Decoherence Resilience of the Non-Hermitian Skin Effect
Pith reviewed 2026-05-10 14:49 UTC · model grok-4.3
The pith
The non-Hermitian skin effect survives dephasing and can be enhanced by it even in the fully incoherent regime.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
In photonic quantum walks realizing non-Hermitian dynamics, the skin effect that concentrates probability at one boundary persists under dephasing decoherence through the fully incoherent limit and produces larger drift velocities than coherent evolution; for amplitude damping the outcome is order-dependent, with preceding damping eliminating the effect in the incoherent limit while subsequent damping permits persistence and enhancement at strong loss.
What carries the argument
Photonic quantum walks with independently tunable dephasing and amplitude-damping channels applied before or after the non-Hermitian loss operator, used to track the evolution of asymmetric probability distributions that signal the skin effect.
Load-bearing premise
The two engineered decoherence channels in the photonic walk fully represent the relevant environmental interactions and introduce no additional effects that would change the observed skin-effect behavior.
What would settle it
Measurement of drift velocities under strong dephasing that remain equal to or smaller than the coherent case, or complete disappearance of boundary accumulation in the fully incoherent limit regardless of damping order, would falsify the reported resilience.
Figures
read the original abstract
Decoherence and dissipation, arising from unavoidable interactions with the environment, can exert a dual influence on transport in physical systems, suppressing coherent propagation while inducing diffusion and mitigating localization in disordered systems. Non-Hermitian physics reveals a qualitatively different scenario, in which structured dissipation can induce directional bulk-to-boundary transport, known as the non-Hermitian skin effect (NHSE), that remains robust against disorder. Whether such transport can persist, be enhanced or hindered under decoherence, remains a largely open question. Here we experimentally address this question using photonic quantum walks with two tunable prototypical decoherence channels, dephasing and amplitude damping. Under dephasing, the NHSE survives up to the fully incoherent regime and is observed to even be enhanced by dephasing, yielding drift velocities that exceed those of coherent dynamics. By contrast, amplitude damping shows a pronounced order dependence: applied before the non-Hermitian loss operator, it suppresses and ultimately eliminates the NHSE in the fully incoherent limit; applied afterward, the NHSE persists and can be enhanced at sufficiently large loss strengths. Our work bridges quantum and classical non-Hermitian dynamics, demonstrates the resilience of the NHSE to decoherence, and opens avenues for harnessing decoherence to enhance directional transport in noisy, nonequilibrium systems.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript experimentally investigates the resilience of the non-Hermitian skin effect (NHSE) to decoherence using photonic discrete-time quantum walks. It demonstrates that dephasing preserves the NHSE up to the fully incoherent regime and can enhance drift velocities beyond coherent dynamics, while amplitude damping exhibits a pronounced dependence on whether it is applied before or after the non-Hermitian loss operator, suppressing the NHSE in one ordering but allowing persistence or enhancement in the other.
Significance. If the reported qualitative contrasts and order dependence hold under quantitative scrutiny, the work provides direct experimental evidence bridging quantum and classical non-Hermitian transport, establishes decoherence resilience of the NHSE, and suggests practical routes to harness environmental noise for directional transport in open systems. The photonic platform's tunability of two distinct Lindblad channels is a notable strength for isolating channel-specific effects.
major comments (2)
- [Results section on dephasing] Results on dephasing (likely §4 or equivalent): the claim that drift velocities exceed coherent dynamics requires explicit comparison of extracted velocities with error bars against the coherent baseline; without this, the 'enhancement' assertion rests on qualitative observation alone and cannot be assessed for statistical significance.
- [Methods and amplitude-damping results] Amplitude-damping order-dependence experiments: the manuscript must clarify how the two application orders are realized in the discrete-step protocol (e.g., interleaving of loss operator and damping channel) to ensure the observed suppression vs. persistence is not an artifact of the specific pulse sequence or timing.
minor comments (2)
- [Figure captions] Figure captions should explicitly state the number of experimental realizations, binning procedure for probability distributions, and fitting method used to extract drift velocities.
- [Throughout] Notation for the non-Hermitian loss operator and the two Lindblad channels should be unified between the abstract, main text, and supplementary material to avoid ambiguity in the order-dependence discussion.
Simulated Author's Rebuttal
We thank the referee for their careful reading of the manuscript, positive assessment of its significance, and recommendation for minor revision. We address each major comment below and have revised the manuscript to incorporate the suggested improvements.
read point-by-point responses
-
Referee: [Results section on dephasing] Results on dephasing (likely §4 or equivalent): the claim that drift velocities exceed coherent dynamics requires explicit comparison of extracted velocities with error bars against the coherent baseline; without this, the 'enhancement' assertion rests on qualitative observation alone and cannot be assessed for statistical significance.
