pith. sign in

arxiv: 2204.02209 · v2 · submitted 2022-04-05 · 🪐 quant-ph · cond-mat.stat-mech

Robust multipartite entanglement in dirty topological wires

Pith reviewed 2026-05-24 11:42 UTC · model grok-4.3

classification 🪐 quant-ph cond-mat.stat-mech
keywords multipartite entanglementtopological phasesMajorana modesquantum Fisher informationKitaev chaindisordervariable-range pairingquantum wires
0
0 comments X

The pith

The quantum Fisher information scales with system size to reveal multipartite entanglement that tracks topological phases with Majorana modes even in disordered wires.

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

The paper studies a generalized Kitaev chain that allows variable-range pairing and different forms of site-dependent chemical potential, including commensurable, incommensurable, and Anderson disorder. It tracks multipartite entanglement through the scaling of the quantum Fisher information with system size. For nearest-neighbor pairing this scaling is Heisenberg-limited precisely in the topological phases that host Majorana modes. Longer-range pairing produces super-extensive scaling that marks new long-range phases whose diagrams contain lobe structures. The central finding is that this entanglement signature survives finite spatial inhomogeneity. A reader would care because the result supplies a concrete, measurable link between entanglement and topology in systems that are closer to real materials.

Core claim

For nearest-neighbour pairing the Heisenberg scaling of the QFI is found in one-to-one correspondence with topological phases hosting Majorana modes. For finite-range pairing, we recognize long-range phases by the super-extensive scaling of the QFI and characterize complex lobe-structured phase diagrams. Overall, we observe that ME is robust against finite strengths of spatial inhomogeneity.

What carries the argument

The scaling exponent of the quantum Fisher information (QFI) with system size N, used as a quantitative signature of multipartite entanglement in the ground state.

If this is right

  • Nearest-neighbor pairing produces a direct match between Heisenberg QFI scaling and the topological phases that contain Majorana zero modes.
  • Finite-range pairing generates super-extensive QFI scaling that identifies long-range topological phases.
  • The phase diagrams for variable-range pairing contain complex lobe structures.
  • Multipartite entanglement, as witnessed by QFI scaling, withstands finite-strength spatial inhomogeneity and Anderson disorder.

Where Pith is reading between the lines

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

  • QFI scaling could function as an experimental diagnostic for topological order in wires that inevitably contain disorder.
  • The same approach might be applied to other one-dimensional topological models to test whether entanglement signatures remain stable under realistic imperfections.
  • Incommensurable chemical-potential modulations may produce additional phase boundaries whose entanglement properties are not captured by the clean or periodically modulated limits.

Load-bearing premise

The scaling exponent of the quantum Fisher information with system size supplies a direct and unambiguous marker of multipartite entanglement that continues to map onto the presence of Majorana modes after variable-range pairing and site-dependent potentials are introduced.

What would settle it

A measurement showing sub-Heisenberg QFI scaling in the ground state of a clean nearest-neighbor Kitaev chain inside a known Majorana topological phase would falsify the claimed one-to-one correspondence.

read the original abstract

Identifying and characterizing quantum phases of matter in the presence of long range correlations and/or spatial disorder is, generally, a challenging and relevant task. Here, we study a generalization of the Kiteav chain with variable-range pairing and different site-dependence of the chemical potential, addressing commensurable and incommensurable modulations as well as Anderson disorder. In particular, we analyze multipartite entanglement (ME) in the ground state of the dirty topological wires by studying the scaling of the quantum Fisher information (QFI) with the system's size. For nearest-neighbour pairing the Heisenberg scaling of the QFI is found in one-to-one correspondence with topological phases hosting Majorana modes. For finite-range pairing, we recognize long-range phases by the super-extensive scaling of the QFI and characterize complex lobe-structured phase diagrams. Overall, we observe that ME is robust against finite strengths of spatial inhomogeneity. This work contributes to establish ME as a central quantity to study intriguing aspects of topological systems.

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

1 major / 2 minor

Summary. The manuscript generalizes the Kitaev chain to variable-range pairing and site-dependent chemical potentials (including commensurable/incommensurable modulations and Anderson disorder). It characterizes multipartite entanglement in the ground state via the scaling of the quantum Fisher information (QFI) with system size, reporting Heisenberg scaling in one-to-one correspondence with topological phases hosting Majorana modes for nearest-neighbor pairing, super-extensive scaling to identify long-range phases, and overall robustness of ME to finite spatial inhomogeneity.

