.
major comments (2)
- [Theorem 18 / Lemma 14] The lower bound applies Lemma 14, stated for an ε-universal processor over all U(d), to a processor only required to program low-depth brickwork circuits. The design νκ is supported inside the low-depth family (Definition 7), which is not a group and is not closed under the twirls used in [16, Appendix A] to prove Lemma 14. Consequently the bound ||P_V-(V⊗I)^{⊗n}||⋄ ≤ 4n√(2ε) is not justified for each V in the support, and the chain (4)-(6) that transfers Holevo information from the ideal ensemble to the program states breaks at its first step. Since Theorem 23 constructs only a restricted processor, the claimed Θ(N polylog N) tightness is not established. Please either prove a restricted version of Lemma 14 with a V-independent K_C, supply an alternative lower bound, or clearly restrict Theorem 18 to full-U(d) universal processors (which would not match the upper bound). This is load-be
- [Theorem 18, proof] The proof assumes, citing [40], a diamond-norm κ-approximate n-design supported on 1D low-depth brickwork circuits with depth O(polylog N) for n=O(polylog N) and κ=Ω(2^{-polylog N}). The depth bound in Table 1 depends on a parameter ξ with t=O(2^{2ξ/5}); the authors should verify that the required range is covered by [40] and state the imported theorem precisely. This is not a criticism of [40] but a missing support in the present derivation.
minor comments (4)
- [Theorem 18, statement] The displayed lower bound contains the factor (1−ϖ/(4√(2ε))−1), which is negative for all allowed ϖ. From the proof, the intended factor is presumably ((1−ϖ)/(4√(2ε))−1); please correct.
- [Section 4, program dimension] d_P is defined as dim span{ψ_{P,U}|U∈U(d)}. For restricted processors the span should be over the programmed family U_{k,ℓ,D}; otherwise the Holevo bound χ(...)≤log d_P is vacuous if the processor is not defined outside the family.
- [Example 25] The claim [∏_{j=1}^k P_{q_j}, ∏_{j=1}^k P_{q'_j}]=0 for any q,q' is false when supports overlap and the Pauli types differ (e.g., X and Z on the same qubit anticommute). The light-cone simplification in the example relies on commutativity; as stated, the example is invalid.
- [Theorem 1 (informal)] The theorem calls the scheme 'optimal universal programming' but the section only proves an upper bound on gate complexity; the word 'optimal' is potentially misleading.
Circularity Check
No significant circularity: the central lower and upper bounds are independent derivations, and cited results are external evidence rather than inputs disguised as predictions.
full rationale
I walked the claimed derivation chain. The central lower bound (Theorem 18) is an information-theoretic argument: it uses Schur–Weyl dimension counting, Holevo information, and the Alicki–Fannes–Winter bound, and it imports Lemma 14 from [16] as a black box. Although [16] shares an author, Lemma 14 is a separately published, parameter-free statement about ε-universal processors over all of U(d); the present paper does not define any quantity in terms of the target program cost c_P, and the lemma does not include the low-depth result as an assumption. The upper bound (Theorem 23) is a clean covering-net counting argument with an explicit postselection processor construction (Eq. 9); again no parameter is fitted and no conclusion is assumed. Theorem 1 and the light-cone discussion restate or extend known complexity facts, not rename the target result. The most delicate point is that Theorem 18 applies Lemma 14 to a processor that may only need to program low-depth brickwork circuits, even though Lemma 14 is stated for full U(d) universality. That is a real hypothesis-mismatch / correctness risk: if the lemma requires full-group universality, the Ω(N polylog N) lower bound would not follow from the given proof. But this is not circularity, because nothing forces ||P_V − (V⊗I)^{⊗n}||⋄ ≤ 4n√(2ε) by definition of the restricted low-depth program family. Similarly, the use of the [40] unitary-design construction as a low-depth brickwork circuit is a cited external construction, not an assumption equivalent to the conclusion. The self-reference to [25] in Remark 19 is a comparison ("improves the bound"), not a load-bearing input. Therefore no circular step is present; the score is 0. If Lemma 14's hypotheses are not satisfied, the lower bound would be unproven, but that would be an open technical correctness issue, not circular derivation.
Assumptions & free parameters
free parameters (2)
- ϖ
- κ
assumptions (7)
- standard math Schur-Weyl duality (Lemma 6) holds for tensor powers of U(d).
