REVIEW 4 major objections 4 minor 159 references
Amplituhedra for generic quantum processes via the TQNN representation of UQC
T0 review · 4 major / 4 minor · reviewed 2026-08-04 · deepseek-v4-flash
Pith's one-line read Within a topological quantum neural network, every universal quantum computation corresponds to a scattering process whose amplitudes are encoded by an amplituhedron, and conversely.
desk verdict A competent, honest speculative proposal that re-derives UQC via TQNNs and then sketches—but does not prove—a correspondence to amplituhedra; worth refereeing as a conjecture. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The central objects are TQNNs—topological quantum field theories formulated on spin-networks—and the Reshetikhin-Turaev (RT) and Turaev-Viro (TV) state-sum invariants, which are related by the chain-mail construction: the TV invariant is the absolute square of the RT invariant. The TV model's dependence on the quantum group U_q(sl(2)) is mirrored by the quantum cluster algebra structure of the amplituhedron's coordinate ring, and matching the deformation parameter q with the canonical form establishes the geometric correspondence. This chain turns topological invariants into scattering amplitudes.
What would settle it
If a specific universal quantum computation, such as a simple two-qubit gate implemented in a TQNN, can be shown not to admit a unique amplitude under any reasonable coarse-graining, or if its purported amplituhedron volume fails to reproduce the unitary transition probability, then the correspondence would be refuted.
Extended reading notes
Core claim
The paper's central discovery is Theorem 2: within a TQNN, a universal quantum computation corresponds to a scattering process with amplitudes given by an amplituhedron, and conversely. This is established by first showing that TQNNs implement UQC (Theorem 1), using the Reshetikhin-Turaev modular functor and its equivalence to the Turaev-Viro state sum, which acts as a quantum error-correcting code. The correspondence to amplituhedra is then argued through a parallel between the quantum group U_q(sl(2)) used in the Turaev-Viro model and the quantum cluster algebra of the amplituhedron's coordinate ring, with the deformation parameter q matched to the canonical form. The result implies that a
Load-bearing premise
Amplituhedra and their amplitudes are only well-defined if the quantum process has well-defined, unique amplitudes, which depends on state purity and the level of coarse-graining; the paper explicitly leaves this as an open question.
Editorial extensions
If this is right
- Any quantum circuit that can be implemented within a TQNN admits a geometric representation as an amplituhedron, allowing amplitudes to be computed without perturbative or off-shell methods.
- The Turaev-Viro model, interpreted as a quantum error-correcting code, provides a concrete physical mechanism for UQC through TQNNs, linking 3-manifold topology to quantum information processing.
- Because computing the TV invariant is #P-hard, the correspondence suggests that evaluating amplituhedron amplitudes for generic processes is computationally hard, with consequences for quantum complexity theory.
- The operational equivalence of computation and scattering, together with the amplituhedron representation, offers a new route for quantum simulation of scattering in scalar field theories and for studying complexity measures such as the momentum/complexity correspondence.
Reading between the lines
- A natural testable extension is to construct explicit amplituhedron volumes for small quantum circuits (e.g., two-qubit gates) and verify that they reproduce known transition probabilities, providing a concrete check of the correspondence.
- If the correspondence holds for all generic quantum processes, it would unify the geometric description of particle physics with quantum information science, potentially offering a 'positive geometry' formulation of quantum gravity, although the paper leaves the uniqueness of amplitudes open.
- The edge complexity of the amplituhedron might serve as an operational, but not within-protocol observable, measure of how much two parties 'speak the same language' in an LOCC protocol, suggesting a new diagnostic for quantum reference frame alignment.
- The link to #P-hardness raises the possibility that the difficulty of computing amplituhedron amplitudes could be used to probe the P vs NP question, if a family of computations is found whose geometry complexity scales in a way that distinguishes the classes.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper develops an operational and formal bridge between universal quantum computation (UQC) and scattering processes. It first argues, using an LOCC/QRF framework, that any computation can be viewed as a scattering process and vice versa. It then reviews TQNNs built from Reshetikhin-Turaev and Turaev-Viro TQFTs, and claims (Theorem 1) that such TQNNs implement UQC, grounding this in known results on topological quantum computation and Turaev-Viro quantum error-correcting codes. The central new claim is Theorem 2 in §4.5: within a TQNN, a UQC corresponds to a scattering process with amplitudes given by an amplituhedron, and conversely. The paper supports this by a series of analogies between the Turaev-Viro model (tetrahedra, 6j-symbols, quantum group U_q(sl(2))) and the amplituhedron (positroid cells, BCFW recursion, cluster algebras), and it postulates a cell-complex map in Eq. (37). The conclusion discusses potential applications and explicitly concedes that well-defined unique amplitudes for generic quantum processes remain an open question.
Significance. If Theorem 2 were established, the paper would provide a genuinely new bridge between topological quantum computation and positive geometry, potentially extending amplituhedron methods from planar N=4 SYM to arbitrary quantum processes. The background material in §§3.2–3.9 is a coherent synthesis of established results: the relation between RT and TV invariants, the construction of TV codes as QECCs, and the universality of the Freedman–Kitaev–Wang model are all supported by standard citations. However, the new claim is not demonstrated. The only constructive step toward Theorem 2 is a postulate (Eq. (37)), and the paper itself states that the well-definedness of amplitudes for generic processes is open. Thus the paper is best read as a speculative research proposal rather than an established formal result.
major comments (4)
- [§4.5, Theorem 2 and Eq. (37)] The central correspondence is asserted, not proved. Theorem 2 is introduced by “the above discussion and details ... can be summarized by,” and the only constructive content is Eq. (37), where the authors “postulate” maps between TV tetrahedra and positroid cells as maps of cell-complexes. No explicit dictionary is given from TQNN data (a triangulated 3-manifold, edge labelings, boundary spin networks, a mapping-class element h, level k) to amplituhedron data (n, k, Z, helicity sector, loop number). Without such a map, the parallels listed in §§4.3–4.5 remain analogies, not a correspondence.