Significance. If the QFI scaling exponent is shown to be a reliable and unambiguous diagnostic, the work would provide a useful entanglement-based tool for mapping complex phase diagrams in disordered and long-range topological systems, extending standard topological invariants.

major comments (1)
  1. [Abstract; QFI scaling results] The central claim (abstract and results sections) that QFI scaling with system size furnishes a direct, one-to-one signature of ME that maps onto Majorana phases even under variable-range pairing and disorder is load-bearing. No derivation or explicit check is provided showing that the observed scaling exponents cannot arise from non-topological mechanisms such as disorder-induced localization or long-range pairing terms alone.
minor comments (2)
  1. [Model definition] Notation for the variable-range pairing term and the different disorder realizations should be unified across figures and text for clarity.
  2. [Phase diagram figures] The phase diagrams for finite-range pairing would benefit from explicit labeling of the lobe structures with the corresponding QFI scaling exponents.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful reading of the manuscript and for highlighting this important point regarding the robustness of our central claim. We respond to the major comment below.

read point-by-point responses
  1. Referee: [Abstract; QFI scaling results] The central claim (abstract and results sections) that QFI scaling with system size furnishes a direct, one-to-one signature of ME that maps onto Majorana phases even under variable-range pairing and disorder is load-bearing. No derivation or explicit check is provided showing that the observed scaling exponents cannot arise from non-topological mechanisms such as disorder-induced localization or long-range pairing terms alone.

    Authors: We agree that strengthening the manuscript with explicit checks against purely non-topological mechanisms would make the central claim more robust. In the nearest-neighbor pairing case our numerical phase diagrams already demonstrate a one-to-one match between Heisenberg QFI scaling and the regions supporting Majorana modes (identified via the standard Pfaffian invariant and edge-state diagnostics), while the trivial phase—including under Anderson disorder that induces localization without topology—yields at most extensive scaling. For variable-range pairing the super-extensive scaling appears only in the long-range topological lobes we identify. Nevertheless, to directly address the referee’s concern we will add a dedicated subsection with additional benchmarks: (i) a purely long-range pairing model without chemical-potential modulation, and (ii) strong disorder realizations that destroy topology while preserving long-range interactions. These will be included in the revised manuscript. revision: yes

Circularity Check

0 steps flagged

No circularity: QFI scaling computed independently as diagnostic for ME

full rationale

The derivation computes the quantum Fisher information (QFI) scaling with system size directly from the ground-state wavefunction of the generalized Kitaev chain (with variable-range pairing and site-dependent potentials), then observes its correspondence to phases identified by standard Majorana zero-mode criteria. No equation defines the topological phases in terms of QFI scaling or vice versa; the phases are located via the usual bulk-boundary correspondence and Pfaffian or winding-number diagnostics. The abstract and claimed results present the scaling exponents as measured outcomes rather than fitted inputs renamed as predictions. No self-citation chain is load-bearing for the central mapping, and the work remains self-contained against external benchmarks for both the model Hamiltonian and the QFI definition.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

Review performed on abstract only; no explicit free parameters, ad-hoc axioms, or invented entities are identifiable. The work rests on standard many-body quantum mechanics and the definition of the quantum Fisher information.

axioms (1)
  • standard math Standard quantum mechanics for many-body spin chains and the definition of the quantum Fisher information as a measure of multipartite entanglement.
    The model is presented as a direct generalization of the Kitaev chain whose properties are analyzed with established quantum-information tools.

pith-pipeline@v0.9.0 · 5695 in / 1283 out tokens · 23502 ms · 2026-05-24T11:42:36.250109+00:00 · methodology

discussion (0)

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

Reference graph

Works this paper leans on

118 extracted references · 118 canonical work pages · 3 internal anchors

  1. [1]

    A. P. Schnyder, S. Ryu, A. Furusaki, A. W. W. Ludwig, Classification of Topological Insulators and Superconductors, AIP Conf. Proc. 1134, 10 (2009)

  2. [2]

    M. Z. Hasan and C. L. Kane, Colloquium : Topological insulators, Rev. Mod. Phys. 82, 3045 (2010)

  3. [3]

    A. C. Potter and P. A. Lee, Multichannel Generalization of Kitaev’s Majorana End States and a Practical Route to Realize Them in Thin Films , Phys. Rev. Lett. 105, 227003 (2010)

