pith. sign in

arxiv: 2604.05473 · v1 · submitted 2026-04-07 · 🪐 quant-ph · physics.optics

Non-Markovian exceptional points in waveguide quantum electrodynamics

Pith reviewed 2026-05-10 20:12 UTC · model grok-4.3

classification 🪐 quant-ph physics.optics
keywords non-Markovian exceptional pointswaveguide quantum electrodynamicsspontaneous emissiongiant atomsrelaxation dynamicsoscillatory decaytime-delayed feedback
0
0 comments X

The pith

Non-Markovian exceptional points arise in the relaxation dynamics of emitters in waveguides.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper establishes that exceptional points can appear directly in the spontaneous emission process within waveguide quantum electrodynamics when non-Markovian effects from time-delayed feedback or structured continua dominate. These points are identified by sharp transitions from exponential decay to oscillatory behavior, visible as real zeros in the excited-state amplitude of the emitter. The demonstration focuses on giant atoms with multiple coupling points to the waveguide and extends to collective emission from separated point-like emitters. A sympathetic reader would care because this shows how non-Markovian physics naturally hosts exceptional-point phenomena in open quantum systems without requiring specially engineered Hamiltonians.

Core claim

We demonstrate the emergence of exceptional points (EPs) in these highly non-Markovian waveguide-QED environments, i.e., non-Markovian EPs. These EPs appear directly in the relaxation dynamics as sharp transitions to oscillatory behavior, manifested by the appearance of real zeros in the excited-state amplitude. We analyze in detail the spontaneous emission of giant atoms with two or more coupling points, highlighting the mechanisms leading to non-Markovian EPs, and show that similar phenomena arise in other waveguide-QED settings, such as the collective spontaneous emission of spatially separated point-like emitters.

What carries the argument

Non-Markovian exceptional points, identified as points in parameter space where the excited-state amplitude develops real zeros that trigger a transition from monotonic decay to oscillatory relaxation.

If this is right

  • Non-Markovian EPs can be realized and tuned in giant-atom configurations by adjusting the number and positions of coupling points.
  • The same transition to oscillatory relaxation appears in collective spontaneous emission from multiple spatially separated emitters.
  • Waveguide-QED platforms become accessible experimental arenas for studying non-Markovian EP physics through ordinary spontaneous emission.
  • The EPs are diagnosed purely from the time-domain amplitude dynamics rather than from eigenvalue coalescence in an effective non-Hermitian matrix.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Similar non-Markovian EPs may appear in other open systems with delayed feedback, such as atoms near mirrors, without needing waveguide-specific geometry.
  • The appearance of real zeros suggests a general route to oscillatory decay in non-Markovian quantum optics that could be tested by varying the separation between coupling points in a single experiment.
  • If confirmed, these points could serve as sensitive probes of dispersion relations or weak loss channels in real waveguides.

Load-bearing premise

The analysis assumes ideal linear dispersion relations in the waveguide and neglects additional loss channels or fabrication imperfections.

What would settle it

A direct measurement of the excited-state population of a giant atom with two coupling points at a separation that the theory predicts should produce a real zero would either show the onset of oscillations at the calculated parameter value or show purely decaying behavior without zeros.

Figures

Figures reproduced from arXiv: 2604.05473 by Stefano Longhi.

Figure 1
Figure 1. Figure 1: FIG. 1. (a) Schematic of a two-level giant atom radiating into a one [PITH_FULL_IMAGE:figures/full_fig_p004_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Behavior of a few dominant poles [PITH_FULL_IMAGE:figures/full_fig_p005_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Numerically-computed spontaneous emission decay of the [PITH_FULL_IMAGE:figures/full_fig_p006_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Numerically-computed spontaneous emission decay of a gi [PITH_FULL_IMAGE:figures/full_fig_p007_4.png] view at source ↗
read the original abstract

