pith. sign in

arxiv: 2607.01786 · v1 · pith:ULTOELCKnew · submitted 2026-07-02 · 🪐 quant-ph · physics.optics

Performance of a two-mode coherent superposed channel in continuous-variable quantum teleportation

Pith reviewed 2026-07-03 12:42 UTC · model grok-4.3

classification 🪐 quant-ph physics.optics
keywords two-mode coherent statessuperposed quantum statescontinuous-variable teleportationnonclassicalitynon-GaussianityWigner functionquantum fidelityBraunstein-Kimble protocol
0
0 comments X

The pith

The two-mode coherent superposed state achieves continuous-variable teleportation fidelities above the classical threshold in certain parameter regimes.

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

This paper introduces a two-mode coherent superposed state generated by applying a superposition operator to two-mode coherent states. It examines the state's nonclassicality and non-Gaussianity using the Wigner distribution and Wigner logarithmic negativity. The state is then used as the entangled resource in the Braunstein-Kimble protocol to teleport coherent and squeezed inputs. The analysis shows that in parameter regimes with stronger non-Gaussian features or nonclassicality, the teleportation fidelity can surpass the classical limit of one half.

Core claim

The two-mode coherent superposed quantum state, produced by the action of the operator A = t a b + r a† b† on the two-mode coherent state |α, β>, exhibits nonclassicality and quantum non-Gaussianity as quantified by the Wigner distribution and Wigner logarithmic negativity. When employed as the entangled resource in the ideal Braunstein-Kimble continuous-variable teleportation protocol, this state yields teleportation fidelities for coherent and squeezed inputs that exceed the classical threshold in specific parameter regimes where the non-Gaussian features or nonclassicality are enhanced.

What carries the argument

The two-mode superposition operator A = t a b + r a† b† applied to two-mode coherent states to create the entangled resource, with the Wigner logarithmic negativity serving as the measure linking non-Gaussianity to teleportation performance.

If this is right

  • Fidelities for coherent and squeezed inputs exceed the classical threshold in regimes of enhanced non-Gaussianity.
  • Increased nonclassicality correlates with higher teleportation efficiency.
  • The results demonstrate the operational significance of such engineered states in CV quantum information processing.
  • The ideal teleportation fidelity depends on the strengths of nonclassicality and non-Gaussianity.

Where Pith is reading between the lines

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

  • This suggests testing the state in other continuous-variable protocols such as entanglement swapping.
  • Experimental generation of the state via the described operator might be feasible with current linear optics.
  • The assumption of an ideal protocol means real-world noise could reduce the observed advantage.
  • Comparing fidelity improvements to those from other non-Gaussian resources like cat states would be informative.

Load-bearing premise

The nonclassicality and non-Gaussianity of the state, as measured by the Wigner function and its logarithmic negativity, directly translate to higher teleportation fidelity in the ideal Braunstein-Kimble protocol.

What would settle it

A direct computation of the teleportation fidelity from the Wigner function of the resource state that finds the fidelity stays at or below one half even in regimes of large Wigner logarithmic negativity.

Figures

Figures reproduced from arXiv: 2607.01786 by Arpita Chatterjee, Deepak.

Figure 1
Figure 1. Figure 1: FIG. 1. A comparison of Wigner function for [PITH_FULL_IMAGE:figures/full_fig_p004_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Wigner logarithmic negativity with respect to state [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Variation of fidelity with coherent state input and wi [PITH_FULL_IMAGE:figures/full_fig_p006_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Variation of fidelity with squeezed state input ( [PITH_FULL_IMAGE:figures/full_fig_p006_4.png] view at source ↗
read the original abstract

Glauber's coherent state is denoted by $\ket{\alpha}$ and its two-mode extension is represented by $\ket{\alpha,\beta}$. In this work, we introduce a two-mode superposition operator $A=tab+ra^\dagger b^\dagger$, whose action on the two-mode coherent state produces the two-mode coherent superposed quantum state $\ket{\psi}=(tab+ra^\dagger b^\dagger)\ket{\alpha,\beta}$. We investigate the nonclassicality and quantum non-Gaussianity of this state by means of the Wigner distribution and Wigner logarithmic negativity. Once its intrinsic nonclassical and non-Gaussian structure is established, the state is employed as the entangled resource in the Braunstein-Kimble continuous-variable (CV) teleportation protocol. We compute the ideal teleportation fidelity for coherent and squeezed inputs and analyze how the strengths of nonclassicality and non-Gaussianity influence the teleportation efficiency. Our results identify specific parameter regimes where enhanced non-Gaussian features or increased nonclassicality enable fidelities beyond the classical threshold, thereby revealing the operational significance of engineered two-mode quantum states in CV quantum information processing.