- [§4.5, after Eq. (37)] Even if a cell-complex map were intended, it must be compatible with the triangulation independence of the Turaev-Viro state sum. The TV invariant does not depend on the choice of triangulation, so any assignment of positroid cells to tetrahedra must be invariant under Pachner moves, or at least accompanied by a rule for how the amplituhedron data transforms under these moves. The paper neither states such a rule nor checks invariance. This is load-bearing because Theorem 2 quantifies over all TQNN computations, not just a preferred triangulation.
- [§4.5, Eq. (36)] The q-matching is not derived. In the TV model q is a root of unity fixed by the level k, while in Eq. (36) q appears as the formal deformation parameter of a quantum torus/cluster algebra via x_i x_j = q^{2 ε_{ij}} x_j x_i. The paper provides no relation between k (or the edge spins) and the cluster data (ε_{ij}, exponents a_{ij}). Moreover, Eq. (36) is presented without derivation from amplituhedron geometry and without checking that its logarithmic singularities reproduce the canonical form. This identification is a free parameter, not a theorem.
- [§5, first paragraph] The paper explicitly concedes: “Amplituhedra are well-defined only if the amplitudes they represent are well-defined. Whether unique amplituhedra can be assigned to a process depends on whether unique amplitudes can be assigned, which in turn depends on state purity and hence the level of effective coarse-graining.” This directly limits the claim of amplituhedra for generic quantum processes. Even in the TQNN-restricted case where transition amplitudes are well defined, Theorem 2 lacks the proof requested in the preceding comments; the generic-process extension is therefore unsupported.
minor comments (4)
- [Eq. (37)] Typographical issues: “postitroid” should be “positroid,” and “tetraheda” should be “tetrahedra.” The notation “positroid (cells) polytopes” is ambiguous; presumably “positroid cell polytopes” or simply “positroid cells” is intended.
- [§4.4, Eq. (26)] The displayed Poisson bracket uses a four-dimensional ε_{μνρσ} together with δ^{(D)}(x−y) in a formula claimed for arbitrary dimension D. This is inconsistent; either the formula should be restricted to D=4 or the ε symbol should be replaced by the appropriate D-dimensional structure.
- [§4.4, Eq. (22)] The exponents γ_j are said to be “determined by the dimension,” but no explicit formula or reference is given. The notation ⟨C_{1⋯k}⟩ is also used without definition in this context.
- [§3.6] “the unimodular functor V” appears to be a typo for “the modular functor V.” This occurs in the first sentence of the fourth paragraph.
Circularity Check
Theorem 2 is not derived: the TQNN–amplituhedron 'correspondence' is created by a q-matching ansatz and by postulating the tetrahedron/positroid-cell map (37), then restated as a theorem.
-
self definitional
[Section 4.5, Eq. (36), and Introduction's summary of the argument]
"the canonical form Ω(3)n,k can be expressed as ... where the exponents aij define a quantum torus algebra with relations x_i x_j = q^{2ϵ_ij} x_j x_i, matching the deformation parameter q in the Turaev-Viro model when ϵ_ij is the skew-symmetric form defining the cluster algebra."
The 'correspondence' between the amplituhedron canonical form and the TV model is produced by identifying the formal cluster-algebra deformation parameter q with the TV deformation parameter q. The paper writes the amplituhedron canonical form with a quantum torus relation x_i x_j = q^{2ϵ_ij} x_j x_i and then says this is 'matching the deformation parameter q in the Turaev-Viro model when ϵ_ij is the skew-symmetric form defining the cluster algebra.' This is a definitional match: the amplituhedron literature's q is a quantization parameter of a cluster algebra, while TV's q is a root of unity from U_q(sl(2)); no argument shows that the skew-symmetric form ϵ_ij turns one into the other. The claimed resemblance is created by the choice of q, and Theorem 2 is then presented as its consequence
-
self definitional
[Section 4.5, Theorem 2 and Eq. (37)]
"Since the Turaev-Viro model is incorporated into a TQNN for UQC (Theorem 1), the above discussion and details, together with those of §2 and §3, can be summarized by: Theorem 2. Within a TQNN, a UQC corresponds to a scattering process with amplitudes given by an amplituhedron, and conversely. Via this correspondence, we can postulates maps TV tetraheda⇄postitroid (cells) polytopes (37) as maps of cell-complexes."
The theorem is introduced as a summary of 'the above discussion', but the discussion consists of structural analogies; the only constructive content that would substantiate the theorem is the map (37), which is explicitly 'postulated' after the theorem is stated. The asserted correspondence is therefore not derived from TQNN or amplituhedron theory; it is stipulated via the very maps the theorem needs to guarantee. No dictionary is given from TQNN data (triangulation, boundary spin labels, level k, mapping-class element) to amplituhedron data (n,k,Z), and no check is made that a tetrahedron-to-positroid-cell map is invariant under the Pachner moves on which the TV state sum's well-definedness rests. Thus Theorem 2 reduces to its own postulate.
full rationale
The TQNN/UQC part of the paper (Theorem 1) is not circular: it leans on external results of Freedman, Kitaev, Larsen, Wang and on the standard RT/TV relation, with self-citations playing only auxiliary expository roles. The problematic part is the new amplituhedron claim. Section 4.5 assembles analogies between TV tetrahedra and positroid cells, 6j recursion and BCFW recursion, and q-deformations, then states Theorem 2. No concrete, well-defined map from a TQNN's triangulation, boundary spin-network labels, level k, or mapping-class-group element to the external data (n,k,Z) of an amplituhedron is given. The only constructive step is Eq. (37), where the maps are 'postulated'; a theorem cannot be supported by postulating the very maps that constitute its conclusion. Likewise, Eq. (36) manufactures the correspondence by declaring the cluster-algebra q to 'match' the TV deformation parameter, a choice rather than a derivation. Section 5's admission that unique amplituhedra require unproven unique amplitudes further shows the central claim is conditional and unsupported, though that is a correctness limitation rather than circularity. Because the central claim reduces, by construction, to a q-matching and a postulated map, the circularity score is 7; the externally grounded TQNN/UQC portion prevents a higher score, and the paper does not rely on a self-citation chain to force the amplituhedron result.
