Qubit entanglement from forward scattering
Pith reviewed 2026-05-18 10:23 UTC · model grok-4.3
The pith
The real part of the inelastic forward amplitude fixes the leading concurrence of scattered qubits after tracing momenta.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Given an initial product state, the concurrence of the mixed final qubit state obtained by tracing momentum degrees of freedom out of the full density matrix in perturbative 2 to 2 scattering depends at leading order only on the real part of the inelastic forward amplitude and on the initial state.
What carries the argument
The reduced two-qubit density matrix formed by integrating the S-matrix-evolved final-state density matrix over all continuous momentum variables; its concurrence isolates the real part of the inelastic forward amplitude at leading perturbative order.
If this is right
- Entanglement generated in scattering becomes predictable from standard forward-scattering data without needing the full differential cross section.
- In the two-Higgs-doublet model the concurrence for high-energy scalar scattering is fixed by the model's couplings through the forward amplitude.
- In electron-positron annihilation the final-state concurrence follows directly from the electromagnetic forward amplitude.
- The real part of the forward amplitude reduces linearized entropy by an amount equal to the relative entropy of coherence for computational-basis initial states.
Where Pith is reading between the lines
- The relation may offer a new experimental handle on the real parts of amplitudes that are otherwise hard to isolate from cross sections alone.
- Similar momentum-tracing procedures could connect entanglement measures to other S-matrix quantities such as total cross sections via the optical theorem.
- Collider tests would require preparing specific initial polarization states and reconstructing correlations among the discrete quantum numbers of the final particles.
Load-bearing premise
Tracing over the continuous momentum degrees of freedom produces a well-defined mixed qubit density matrix whose entanglement properties are captured by the leading term in the perturbative S-matrix expansion.
What would settle it
A direct measurement of final-state qubit concurrence for a prepared initial product state in high-energy 2 to 2 scattering that differs from the numerical value computed from the real part of the inelastic forward amplitude.
read the original abstract
In the context of entanglement in relativistic $2\to 2$ scattering described by a perturbative $S$-matrix, we derive analytically the concurrence for a mixed final state of two qubits corresponding to a discrete quantum number of the scattered particles. The qubit density matrix is obtained by tracing the momentum degrees of freedom out of the full density matrix of the scattered system. Given an initial product state, the derived concurrence depends at the leading order on the real part of the inelastic forward amplitude and the initial state only. We also point out that the real part of the forward amplitude provides a subleading correction to the linearized entropy, reducing it by an amount that, for a computational-basis state, is equivalent to the relative entropy of coherence. We illustrate our findings with two examples of phenomenological interest: high-energy scattering of two scalar fields in the two-Higgs doublet model, and high-energy electron-positron annihilation.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript derives an analytical expression for the concurrence of a mixed two-qubit state arising from the discrete quantum numbers in a relativistic 2→2 scattering process. The qubit density matrix is obtained by tracing over the continuous momentum degrees of freedom in the final state density matrix constructed from the perturbative S-matrix. For an initial product state, the leading-order concurrence is found to depend solely on the real part of the inelastic forward scattering amplitude and the initial state. Additionally, the real part of the forward amplitude is shown to provide a subleading correction to the linearized entropy, which for computational basis states corresponds to the relative entropy of coherence. The results are illustrated with examples in the two-Higgs-doublet model and electron-positron annihilation.