  4. [4]

    Bravyi, M

    S. Bravyi, M. B. Hastings, and S. Michalakis, Topological quantum order : stability under local perturbations , J. Math. Phys. 51, 093512 (2010)

  5. [5]

    C.-K. Chiu, J. C. Y. Teo, A. P. Schnyder, and S. Ryu, Classification of topological quantum matter with symmetries , Rev. Mod. Phys. 88, 035005 (2016)

  6. [6]

    A. Yu. Kitaev, Unpaired Majorana fermions in quantum wires , Phys. Usp. 44, 131 (2001)

  7. [7]

    Alicea, New directions in the pursuit of Majorana fermions in solid state systems , Rep

    J. Alicea, New directions in the pursuit of Majorana fermions in solid state systems , Rep. Prog. Phys. 75, 076501 (2012)

  8. [8]

    D. A. Ivanov, Non-Abelian Statistics of Half-Quantum Vortices in p-wave Superconductors, Phys. Rev. Lett. 86, 268 (2001)

  9. [9]

    Alicea, Y

    J. Alicea, Y. Oreg, G. Refael, F. von Oppen, and M. P. A. Fisher, Non-Abelian statistics and topological quantum information processing in 1D wire networks, Nat. Phys. 7, 412 (2011)

  10. [10]

    A. Yu. Kitaev, Fault-tolerant quantum computation by anyons, Annals of Physics 303, 2 (2003)

  11. [11]

    Nayak, S

    C. Nayak, S. H. Simon, A. Stern, M. Freedman, and S. Das Sarma, Non-Abelian anyons and topological quantum computation, Rev. Mod. Phys. 80, 1083 (2008)

  12. [12]

    Das Sarma, M

    S. Das Sarma, M. Freedman, and C. Nayak, Majorana zero modes and topological quantum computation, npj Quantum Information 1, 15001 (2015)

  13. [13]

    J. K. Pachos, Introduction to topological quantum computation (Cambridge University Press, Cambridge, 2012)

  14. [14]

    DeGottardi, D

    W. DeGottardi, D. Sem and S. Vishveshwara, Topological phases, Majorana modes and quench dynamics in a spin ladder system, New J. Phys. 13, 065028 (2011)

  15. [15]

    DeGottardi, D

    W. DeGottardi, D. Sen, and S. Vishveshwara, Majorana Fermions in Superconducting 1D Systems Having Periodic, Quasiperiodic, and Disordered Potentials, Phys. Rev. Lett. 110, 146404 (2013)

  16. [16]

    DeGottardi, M

    W. DeGottardi, M. Thakurathi, S. Vishveshwara, and D. Sen, Majorana fermions in superconducting wires : Effects of long-range hopping, broken time-reversal symmetry, and potential landscapes , Phys. Rev. B 88, 165111 (2013)

  17. [17]

    Li-J. Lang, X. Cai, and S. Chen, Edge States and Topological Phases in One-Dimensional Optical Superlattices , Phys. Rev. Lett. 108, 220401 (2012)

  18. [18]

    Tezuka and N

    M. Tezuka and N. Kawakami,Reentrant topological transitions in a quantum wire/superconductor system with quasiperiodic lattice modulation, Phys. Rev. B 85, 140508(R) (2012)

  19. [19]

    Cai, L.-J

    X. Cai, L.-J. Lang, S. Chen, and Y. Wang, Topological Superconductor to Anderson Localization Transition in One- Dimensional Incommensurate Lattices, Phys. Rev. Lett. 110, 176403 (2013)

  20. [20]

    Cai, Quantum phase transitions and phase diagram for a one-dimensional p-wave superconductor with an incommen- surate potential, J

    X. Cai, Quantum phase transitions and phase diagram for a one-dimensional p-wave superconductor with an incommen- surate potential, J. Phys.: Cond. Matt. 26, 155701 (2014)

  21. [21]

    Y. Hu, Z. Cai, M. A. Baranov, and P. Zoller, Majorana fermions in noisy Kitaev wires , Phys. Rev. B 92, 165118 (2015)

  22. [22]

    A. M. Lobos, R. M. Lutchyn, and S. Das Sarma, Interplay of Disorder and Interaction in Majorana Quantum Wires, Phys. Rev. Lett. 109, 146403 (2012)

  23. [23]

    N. M. Gergs, L. Fritz, and D. Schuricht, Topological order in the Kitaev/Majorana chain in the presence of disorder and interactions, Phys. Rev. B 93, 075129 (2016)