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

2 major / 2 minor

Summary. The paper defines a two-mode coherent superposed state |ψ⟩ = (t ab + r a†b†)|α,β⟩, quantifies its nonclassicality and non-Gaussianity via the Wigner distribution and Wigner logarithmic negativity, and inserts it as the entangled resource into the ideal Braunstein-Kimble CV teleportation protocol. Fidelity is computed for coherent and squeezed inputs via overlap integrals or characteristic functions, with the central claim that regimes of enhanced WLN yield F > 1/2 (classical threshold), thereby demonstrating the operational value of such engineered states.

Significance. If the results hold after isolating the role of non-Gaussianity, the work would establish concrete parameter regimes in which non-Gaussian two-mode resources improve CV teleportation performance, providing a useful benchmark for experiments with engineered continuous-variable states.

major comments (2)
  1. [Teleportation fidelity section] The fidelity calculation (described after the WLN definition) reports F > 1/2 in high-WLN regimes, but t, r, α, β simultaneously tune both WLN and two-mode entanglement (via reduced covariance or logarithmic negativity). No comparison is made to a Gaussian state with matched entanglement, so the observed correlation does not establish that non-Gaussianity is the causal driver of the fidelity gain.
  2. [Results and discussion] The claim that 'enhanced non-Gaussian features enable fidelities beyond the classical threshold' (final paragraph) rests on the assumption that WLN directly improves teleportation efficiency in the Braunstein-Kimble protocol, yet the manuscript provides no control calculation or partial derivative isolating WLN from entanglement at fixed parameters.
minor comments (2)
  1. [State definition] The normalization constant for |ψ⟩ is not stated explicitly after the definition of A; this should be added to allow reproduction of the Wigner function.
  2. [Figures] Figure captions for fidelity plots should include the classical threshold F = 1/2 as a reference line.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading and constructive comments. The concerns regarding the need to isolate non-Gaussianity from entanglement in the fidelity analysis are valid, and we address each point below with plans for revision.

read point-by-point responses
  1. Referee: [Teleportation fidelity section] The fidelity calculation (described after the WLN definition) reports F > 1/2 in high-WLN regimes, but t, r, α, β simultaneously tune both WLN and two-mode entanglement (via reduced covariance or logarithmic negativity). No comparison is made to a Gaussian state with matched entanglement, so the observed correlation does not establish that non-Gaussianity is the causal driver of the fidelity gain.

    Authors: We agree that the current results demonstrate a correlation between high WLN and F > 1/2 but do not isolate causality from entanglement. In the revised manuscript we will add explicit comparisons to two-mode squeezed vacuum states with logarithmic negativity matched to selected points of our non-Gaussian states, recomputing fidelities to quantify any additional gain attributable to non-Gaussianity. revision: yes

  2. Referee: [Results and discussion] The claim that 'enhanced non-Gaussian features enable fidelities beyond the classical threshold' (final paragraph) rests on the assumption that WLN directly improves teleportation efficiency in the Braunstein-Kimble protocol, yet the manuscript provides no control calculation or partial derivative isolating WLN from entanglement at fixed parameters.

    Authors: The referee is correct that no such control is present. We will revise the Results and discussion section to include control calculations that hold entanglement (logarithmic negativity) fixed while varying WLN, or direct side-by-side fidelity comparisons against Gaussian resources at matched entanglement, thereby qualifying the claim appropriately. revision: yes

Circularity Check

0 steps flagged

No circularity detected; derivation is a direct computational pipeline

full rationale

The paper defines the state |ψ⟩ via the operator A acting on |α,β⟩, computes its Wigner function and WLN using standard definitions, then evaluates teleportation fidelity in the Braunstein-Kimble protocol via overlap or characteristic function. Fidelity is obtained directly from the state parameters without any fitted input renamed as prediction, self-definitional loop, or load-bearing self-citation. The reported correlation between non-Gaussianity and fidelity >1/2 is an analysis of computed quantities, not a claim that one is constructed from the other. The chain is self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