- domain assumption Lemma 14 from [16]: for an ε-universal processor over U(d), channels P_U exist with ||P_U-(U⊗I)^⊗n||⋄≤4n√(2ε).
- domain assumption Polylog-depth approximate unitary t-designs with t=O(polylog N) exist on N qubits (Schuster, Haferkamp, Huang [40]).
- standard math Alicki-Fannes-Winter entropy continuity bound (Lemma 16).
- standard math Dimension identity d_n = binom(n+d^2-1, d^2-1) and the lower-bound inequality in Lemma 17.
- domain assumption Covering number bound for U(d) (Lemma 21 from [23]).
- domain assumption Error propagation across a brickwork circuit: ℓ gates each ε-close give total error ℓε (Lemma 13).
Cite this review
Pith. "Pith review of Resource quantification for programming low-depth quantum circuits." pith.science (2026). https://pith.science/paper/EISNVURP
@misc{pith2026250909642,
author = {Pith},
title = {Pith review of: Resource quantification for programming low-depth quantum circuits},
year = {2026},
howpublished = {\url{https://pith.science/paper/EISNVURP}},
note = {Machine review of arXiv:2509.09642}
}
abstract
Noisy intermediate-scale quantum (NISQ) devices pave the way for implementing quantum algorithms that offer quantum advantages over their classical counterparts. Due to the intrinsic noise and decoherence in the physical system, NISQ machines are naturally modeled as large-scale, low-depth quantum circuits. In practice, executing such circuits requires sending program states that encode the relevant instructions to a programmable quantum computer, typically through a cloud service. Existing programming approaches designed for generic unitary transformations are computationally inefficient in the low-depth setting, and therefore remain unsatisfactory. As such, to realize NISQ algorithms, it is crucial to find an efficient way to program low-depth circuits as the number of qubits $N$ increases. Here, we investigate the circuit complexity and the size of quantum memory, known as the program cost, required to program low-depth brickwork circuits. We establish a tight worst-case program cost of $\Theta(N \mathrm{polylog} N)$ for universally programming low-depth brickwork circuits in the large-$N$ regime. Moreover, we analyze the trade-off between the cost of describing the layout of local gates and the cost of programming them to implement the target unitaries via the light-cone argument. Our findings suggest that faithful gate-wise programming is essentially optimal in the low-depth regime.
Figures
Reference graph
Works this paper leans on
-
[16]
Optimal universal program- ming of unitary gates
Yuxiang Yang, Renato Renner, and Giulio Chiribella. “Optimal universal program- ming of unitary gates”. Phys. Rev. Lett.125, 210501 (2020)
2020
-
[40]
Random unitaries in extremely low depth
Thomas Schuster, Jonas Haferkamp, and Hsin-Yuan Huang. “Random unitaries in extremely low depth”. Science389, 92–96 (2025)
2025
-
[1]
Quantum Computing in the NISQ era and beyond
John Preskill. “Quantum Computing in the NISQ era and beyond”. Quantum2, 79 (2018)
2018
-
[2]
A fast quantum mechanical algorithm for database search
Lov K. Grover. “A fast quantum mechanical algorithm for database search”. In Pro- ceedingsofthe28thAnnualACMSymposiumonTheoryofComputing. Page212–219. STOC ’96New York, NY, USA (1996). Association for Computing Machinery
1996
-
[3]
Polynomial-time algorithms for prime factorization and discrete loga- rithms on a quantum computer
Peter W. Shor. “Polynomial-time algorithms for prime factorization and discrete loga- rithms on a quantum computer”. SIAM Journal on Computing26, 1484–1509 (1997)
1997
-
[4]
Quantum algorithm for linear systems of equations
Aram W. Harrow, Avinatan Hassidim, and Seth Lloyd. “Quantum algorithm for linear systems of equations”. Phys. Rev. Lett.103, 150502 (2009). 20
2009
-
[5]
Noisy intermediate-scale quantum algorithms
Kishor Bharti, Alba Cervera-Lierta, Thi Ha Kyaw, Tobias Haug, Sumner Alperin-Lea, Abhinav Anand, Matthias Degroote, Hermanni Heimonen, Jakob S. Kottmann, Tim Menke, Wai-Keong Mok, Sukin Sim, Leong-Chuan Kwek, and Alán Aspuru-Guzik. “Noisy intermediate-scale quantum algorithms”. Rev. Mod. Phys.94, 015004 (2022)
2022
-
[6]
Shallowquantumcircuits: Algorithms, complexity, andfaulttolerance
YunchaoLiu. “Shallowquantumcircuits: Algorithms, complexity, andfaulttolerance”. PhD thesis. University of California, Berkeley. (2024)
2024
Show all 54 references
-
[7]
Quantum advantage with shallow circuits
Sergey Bravyi, David Gosset, and Robert König. “Quantum advantage with shallow circuits”. Science362, 308–311 (2018)
2018
-
[8]
Exponential separation between shallow quantum circuits and unbounded fan-in shallow classical circuits
Adam Bene Watts, Robin Kothari, Luke Schaeffer, and Avishay Tal. “Exponential separation between shallow quantum circuits and unbounded fan-in shallow classical circuits”. In Proceedings of the 51st Annual ACM SIGACT Symposium on Theory of Computing. Page 515–526. STOC 2019New...