Assumptions & free parameters
free parameters (1)
- Identification of q in TV model with q in amplituhedron cluster algebra =
q (deformation parameter, value e^{π i /5} for UQC)
assumptions (4)
- domain assumption Any measurable physical process can be interpreted as computation (from [13]).
- domain assumption TQNNs simulate the Turaev-Viro invariant (from [23]).
- standard math The RT modular functor for U_q(sl(2)) at q=e^{πi/5} is universal for quantum computation ([83]).
- ad hoc to paper There exists a map between TV tetrahedra and amplituhedron positroid cells as cell complexes (eq. 37).
invented entities (1)
-
Amplituhedra for generic quantum processes
Cite this review
Pith. "Pith review of Amplituhedra for generic quantum processes via the TQNN representation of UQC." pith.science (2026). https://pith.science/paper/CDCX7CAF
@misc{pith2026250919772,
author = {Pith},
title = {Pith review of: Amplituhedra for generic quantum processes via the TQNN representation of UQC},
year = {2026},
howpublished = {\url{https://pith.science/paper/CDCX7CAF}},
note = {Machine review of arXiv:2509.19772}
}
read the original abstract
We study the relationship between computation and scattering both operationally (hence phenomenologically) and formally. We develop a representation of universal quantum computation (UQC) within the formalism of topological quantum neural networks (TQNNs), using the Reshetikhin-Turaev and Turaev-Viro models to show how TQNNs implement quantum error-correcting codes. We then exhibit a formal correspondence between TQNNs and amplituhedra to support the existence of amplituhedra for representing generic quantum processes. This construction shows how amplituhedra are geometric representations of underlying topological structures. We conclude by pointing to applications areas enabled by these results.
Figures
Reference graph
Works this paper leans on
-
[1]
Feynman, R. P. Simulating physics with computers.Int. J. Theor. Phys.21 (1982), 467–488
1982
-
[2]
Universal quantum simulations.Science273 (1996), 1073–1078
Lloyd, S. Universal quantum simulations.Science273 (1996), 1073–1078
1996
-
[3]
and Huang, Y.-t.Scattering Amplitudes in Gauge Theory and Gravity
Elvang, H. and Huang, Y.-t.Scattering Amplitudes in Gauge Theory and Gravity. Cambridge Univ. Press, Cambridge UK, 2015
2015
-
[4]
Henn, J. M. and Plefka, J. C.Scattering Amplitudes in Gauge Theories. Lecture Notes in Physics 883, Springer Heidelberg-New York (2014), 1–195
2014
-
[5]
P., Lee, K
Jordan, S. P., Lee, K. S. M. and Preskill, J. Quantum computation of scattering in scalar quantum field theories.Quantum Information and Computation14 (2014), 1014–1080
2014
-
[6]
A., Quaglioni, S., Pederiva, F
Turro, F., Wendt, K. A., Quaglioni, S., Pederiva, F. and Roggero, A. Evalua- tion of phase shifts for non-relativistic elastic scattering using quantum computers. arXiv:2407.04155v2 [quant-ph]. 32
-
[7]
Nielsen, M. A. and Chuang, I. L.Quantum Computation and Quantum Information. Cambridge Univ. Press. 2000
2000
-
[8]
Shor, P. W. Algorithms for quantum computation: discrete logarithms and factoring. Proc. 35th Ann. Sympos. on Found. Comp. Sci., Santa Fe NM (1994), 124–134
1994
Show all 159 references
-
[9]
and Milburn, G
Knill, E., Laflamme, R. and Milburn, G. J. A scheme for efficient quantum compu- tation with linear optics.Nature409 (2001), 46–52
2001
-
[10]
M., Gosset, D
Childs, A. M., Gosset, D. and Webb, Z. Universal computation by multiparticle quantum walk.Science339(6121) (2013), 791–794
2013
-
[11]
and Thomas, N
Bao, N., Hayden, P., Salton, G. and Thomas, N. Universal quantum computation by scattering in the Fermi-Hubbard model.New J. Phys.17 (2015), 093028
2015
-
[12]
Consequences of nonclassical measurement for the algorithmic description of continuous dynamical systems.J
Fields, C. Consequences of nonclassical measurement for the algorithmic description of continuous dynamical systems.J. Expt. Theor. Artif. Intell.1 (1989) 171-178
1989
-
[13]
When does a physical system compute?Proc
Horsman, C., Stepney, S., Wagner, R.C., and Kendon, V. When does a physical system compute?Proc. R. Soc. A470 (2014), 20140182
2014
-
[14]
White, C. D. and White, M. J. Magic states of Top quarks.Phys. Rev. D110 (2024), 116016
2024
-
[15]
and Trnka, J
Arkani-Hamed, N. and Trnka, J. The Amplituhedron.J. High Energy Physics30 (2014), 30
2014
-
[16]
Chitambar, E., Leung, D., Manˇ cinska, L., Ozols. M. and Winter, A. Everything you always wanted to know about LOCC (but were afraid to ask).Commun. Math. Phys. 328 (2014), 303-326
2014
-
[17]
Fields, C., Glazebrook, J. F. and Marcian` o, A. Sequential measurements, topological quantum field theories, and topological quantum neural networks.Fortschr. Physik 70 (2022), 202200104
2022
-
[18]
D., Rudolph, T