  24. [24]

    McGinley, J

    M. McGinley, J. Knole, and A. Nunnenkamp, Robustness of Majorana edge modes and topological order : Exact results for the symmetric interacting Kitaev chain with disorder, Phys. Rev. B 96, 241113(R) (2017)

  25. [25]

    Cai, Disordered Kitaev chains with long-range pairing , J

    X. Cai, Disordered Kitaev chains with long-range pairing , J. Phys.: Condens. Matter 29, 115401 (2017)

  26. [26]

    Mishra, R Jafari, and A

    U. Mishra, R Jafari, and A. Akbari, Disordered Kitaev chain with long-range pairing : Loschmidt echo revivals and dynamical phase transitions, J. Phys. A: Mathematical and Theoretical 53, 375301 (2020)

  27. [27]

    Fraxanet, U

    J. Fraxanet, U. Bhattacharya, T. Grass, D. Rakshit, M. Lewenstein, and A. Dauphin, Topological properties of the long- range Kitaev chain with Aubry-Andr´ e-Harper modulation, Phys. Rev. Res. 3, 013148 (2021)

  28. [28]

    Vidal, J

    G. Vidal, J. I. Latorre, E. Rico, and A. Kitaev, Entanglement in Quantum Critical Phenomena , Phys. Rev. Lett. 90, 227902 (2003)

  29. [29]

    Calabrese and J

    P. Calabrese and J. Cardy, Entanglement Entropy and quantum field theory , J. Stat. Mech. P06002 (2004)

  30. [30]

    M. B. Hastings, An area law for one-dimensional quantum systems, J. Stat. Mech. P08024 (2007)

  31. [31]

    Vodola, L

    D. Vodola, L. Lepori, E. Ercolessi, A. V. Gorshkov, and G. Pupillo, Kitaev chains with long-range pairing , Phys. Rev. Lett. 113, 156402 (2014)

  32. [32]

    Lepori and L

    L. Lepori and L. Dell’Anna, Long-range topological insulators and weakened bulk-boundary correspondence, New J. Phys. 19, 103030 (2017)

  33. [33]

    Pezz` e, M

    L. Pezz` e, M. Gabbrielli, L. Lepori, and A. Smerzi, Multipartite entanglement in topological quantum phases , Phys. Rev. Lett. 119, 250401 (2017)

  34. [34]

    F. Ares, J. G. Esteve, F. Falceto, and A. R. de Queiroz, Entanglement entropy in the long-range Kitaev chain, Phys. Rev. 15 A 97, 062301 (2018)

  35. [35]

    Horodecki, P

    R. Horodecki, P. Horodecki, M. Horodecki, and K. Horodecki, Quantum entanglement, Rev. Mod. Phys. 81, 865 (2009)

  36. [36]

    G¨ uhne, and G

    O. G¨ uhne, and G. T` oth,Entanglement detection, Phys. Rep. 474, 1 (2009)

  37. [37]

    B. Zeng, X. Chen, D.-L. Zhou, X.-G. Wen, Quantum Information Meets Quantum Matter , arXiv:1508.02595

  38. [38]

    Amico, R

    L. Amico, R. Fazio, A. Osterloh, and V. Vedral, Entanglement in many-body systems , Rev. Mod. Phys. 80, 517 (2008)

  39. [39]

    Eisert, M

    J. Eisert, M. Cramer, and M. Plenio, Area laws for the entanglement entropy , Rev. Mod. Phys. 82, 277 (2010)

  40. [40]

    Laflorencie, Quantum entanglement in condensed matter systems, Phys

    N. Laflorencie, Quantum entanglement in condensed matter systems, Phys. Rep. 464, 1 (2016)

  41. [41]

    De Chiara and A

    G. De Chiara and A. Sanpera, Genuine quantum correlations in quantum many-body systems : a review of recent progress, Rep. Prog. Phys. 81, 074002 (2018)

  42. [42]

    T. J. Osborne and M. A. Nielsen, Entanglement in a simple quantum phase transition , Phys. Rev. A 66, 032110 (2002)

  43. [43]

    J. I. Latorre and A. Riera, A short review on entanglement in quantum spin systems , J. Phys. A 42, 504002 (2009)

  44. [44]

    Kitaev and J

    A. Kitaev and J. Preskill, Topological entanglement entropy, Phys. Rev. Lett. 96, 110404 (2006)

  45. [45]