Spontaneous emission of a quantum emitter, such as an excited atom, is a fundamental process in quantum electrodynamics (QED), typically associated with exponential decay to the ground state accompanied by irreversible photon emission. This simple Markovian picture, however, is profoundly modified in the presence of time-delayed feedback, structured continua, or cooperative emission, as occurs when an emitter radiates in front of a mirror, when several emitters radiate collectively, or in the case of a giant atom. In such regimes, strong non-Markovian dynamics arise from photon reabsorption and interference effects, leading to pronounced deviations from exponential decay. Here we demonstrate the emergence of exceptional points (EPs) in these highly non-Markovian waveguide-QED environments, i.e., non-Markovian EPs. These EPs appear directly in the relaxation dynamics as sharp transitions to oscillatory behavior, manifested by the appearance of real zeros in the excited-state amplitude. We analyze in detail the spontaneous emission of giant atoms with two or more coupling points, highlighting the mechanisms leading to non-Markovian EPs, and show that similar phenomena arise in other waveguide-QED settings, such as the collective spontaneous emission of spatially separated point-like emitters. Our results reveal waveguide-QED systems as experimentally accessible platforms for realizing and exploring non-Markovian EP physics.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

0 major / 2 minor

Summary. The manuscript claims to demonstrate the emergence of non-Markovian exceptional points (EPs) in waveguide-QED systems. Through analytical solutions of the non-Markovian dynamics equations for giant atoms with multiple coupling points and for collective emission from spatially separated point emitters, the authors identify EPs as sharp transitions to oscillatory relaxation behavior, manifested by the appearance of real zeros in the excited-state amplitude under linear dispersion relations.

Significance. If the central derivations hold, this work is significant for extending EP physics into experimentally relevant non-Markovian regimes of waveguide QED. The analytical treatment of time-delayed feedback and interference effects in idealized models provides a clear link between non-Markovian dynamics and observable dynamical transitions, which could guide experiments in superconducting circuits or photonic waveguides. Credit is due for the direct identification of EPs via real zeros in the amplitude without reduction to fitted parameters.

minor comments (2)
  1. The discussion of experimental feasibility would be strengthened by a brief paragraph addressing how fabrication imperfections or additional loss channels (the weakest assumption noted in the analysis) might affect the visibility of the real zeros in the excited-state amplitude.
  2. Standardize notation for propagation delays and coupling strengths across the giant-atom and collective-emitter sections to improve readability.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for the positive summary, significance assessment, and recommendation of minor revision. No specific major comments were provided in the report.

Circularity Check

0 steps flagged

No significant circularity detected

full rationale

The paper's central demonstration proceeds by direct solution of the integro-differential or delay-differential equations for the excited-state amplitude under linear dispersion and multiple coupling points (giant atoms or collective emitters). The non-Markovian EPs are identified as the parameter values at which the amplitude develops real zeros, marking the onset of oscillatory relaxation; this identification follows mathematically from the structure of the equations themselves without any fitted parameters, self-referential definitions, or load-bearing self-citations that reduce the result to prior unverified claims. The derivation remains self-contained within the idealized model and does not rename known empirical patterns or smuggle ansatzes via citation chains.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The claim rests on standard waveguide-QED models with geometric parameters (coupling points, delays) treated as tunable inputs rather than derived quantities.

free parameters (1)
  • coupling strengths and propagation delays
    These are chosen to realize the giant-atom or collective-emitter geometries that produce the reported zeros and oscillations.
axioms (1)
  • domain assumption Linear dispersion relation in the waveguide and neglect of higher-order photon processes
    Standard assumption invoked when writing the equations of motion for the excited-state amplitude.

pith-pipeline@v0.9.0 · 5526 in / 1206 out tokens · 34774 ms · 2026-05-10T20:12:37.407554+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

What do these tags mean?
matches
The paper's claim is directly supported by a theorem in the formal canon.
supports
The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends
The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses
The paper appears to rely on the theorem as machinery.
contradicts
The paper's claim conflicts with a theorem or certificate in the canon.
unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Reference graph

Works this paper leans on

21 extracted references · 21 canonical work pages · 1 internal anchor

  1. [1]

    Non-Markovian exceptional points in waveguide quantum electrodynamics

    However, this simple pic- ture is profoundly modified in structured environments or in collective atom emission, where memory effects, interference, and time-delayed feedback become relevant3–11. A paradigmatic example is provided by a point-like two- level emitter radiating in front of a mirror 12–16. In this case, the finite round-trip time of photons i...

  2. [2]

    Berechnung der natürlichen Linienbreite auf Grund der Diracschen Lichttheorie,

    4g1g3 (41) τ=− 4vg π g1g3 g2 2(g1 +g 3)2 .(42) By lettingϕ=0, condition (41) provides a constraint on the coupling constantsg 1,g 2,g 3, whereas Eq.(42) yields the condition on the delay timeτ=d/v g. Note that, sinceτ should be positive, the conditiong 1g3 <0 is necessary to obtain a third-order EP. For example, assumingg 1 =g 2 and ϕ=0, the third-order E...

