Abstract:Compact algebraic equations are derived, which connect the binding energy and the asymptotic normalization constant (ANC) of a subthreshold bound state with the effective-range expansion of the corresponding partial wave. These relations are established for positively-charged and neutral particles, using the analytic continuation of the scattering (S) matrix in the complex wave-number plane. Their accuracy is checked on simple local potential models for the 16 O+n, 16 O+p and 12 C+α nuclear systems, with exoti… Show more
“…When effective ranges are calculated as well, one can extract near-threshold bound-state properties such as asymptotic normalization constants from scattering parameters with relations as given, e.g., in Refs. [9,10]. These constants can be used to determine the overall normalization of the S-factor for astrophysical nuclear reaction rates [11].…”
We present a fully perturbative calculation of the quartet-channel proton-deuteron scattering length up to next-to-next-to-leading order in pionless effective field theory. We use a framework that consistently extracts the Coulomb-modified effective range function for a screened Coulomb potential in momentum space and allows for a clear linear extrapolation back to the physical limit without screening. Our result of 4 a p-d = (10.9 ± 0.4) fm agrees with older experimental determinations of this quantity but deviates from potential-model calculations and a more recent result from Black et al., which find larger values around 14 fm. As a possible resolution to this discrepancy, we discuss the scheme dependence of Coulomb subtractions in a three-body system.
“…When effective ranges are calculated as well, one can extract near-threshold bound-state properties such as asymptotic normalization constants from scattering parameters with relations as given, e.g., in Refs. [9,10]. These constants can be used to determine the overall normalization of the S-factor for astrophysical nuclear reaction rates [11].…”
We present a fully perturbative calculation of the quartet-channel proton-deuteron scattering length up to next-to-next-to-leading order in pionless effective field theory. We use a framework that consistently extracts the Coulomb-modified effective range function for a screened Coulomb potential in momentum space and allows for a clear linear extrapolation back to the physical limit without screening. Our result of 4 a p-d = (10.9 ± 0.4) fm agrees with older experimental determinations of this quantity but deviates from potential-model calculations and a more recent result from Black et al., which find larger values around 14 fm. As a possible resolution to this discrepancy, we discuss the scheme dependence of Coulomb subtractions in a three-body system.
“…In this procedure the elastic scattering phase shift is analytically approximated in the physical region with the subsequent analytical continuation to the bound state pole. This analytical approximation in the physical region can be done using different approaches: Pade approximation [2], effective range expansion [3][4][5]. There is also a possibility to solve N/D equations, which take into account the right unitary cut and the left dynamical singularities.…”
“…This method was used in [8] to obtain the S wave VCs and ANCs for the process 6 Li → α + d, by Yu.V. Orlov et al [9] for the systems 3 H, 2,3,5 He, 5 Li, 8 Be, and by J.-M. Sparenberg et al [10] for the systems 16 O + n, 16 O + p, and 12 C + α.…”
Abstract. The problem of obtaining characteristics of bound nuclear states from continuum states data is discussed. It is shown that the ambiguities due to the existence of phase-equivalent potentials can be resolved by using the analytic properties of scattering amplitudes. The methods of determination of asymptotic normalization coefficients and vertex constants are considered. The asymptotic normalization coefficients for 6 Li in the α+d channel are found by analytic continuation of the two-channel effective range expansion. The account of inelastic channels within the effective range approach is discussed.
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