Bartlett, S. D., Rudolph, T. and Spekkens, R. W. Reference frames, super-selection rules, and quantum information.Rev. Mod. Phys.79 (2007), 555-609
2007
-
[19]
Atiyah, M. F. Topological quantum field theory.Publ. Math. IH ´ES68 (1988), 175– 186
1988
-
[20]
Quantum theory, the Church-Turing principle, and the universal quantum computer.Proc
Deutsch, D. Quantum theory, the Church-Turing principle, and the universal quantum computer.Proc. R. Soc. London A400 (1985), 97-117
1985
-
[21]
Angular momentum: An approach to combinatorial space-time
Penrose, R. Angular momentum: An approach to combinatorial space-time. In (T. Bastin ed.)Quantum Theory and Beyond, pp. 151–180. Cambridge Univ. Press, Cam- bridge UK, 1971. 33
1971
-
[22]
The future of spin networks
Smolin, L. The future of spin networks. (1997) arXiv:gr-qc/9702030
1997 arXiv
-
[23]
Marcian` o, A., Chen, D., Fabrocini, F. et al. Quantum neural networks and topological quantum field theories.Neural Networks153 (2022), 164–178
2022
-
[24]
Marcian` o, A., Zappala, E., Torda, T. et al. Deep neural networks as the semi- classical limit of topological quantumm neural networks: the problem of general- ization. arXiv:2210.13741v2, 2024
2024 arXiv
-
[25]
H., Kitaev, A
Freedman, M. H., Kitaev, A. and Wang, Z. Simulation of topological field theories by quantum computers.. Comm. Math. Phys.227(3) (2002), 587–603
2002
-
[26]
H., Kitaev, A., Larsen, M
Freedman, M. H., Kitaev, A., Larsen, M. J. and Wang, Z. Topological quantum computation.Bull. Amer. Soc.40(1) (2002), 31–38
2002
-
[27]
and Reichardt, B
Koenig, R., Kuperberg, G. and Reichardt, B. W. Quantum computation with Turaev- Viro codes.Annals of Physics325 (2010), 2707–2749
2010
-
[28]
Fields, C., Glazebrook, J. F. and Marcian` o, A. Communication protocols and QECCs from the perspective of TQFT, Part I: Constructing LOCC protocols and QECCs from TQFTs.Fortschr. Physik72 (2024), 202400049
2024
-
[29]
and Marcian` o, A
Fields, C. and Marcian` o, A. Holographic screens are classical information channels. Quant. Rep.2 (2019), 326–336
2019
-
[30]
Fields, C., Glazebrook, J. F. and Marcian` o, A. The physical meaning of the Holo- graphic Principle.Quanta11 (2022), 72-96
2022
-
[31]
Fields, C.; Glazebrook, J. F. Information flow in context-dependent hierarchical Bayesian inference.J. Expt. Theor. Artif. Intell.34 (2022), 111–142
2022
-
[32]
and Glazebrook, J
Fields, C. and Glazebrook, J. F. Separability, contextuality, and the quantum Frame Problem.Int. J. Theor. Phys.62 (2023), 159
2023
-
[33]
F., Marcian` o, A
Fields, C., Glazebrook, J. F., Marcian` o, A. and Zappala, E. ER=EPR is an opera- tional theorem.Phys. Lett. B860 (2025), 139150
2025
-
[34]
Mikusch, M., Barbado, L. C. and Brukner, ˘C. Transformations of spin in quantum reference frames.Phys. Rev. Res.3 (2021), 043138, 12pp
2021
-
[35]
and Loveridge, L
Carette, T., G lowacki, J. and Loveridge, L. Operational quantum reference frames. Quantum(9) (2025), 1680
2025
-
[36]
C., Girelli, F
Palmer, M. C., Girelli, F. and Bartlett, S. D. Changing quantum reference frames. Phys. Rev. A89 (2014), 052121
2014
-
[37]
and Brukner, ˘C
Giacomini, F., Castro-Ruiz, E. and Brukner, ˘C. Relativisic quantum reference frames: the operational meaning of spin.Phys. Rev. Lett.123 (2019), 090404. 34
2019
-
[38]
and Brukner, ˘C
Giacomini, F., Castro-Ruiz, E. and Brukner, ˘C. Quantum mechanics and the covari- ance of physical laws in quantum reference frames.Nat. Commun.10 (2019), 1
2019
-
[39]
and Galley, T
de la Hamette, A.-C. and Galley, T. D. Quantum reference frames for general sym- metry groups.Quantum4 (2020), 367
2020
-
[40]
On Computable Numbers, with an Application to the Entscheidungsprob- lem.Proc
Turing, A. On Computable Numbers, with an Application to the Entscheidungsprob- lem.Proc. London Math. Soc.s2-42(1) (1937), 230–265
1937
-
[41]
and Seligman, J.Information Flow: The Logic of Distributed Systems (Cambridge Tracts in Theoretical Computer Science, 44)
Barwise, J. and Seligman, J.Information Flow: The Logic of Distributed Systems (Cambridge Tracts in Theoretical Computer Science, 44). Cambridge, UK: Cambridge University Press, 1997
1997
-
[42]
and Glazebrook, J
Fields, C. and Glazebrook, J. F. A mosaic of Chu spaces and Channel Theory I: Category-theoretic concepts and tools.J. Expt. Theor. Artif. Intell.31 (2019), 177- 213
2019
-
[43]
P and Welling, M
Kingma, D. P and Welling, M. An Introduction to variational autoencoders.Foun- dations and Trends in Machine Learning12(4) (2019), 307–392
2019
-
[44]
Chu spaces.School on Category Theory and Applications (Coimbra 1999), Vol
Pratt, V. Chu spaces.School on Category Theory and Applications (Coimbra 1999), Vol. 21 ofTextos Mat. S´ er. B, University of Coimbra, Coimbra. (pp. 39–100), 1999
1999
-
[45]