2019
-
[9]
Delegating private quantum computations
Anne Broadbent. “Delegating private quantum computations”. Canadian Journal of Physics93, 941–946 (2015)
2015
-
[10]
A one-query lower bound for unitary synthesis and breaking quantum cryptography
Alex Lombardi, Fermi Ma, and John Wright. “A one-query lower bound for unitary synthesis and breaking quantum cryptography”. In Proceedings of the 56th Annual ACM Symposium on Theory of Computing. Page 979–990. STOC 2024New York, NY, USA (2024). Association for Computing Machinery
2024
-
[11]
Programmable quantum gate arrays
M. A. Nielsen and Isaac L. Chuang. “Programmable quantum gate arrays”. Physical Review Letters79, 321–324 (1997)
1997
-
[12]
Probabilistic implementation of universal quantum processors
Mark Hillery, Vladimír Bužek, and Mário Ziman. “Probabilistic implementation of universal quantum processors”. Phys. Rev. A65, 022301 (2002)
2002
-
[13]
Measurement-based quantum computation beyond the one-way model
D. Gross, J. Eisert, N. Schuch, and D. Perez-Garcia. “Measurement-based quantum computation beyond the one-way model”. Phys. Rev. A76, 052315 (2007)
2007
-
[14]
Asymptotic teleportation scheme as a uni- versal programmable quantum processor
Satoshi Ishizaka and Tohya Hiroshima. “Asymptotic teleportation scheme as a uni- versal programmable quantum processor”. Phys. Rev. Lett.101, 240501 (2008)
2008
-
[15]
Resource quan- tification for the no-programing theorem
Aleksander M. Kubicki, Carlos Palazuelos, and David Pérez-García. “Resource quan- tification for the no-programing theorem”. Physical Review Letters122(2019)
2019
-
[17]
Programmability of covariant quantum channels
Martina Gschwendtner, Andreas Bluhm, and Andreas Winter. “Programmability of covariant quantum channels”. Quantum5, 488 (2021)
2021
-
[18]
Port-Based State Preparation and Appli- cations
Garazi Muguruza and Florian Speelman. “Port-Based State Preparation and Appli- cations”. Quantum8, 1573 (2024)
2024
-
[19]
Quantum advantage in storage and retrieval of isometry channels
Satoshi Yoshida, Jisho Miyazaki, and Mio Murao. “Quantum advantage in storage and retrieval of isometry channels” (2025). arXiv:2507.10784
2025 arXiv
-
[20]
Computational complexity: A modern approach
Sanjeev Arora and Boaz Barak. “Computational complexity: A modern approach”. Cambridge University Press. (2009)
2009
-
[21]
Linear growth of quantum circuit complexity
Jonas Haferkamp, Philippe Faist, Naga B. T. Kothakonda, Jens Eisert, and Nicole Yunger Halpern. “Linear growth of quantum circuit complexity”. Nature Physics18, 528–532 (2022). 21
2022
-
[22]
Approximatet-designs in generic circuit architectures
Daniel Belkin, James Allen, Soumik Ghosh, Christopher Kang, Sophia Lin, James Sud, Frederic T. Chong, Bill Fefferman, and Bryan K. Clark. “Approximatet-designs in generic circuit architectures”. PRX Quantum5, 040344 (2024)
2024
-
[23]
Learning quantum states and unitaries of bounded gate complex- ity
Haimeng Zhao, Laura Lewis, Ishaan Kannan, Yihui Quek, Hsin-Yuan Huang, and Matthias C. Caro. “Learning quantum states and unitaries of bounded gate complex- ity”. PRX Quantum5(2024)
2024
-
[24]
Learning shallow quantum circuits
Hsin-Yuan Huang, Yunchao Liu, Michael Broughton, Isaac Kim, Anurag Anshu, Zeph Landau, and Jarrod R. McClean. “Learning shallow quantum circuits”. In Proceedings of the 56th Annual ACM Symposium on Theory of Computing. Page 1343–1351. STOC 2024New York, NY, USA (2024). Associa...