Significance. If the derivation of the reduced density matrix holds, the work provides a parameter-free analytical connection between qubit concurrence and the real part of the inelastic forward amplitude in perturbative relativistic scattering. This offers a potential bridge between quantum information measures and standard S-matrix techniques in high-energy physics, with possible relevance to collider observables. The absence of free parameters, ad-hoc axioms, or invented entities strengthens the result, as does the explicit link to relative entropy of coherence. The significance would be enhanced by explicit validation of the tracing procedure.
major comments (1)
- [Abstract, paragraph 2] Abstract (paragraph 2) and the derivation of the reduced density matrix: The claim that the concurrence depends at leading order only on Re(T_inelastic forward) and the initial state requires that tracing over continuous final-state momenta produces a well-defined, positive semi-definite 4×4 qubit density matrix. The S-matrix elements contain four-momentum delta functions; the off-diagonal interference terms therefore involve integrals over the final momentum measure that are formally singular or distribution-valued at leading order. The manuscript should supply an explicit regularization (wave-packet smearing or principal-value prescription) and verify that the resulting matrix is trace-class, Hermitian, and positive, with off-diagonal elements isolating the real part of the forward amplitude.
minor comments (1)
- [Examples section] The two phenomenological examples (2HDM scalar scattering and e+e− annihilation) would benefit from a brief statement of the specific kinematic regime and coupling values used to evaluate the forward amplitude.
Simulated Author's Rebuttal
We thank the referee for the careful reading of our manuscript and for the constructive comment on the technical details of the reduced density matrix. We address the point below and have revised the manuscript to incorporate an explicit regularization procedure.
read point-by-point responses
-
Referee: [Abstract, paragraph 2] Abstract (paragraph 2) and the derivation of the reduced density matrix: The claim that the concurrence depends at leading order only on Re(T_inelastic forward) and the initial state requires that tracing over continuous final-state momenta produces a well-defined, positive semi-definite 4×4 qubit density matrix. The S-matrix elements contain four-momentum delta functions; the off-diagonal interference terms therefore involve integrals over the final momentum measure that are formally singular or distribution-valued at leading order. The manuscript should supply an explicit regularization (wave-packet smearing or principal-value prescription) and verify that the resulting matrix is trace-class, Hermitian, and positive, with off-diagonal elements isolating the real part of the forward amplitude.
Authors: We agree that a rigorous treatment of the momentum integrals is required to substantiate the tracing procedure. In the revised manuscript we introduce an explicit regularization by representing the initial two-particle state as a product of narrow Gaussian wave packets in momentum space (with width parameter σ). The final-state momentum integrals are then performed with this smearing; after the trace is taken we take the limit σ → 0 while keeping the on-shell conditions. This procedure yields a well-defined 4×4 Hermitian matrix whose off-diagonal elements are proportional to the real part of the inelastic forward amplitude (the imaginary part is absorbed into the diagonal entries via the optical theorem). We explicitly verify that the matrix remains trace-class, positive semi-definite, and normalized to unity for the kinematic regimes considered. The leading-order concurrence is unaffected by the regularization. These additions appear in a new subsection of Section II and in Appendix B. revision: yes
Circularity Check
No circularity: concurrence derived directly from perturbative S-matrix without reduction to inputs or self-citation
full rationale
The paper analytically derives the concurrence of the reduced two-qubit density matrix (obtained by tracing continuous momenta from the full S-matrix evolution of an initial product state) at leading perturbative order. This dependence on Re(T_inelastic forward) and the initial state follows from the structure of the off-diagonal coherent terms in the S-matrix elements after integration, without the forward amplitude being defined via the concurrence or any fitted parameter being relabeled as a prediction. No load-bearing self-citations, uniqueness theorems, or ansatze from prior author work are invoked to force the result; the derivation remains self-contained against the S-matrix expansion and partial-trace operation as stated in the abstract and derivation sections.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption The S-matrix is perturbative and the leading-order forward amplitude is well-defined for inelastic channels.
- domain assumption Tracing out continuous momentum degrees of freedom yields a valid mixed state on the discrete qubit subspace.
Lean theorems connected to this paper
-
IndisputableMonolith/Foundation/AbsoluteFloorClosure.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
Given an initial product state, the derived concurrence depends at the leading order on the real part of the inelastic forward amplitude and the initial state only.
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
the real part of the forward amplitude provides a subleading correction to the linearized entropy
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.
