4.7 Article

Semiempirical formula for electroweak response functions in the two-nucleon emission channel in neutrino-nucleus scattering

期刊

PHYSICAL REVIEW D
卷 104, 期 11, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.104.113006

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资金

  1. Spanish Agencia Estatal de investigacion [FIS2017-85053-C2-1-P, PID2020- 114767 GB-I00]
  2. Junta de Andalucia [FQM-225]
  3. European Regional Development Funds [A-FQM-390-UGR20]
  4. Agencia Estatal de Investigacion
  5. European Social Fund

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The study proposed a semiempirical formula for the inclusive electroweak response functions in the two-nucleon emission channel, which is determined by expanding the meson-exchange currents and hadronic tensor into separate contributions. This formula effectively describes the energy transfer dependence and can be applied to neutrinos, antineutrinos, and electrons for cross-section calculations.
A semiempirical formula for the inclusive electroweak response functions in the two-nucleon emission channel is proposed. The method consists in expanding each one of the vector-vector, axial-axial, and vector-axial responses as sums of six subresponses. These correspond to separating the meson-exchange currents as the sum of three currents of similar structure and expanding the hadronic tensor as the sum of the separate contributions from each current plus the interferences between them. For each subresponse, we factorize the coupling constants, the electroweak form factors, the phase space, and the delta propagator, for the delta-forward current. The remaining spin-isospin contributions are encoded in coefficients for each value of the momentum transfer, q. The coefficients are fitted to the exact results in the relativistic mean field model of nuclear matter, for each value of q. The dependence on the energy transfer omega is well described by the semiempirical formula. The q-dependency of the coefficients of the subresponses can be parametrized or can be interpolated from the provided tables. The description of the five theoretical responses is quite good. The parameters of the formula, the Fermi momentum, number of particles, relativistic effective mass, vector energy, the electroweak form factors, and the coupling constants, can be modified easily. This semiempirical formula can be applied to the cross section of neutrinos, antineutrinos, and electrons.

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