Chu spaces from the representational viewpoint.Ann
Pratt, V. Chu spaces from the representational viewpoint.Ann. Pure Appl. Logic96 (1999), 319–333
1999
-
[46]
Baez, J. C. Spin network states in gauge theory.Adv. Math.117 (1996), 253–272
1996
-
[47]
and Suresh, D
Vaid, D. and Suresh, D. Coherent states and particle scattering in loop quantum gravity.Eur. Phys. J. C82 (2022), 723
2022
-
[48]
Basu S. K. Transformations on directed graphs.J. Comb. Theor.9 (1970), 244–256
1970
-
[49]
Cooper, D. C. Theoretical results concerning programs regarded as directed graphs. In (D. Mitchic, ed.)Proc. Second Machine Intelligence ConferenceEdinburgh, July
-
[50]
and van der Veen, R
Garoufalidis, S. and van der Veen, R. (with an appendix by D. Zagier).Geom. Topol. 17 (2013), 1–37
2013
-
[51]
Garcia-Escartin, J. C. and Chamorro-Posada, P. Universal quantum computation with the orbital angular momentum of a single photon.Journal of Optics13(6) (2010), 064022
2010
-
[52]
Reck, M., Zeilinger, A., Bernstein, H. J. and Bertani. P. Experimental realization of any discrete unitary operator.Phys. Rev. Lett.73(1) (1994), 58–62
1994
-
[53]
Experimental realization of any discrete operator
Svozil, K. Experimental realization of any discrete operator. (1996) arXiv:quant- ph/9612010v1 35
1996
-
[54]
and Sun, C
Yang, S., Song, Z. and Sun, C. Beam splitter for spin waves in quantum spin network. Eur. Phys. J.52 (2006), 377–381
2006
-
[55]
S., Messina, A
Grimaudo, R., Magalh˜ aese de Castro, A. S., Messina, A. and Valenti, D. Spin-chain star systems: entangling multiple chains of spin qubits.Fortschr. Physik70 (2022), 2200042
2022
-
[56]
and Song, Z
Jin, L. and Song, Z. Generation of GHZ and W states for stationary qubits in spin network via resonance scattering.Phys. Rev. A79 (2009), 04234
2009
-
[57]
Quantum computational networks.Proc
Deutsch, D. Quantum computational networks.Proc. Royal Soc. London A425 (1989), 73–90
1989
-
[58]
Fault-tolerant quantum computation by anyons.Annals of Physics303 (1977), 2-30
Kitaev, A. Fault-tolerant quantum computation by anyons.Annals of Physics303 (1977), 2-30
1977
-
[59]
F.The Geometry and Physics of Knots
Atiyah, M. F.The Geometry and Physics of Knots. Cambridge Univ. Press, Cam- bridge UK, 1990
1990
-
[60]
and Regge, T
Ponzano, G. and Regge, T. Semiclassical limit of Racah coefficients. In (F. Bloch, ed.)Spectroscopic and group theoretical methods in physics. North Holland, 1968
1968
-
[61]
and Viro, O
Turaev, V. and Viro, O. State sum invariants of 3-manifolds and quantum 6j symbols. Topology31 (1992), 865–902
1992
-
[62]
Foxon, T. J. Spin networks, Turaev-Viro theory and the loop representation.Class. Quant. Grav.12 (1995), 951–964
1995
-
[63]
Basis of the Ponzano-Regge-Turaev-Viro-Ooguri quantum gravity model is the loop representation basis.Phys
Rovelli, C. Basis of the Ponzano-Regge-Turaev-Viro-Ooguri quantum gravity model is the loop representation basis.Phys. Rev. D48 (1993), 2702-2707
1993
-
[64]
On Witten’s 3-maiifold invariants, preprint (1991), https://canyon23.net/math/1991TQFTNotes.pdf
Walker, K. On Witten’s 3-maiifold invariants, preprint (1991), https://canyon23.net/math/1991TQFTNotes.pdf
1991
-
[65]
Shadow links and face models of statistical mechanics.J
Turaev, V. Shadow links and face models of statistical mechanics.J. Diff. Geom.36 (1992), 35–74
1992
-
[66]
Barrett, J. W. and Westbury, B. W. Spherical categories.Adv. Math.143 (1999), 357–375
1999
-
[67]
Skein theory and Turaev-Viro invariants.Topology34(4) (1995), 771–787
Roberts, J. Skein theory and Turaev-Viro invariants.Topology34(4) (1995), 771–787
1995
-
[68]
G.Quantum Invariants of Knots and 3-Manifolds
Turaev, V. G.Quantum Invariants of Knots and 3-Manifolds. De Gruyter, Berlin DE, 2010
2010
-
[69]
Turaev, Y. G. and Viro, O. Y. State sum invariants of 3-manifolds and quantum 6j-symbols.Topology31 (1992), 865–902. 36
1992
-
[70]
and Turaev, V
Reshetikhin, N. and Turaev, V. Invariants of 3-manifolds via link polynomials and quantum groups.Invent. Math.103 (1991), 547–597
1991
-
[71]
H., Lins, S
Kauffman, L. H., Lins, S. Temperley-Lieb recoupling theory and invariants of 3- manifolds.Princeton University PressPrinceton NY, 1994
1994
-
[72]
Lickorish, W. B. The skein method for three-manifold invariants,Journal of Knot Theory and Its Ramifications02(02) (1993), 171–194
1993
-
[73]
Lickorish, W. B. Skeins and handlebodies,Pacific J. Math.159 (1993), 337–349
1993
-
[74]
Lickorish, W. B. R. A representation of orientable combinatorial 3-manifolds,Annals of Mathematics, 76 (3) (1962), 531–540
1962
-
[75]
Wallace, A. H. Modifications and cobounding manifolds,Canadian Journal of Math- ematics, 12 (1960), 503–528
1960
-
[76]
Quantum groups and subfactors of type B, C, and D,Communications in Mathematical Physics, 133(2) (1990), 383–432