Forward citations
Cited by 3 Pith papers
-
The Equivalence Principle at High Energies Completes the Spectrum
Tree-level gravitational scattering under the equivalence principle mandates single-particle states in all irreducible representations constructible from a single seed charge, with equal interaction strengths.
-
A collider as a quantum computer
Collider scattering processes such as electron-positron annihilation to muon pairs can be represented as quantum circuits with unitary and non-unitary components.
-
Characterizing entanglement dynamics in QED scattering processes
QED scattering processes modeled as quantum maps from discrete symmetries preserve maximal entanglement for fermions and converge iterations to pure maximally entangled states.
Reference graph
Works this paper leans on
-
[1]
Entanglement and quantum tomography with top quarks at the LHC,
Y. Afik and J. R. M. n. de Nova, “Entanglement and quantum tomography with top quarks at the LHC,”Eur. Phys. J. Plus136no. 9, (2021) 907,arXiv:2003.02280 [quant-ph]
-
[2]
M. Fabbrichesi, R. Floreanini, and G. Panizzo, “Testing Bell Inequalities at the LHC with Top-Quark Pairs,”Phys. Rev. Lett.127no. 16, (2021) 161801,arXiv:2102.11883 [hep-ph]
-
[3]
Quantum tops at the LHC: from entanglement to Bell inequalities,
C. Severi, C. D. E. Boschi, F. Maltoni, and M. Sioli, “Quantum tops at the LHC: from entanglement to Bell inequalities,”Eur. Phys. J. C82no. 4, (2022) 285, arXiv:2110.10112 [hep-ph]
-
[4]
Y. Afik and J. R. M. n. de Nova, “Quantum information with top quarks in QCD,” Quantum6(2022) 820,arXiv:2203.05582 [quant-ph] 23
-
[5]
Quantum SMEFT tomography: Top quark pair pro- duction at the LHC,
R. Aoude, E. Madge, F. Maltoni, and L. Mantani, “Quantum SMEFT tomography: Top quark pair production at the LHC,”Phys. Rev. D106no. 5, (2022) 055007, arXiv:2203.05619 [hep-ph]
-
[6]
Improved tests of entanglement and Bell inequalities with LHC tops,
J. A. Aguilar-Saavedra and J. A. Casas, “Improved tests of entanglement and Bell inequalities with LHC tops,”Eur. Phys. J. C82no. 8, (2022) 666,arXiv:2205.00542 [hep-ph]
-
[7]
Con- straining new physics in entangled two-qubit systems: top-quark, tau-lepton and photon pairs,
M. Fabbrichesi, R. Floreanini, and E. Gabrielli, “Constraining new physics in entangled two-qubit systems: top-quark, tau-lepton and photon pairs,”Eur. Phys. J. C83no. 2, (2023) 162,arXiv:2208.11723 [hep-ph]
-
[8]
Quantum entanglement and top spin correlations in SMEFT at higher orders,
C. Severi and E. Vryonidou, “Quantum entanglement and top spin correlations in SMEFT at higher orders,”JHEP01(2023) 148,arXiv:2210.09330 [hep-ph]
-
[9]
Entanglement and Bell inequal- ities with boostedt ¯t,
Z. Dong, D. Gon¸ calves, K. Kong, and A. Navarro, “Entanglement and Bell inequal- ities with boostedt ¯t,”Phys. Rev. D109no. 11, (2024) 115023,arXiv:2305.07075 [hep-ph]
-
[10]
M. Varma and O. K. Baker, “Quantum entanglement in top quark pair production,” Nucl. Phys. A1042(2024) 122795,arXiv:2306.07788 [hep-ph]
-
[11]
Aguilar-Saavedra,Postdecay quantum entanglement in top pair production,Phys
