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Research PaperResearchia:202604.23034

Rank-2 Electromagnetic Backgrounds and Angular Momentum Barriers in Gravitomagnetic Spin-Quadrupole Searches

Leonardo A. Pachon

Abstract

We present a complete analysis of the angular momentum selection rules and electromagnetic backgrounds that constrain any spectroscopic search for the gravitomagnetic spin-quadrupole coupling in highly charged ions. A sequence of four barriers is identified: (i)~the Wigner-Eckart theorem mandates $j \geq 3/2$ electronic states for sensitivity to the rank-2 gravitomagnetic operator, excluding the deformation-immune $j=1/2$ states; (ii)~the nuclear electric quadrupole hyperfine interaction (HFS-E2...

Submitted: April 23, 2026Subjects: Quantum Physics; Quantum Computing

Description / Details

We present a complete analysis of the angular momentum selection rules and electromagnetic backgrounds that constrain any spectroscopic search for the gravitomagnetic spin-quadrupole coupling in highly charged ions. A sequence of four barriers is identified: (i)~the Wigner-Eckart theorem mandates jβ‰₯3/2j \geq 3/2 electronic states for sensitivity to the rank-2 gravitomagnetic operator, excluding the deformation-immune j=1/2j=1/2 states; (ii)~the nuclear electric quadrupole hyperfine interaction (HFS-E2) generates an ∼18\sim 18-orders-of-magnitude electromagnetic background in the required j=3/2j=3/2 channel; (iii)~second-order HFS mixing between fine-structure levels leaves a residual ∼10βˆ’6\sim 10^{-6} eV even after centroid extraction; (iv)~tensor nuclear polarizability (TNP), scaling with B(E2)B(E2) rather than QsQ_s, introduces an independent rank-2 background of ∼10βˆ’12\sim 10^{-12} eV. We derive the algebraic conditions under which a multi-isotope, multi-transition Generalized King Plot can separate these backgrounds from the gravitational signal, and show that the minimum experimental topology requires three transitions and Noddβ‰₯Nbkg+1N_{\text{odd}} \geq N_{\text{bkg}} + 1 odd-spin isotopes with linearly independent nuclear parameters. For the molybdenum chain, this yields a first laboratory-derivable bound βˆ£Ο‡βˆ’1βˆ£β‰²108βˆ’109|Ο‡- 1| \lesssim 10^{8} - 10^9 on the gyrogravitational ratio, limited by current precision on nuclear quadrupole moments and transition rates. We quantify the experimental milestones needed to improve this bound by each order of magnitude, providing a roadmap for future searches.


Source: arXiv:2604.20717v1 - http://arxiv.org/abs/2604.20717v1 PDF: https://arxiv.org/pdf/2604.20717v1 Original Link: http://arxiv.org/abs/2604.20717v1

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Date:
Apr 23, 2026
Topic:
Quantum Computing
Area:
Quantum Physics
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