Wenzl, H. Quantum groups and subfactors of type B, C, and D,Communications in Mathematical Physics, 133(2) (1990), 383–432
1990
-
[77]
and Zappal` a, E
Lulli, M., Marcian` o, A. and Zappal` a, E. Exact Evaluation of Hexagonal Spin- Networks for Topological Quantum Neural Networks,Fortschritte der Physik, 73(6) (2025), e70005
2025
-
[78]
Kirillov Jr, Alexander, String-net model of Turaev-Viro invariants arXiv preprint arXiv:1106.6033 2011
2011 arXiv
-
[79]
Levin, M. A. and Wen, X.-G., String-net condensation: A physical mechanism for topological phases,Physical Review B—Condensed Matter and Materials Physics71 (2005), 045110
2005
-
[80]
and Laflamme, R
Knill, E. and Laflamme, R. Theory of quantum error-correcting codes.Phys. Rev. A 55 (1997), 900–911
1997
-
[81]
and Wakui, M
Kawahigashi, Y., Sato, N. and Wakui, M. (2 + 1)-dimensional topological quantum field theory and Dehn surgery formula for 3-manifold invariants.Adv. Math.195 (2005), 165–204
2005
-
[82]
and Lo, C
Alagic, G. and Lo, C. Quantum invariants of 3-manifolds and NP vs #P.Quantum Information and Computation17(1,2) (2017), 0125–0146
2017
-
[83]
H., Larsen, M
Freedman, M. H., Larsen, M. and Wang, Z. A modular functor which is universal for quantum computation,Communications in Mathematical Physics, 227 (2002), 605–622
2002
-
[84]
Freedman, M. H. P/NP, and the quantum field computer.Proc. Nat. Acad. Sci. USA 95 (1998), 98–111. 37
1998
-
[85]
and Post- nikov, A.Grassmannian Geometry of Scattering Amplitudes
Arkani-Hamed, N., Bourjaily, J., Cachazo, F., Goncharov, A., Trnka, J. and Post- nikov, A.Grassmannian Geometry of Scattering Amplitudes. Cambridge University Press, Cambridge UK, 2016
2016
-
[86]
and Sturmfels, B
Speyer, D. and Sturmfels, B. The tropical Grassmannian.Advances in Geometry4(3) (2004), 389–411
2004
-
[87]
Ardila-Mantilla, F., The geometry of geometries: matroid theory, old and new, In, Proc. Int. Cong. Math.6 (2022), 4510-4541
2022
-
[88]
, Recent developments in algebraic combinatorics, InIsrael Journal of Mathematics143.1 (2004), 317-339
Stanley, R.P. , Recent developments in algebraic combinatorics, InIsrael Journal of Mathematics143.1 (2004), 317-339
2004
-
[89]
Neukirch, J., Algebraic Number Theory, Springer Berlin, Heidelberg, 2196-9701
-
[90]
and W¨ uthrich, C., Spacetime is as spacetime does, InStud
Lam, V. and W¨ uthrich, C., Spacetime is as spacetime does, InStud. Hist. Phil. Sci. B64 (2018), 39-51
2018
-
[91]
Travaglini, G., Brandhuber, A., Dorey, P., McLoughlin, T., Abreu, S., Bern, Z., Bjerrum-Bohr, N. E. J., Bl¨ umlein, J., Britto, R. and Carrasco, J. J. M.et al., The SAGEX review on scattering amplitudes, InJ. Phys. A55, 44 (2022), 443001
2022
-
[92]
M., Celestial Holography, [arXiv:2111.11392 [hep-th]]
Pasterski, S., Pate, M., and Raclariu, A. M., Celestial Holography, [arXiv:2111.11392 [hep-th]]
-
[93]
and Trnka, J., Nonperturbative negative geometries: amplitudes at strong coupling and the amplituhedron, InJHEP03 (2022), 108
Arkani-Hamed, N., Henn, J. and Trnka, J., Nonperturbative negative geometries: amplitudes at strong coupling and the amplituhedron, InJHEP03 (2022), 108
2022
-
[94]
Bern, Z., and Trnka, J., Snowmass TF04 Report: Scattering Amplitudes and their Applications, [arXiv:2210.03146 [hep-th]]
-
[95]
Topological Quantum Field Theory,Commun
Witten, E. Topological Quantum Field Theory,Commun. Math. Phys.117 (1988), 353
1988
-
[96]
and Thompson, G
Birmingham, D., Blau, M., Rakowski, M. and Thompson, G. Geometry of topological field theory.Phys. Rept.209 (1991), 129–340
1991
-
[97]
Differential geometry of Grassmann manifolds.Proc
Wong, Y.-C. Differential geometry of Grassmann manifolds.Proc. Natl. Acad. Sci. USA57 (3), 589–594
-
[98]
M., Goresky
Gelfand, I. M., Goresky. R. M., MacPherson, R. D. and Serganova, V. V. Combina- torial geometries, convex polyhedra, and Schubert cells.Adv. in Math.63(3) (1987), 301–316
1987
-
[99]
and Postnikov, A
Lam, T. and Postnikov, A. Alcoved polytopes I.Discrete and Combinatorial Geometry 38(3) (2007), 453-478
2007
-
[100]
and Hynbida, J
Dittrich, B. and Hynbida, J. Ising model from intertwiners.Ann. Inst. Henri Poincar´ e Comb. Phys. Interact.3 (2016), 363–380. 38
2016
-
[101]
and Zhang, Y
Guevara, A. and Zhang, Y. Planar matrices and arrays of Feynman diagrams: poles for higherk.Commun. in Theor. Phys.76(4), 045001
-
[102]
and Williams, L
Lukowski, T., Parisi, M. and Williams, L. K. The positive tropical Grassmannian, the hypersimplex, and them= 2 amplituhedron.Int. Math. Res. Notes19 (2023), 16778–16836
2023
-
[103]
and Williams, L
Parisi, M., Sherman-Bennett, M. and Williams, L. K. Them= 2 amplituhedron and the hypersimplex: signs, clusters, tilings, Eulerian numbers.Comm. Amer. Math. Soc.3 (2023), 329–399
2023
-
[104]
and Williams, L