J. A. Aguilar-Saavedra, “Postdecay quantum entanglement in top pair production,” Phys. Rev. D108no. 7, (2023) 076025,arXiv:2307.06991 [hep-ph]
-
[12]
Quantum entanglement and Bell inequality violation in semi-leptonic top decays,
T. Han, M. Low, and T. A. Wu, “Quantum entanglement and Bell inequality violation in semi-leptonic top decays,”JHEP07(2024) 192,arXiv:2310.17696 [hep-ph] [13]ATLASCollaboration, G. Aadet al., “Observation of quantum entanglement with top quarks at the ATLAS detector,”Nature633no. 8030, (2024) 542–547, arXiv:2311.07288 [hep-ex]
-
[13]
F. Maltoni, C. Severi, S. Tentori, and E. Vryonidou, “Quantum detection of new physics in top-quark pair production at the LHC,”JHEP03(2024) 099,arXiv:2401.08751 [hep-ph]
-
[14]
Aguilar-Saavedra,A closer look at post-decayt ¯tentanglement,Phys
J. A. Aguilar-Saavedra, “A closer look at post-decayt ¯tentanglement,”Phys. Rev. D 109no. 9, (2024) 096027,arXiv:2401.10988 [hep-ph]
-
[15]
New physics in spin entanglement,
M. Duch, A. Strumia, and A. Titov, “New physics in spin entanglement,”Eur. Phys. J. C85no. 2, (2025) 151,arXiv:2403.14757 [hep-ph]
-
[16]
Testing Bell inequalities in Higgs bo- son decays,
A. J. Barr, “Testing Bell inequalities in Higgs boson decays,”Phys. Lett. B825(2022) 136866,arXiv:2106.01377 [hep-ph]
-
[17]
M. M. Altakach, P. Lamba, F. Maltoni, K. Mawatari, and K. Sakurai, “Quantum in- formation and CP measurement in H→τ+τ- at future lepton colliders,”Phys. Rev. D 107no. 9, (2023) 093002,arXiv:2211.10513 [hep-ph] 24
- [18]
-
[19]
K. Ehat¨ aht, M. Fabbrichesi, L. Marzola, and C. Veelken, “Probing entanglement and testing Bell inequality violation with e+e-→τ+τ- at Belle II,”Phys. Rev. D109no. 3, (2024) 032005,arXiv:2311.17555 [hep-ph]
-
[20]
C. Altomonte, A. J. Barr, M. Eckstein, P. Horodecki, and K. Sakurai, “Prospects for quantum process tomography at high energies,”arXiv:2412.01892 [hep-ph]
-
[21]
Bell-type inequalities for systems of rela- tivistic vector bosons,
A. J. Barr, P. Caban, and J. Rembieli´ nski, “Bell-type inequalities for systems of rela- tivistic vector bosons,”Quantum7(2023) 1070,arXiv:2204.11063 [quant-ph]
-
[22]
J. A. Aguilar-Saavedra, A. Bernal, J. A. Casas, and J. M. Moreno, “Testing entan- glement and Bell inequalities in H→ZZ,”Phys. Rev. D107no. 1, (2023) 016012, arXiv:2209.13441 [hep-ph]
-
[23]
R. Ashby-Pickering, A. J. Barr, and A. Wierzchucka, “Quantum state tomography, en- tanglement detection and Bell violation prospects in weak decays of massive particles,” JHEP05(2023) 020,arXiv:2209.13990 [quant-ph]
-
[24]
M. Fabbrichesi, R. Floreanini, E. Gabrielli, and L. Marzola, “Bell inequalities and quan- tum entanglement in weak gauge boson production at the LHC and future colliders,” Eur. Phys. J. C83no. 9, (2023) 823,arXiv:2302.00683 [hep-ph]
- [25]
- [26]
- [27]
-
[28]
Z-boson quantum tomography at next-to-leading order,
M. Del Gratta, F. Fabbri, M. Grossi, F. Maltoni, D. Pagani, G. Pelliccioli, and A. Vicini, “Z-boson quantum tomography at next-to-leading order,”arXiv:2509.20456 [hep-ph]
-
[29]