4 free parameters · 2 axioms · 1 invented entities

The central claim rests on the definition of the new operator, the assumption that the generated state remains normalizable, and the premise that Wigner-based measures of nonclassicality and non-Gaussianity are the relevant predictors of teleportation performance. No external benchmarks or machine-checked derivations are mentioned.

free parameters (4)
  • t
    Weight of the a b term in the superposition operator A
  • r
    Weight of the a† b† term in the superposition operator A
  • α
    Amplitude of the first coherent mode
  • β
    Amplitude of the second coherent mode
axioms (2)
  • standard math Two-mode coherent states |α,β⟩ are valid quantum states
    Standard background fact in quantum optics
  • domain assumption The operator A produces a normalizable state suitable for use as an entangled resource
    Required for the state |ψ⟩ to be physically usable in the teleportation protocol
invented entities (1)
  • two-mode coherent superposed state |ψ⟩ no independent evidence
    purpose: Entangled resource for CV teleportation
    New state introduced by the operator A; no independent experimental evidence supplied in the abstract

pith-pipeline@v0.9.1-grok · 5729 in / 1515 out tokens · 69286 ms · 2026-07-03T12:42:09.231212+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

47 extracted references

  1. [1]

    Fur ther, the fidelity decreases with respect to α , β , t, r and oscilla- tory with respect to φ

    It is seen that the fidelity for input squeezed state is just greater than the threshold limit. Fur ther, the fidelity decreases with respect to α , β , t, r and oscilla- tory with respect to φ . Teleportation of a squeezed state is more demanding than that of coherent state because Gaussian entangled channels often fail to preserve quadrature squee z- ing ...

  2. [2]

    E. N. Popov and N. V . Larionov, Glauber- sudarshan p function in the model of a single- emitter laser generating in strong coupling regime, in Saratov Fall Meeting 2015: Third International Symposium o n Optics and Biophotonics and Seventh Finnish-Russian Phot onics and Laser Symposium V ol. 9917, edited by E. A. Genina, V . V . Tuchin, V . L. Derbov, D....

  3. [3]

    G. S. Agarwal and K. Tara, Nonclassical properties of states generated by the excitations on a coherent state, Physical Review A 43, 492 (1991)

  4. [4]

    R. R. Puri, Mathematical Methods of Quantum Optics (Springer, Berlin, 2001)

  5. [5]

    Chatterjee, Lower- versus higher-order nonclassicalities for a coherent superposed quantum state , Journal of the Optical Society of America B: Optical Physics 38, 3212 (2021)

    Deepak and A. Chatterjee, Lower- versus higher-order nonclassicalities for a coherent superposed quantum state , Journal of the Optical Society of America B: Optical Physics 38, 3212 (2021)

  6. [6]

    Eisert, S

    J. Eisert, S. Scheel, and M. B. Plenio, Distilling gaus- sian states with gaussian operations is impossible, Physical Review A Lett. 89, 137903 (2002)

  7. [7]

    Fiur´ aˇ sek, Gaussian transformations and distillation of entangled gaussian states, Physical Review A Lett

    J. Fiur´ aˇ sek, Gaussian transformations and distillation of entangled gaussian states, Physical Review A Lett. 89, 137904 (2002)

  8. [8]

    Lloyd and S

    S. Lloyd and S. L. Braunstein, Quantum computation over c on- tinuous variables, Physical Review A Lett. 82, 1784 (1999)

  9. [9]

    Chatterjee, Detecting nonclassicality an d non-gaussianity of a coherent superposed quantum state, Journal of Physics B: Atomic, Molecular and Optical Physics 56, 015401 (2022)

    Deepak and A. Chatterjee, Detecting nonclassicality an d non-gaussianity of a coherent superposed quantum state, Journal of Physics B: Atomic, Molecular and Optical Physics 56, 015401 (2022)

  10. [10]

    Deepak and A. Chatterjee, Entanglement and non- gaussianity in photon-added and photon-subtracted dis- placed fock states and their role in ideal cv teleportation, Physica Scripta 99, 095124 (2024) . 7

  11. [11]