Authors: We agree that quantitative support with error bars is required to rigorously establish the enhancement. While the original figures display the qualitative trend, we have revised the dephasing results section to include a new panel (or supplementary figure) reporting the extracted drift velocities with error bars obtained from multiple independent experimental runs. These values are directly compared to the coherent-dynamics baseline, and the text has been updated to reference the statistical significance of the observed enhancement. revision: yes
-
Referee: [Methods and amplitude-damping results] Amplitude-damping order-dependence experiments: the manuscript must clarify how the two application orders are realized in the discrete-step protocol (e.g., interleaving of loss operator and damping channel) to ensure the observed suppression vs. persistence is not an artifact of the specific pulse sequence or timing.
Authors: We appreciate this request for clarification. In the revised Methods section we now explicitly describe the two orders: the 'before' configuration applies the amplitude-damping channel immediately prior to the non-Hermitian loss operator in each discrete time step, while the 'after' configuration applies the damping channel immediately after the loss operator. A schematic of the pulse sequence and timing for both orderings has been added to demonstrate that the reported suppression versus persistence arises from the intended channel ordering rather than from any implementation artifact. revision: yes
Circularity Check
No significant circularity; purely experimental observations
full rationale
The paper reports direct experimental measurements in a photonic discrete-time quantum walk realizing non-Hermitian evolution plus two Lindblad channels (dephasing and amplitude damping). No mathematical derivation, fitted parameter, or prediction is claimed; the central results (NHSE survival/enhancement under dephasing, order-dependent suppression under amplitude damping) are read out from observed probability distributions and drift velocities. The work contains no self-citation load-bearing steps, no ansatz smuggling, and no reduction of outputs to inputs by construction. The experimental protocol is self-contained against the stated observables.
Axiom & Free-Parameter Ledger
free parameters (2)
- dephasing strength
- amplitude damping strength
axioms (1)
- domain assumption The photonic quantum walk with added loss operator accurately models the non-Hermitian skin effect in the presence of the two specified decoherence channels.
Reference graph
Works this paper leans on
-
[1]
The system then evolves fortsteps asρ t =U tρ0U †t. Decoherence bridges the quantum and classical walks, pro- viding a tunable pathway from coherent quantum evolution to classical stochastic dynamics [54]. Here we focus on two ubiquitous forms of decoherence, dephasing and ampli- tude damping, whose combined action can effectively cap- ture a wide variety...
-
[2]
Zurek, W. H. Decoherence, einselection, and the quantum ori- gins of the classical.Rev. Mod. Phys.75, 715–775 (2003)
work page 2003
-
[3]
Plenio, M. B. & Huelga, S. F. Dephasing-assisted transport: quantum networks and biomolecules.New J. Phys.10, 113019 (2008)
work page 2008
-
[4]
Caruso, F., Chin, A. W., Datta, A., Huelga, S. F. & Plenio, M. B. Highly efficient energy excitation transfer in light-harvesting complexes: The fundamental role of noise-assisted transport. J. Chem. Phys.131, 105106 (2009)
work page 2009
-
[5]
Viciani, S., Lima, M., Bellini, M. & Caruso, F. Observation of noise-assisted transport in an all-optical cavity-based network. Phys. Rev. Lett.115, 083601 (2015)
work page 2015
-
[6]
Bender, C. M. Making sense of non-Hermitian Hamiltonians. Rep. Prog. Phys.70, 947 (2007)
work page 2007
- [7]
-
[8]
Parity-time symmetry meets photonics: A new twist in non-Hermitian optics.Europhys
Longhi, S. Parity-time symmetry meets photonics: A new twist in non-Hermitian optics.Europhys. Lett.120, 64001 (2017)