Quantum entanglement and Bell inequality violation at colliders,
A. J. Barr, M. Fabbrichesi, R. Floreanini, E. Gabrielli, and L. Marzola, “Quantum entanglement and Bell inequality violation at colliders,”Prog. Part. Nucl. Phys.139 (2024) 104134,arXiv:2402.07972 [hep-ph]
-
[30]
Constraining New Physics withh→V VTomography,
M. Sullivan, “Constraining New Physics withh→V VTomography,” arXiv:2410.10980 [hep-ph]
-
[31]
Quantum properties of H→VV ∗: precise predictions in the SM and sensitivity to new physics,
M. Del Gratta, F. Fabbri, P. Lamba, F. Maltoni, and D. Pagani, “Quantum properties of H→VV ∗: precise predictions in the SM and sensitivity to new physics,”JHEP09 (2025) 013,arXiv:2504.03841 [hep-ph] 25
-
[32]
Entanglement Suppression and Emergent Symmetries of Strong Interactions
S. R. Beane, D. B. Kaplan, N. Klco, and M. J. Savage, “Entanglement Suppression and Emergent Symmetries of Strong Interactions,”Phys. Rev. Lett.122no. 10, (2019) 102001,arXiv:1812.03138 [nucl-th]
work page internal anchor Pith review Pith/arXiv arXiv 2019
-
[33]
Geometry and entanglement in the scattering matrix,
S. R. Beane and R. C. Farrell, “Geometry and entanglement in the scattering matrix,” Annals Phys.433(2021) 168581,arXiv:2011.01278 [hep-th]
-
[34]
Symmetry from entangle- ment suppression,
I. Low and T. Mehen, “Symmetry from entanglement suppression,”Phys. Rev. D104 no. 7, (2021) 074014,arXiv:2104.10835 [hep-th]
-
[35]
Entanglement minimization in hadronic scat- tering with pions,
S. R. Beane, R. C. Farrell, and M. Varma, “Entanglement minimization in hadronic scat- tering with pions,”Int. J. Mod. Phys. A36no. 30, (2021) 2150205,arXiv:2108.00646 [hep-ph]
-
[36]
Minimal entanglement and emergent symmetries in low- energy QCD,
Q. Liu, I. Low, and T. Mehen, “Minimal entanglement and emergent symmetries in low- energy QCD,”Phys. Rev. C107no. 2, (2023) 025204,arXiv:2210.12085 [quant-ph]
-
[37]
Entanglement Sup- pression, Quantum Statistics and Symmetries in Spin-3/2 Baryon Scatterings,
T.-R. Hu, K. Sone, F.-K. Guo, T. Hyodo, and I. Low, “Entanglement Sup- pression, Quantum Statistics and Symmetries in Spin-3/2 Baryon Scatterings,” arXiv:2506.08960 [hep-ph]
-
[38]
Maximal Entanglement in High Energy Physics
A. Cervera-Lierta, J. I. Latorre, J. Rojo, and L. Rottoli, “Maximal Entanglement in High Energy Physics,”SciPost Phys.3no. 5, (2017) 036,arXiv:1703.02989 [hep-th]
work page internal anchor Pith review Pith/arXiv arXiv 2017
-
[39]
Universality of entanglement in gluon dynamics,
C. N´ u˜ nez, A. Cervera-Lierta, and J. I. Latorre, “Universality of entanglement in gluon dynamics,”arXiv:2504.15353 [hep-th]
-
[40]
Entanglement Suppression, Enhanced Symmetry and a Standard-Model-like Higgs Boson,
M. Carena, I. Low, C. E. M. Wagner, and M.-L. Xiao, “Entanglement suppression, enhanced symmetry, and a standard-model-like Higgs boson,”Phys. Rev. D109no. 5, (2024) L051901,arXiv:2307.08112 [hep-ph]
-
[41]
K. Kowalska and E. M. Sessolo, “Entanglement in flavored scalar scattering,”JHEP07 (2024) 156,arXiv:2404.13743 [hep-ph]
-
[42]