Tsukerman, E. and Williams, L. Bruhat interval polytopes.Adv. in Math.285 (2015), 766–810
2015
-
[105]
and Postnikov, A
Lam, T. and Postnikov, A. Polypositroids.Forum of Mathematics, Sigma12 (2024), 42
2024
-
[106]
Positive Grassmannian and polyhedral subdivions.Proc
Postnikov, A. Positive Grassmannian and polyhedral subdivions.Proc. Int. Cong. Math. (2018). World Scientific, April (2019), 3181–3211
2018
-
[107]
Rinc´ on,, F
Ardila, F. Rinc´ on,, F. and Williams, L. Positroids, non-crossing partitions, and posi- tively oriented manifolds. In (C. Clivans, ed.)26th International Conference on For- mal Power Series and Algebraic Combinatorics (FPSAC), pp. 655–666. DePaul Univ., Chicago IL (2014)
2014
-
[109]
and Parisi, M
Damgaard, D., Ferro, L., /Lukowski, T. and Parisi, M. The momentum amplituhe- dron.JHEP08 (2019), 042
2019
-
[110]
Cambridge Univ
Hatcher, A.Algebraic Topology. Cambridge Univ. Press, Cambridge UK, 2002
2002
-
[111]
Galashin, P., Karp, S. N. and Lam, T. The totally nonnegative Grassmannian is a ball.Adv. Math.397 (2022), 108–123
2022
-
[112]
Galashin, P., Karp, S. N. and Lam, T. Regularity theorem for totally nonnegative flag varities.J. Amer. Math. Soc.35 (2022), 513–579
2022
- [113]
-
[114]
and Huang, Y
Elvang, H. and Huang, Y. T., Scattering Amplitudes in Gauge Theory and Gravity, Cambridge University Press (2015)
2015
-
[115]
and Suresh, D., Coherent states and particle scattering in loop quantum gravity, InEur
Vaid, D. and Suresh, D., Coherent states and particle scattering in loop quantum gravity, InEur. Phys. J. C82, 8, (2022), 723
2022
-
[116]
Quantum Grav.4 (1987), 1565
Barrett, J.W., The geometry of classical Regge calculus, InClass. Quantum Grav.4 (1987), 1565. 39
1987
-
[117]
Freidel, L., Group field theory: An Overview, InInt. J. Theor. Phys.44 (2005), 1769-1783
2005
-
[118]
Press (2004)
Rovelli, C.Quantum Gravity.Cambridge Univ. Press (2004)
2004
-
[119]
and Vidotto, F.Covariant Loop Quantum Gravity.Cambridge Univ
Rovelli, C. and Vidotto, F.Covariant Loop Quantum Gravity.Cambridge Univ. Press (2014)
2014
-
[120]
Gresnigt, N., Marciano, A., and Zappala, E., Dynamical emergence ofSU q(2) from the regularization of (2 + 1)Dgravity with a cosmological constant, InPhys. Rev. D 107, 4 (2023), 046018
2023
-
[121]
and Gordon, R
Schulten, K. and Gordon, R. G., Exact Recursive Evaluation of 3J and 6J Coefficients for Quantum Mechanical Coupling of Angular Momenta, InJ. Math. Phys.16 (1975), 1961-1970
1975
-
[122]
and Witten, E., Direct proof of tree-level recursion relation in Yang-Mills theory, InPhys
Britto, R., Cachazo, F., Feng, B. and Witten, E., Direct proof of tree-level recursion relation in Yang-Mills theory, InPhys. Rev. Lett.94 (2005), 181602
2005
-
[123]
and Martin-Dussaud, P., Causal Structure in Spin Foams, InUniverse 10, 4 (2024), 181
Bianchi, E. and Martin-Dussaud, P., Causal Structure in Spin Foams, InUniverse 10, 4 (2024), 181
2024
-
[124]
High Energ
Skinner, D., A Direct Proof of BCFW Recursion for Twistor-Strings, InJ. High Energ. Phys.01 (2011), 072
2011
-
[125]
and Trnka, J
Arkani-Hamed, N., Thomas, H. and Trnka, J. Unwinding the amplituhedron in binary, InJ. High Energ. Phys.01 (2018), 016
2018
-
[126]
H., Ferro, L., Lukowski, T
Damgaard, P. H., Ferro, L., Lukowski, T. and Moerman, R., The momentum ampli- tuhedron, InJ. High Energ. Phys.42 (2019)
2019
-
[127]
and Moerman, R., From momentum amplituhedron bound- aries toamplitude singularities and back, InJ
Ferro, L., Lukowski, T. and Moerman, R., From momentum amplituhedron bound- aries toamplitude singularities and back, InJ. High Energ. Phys.07, 7 (2020), 201
2020
-
[128]
and Lam, T
Arkani-Hamed, N., Bai, Y. and Lam, T. Positive geometries and canonical forms,J. High Energ. Phys.11 (2017), 039
2017
-
[129]
and Reshetikhin, N
Cattaneo, A.S., Mnev, P. and Reshetikhin, N. Perturbative quantum gauge theories on manifolds with boundary, InCommun. Math. Phys.357 (2018), 631-730
2018
-
[130]
and Paquette, N.M
Costello, K. and Paquette, N.M. Twisted holography,Adv. Theor. Math. Phys.27 (2023), 1-145
2023
-
[131]
Postnikov, A., Total positivity, Grassmannians, and networks, [arXiv:math/0609764 [math.CO]]
-
[132]
Twistors and amplitudes.Phil
Hodges, A. Twistors and amplitudes.Phil. Trans. R. Soc. A373 (2015), 20140248. 40
2015
-
[133]
and Goncharov, A.B
Fock, V.V. and Goncharov, A.B. Cluster ensembles, quantization and the dilogarithm. Ann. Sci. ´Ec. Norm. Sup´ er.42 (2009), 865–930
2009
-
[134]
How device-independent approaches change the meaning of physical theory.Stud
Grinbaum, A. How device-independent approaches change the meaning of physical theory.Stud. Hist. Phil. Mod. Phys.58 (2017), 22–30
2017
-
[135]
F., Marcian` o, A