work page 2017
- [9]
-
[10]
Bergholtz, E. J., Budich, J. C. & Kunst, F. K. Exceptional topol- ogy of non-Hermitian systems.Rev. Mod. Phys.93, 015005 (2021)
work page 2021
-
[11]
Hu, J.et al.Non-Hermitian swallowtail catastrophe revealing transitions among diverse topological singularities.Nat. Phys. 19, 1098–1103 (2023)
work page 2023
-
[12]
Xiao, L.et al.Non-Hermitian physics in photonic systems. Photon. Insights4, R09 (2025)
work page 2025
-
[13]
He, Y . & Ozawa, T. Anomalous wave-packet dynamics in one-dimensional non-Hermitian lattices.arXiv preprint arXiv:2512.07484(2025)
- [14]
-
[15]
Xue, P.et al.Self acceleration from spectral geometry in dissipative quantum-walk dynamics.Nat. Commun.15, 4381 (2024)
work page 2024
-
[16]
Sun, Y .et al.Photonic Floquet skin-topological effect.Phys. Rev. Lett.132, 063804 (2024)
work page 2024
- [17]
-
[18]
Xing, Z.-Y ., Chen, S. & Hu, H. Universal spreading dynam- ics in quasiperiodic non-Hermitian systems.Phys. Rev. B111, L180203 (2025)
work page 2025
-
[19]
Chen, W., ¨Ozdemir, S. K., Zhao, G., Wiersig, J. & Yang, L. Exceptional points enhance sensing in an optical microcavity. Nature548, 192–196 (2017)
work page 2017
-
[20]
Kononchuk, R., Cai, J., Ellis, F., Thevamaran, R. & Kottos, T. Exceptional-point-based accelerometers with enhanced signal- to-noise ratio.Nature607, 697–702 (2022)
work page 2022
-
[21]
Xiao, L.et al.Non-Hermitian sensing in the absence of excep- tional points.Phys. Rev. Lett.133, 180801 (2024)
work page 2024
-
[22]
Gong, Z.et al.Topological phases of non-Hermitian systems. Phys. Rev. X8, 031079 (2018)
work page 2018
- [23]
-
[24]
Wang, K.et al.Generating arbitrary topological windings of a non-Hermitian band.Science371, 1240–1245 (2021)
work page 2021
-
[25]
Song, W.et al.Observation of Weyl interface states in non- Hermitian synthetic photonic systems.Phys. Rev. Lett.130, 043803 (2023)
work page 2023
-
[26]
Liang, J.et al.Twist-induced non-Hermitian topology of exciton–polaritons.Nat. Phys.22, 151–157 (2026)
work page 2026
- [27]
-
[28]
Kunst, F. K., Edvardsson, E., Budich, J. C. & Bergholtz, E. J. Biorthogonal bulk-boundary correspondence in non-Hermitian systems.Phys. Rev. Lett.121, 026808 (2018)
work page 2018
- [29]
- [30]
- [31]
-
[32]
Wang, W., Wang, X. & Ma, G. Non-Hermitian morphing of topological modes.Nature608, 50–55 (2022)
work page 2022
- [33]
- [34]
-
[35]
Erratic non-Hermitian skin localization.Phys
Longhi, S. Erratic non-Hermitian skin localization.Phys. Rev. Lett.134, 196302 (2025)
work page 2025
-
[36]
Wei, Z., Fan, J.-Y ., Cao, K., Ma, X.-R. & Kou, S.- P. Generalized non-Hermitian skin effect.arXiv preprint arXiv:2505.10252(2025)
work page internal anchor Pith review arXiv 2025
-
[37]
Li, Y ., Liang, C., Wang, C., Lu, C. & Liu, Y .-C. Gain-loss- induced hybrid skin-topological effect.Phys. Rev. Lett.128, 223903 (2022)
work page 2022
-
[38]
Liang, Q.et al.Dynamic signatures of non-Hermitian skin effect and topology in ultracold atoms.Phys. Rev. Lett.129, 070401 (2022)
work page 2022
-
[39]
Li, Z.et al.Observation of dynamic non-Hermitian skin effects. Nat. Commun.15, 6544 (2024)
work page 2024
-
[40]
Zhao, E.et al.Two-dimensional non-Hermitian skin effect in an ultracold fermi gas.Nature637, 565–573 (2025)
work page 2025
-
[41]
Longhi, S., Gatti, D. & Della Valle, G. Robust light transport in 8 non-Hermitian photonic lattices.Sci. Rep.5, 13376 (2015)
work page 2015
-
[42]
Li, L., Lee, C. H. & Gong, J. Topological switch for non- Hermitian skin effect in cold-atom systems with loss.Phys. Rev. Lett.124, 250402 (2020)
work page 2020
-
[43]
Gu, Z.et al.Transient non-Hermitian skin effect.Nat. Com- mun.13, 7668 (2022)
work page 2022
-
[44]
Zhu, B.et al.Anomalous single-mode lasing induced by non- linearity and the non-Hermitian skin effect.Phys. Rev. Lett. 129, 013903 (2022)
work page 2022
-
[45]
Jiang, T.et al.Observation of non-Hermitian boundary induced hybrid skin-topological effect excited by synthetic complex fre- quencies.Nat. Commun.15, 10863 (2024)