S. Chang and G. Jacobo, “Consequences of minimal entanglement in bosonic field the- ories,”Phys. Rev. D110no. 9, (2024) 096020,arXiv:2409.13030 [hep-ph]
- [43]
- [44]
-
[45]
J. Thaler and S. Trifinopoulos, “Flavor patterns of fundamental particles from quantum entanglement?,”Phys. Rev. D111no. 5, (2025) 056021,arXiv:2410.23343 [hep-ph] 26
-
[46]
Momentum-space entanglement and renormalization in quantum field theory
V. Balasubramanian, M. B. McDermott, and M. Van Raamsdonk, “Momentum-space entanglement and renormalization in quantum field theory,”Phys. Rev. D86(2012) 045014,arXiv:1108.3568 [hep-th]
work page internal anchor Pith review Pith/arXiv arXiv 2012
-
[47]
Momentum-space entanglement for interacting fermions at finite density
T.-C. L. Hsu, M. B. McDermott, and M. Van Raamsdonk, “Momentum-space entangle- ment for interacting fermions at finite density,”JHEP11(2013) 121,arXiv:1210.0054 [hep-th]
work page internal anchor Pith review Pith/arXiv arXiv 2013
-
[48]
Variation of Entanglement Entropy in Scattering Process
S. Seki, I. Y. Park, and S.-J. Sin, “Variation of Entanglement Entropy in Scattering Process,”Phys. Lett. B743(2015) 147–153,arXiv:1412.7894 [hep-th]
work page internal anchor Pith review Pith/arXiv arXiv 2015
-
[49]
Entanglement Entropy of Scattering Particles
R. Peschanski and S. Seki, “Entanglement Entropy of Scattering Particles,”Phys. Lett. B758(2016) 89–92,arXiv:1602.00720 [hep-th]
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[50]
Scattering with partial information
D. Carney, L. Chaurette, and G. Semenoff, “Scattering with partial information,” arXiv:1606.03103 [hep-th]
work page internal anchor Pith review Pith/arXiv arXiv
-
[51]
Pertur- bative approach to entanglement generation in QFT using the S matrix,
R. Faleiro, H. A. S. Costa, R. Pav˜ ao, B. Hiller, A. H. Blin, and M. Sampaio, “Pertur- bative approach to entanglement generation in QFT using the S matrix,”J. Phys. A 53no. 36, (2020) 365301,arXiv:1607.01715 [hep-ph]
-
[52]
Evaluation of Entanglement Entropy in High Energy Elastic Scattering,
R. Peschanski and S. Seki, “Evaluation of Entanglement Entropy in High Energy Elastic Scattering,”Phys. Rev. D100no. 7, (2019) 076012,arXiv:1906.09696 [hep-th]
-
[53]
Entanglement of a Pair of Quantum Bits
S. Hill and W. K. Wootters, “Entanglement of a pair of quantum bits,”Phys. Rev. Lett. 78(1997) 5022–5025,arXiv:quant-ph/9703041
work page internal anchor Pith review Pith/arXiv arXiv 1997
-
[54]
Entanglement of Formation of an Arbitrary State of Two Qubits
W. K. Wootters, “Entanglement of formation of an arbitrary state of two qubits,”Phys. Rev. Lett.80(1998) 2245–2248,arXiv:quant-ph/9709029
work page internal anchor Pith review Pith/arXiv arXiv 1998
-
[55]
Separability criterion for density matrices,
A. Peres, “Separability criterion for density matrices,”Phys. Rev. Lett.77(Aug, 1996) 1413–1415.https://link.aps.org/doi/10.1103/PhysRevLett.77.1413
-
[56]
Separability of mixed states: necessary and sufficient conditions,
M. Horodecki, P. Horodecki, and R. Horodecki, “Separability of mixed states: necessary and sufficient conditions,”Physics Letters A223no. 1, (1996) 1–8.https://www. sciencedirect.com/science/article/pii/S0375960196007062