    Lee and H

    S.-Y . Lee and H. Nha, Quantum state engineering by a coherent superposition of photon subtraction and addition , Physical Review A 82, 053812 (2010)

  12. [12]

    Chatterjee, Realistic continuous-varia ble quan- tum teleportation using a displaced fock state channel, Quantum Information Processing 21, 145 (2022)

    Deepak and A. Chatterjee, Realistic continuous-varia ble quan- tum teleportation using a displaced fock state channel, Quantum Information Processing 21, 145 (2022)

  13. [13]

    S. L. Braunstein and H. J. Kimble, Teleportation of cont inuous quantum variables, Physical Review Letters 80, 869 (1998)

  14. [14]

    Chatterjee, Lower-versus higher-order n on- classicalities for a coherent superposed quantum state, Journal of the Optical Society of America B 38, 3212 (2021)

    Deepak and A. Chatterjee, Lower-versus higher-order n on- classicalities for a coherent superposed quantum state, Journal of the Optical Society of America B 38, 3212 (2021)

  15. [15]

    Royer, Wigner function as the expectation value of a p arity operator, Physical Review A 15, 449 (1977)

    A. Royer, Wigner function as the expectation value of a p arity operator, Physical Review A 15, 449 (1977)

  16. [16]

    J. Lee, J. Kim, and H. Nha, Demonstrat- ing higher-order nonclassical effects by photon- added classical states: realistic schemes, Journal of the Optical Society of America B: Optical Physics 26, 1363 (2009)

  17. [17]

    R. J. Glauber, Coherent and incoherent states of the rad iation field, Physical Review A 131, 2766 (1963)

  18. [18]

    Safaeian and M

    O. Safaeian and M. K. Tavassoly, Deformed photon-added nonlinear coherent states and their non-classical propert ies, Journal of Physics A: Mathematical and Theoretical 44, 225301 (2011)

  19. [19]

    V . I. Man’ko, G. Marmo, E. C. G. Sudarshan, and F. Zaccaria, f-oscillators and nonlinear coherent states, Physica Scripta 55, 528 (1997)

  20. [20]

    Rom´ an-Ancheyta, O

    R. Rom´ an-Ancheyta, O. de los Santos- S´ anchez, and J. R´ ecamier, Ladder operators and coherent states for nonlinear potentials, Journal of Physics A: Mathematical and Theoretical 44, 435304 (2011)

  21. [21]

    Roy and P

    B. Roy and P . Roy, New nonlinear coherent states and some of their nonclassical properties, Journal of Optics B: Quantum and Semiclassical Optics 2, 65 (2000)

  22. [22]

    R. L. de Matos Filho and W. V ogel, Nonlinear coherent sta tes, Physical Review A 54, 4560 (1996)

  23. [23]

    R´ ecamier, M

    J. R´ ecamier, M. Gorayeb, W. L. Moch´ an, and J. L. Paz, Nonlinear coherent states and some of their properties, International Journal of Theoretical Physics 47, 673 (2008)

  24. [24]

    de los Santos-S´ anchez and J

    O. de los Santos-S´ anchez and J. R´ ecamier, Non- linear coherent states for nonlinear systems, Journal of Physics A: Mathematical and Theoretical 44, 145307 (2011)

  25. [25]

    Sivakumar, Photon-added coher- ent states as nonlinear coherent states, Journal of Physics A: Mathematical and Theoretical 32, 3441 (1999)

    S. Sivakumar, Photon-added coher- ent states as nonlinear coherent states, Journal of Physics A: Mathematical and Theoretical 32, 3441 (1999)

  26. [26]

    Rom´ an-Ancheyta, C

    R. Rom´ an-Ancheyta, C. Gonz´ alez Guti´ errez, and J. R´ ecamier, Photon-added nonlinear coherent states for a one-mode field in a kerr medium, Journal of the Optical Society of America B 31, 38 (2013)

  27. [27]

    P . D. Drummond and D. F. Walls, Quantum theory of optical bistability. i. nonlinear polarisability model , Journal of Physics A: Mathematical and Theoretical 13, 725 (1980)

  28. [28]

    Roknizadeh and M

    R. Roknizadeh and M. K. Tavassoly, The construc- tion of some important classes of generalized co- herent states: the nonlinear coherent states method, Journal of Physics A: Mathematical and Theoretical 37, 8111 (2004)

