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Nuclear spin structure in dark matter search: The finite momentum transfer limit

V. A. Bednyakov, F. Simkovic

Abstract

Spin-dependent elastic scattering of weakly interacting massive dark matter particles (WIMP) off nuclei is reviewed. All available, within different nuclear models, structure functions S(q) for finite momentum transfer (q>0) are presented. These functions describe the recoil energy dependence of the differential event rate due to the spin-dependent WIMP-nucleon interactions. This paper, together with the previous paper ``Nuclear spin structure in dark matter search: The zero momentum transfer limit'', completes our review of the nuclear spin structure calculations involved in the problem of direct dark matter search.

Nuclear spin structure in dark matter search: The finite momentum transfer limit

Abstract

Spin-dependent elastic scattering of weakly interacting massive dark matter particles (WIMP) off nuclei is reviewed. All available, within different nuclear models, structure functions S(q) for finite momentum transfer (q>0) are presented. These functions describe the recoil energy dependence of the differential event rate due to the spin-dependent WIMP-nucleon interactions. This paper, together with the previous paper ``Nuclear spin structure in dark matter search: The zero momentum transfer limit'', completes our review of the nuclear spin structure calculations involved in the problem of direct dark matter search.

Paper Structure

This paper contains 15 sections, 44 equations, 12 figures, 8 tables.

Figures (12)

  • Figure 1: Structure functions $S^{19}_{00}$ (bottom), $S^{19}_{11}$ (middle), and $S^{19}_{01}$ (top) for $^{18}$F as a function of the recoil energy $E = u b^{-2}/ M_A$ in keV calculated by (\ref{['SF-F19-pi']}). With $v_{\max} \approx 600(700)$ km/s for the $^{18}$F target one has $E_{\max} \approx 140(190)$ keV.
  • Figure 2: Spin structure functions for $^{23}$Na $S^{23}_{00}$ (middle), $S^{23}_{11}$ (bottom), and $S^{23}_{01}$ (top) versus the recoil energy. Left: $S^{23}_{ij}$ approximations from Ressell and Dean Ressell:1997kx in accordance with (\ref{['Nuclear.spin.Na-23']}). Right: $S^{23}_{ij}$ from Vergados et al. Divari:2000dc following (\ref{['SF-Na23']}). With $v_{\max} \approx 700$ km/s for $^{23}$Na target one has $E_{\max} \approx 230$ keV.
  • Figure 3: Structure functions $S^{27}_{00}$ (middle), $S^{27}_{11}$ (bottom), and $S^{27}_{01}$ (top) for $^{27}$Al as a function of the recoil energy calculated by (\ref{['Nuclear.spin.AL-27']}). For $^{27}$Al and the WIMP maximal velocity of 700 km/s the maximum momentum transfer is $q_{\max} \approx 117$ MeV and $E_{\max} \approx 270$ keV.
  • Figure 4: Spin structure functions $S^{29}_{00}$ (top) $S^{29}_{11}$ (middle), and $S^{29}_{01}$ (bottom) for $^{29}$Si as a function of the recoil energy. Left: results of Ressell et al. Ressell:1993qm. Right: these structure functions from Vergados et al. Divari:2000dc following equations (\ref{['SF-Si29-pi']}). With $v_{\max} \approx 700$ km/s, for $^{29}$Si target one has $E_{\max} \approx 290$ keV.
  • Figure 5: $^{39}$K spin structure functions $S^{39}_{00}$ (top), $S^{39}_{11}$ (middle), and $S^{39}_{01}$ (bottom) versus the recoil energy, calculated by (\ref{['SF-39K']}) from Engel, Ressell, Towner and Ormand Engel:1995gw. With $v_{\max}=700$ km/s, for $^{39}$K one has $q_{\max} = 169$ MeV, $E_{\max} = 390$ keV.
  • ...and 7 more figures