{"paper":{"title":"Photon Quantization and Propagator in Rotating Coordinates","arxiv_id":"2610.02656","primary_cat":"hep-ph","submitted_at":"2026-10-02T01:24:29+00:00","version_compiled":"v1"},"notice":"Every quoted sentence is the authors' text from the arXiv listing abstract. Labels and probabilities are the outputs of classifier-1.13.0 on the question bank abstract-p1-20260923, exactly as returned. No sentence in this record was written by a language model.","schema":"pith.compiled-record/v0","status":"compiled","abstract":{"source":"arXiv listing abstract v1","sentences":[{"i":0,"p":1.0,"id":"s0","own":true,"role":"contribution","text":"We construct the quantized electromagnetic field and the corresponding photon propagators in a rigidly rotating cylindrical reference frame.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.96,"main_claim_p":0.19,"quantitative":false,"quantitative_p":0.04,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":1.0,"interpretation":0.0}},{"i":1,"p":0.99,"id":"s1","own":true,"role":"method","text":"Starting from covariant Maxwell theory, we formulate the gauge-fixed field equations and solve them in cylindrical coordinates.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.93,"main_claim_p":0.03,"quantitative":false,"quantitative_p":0.04,"role_probabilities":{"gap":0.0,"method":0.99,"result":0.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.01,"interpretation":0.0}},{"i":2,"p":0.66,"id":"s2","own":false,"role":"background","text":"The vector nature of the electromagnetic field requires distinguishing orbital and intrinsic angular momentum, with the total angular momentum as the natural quantum number.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.34,"main_claim_p":0.06,"quantitative":false,"quantitative_p":0.15,"role_probabilities":{"gap":0.0,"method":0.18,"result":0.01,"background":0.66,"limitation":0.0,"future_work":0.0,"contribution":0.05,"interpretation":0.1}},{"i":3,"p":0.69,"id":"s3","own":true,"role":"method","text":"We construct the two independent physical photon modes in terms of Bessel functions by solving the coupled differential equations, and provide an alternative construction based on a covariant basis of vector eigenfunctions generated by a covariantly constant tetrad.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.95,"main_claim_p":0.12,"quantitative":true,"quantitative_p":0.72,"role_probabilities":{"gap":0.0,"method":0.69,"result":0.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.31,"interpretation":0.0}},{"i":4,"p":0.86,"id":"s4","own":true,"role":"method","text":"After normalizing the modes with the Maxwell inner product, we quantize the electromagnetic field and define the corresponding photon states and greater and lesser two-point functions.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.95,"main_claim_p":0.08,"quantitative":false,"quantitative_p":0.16,"role_probabilities":{"gap":0.0,"method":0.86,"result":0.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.14,"interpretation":0.0}},{"i":5,"p":0.83,"id":"s5","own":true,"role":"result","text":"The physical time-ordered propagator is obtained directly from the quantized modes, with its transverse dependence encoded in polarization kernels that retain the cylindrical spatial structure and its spectral poles exhibiting the rotational energy shift.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.94,"main_claim_p":0.25,"quantitative":false,"quantitative_p":0.06,"role_probabilities":{"gap":0.0,"method":0.02,"result":0.83,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.14,"interpretation":0.01}},{"i":6,"p":0.75,"id":"s6","own":true,"role":"method","text":"The full gauge-fixed photon propagator is constructed in two complementary ways: from the scalar Green function combined with the tensor transformation of the inertial Feynman-gauge propagator, and from the covariant vector eigensystem through its spectral decomposition and the Fock--Schwinger proper-time representation.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.94,"main_claim_p":0.17,"quantitative":false,"quantitative_p":0.4,"role_probabilities":{"gap":0.0,"method":0.75,"result":0.01,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.24,"interpretation":0.0}},{"i":7,"p":0.7,"id":"s7","own":true,"role":"result","text":"We verify that both constructions satisfy the Green-function equation for the complete gauge-fixed Maxwell operator, providing the propagator required for covariant perturbative calculations with internal photon lines.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.94,"main_claim_p":0.36,"quantitative":false,"quantitative_p":0.12,"role_probabilities":{"gap":0.0,"method":0.04,"result":0.7,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.19,"interpretation":0.07}}]},"compiled":{"main_claim":{"p":0.8,"text":"We verify that both constructions satisfy the Green-function equation for the complete gauge-fixed Maxwell operator, 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