  3. [3]

    Light interference from single atoms and their mirror images,

    10J. Eschner, C. Raab, F. Schmidt-Kaler, and R. Blatt, "Light interference from single atoms and their mirror images,"Nature413(2001): 495-498. 11A. F. van Loo, A. Fedorov, K. Lalumiere, B. C. Sanders, A. Blais, and A. Wallraff, "Photon-mediated interactions between distant artificial atoms," Science342(2013): 1494-1496. 12R. J. Cook and P. W. Milonni, "Q...

  4. [4]

    Designing frequency- dependent relaxation rates and Lamb shifts for a giant artificial atom,

    18A. F. Kockum, P. Delsing, and G. Johansson, “Designing frequency- dependent relaxation rates and Lamb shifts for a giant artificial atom,” Phys. Rev. A90(2014): 013837. 19M. V . Gustafsson, T. Aref, A. F. Kockum, M. K. Ekström, G. Johansson, and P. Delsing, “Propagating phonons coupled to an artificial atom,”Sci- ence346(2014): 207–211. 20L. Guo, A. L. ...

  5. [5]

    Beyond spontaneous emission: Giant atom bounded in the continuum,

    28S. Guo, Y . Wang, T. Purdy, and J. Taylor, “Beyond spontaneous emission: Giant atom bounded in the continuum,”Phys. Rev. A102(2020): 033706. 29W. Zhao and Z. Wang, “Single-photon scattering and bound states in an atom-waveguide system with two or multiple coupling points,”Phys. Rev. A101(2020): 053855. 30X. Wang, T. Liu, A. F. Kockum, H.-R. Li, and F. N...

  6. [6]

    Non- reciprocal and chiral single-photon scattering for giant atoms,

    33Y .-T. Chen, L. Du, L. Guo, Z. Wang, Y . Zhang, Y . Li, and J.-H. Wu, “Non- reciprocal and chiral single-photon scattering for giant atoms,”Commun. Phys.5(2022):

  7. [7]

    Giant atoms in a synthetic frequency dimension,

    34L. Du, Y . Zhang, J.-H. Wu, A. F. Kockum, and Y . Li, “Giant atoms in a synthetic frequency dimension,”Phys. Rev. Lett.128(2022): 223602. 35W. Cheng, Z. Wang, and Y .-X. Liu, “Topology and retardation effect of a giant atom in a topological waveguide,”Phys. Rev. A106(2022): 033522. 36Y . T. Zhu, S. Xue, R. B. Wu, W. L. Li, Z. H. Peng, and M. Jiang, “Spa...

  8. [8]

    Oscillating bound states in non- Markovian photonic lattices,

    41K. H. Lim, W.-K. Mok, and L.-C. Kwek, “Oscillating bound states in non- Markovian photonic lattices,”Phys. Rev. A107(2023): 023716. 42X. Zhang, C. Liu, Z. Gong, and Z. Wang, “Quantum interference and con- trollable magic cavity QED via a giant atom in a coupled resonator waveg- uide,”Phys. Rev. A108(2023): 013704. 43C. Joshi, F. Yang, and M. Mirhosseini...

  9. [9]

    Gong, Z.-Y

    54L. Du, Y . Zhang, and Y . Li, “A giant atom with modulated transition fre- quency,”Front. Phys.18(2023): 12301. 55L. Du, L. Guo, Y . Zhang, and A. F. Kockum, “Giant emitters in a struc- tured bath with non-Hermitian skin effect,”Phys. Rev. Research5(2023): L042040. 56X. Wang, H.-B. Zhu, T. Liu, and F. Nori, “Realizing quantum optics in structured enviro...

  10. [10]

    Microwave photonics with superconducting quantum circuits,

    69X. Gu, A. F. Kockum, A. Miranowicz, Y .-x. Liu, and F. Nori, “Microwave photonics with superconducting quantum circuits,”Phys. Rep.718–719 (2017): 1–102. 70T. Kato,Perturbation Theory for Linear Operators(Springer, New York, 1966). 71W. D. Heiss, “The physics of exceptional points,”J. Phys. A: Math. Theor. 45(2012): 444016. 72M. V . Berry, “Physics of n...