work page 2024
-
[46]
McDonald, A. & Clerk, A. A. Exponentially-enhanced quan- tum sensing with non-Hermitian lattice dynamics.Nat. Com- mun.11, 5382 (2020)
work page 2020
-
[47]
Zhou, X., Zhang, W., Cao, W. & Zhang, X. Non-Hermitian Flo- quet topological sensors for ultrasensitive detection of dynamic signals.Phys. Rev. Lett.135, 106601 (2025)
work page 2025
-
[48]
Sannia, A., Giorgi, G. L., Longhi, S. & Zambrini, R. Skin effect in quantum neural networks.Opt. Quantum3, 189 (2025)
work page 2025
-
[49]
Lin, Z.et al.Observation of topological transition in Floquet non-Hermitian skin effects in silicon photonics.Phys. Rev. Lett. 133, 073803 (2024)
work page 2024
-
[50]
Xiao, L.et al.Non-Hermitian bulk–boundary correspondence in quantum dynamics.Nat. Phys.16, 761–766 (2020)
work page 2020
- [51]
-
[52]
Kuo, P.-C.et al.Non-Markovian skin effect.Phys. Rev. Res.7, L012068 (2025)
work page 2025
-
[53]
Incoherent non-Hermitian skin effect in photonic quantum walks.Light
Longhi, S. Incoherent non-Hermitian skin effect in photonic quantum walks.Light. Sci. Appl.13, 95 (2024)
work page 2024
-
[54]
Brun, T. A., Carteret, H. A. & Ambainis, A. Quantum to clas- sical transition for random walks.Phys. Rev. Lett.91, 130602 (2003)
work page 2003
-
[55]
Schreiber, A.et al.Decoherence and disorder in quantum walks: from ballistic spread to localization.Phys. Rev. Lett. 106, 180403 (2011)
work page 2011
-
[56]
Engel, G. S.et al.Evidence for wavelike energy transfer through quantum coherence in photosynthetic systems.Nature 446, 782–786 (2007)
work page 2007
- [57]
-
[58]
H., Gerhards, L., Solov’yov, I
Alvarez, P. H., Gerhards, L., Solov’yov, I. A. & de Oliveira, M. C. Quantum phenomena in biological systems.Front. Quan- tum Sci. Technol.3, 1466906 (2024)
work page 2024
-
[59]
Lifshitz-like metastability and optimal dephasing in dissipative bosonic lattices.Front
Longhi, S. Lifshitz-like metastability and optimal dephasing in dissipative bosonic lattices.Front. Phys.21, 023201 (2026)
work page 2026
-
[60]
Sone, K., Yokomizo, K., Kawaguchi, K. & Ashida, Y . Hermi- tian and non-Hermitian topology in active matter.Rep. Prog. Phys.89, 016501 (2026)
work page 2026
-
[61]
Martinez, J. E., Fuentes, P., Crespo, P. M. & Garcia-Frias, J. Approximating decoherence processes for the design and simu- lation of quantum error correction codes on classical computers. IEEE Access8, 172623 (2020)
work page 2020
-
[62]
Martinez, E. J., Fuentes, P., Crespo, P. & Garcia-Frias, J. Time- varying quantum channel models for superconducting qubits. npj Quantum Inf.7, 115 (2021)
work page 2021
-
[63]
A.et al.Discrete single-photon quantum walks with tunable decoherence.Phys
Broome, M. A.et al.Discrete single-photon quantum walks with tunable decoherence.Phys. Rev. Lett.104, 153602 (2010)
work page 2010
-
[64]
Cardano, F.et al.Quantum walks and wavepacket dynamics on a lattice with twisted photons.Sci. Adv.1, e1500087 (2015)
work page 2015
-
[65]
Wang, B., Chen, T. & Zhang, X. Experimental observation of topologically protected bound states with vanishing Chern numbers in a two-dimensional quantum walk.Phys. Rev. Lett. 121, 100501 (2018)
work page 2018
-
[66]
Chiuri, A.et al.Experimental realization of optimal noise esti- mation for a general Pauli channel.Phys. Rev. Lett.107, 253602 (2011)
work page 2011
-
[67]
arXiv preprint arXiv:2510.27534(2025)
Fei, Y .-Y .et al.Experimental quantum channel purification. arXiv preprint arXiv:2510.27534(2025)
-
[68]
AcknowledgementsThis work is supported by the National Key R&D Program of China (Grant No
See Supplemental Material for more details. AcknowledgementsThis work is supported by the National Key R&D Program of China (Grant No. 2023YFA1406701) and the National Natural Science Foundation of China (Grant Nos. 12025401, 92265209, 12474352 and 92476106). S.L. acknowledges the Spanish Agencia Estatal de Investigacion (Grant No. MDM-2017-0711). K.K.W. ...
work page 2017
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.