  29. [29]

    de los Santos-S´ anchez and J

    O. de los Santos-S´ anchez and J. R´ ecamier, The f-defor med jaynes–cummings model and its nonlinear coherent states, Journal of Physics B: Atomic, Molecular and Optical Physics 45, 015502 (2012)

  30. [30]

    Chatterjee, Nonclassicality versus quan tum non-gaussianity of photon-subtracted displaced fock stat e, Canadian Journal of Physics 101, 560 (2023)

    Deepak and A. Chatterjee, Nonclassicality versus quan tum non-gaussianity of photon-subtracted displaced fock stat e, Canadian Journal of Physics 101, 560 (2023)

  31. [31]

    Barbieri, N

    M. Barbieri, N. Spagnolo, M. G. Genoni, F. Ferrey- rol, R. Blandino, M. G. A. Paris, P . Grangier, and R. Tualle-Brouri, Non-gaussianity of quantum states: an experimental test on single-photon-added coherent states , Physical Review A 82, 063833 (2010)

  32. [32]

    Wenger, R

    J. Wenger, R. Tualle-Brouri, and P . Grangier, Non- gaussian statistics from individual pulses of squeezed lig ht, Physical Review A Lett. 92, 153601 (2004)

  33. [33]

    R´ ecamier, W

    J. R´ ecamier, W. L. Moch´ an, M. Gorayeb, J. L. Paz, and R. J´ auregui, Uncertainty relations for a deformed oscilla tor, International Journal of Modern Physics B 20, 1851 (2006)

  34. [34]

    R. J. Glauber, The quantum theory of optical coherence, Physical Review A 130, 2529 (1963)

  35. [35]

    A. I. Lvovsky and S. A. Babichev, Synthesis and tomo- graphic characterization of the displaced fock state of lig ht, Physical Review A 66, 011801 (2002)

  36. [36]

    Mandel, Sub-Poissonian photon statistics in resona nce fluo- rescence, Optics Letters 4, 205 (1979)

    L. Mandel, Sub-Poissonian photon statistics in resona nce fluo- rescence, Optics Letters 4, 205 (1979)

  37. [37]

    R. R. Puri and G. S. Agarwal, Su(1,1) coherent states defi ned via a minimum-uncertainty product and an equality of quadra - ture variances, Physical Review A 53, 1786 (1996)

  38. [38]

    Zavatta, S

    A. Zavatta, S. Viciani, and M. Bellini, Single-photon e xcitation of a coherent state: catching the elementary step of stimula ted light emission, Physical Review A 72, 023820 (2005)

  39. [39]

    C. T. Lee, Simple criterion for nonclassical two-mode s tates, Journal of the Optical Society of America B: Optical Physics 15, 1187 (1998)

  40. [40]

    H. M. Cessa and P . Knight, Series representation of quan tum- field quasiprobabilities, Physical Review A 48, 2479 (1993)

  41. [41]

    Boiteux and A

    M. Boiteux and A. Levelut, Semicoherent states, Journal of Physics A: Mathematical and Theoretical 6, 589 (1973)

  42. [42]

    M. S. Kim, H. Jeong, A. Zavatta, V . Parigi, and M. Bellini, Scheme for proving the bosonic com- mutation relation using single-photon interference, Physical Review A Lett. 101, 260401 (2008)

  43. [43]

    Zavatta, S

    A. Zavatta, S. Viciani, and M. Bellini, Quantum-to-cla ssical transition with single-photon-added coherent states of li ght, Science 306, 660 (2004)

  44. [44]

    F. A. M. de Oliveira, M. S. Kim, P . L. Knight, and V . Buzek, Properties of displaced number states, Physical Review A 41, 2645 (1990)

  45. [45]

    J. M. Raimond, T. Meunier, P . Bertet, S. Gleyzes, P . Maioli, A. Auffeves, G. Nogues, M. Brune, and S. Haroche, Probing a quantum field in a photon box, Journal of Physics B: Atomic, Molecular and Optical Physics 38, S535 (2005)

  46. [46]

    R. J. Glauber, Photon correlations, Physical Review A Lett. 10, 84 (1963)

  47. [47]

    Mandel and E

    L. Mandel and E. Wolf, Optical coherence and quantum opt ics, Cambridge University , 1102 (1995)