2024
-
[25]
Compression of quantum shallow-circuit states
Yuxiang Yang. “Compression of quantum shallow-circuit states”. Phys. Rev. Lett.134(2025)
2025
-
[26]
Quantum computation and quantum infor- mation: 10th anniversary edition
Michael A. Nielsen and Isaac L. Chuang. “Quantum computation and quantum infor- mation: 10th anniversary edition”. Cambridge University Press. (2012)
2012
-
[27]
On the pauli spectrum ofQAC0
Shivam Nadimpalli, Natalie Parham, Francisca Vasconcelos, and Henry Yuen. “On the pauli spectrum ofQAC0”. In Proceedings of the 56th Annual ACM Symposium on Theory of Computing. Page 1498–1506. STOC ’24. ACM (2024)
2024
-
[28]
Symmetry, representations, and invariants
Roe Goodman and Nolan R. Wallach. “Symmetry, representations, and invariants”. Springer New York. (2009)
2009
-
[29]
Applications of coherent classical communication and the schur transform to quantum information theory
Aram W. Harrow. “Applications of coherent classical communication and the schur transform to quantum information theory”. PhD thesis. Massachusetts Institute of Technology. (2005)
2005
-
[30]
Simple Con- structions of Linear-Depth t-Designs and Pseudorandom Unitaries
Tony Metger, Alexander Poremba, Makrand Sinha, and Henry Yuen. “ Simple Con- structions of Linear-Depth t-Designs and Pseudorandom Unitaries ”. In 2024 IEEE 65th Annual Symposium on Foundations of Computer Science (FOCS). Pages 485–
2024
-
[31]
Exact and approximate unitary 2-designs and their application to fidelity estimation
Christoph Dankert, Richard Cleve, Joseph Emerson, and Etera Livine. “Exact and approximate unitary 2-designs and their application to fidelity estimation”. Phys. Rev. A80, 012304 (2009)
2009
-
[32]
Optimal quantum learning of a unitary transformation
Alessandro Bisio, Giulio Chiribella, Giacomo Mauro D’Ariano, Stefano Facchini, and Paolo Perinotti. “Optimal quantum learning of a unitary transformation”. Phys. Rev. A81, 032324 (2010)
2010
-
[33]
Scalable noise estimation with random unitary operators
Joseph Emerson, Robert Alicki, and Karol Zyczkowski. “Scalable noise estimation with random unitary operators”. Journal of Optics B: Quantum and Semiclassical Optics7, S347–S352 (2005)
2005
-
[34]
Creating superpositions that correspond to efficiently integrable probability distributions
Lov Grover and Terry Rudolph. “Creating superpositions that correspond to efficiently integrable probability distributions” (2002). arXiv:quant-ph/0208112
2002 arXiv
-
[35]
An efficient high dimensional quantum Schur transform
Hari Krovi. “An efficient high dimensional quantum Schur transform”. Quantum3, 122 (2019)
2019
-
[36]
Quantum state preparation with optimal circuit depth: Implementations and applications
Xiao-Ming Zhang, Tongyang Li, and Xiao Yuan. “Quantum state preparation with optimal circuit depth: Implementations and applications”. Phys. Rev. Lett.129, 230504 (2022)
2022
-
[37]
Approximate unitary t-designs by short ran- dom quantum circuits using nearest-neighbor and long-range gates
Aram W. Harrow and Saeed Mehraban. “Approximate unitary t-designs by short ran- dom quantum circuits using nearest-neighbor and long-range gates”. Communications in Mathematical Physics401, 1531–1626 (2023). 22
2023
-
[38]
Efficient approximate unitary designs from random pauli rotations
Jeongwan Haah, Yunchao Liu, and Xinyu Tan. “Efficient approximate unitary designs from random pauli rotations”. In 2024 IEEE 65th Annual Symposium on Foundations of Computer Science (FOCS). Pages 463–475. (2024)
2024
-
[39]
Incompressibility and spectral gaps of random circuits
Chi-Fang Chen, Jeongwan Haah, Jonas Haferkamp, Yunchao Liu, Tony Metger, and Xinyu Tan. “Incompressibility and spectral gaps of random circuits” (2024). arXiv:2406.07478
