The above equations could be numerically solved order by order at given k and G with parity Π = − (− 1)G

gsgp order equations:                            v(1)(1, 1)′ 1 +v(1)(1, 1) 1 h′ G+1 hG+1 + G + 2 r v(1)(1, 1) 1 − (ε − gσv) hG hG+1 u(1)(1, 1) 1 +σsu(1)(

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Quantum fluctuation energies over a spatially inhomogeneous field background in a chiral soliton model

nucl-th · 2025-03-06 · unverdicted · novelty 2.0

Finite quantum fluctuation energies over chiral soliton backgrounds are numerically evaluated at different parities and grand spins via phase shift analysis and Born-subtraction renormalization.

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Quantum fluctuation energies over a spatially inhomogeneous field background in a chiral soliton model nucl-th · 2025-03-06 · unverdicted · none · ref 9
Finite quantum fluctuation energies over chiral soliton backgrounds are numerically evaluated at different parities and grand spins via phase shift analysis and Born-subtraction renormalization.

The above equations could be numerically solved order by order at given k and G with parity Π = − (− 1)G

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