Fields, C., Glazebrook, J. F., Marcian` o, A. and Zappala, E. Whether a quantum com- putation employs nonlocal resources is operationally undecidable.EPL151 (2025), 48001
2025
-
[136]
Cie´ slinski, P., de la Hamette, A.-C
Cepollaro, C., Akil, A. Cie´ slinski, P., de la Hamette, A.-C. and Brukner, ˇC. Sum of entanglement and subsystem coherence is invariant under quantum reference frame transformations.Phys. Rev. Lett.135 (2025), 010201
2025
-
[137]
Barb´ on, J. L. F., Martin-Garcia, J. and Sasieta, M. Proof of a momentum/complexity correspondence.Physical Review D102 (2020), 101901(R)
2020
-
[138]
G¨ odel and the End of Physics
Hawking, S. G¨ odel and the End of Physics. Lecture at the Dirac Centennial Cel- ebration. Centre for Mathematical Sciences, University of Cambridge, Cambridge, UK, 2002. Available online: https://www.damtp.cam.ac.uk/events/strings02/dirac/ hawking.html (accessed on 13 January 2024)
2002
-
[139]
A., Dreiner, H
Abel, S. A., Dreiner, H. K., Sengupta, R. and Ubaldi, L. Colliders are testing neither locality via Bell’s inequality nor entanglement versus non-entanglement. arXiv:2507.15949v1 [hep-ph]
-
[140]
Rinaldi, E., Han, X., Hassan, M. et al. Matrix-model simulation using quantum computing, deep learning, and lattice Monte Carlo.PRX Quantum3 (2022), 010324
2022
-
[141]
Hardy, A., Mukhopadhyay, P., Alam, M S. et al. Optimized quantum simulation algorithms for scalar quantum field theories. (2024) arXiv:2407.13819v1 [quant-ph]
2024
-
[142]
and Rothstein, I
Goldberger, W. and Rothstein, I. Z. Virtual Hawking Radiation.Phys. Rev. Lett.125 (2020), 211301
2020
-
[143]
Baez, J. C. An introduction to spin foam models of BF theory and quantum gravity. In ( Gausterer, H., Pittner, L. and Grosse, H. eds.)Geometry and Quantum Physics pp. 25–93. Lecture Notes in Physics 543. Springer, Berlin-Heidelberg, 2000
2000
-
[144]
and Livine, E
Bonzom, V., Costantino, F. and Livine, E. R. Duality between spin networks and the 2D Ising model.Commun. Math. Phys.344(2) (2016), 531–579
2016
-
[145]
and Tessler, R
Even-Zohar, C., Lakrec, T. and Tessler, R. J. The BCFW triangulation of the ampli- tuhedron. In (Davis, ed.)Proceedings of the 35th Conference on Formal Power Series and Algebraic Combinatorics,S´ eminaire Lotharingien de Combinatoire89B Article 47 (2023), arXiv:2112.02703. 41
2023
-
[146]
and Glazebrook, J
Fields, C. and Glazebrook, J. F. Representing measurement as a thermodynamic symmetry breaking.Symmetry12 (2020), 810
2020
-
[147]
F., and Marcian` o, A
Fields, C., Glazebrook, J. F., and Marcian` o, A. Reference frame induced symmetry breaking on holographic screens.Symmetry13 (2021), 408
2021
-
[148]
Fields, C., Glazebrook, J. F. and Marcian` o, A. Communication protocols and QECCs from the perspective of TQFT, Part II: QECCs as spacetimes.Fortschr. Physik72 (2024), 202400050
2024
-
[149]
Friston, K., Glazebrook, J
Fields, C., Fabrocini, F. Friston, K., Glazebrook, J. F., Hazan, H., Levin, L. and Marcian` o, A. Control flow in active inference systems. Part I: Classical and quantum formulations of active inference.IEEE Transactions on Molecular, Biological, and Multi-Scale Communications...
2023
-
[150]
and Hnybida, J
Freidel, L. and Hnybida, J. On the exact evaluation of spin networks.J. Math. Phys. 54(11) (2014), 112301
2014
-
[151]
and Pylyavskyy, P
Galashin, P. and Pylyavskyy, P. Ising model and the positive orthogonal Grassmanian. Duke Math. J.69(10) (2020), 1877–1942
2020
-
[152]
Gradute Texts in Mathematics 221, Springer Berlin-Heidelberg-New York, 2003
Gr¨ unbaum, B.Convex Polytopes2nd edn. Gradute Texts in Mathematics 221, Springer Berlin-Heidelberg-New York, 2003
2003
-
[153]
N., Williams, L
Karp, S. N., Williams, L. K. and Zhang, Y. X. Decompostiosn of amplituhedra.Ann. Inst. Henri Poincar´ e Comb. Phys Interact.7(3) (2020), 303–363
2020
-
[154]
and Puchta, J
Kisielowski, M., Lewandowski, J. and Puchta, J. Feynman diagramatic approach to spinfoams.Classical and Quantum Gravity29(1) (2011), 15009
2011
-
[155]
K., Wang, E
Li, T., Lai, W. K., Wang, E. and Xing, H. Scattering amplitude from quantum computing with reduction formula.Phys. Rev. D109 (2024), 036025
2024
-
[156]
and Susskind, L
Maldacena, J. and Susskind, L. Cool horizons for entangled black holes.Fortschr. Physik61 (2013), 781-811
2013
-
[157]
and Rovelli, C
Reisenberger, M. and Rovelli, C. Spin foams as Feynman diagrams.2001: A Rela- tivistic Spacetime Odysseypp. 431–448, World Scientific Press, 2003
2001
-
[158]
Copenhagen vs Everett, teleportation, and ER=EPR.Forschr
Susskind, L. Copenhagen vs Everett, teleportation, and ER=EPR.Forschr. Physik 64(6-7) (2016), 551–564
2016
-
[159]
M.Lectures on Polytopes
Ziegler, G. M.Lectures on Polytopes. Springer and Busimess Media, 2012. 42
2012
-
[1966]
Oliver and Boyd, Edinburgh UK, 1966
1966
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