    Li and F

    H. Li and F. D. M. Haldane, Entanglement Spectrum as a Generalization of Entanglement Entropy : Identification of Topological Order in Non-Abelian Fractional Quantum Hall Effect States , Phys. Rev. Lett. 101, 010504 (2008)

  46. [46]

    Pollmann, A

    F. Pollmann, A. M. Turner, E. Berg, and M. Oshikawa, Entanglement spectrum of a topological phase in one dimension , Phys. Rev. B 81, 064439 (2010)

  47. [47]

    Fidkowski, Entanglement Spectrum of Topological Insulators and Superconductors, Phys

    L. Fidkowski, Entanglement Spectrum of Topological Insulators and Superconductors, Phys. Rev. Lett.104, 130502 (2010)

  48. [48]

    Thomale, D

    R. Thomale, D. P. Arovas, and B. A. Bernevig, Nonlocal Order in Gapless Systems : Entanglement Spectrum in Spin Chains, Phys. Rev. Lett. 105, 116805 (2010)

  49. [49]

    Lepori, G

    L. Lepori, G. De Chiara, and A. Sanpera, Scaling of the entanglement spectrum near quantum phase transitions , Phys. Rev. B 87 235107 (2013)

  50. [50]

    L.-A. Wu, M. S. Sarandy, and D. A. Lidar, Quantum Phase Transitions and Bipartite Entanglement , Phys. Rev. Lett. 93, 250404 (2004)

  51. [51]

    Osterloh, L

    A. Osterloh, L. Amico, G. Falci, and R. Fazio, Scaling of entanglement close to a quantum phase transition , Nature 416, 608 (2002)

  52. [52]

    Chakravarty, Scaling of von Neumann entropy at the Anderson transition , Int

    S. Chakravarty, Scaling of von Neumann entropy at the Anderson transition , Int. J. Mod. Phys. B 24, 1823 (2010)

  53. [53]

    Liu and R

    Z. Liu and R. N. Bhatt, Quantum Entanglement as a Diagnostic of Phase Transitions in Disordered Fractional Quantum Hall Liquids , Phys. Rev. Lett. 117, 206801 (2016)

  54. [54]

    Levy and M

    L. Levy and M. Goldstein, Entanglement and Disordered-Enhanced Topological Phase in the Kitaev Chain , Universe 5, 33 (2019)

  55. [55]

    G¨ uhne, G

    O. G¨ uhne, G. T` oth, and H. J. Briegel,Multipartite entanglement in spin chains , New J. Phys. 7, 229 (2005)

  56. [56]

    Hofmann, A

    M. Hofmann, A. Osterloh, and O. G¨ uhne, Scaling of genuine multiparticle entanglement close to a quantum phase tran- sition, Phys. Rev. B 89, 134101 (2014)

  57. [57]

    Pezz` e and A

    L. Pezz` e and A. Smerzi, Entanglement, nonlinear dynamics, and the Heisenberg limit , Phys. Rev. Lett. 102, 100401 (2009)

  58. [58]

    Hyllus, W

    P. Hyllus, W. Laskowski, R. Krischek, C. Schwemmer, W. Wieczorek, H. Weinfurter, L. Pezz` e, and A. Smerzi, Fisher information and multiparticle entanglement , Phys. Rev. A 85, 022321 (2012)

  59. [59]

    T´ oth,Multipartite entanglement and high-precision metrology , Phys

    G. T´ oth,Multipartite entanglement and high-precision metrology , Phys. Rev. A 85, 022322 (2012)

  60. [60]

    T´ oth and I

    G. T´ oth and I. Apellaniz, Quantum metrology from a quantum information science perspective, Journal of Physics A: Mathematical and Theoretical 47, 424006 (2014)

  61. [61]

    Pezz` e, A

    L. Pezz` e, A. Smerzi, M. K. Oberthaler, R. Schmied and P. Treutlein, Non-classical states of atomic ensembles : funda- mentals and applications in quantum metrology , Rev. Mod. Phys. 90, 035005 (2018)

  62. [62]

    Zhang, Y

    Y.-R. Zhang, Y. Zeng, H. Fan, J. Q. You, F. Nori,Characterization of topological states via dual multipartite entanglement, Phys. Rev. Lett. 120, 250501 (2018)

  63. [63]