  11. [11]

    Exceptional points in open quantum systems,

    73M. Muller and I. Rotter, “Exceptional points in open quantum systems,”J. Phys. A41(2008): 244018. 74M.-A. Miri and A. Alu, “Exceptional points in optics and photonics,”Sci- ence363(2019): eaar7709. 75S. K. Ozdemir, S. Rotter, F. Nori, and L. Yang, “Parity-time symmetry and exceptional points in photonics,”Nat. Mater.18(2019):

  12. [12]

    Quantum and classical exceptional points at the nanoscale: Properties and applications,

    76Y .-W. Lu, W. Li, and X.-H. Wang, “Quantum and classical exceptional points at the nanoscale: Properties and applications,”ACS Nano19(2025):

  13. [13]

    Topological energy transfer in an optomechanical system with exceptional points,

    77H. Xu, D. Mason, L. Jiang, and J. G. E. Harris, “Topological energy transfer in an optomechanical system with exceptional points,”Nature537 (2016):

  14. [14]

    Quantum state tomography across the exceptional point in a single dissipative qubit,

    78M. Naghiloo, M. Abbasi, Y . N. Joglekar, and K. W. Murch, “Quantum state tomography across the exceptional point in a single dissipative qubit,”Nat. Phys.15(2019): 1232–1236. 79F. Minganti, A. Miranowicz, R.W. Chhajlany, and F. Nori, "Quantum ex- ceptional points of non-Hermitian Hamiltonians and Liouvillians: The ef- fects of quantum jumps,"Phys. Rev. ...

  15. [15]

    Coalescence of non-Markovian dissipation, quantum Zeno effect, and non-Hermitian physics in a simple realistic quantum system,

    89G. Mouloudakis and P. Lambropoulos, “Coalescence of non-Markovian dissipation, quantum Zeno effect, and non-Hermitian physics in a simple realistic quantum system,”Phys. Rev. A106(2022): 053709. 90A. Wilkey, J. Suelzer, Y . N. Joglekar, and G. Vemuri, “Theoretical and ex- perimental characterization of non-Markovian anti-parity-time systems,” Commun. Ph...

  16. [16]

    Exceptional points in a non-Markovian anti-parity-time symmetric system,

    91A. Wilkey, Y . N. Joglekar, and G. Vemuri, “Exceptional points in a non-Markovian anti-parity-time symmetric system,”Photonics10(2023):

  17. [17]

    Emergent Liouvillian exceptional points from exact principles,

    92S. Khandelwal and G. Blasi, “Emergent Liouvillian exceptional points from exact principles,”Quantum9(2025):

  18. [18]

    Non-Markovian quantum exceptional points,

    93J.-D. Lin, P.-C. Kuo, N. Lambert, A. Miranowicz, F. Nori, and Y .-N. Chen, “Non-Markovian quantum exceptional points,”Nat. Commun.16(2025):

  19. [19]

    Experimental observation of non-Markovian quantum exceptional points,

    94H.-L. Zhang, P.-R. Han, F. Wu, W. Ning, Z.-B. Yang, and S.-B. Zheng, “Experimental observation of non-Markovian quantum exceptional points,”Phys. Rev. Lett.135(2025): 230203. 95S. Longhi, “Phase transitions and virtual exceptional points in quantum emitters coupled to dissipative baths,”J. Appl. Phys.138(2025): 184401. 96W. C. Wong, B. Zeng, and J. Li, ...

  20. [20]

    Analysis of a system of linear delay differential equations,

    105F. M. Asl and A. G. Ulsoy, “Analysis of a system of linear delay differential equations,”J. Dyn. Syst. Meas. Control125(2003):

  21. [21]

    Giant-cavity-based quantum sen- sors with enhanced performance,

    106Y . T. Zhu, R. Wu, Z. Peng, and S. Xue, “Giant-cavity-based quantum sen- sors with enhanced performance,”Frontiers in Physics10(2022): 896596. 107Q. Wu, X. Qi, B. Wu, M. Ren, Y . Xu, Z. Guo, H. Jiang, H. Chen, and Y . Sun, “Frequency-detuned exceptional surface assisted by the self- coherence effect of a giant atom,”Opt. Express33(2025): 20322–20333