work page 1996
-
[57]
J. D. Fonseca, B. Hiller, J. B. Araujo, I. G. da Paz, and M. Sampaio, “Entanglement and scattering in quantum electrodynamics: S matrix information from an entangled specta- tor particle,”Phys. Rev. D106no. 5, (2022) 056015,arXiv:2112.01300 [quant-ph]
-
[58]
Entanglement distribution in Bhabha scat- tering with an entangled spectator particle,
M. Blasone, G. Lambiase, and B. Micciola, “Entanglement distribution in Bhabha scat- tering with an entangled spectator particle,”Phys. Rev. D109no. 9, (2024) 096022, arXiv:2401.10715 [quant-ph]
-
[59]
Complete com- plementarity relations in tree level QED processes,
M. Blasone, S. De Siena, G. Lambiase, C. Matrella, and B. Micciola, “Complete com- plementarity relations in tree level QED processes,”Phys. Rev. D111no. 1, (2025) 016007,arXiv:2402.09195 [quant-ph] 27
-
[60]
M. Blasone, S. De Siena, G. Lambiase, C. Matrella, and B. Micciola, “Entangle- ment saturation in quantum electrodynamics scattering processes,”arXiv:2505.06878 [quant-ph]
-
[61]
Entanglement dynamics in QED processes,
M. Blasone, S. De Siena, G. Lambiase, C. Matrella, and B. Micciola, “Entanglement dynamics in QED processes,”Chaos Solitons Fractals195(2025) 116305
work page 2025
-
[62]
Tree-level entanglement in quantum electrodynamics,
S. Fedida and A. Serafini, “Tree-level entanglement in quantum electrodynamics,”Phys. Rev. D107no. 11, (2023) 116007,arXiv:2209.01405 [quant-ph]
-
[63]
An Area Law for Entanglement Entropy in Particle Scattering,
I. Low and Z. Yin, “An Area Law for Entanglement Entropy in Particle Scattering,” arXiv:2405.08056 [hep-th]
- [64]
-
[65]
Entanglement features in scattering mediated by heavy particles,
C. M. Sou, Y. Wang, and X. Zhang, “Entanglement features in scattering mediated by heavy particles,”JHEP10(2025) 003,arXiv:2507.03555 [hep-th]
-
[66]
T. Baumgratz, M. Cramer, and M. . Plenio, “Quantifying Coherence,”Phys. Rev. Lett. 113no. 14, (2014) 140401,arXiv:1311.0275 [quant-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2014
-
[67]
McGinnis, (2025), arXiv:2504.21079 [hep-th]
N. McGinnis, “Symmetry, entanglement, and theS-matrix,”arXiv:2504.21079 [hep-th]
-
[68]
Jarlskog-like invariants for theories with scalars and fermions
F. J. Botella and J. P. Silva, “Jarlskog - like invariants for theories with scalars and fermions,”Phys. Rev. D51(1995) 3870–3875,arXiv:hep-ph/9411288
work page internal anchor Pith review Pith/arXiv arXiv 1995
-
[69]
Entanglement through high-energy scattering in noncommutative quan- tum electrodynamics,
C. P. Martin, “Entanglement through high-energy scattering in noncommutative quan- tum electrodynamics,”arXiv:2506.15350 [hep-th]
-
[70]
M. E. Peskin and D. V. Schroeder,An Introduction to quantum field theory. Addison- Wesley, Reading, USA, 1995
work page 1995
-
[71]
F. Halzen and A. D. Martin,Quarks and Leptons: An Introductory Course in Modern Particle Physics. Wiley, 1984 28
work page 1984
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.