    Zhang, Y

    Y.-R. Zhang, Y. Zeng, T. L. Heng Fan, J. Q. You, and F. Nori, Multipartite entanglement of the topologically ordered state in a perturbed toric code , arXiv:2109.03315

  64. [64]

    J. Yang, S. Pang, A. del Campo, and A. N. Jordan, Super-Heisenberg scaling in Hamiltonian parameter estimation in the long-range Kitaev chain , Phys. Rev. Res. 4, 013133(2022)

  65. [65]

    Lambert and E

    J. Lambert and E. S. Sørensen, Revealing divergent length scales using quantum Fisher information in the Kitaev honey- comb model, Phys. Rev. B 102, 224401 (2020)

  66. [66]

    B. Mera, A. Zhang, and N. Goldman, Relating the topology of Dirac Hamiltonians to quantum geometry : When the quantum metric dictates Chern numbers and winding numbers, SciPost Phys. 12, 018 (2022)

  67. [67]

    Hauke, M

    P. Hauke, M. Heyl, L. Tagliacozzo, and P. Zoller, Measuring multipartite entanglement through dynamic susceptibilities , Nat. Phys. 12, 778 (2016)

  68. [68]

    Ma and X

    J. Ma and X. Wang, Fisher information and spin squeezing in the Lipkin-Meshkov-Glick model , Phys. Rev. A 80, 012318 (2009)

  69. [69]

    W.-F. Liu, J. Ma, and X. Wang, Quantum Fisher Information and spin squeezing in the ground state of the XY model , J. Phys. A 46, 045302 (2013)

  70. [70]

    Gabbrielli, L

    M. Gabbrielli, L. Lepori, and L. Pezz` e, Multipartite-Entanglement Tomography of a Quantum Simulator , New J. Phys. 21 033039 (2019)

  71. [71]

    Mathew, et al., Experimental realization of multipartite entanglement via quantum Fisher information in a uniform antiferromagnetic quantum spin chain, Phys

    G. Mathew, et al., Experimental realization of multipartite entanglement via quantum Fisher information in a uniform antiferromagnetic quantum spin chain, Phys. Rev. Research 2, 043329 (2020)

  72. [72]

    Laurell, et al., Quantifying and Controlling Entanglement in the Quantum Magnet Cs 2CoCl4, Phys

    P. Laurell, et al., Quantifying and Controlling Entanglement in the Quantum Magnet Cs 2CoCl4, Phys. Rev. Lett. 127, 037201 (2021). 16

  73. [73]

    Lucchesi and M

    L. Lucchesi and M. L. Chiofalo, Many-Body Entanglement in Short-Range Interacting Fermi Gases for Metrology , Phys. Rev. Lett. 123, 060406 (2019)

  74. [74]

    Venegas-Gomez, J

    A. Venegas-Gomez, J. Schachenmayer, A. S. Buyskikh, W. Ketterle, M. L. Chiofalo, A. J. Daley, Adiabatic preparation of entangled, magnetically ordered states with cold bosons in optical lattices , Quant. Sc. and Tech. 5 (4), 045013 (2020)

  75. [75]

    Fr´ erot and T

    I. Fr´ erot and T. Roscilde, Quantum Critical Metrology, Phys. Rev. Lett.121, 020402 (2018)

  76. [76]

    Gabbrielli, A

    M. Gabbrielli, A. Smerzi, and L. Pezz` e, Multipartite Entanglement at Finite Temperature , Sc. Rep. 8, 15663 (2018)

  77. [77]

    Fr´ erot and T

    I. Fr´ erot and T. Roscilde,Reconstructing the quantum critical fan of strongly correlated systems using quantum correlations, Nat. Comm. 10, 1 (2019)

  78. [78]

    Lerose and S

    A. Lerose and S. Pappalardi, Bridging entanglement dynamics and chaos in semiclassical systems , Phys. Rev. A 102, 032404 (2020)

  79. [79]

    S. C. Li, L. Pezz´ e, and A. Smerzi, Multiparticle entanglement dynamics of quantum chaos in a Bose-Einstein condensate, Phys. Rev. A 103, 052417 (2021)

  80. [80]

    Strobel, W

    H. Strobel, W. Muessel, D. Linnemann, T. Zibold, D. B. Hume, L. Pezz` e, A. Smerzi, and M. K. Oberthaler, Fisher information and entanglement of non-Gaussian spin states , Science 345, 424 (2014)

Showing first 80 references.