2024 arXiv
-
[41]
Optimal estimation of group transformations using entanglement
G. Chiribella, G. M. D’Ariano, and M. F. Sacchi. “Optimal estimation of group transformations using entanglement”. Phys. Rev. A72, 042338 (2005)
2005
-
[42]
Query-optimal estimation of unitary channels in diamond distance
Jeongwan Haah, Robin Kothari, Ryan O’Donnell, and Ewin Tang. “Query-optimal estimation of unitary channels in diamond distance”. In 2023 IEEE 64th Annual Symposium on Foundations of Computer Science (FOCS). Pages 363–390. (2023)
2023
-
[43]
Synthesis of quantum logic circuits
Vivek V. Shende, Stephen S. Bullock, and Igor L. Markov. “Synthesis of quantum logic circuits”. In Proceedings of the 2005 Asia and South Pacific Design Automation Conference. Page 272–275. ASP-DAC ’05New York, NY, USA (2005). Association for Computing Machinery
2005
-
[44]
Classical and quantum computation
Alexei Yu Kitaev, Alexander Shen, and Mikhail N Vyalyi. “Classical and quantum computation”. Number 47 in Graduate Studies in Mathematics. American Mathemat- ical Soc. (2002)
2002
-
[45]
Bounds for the quantity of information transmitted by a quantum communication channel
Alexander Semenovich Holevo. “Bounds for the quantity of information transmitted by a quantum communication channel”. Problemy Peredachi Informatsii9, 3–11 (1973). url:https://www.mathnet.ru/eng/ppi903
1973
-
[46]
Tight uniform continuity bounds for quantum entropies: Condi- tional entropy, relative entropy distance and energy constraints
Andreas Winter. “Tight uniform continuity bounds for quantum entropies: Condi- tional entropy, relative entropy distance and energy constraints”. Communications in Mathematical Physics347, 291–313 (2016)
2016
-
[47]
Asymptotic values for degrees associated with strips of young dia- grams
Amitai Regev. “Asymptotic values for degrees associated with strips of young dia- grams”. Advances in Mathematics41, 115–136 (1981)
1981
-
[48]
Optimal compression for identically prepared qubit states
Yuxiang Yang, Giulio Chiribella, and Masahito Hayashi. “Optimal compression for identically prepared qubit states”. Phys. Rev. Lett.117, 090502 (2016)
2016
-
[49]
On the computa- tional power ofQAC 0 with barely superlinear ancillae
Anurag Anshu, Yangjing Dong, Fengning Ou, and Penghui Yao. “On the computa- tional power ofQAC 0 with barely superlinear ancillae”. In Proceedings of the 57th Annual ACM Symposium on Theory of Computing. Page 1476–1487. STOC ’25New York, NY, USA (2025). Association for Computi...
2025
-
[50]
Operator lipschitz functions (english trans- lation)
Alexei Aleksandrov and Vladimir Peller. “Operator lipschitz functions (english trans- lation)” (2016). arXiv:1611.01593
2016 arXiv
-
[51]
Quantum state and unitary learn- ing implies circuit lower bounds
Nai-Hui Chia, Daniel Liang, and Fang Song. “Quantum state and unitary learn- ing implies circuit lower bounds”. In Nika Haghtalab and Ankur Moitra, edi- tors, Proceedings of Thirty Eighth Conference on Learning Theory. Volume 291 of Proceedings of Machine Learning Research, pa...
2025
-
[52]
On the geometry of stabi- lizer states
Héctor J. García, Igor L. Markov, and Andrew W. Cross. “On the geometry of stabi- lizer states”. Quantum Info. Comput.14, 683–720 (2014)
2014
-
[53]
Restrictions on realizable unitary operations imposed by symmetry and locality
Iman Marvian. “Restrictions on realizable unitary operations imposed by symmetry and locality”. Nature Physics18, 283–289 (2022). 23
2022
-
[492]
IEEE Computer Society
Los Alamitos, CA, USA (2024). IEEE Computer Society
2024
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