// // ******************************************************************** // * License and Disclaimer * // * * // * The Geant4 software is copyright of the Copyright Holders of * // * the Geant4 Collaboration. It is provided under the terms and * // * conditions of the Geant4 Software License, included in the file * // * LICENSE and available at http://cern.ch/geant4/license . These * // * include a list of copyright holders. * // * * // * Neither the authors of this software system, nor their employing * // * institutes,nor the agencies providing financial support for this * // * work make any representation or warranty, express or implied, * // * regarding this software system or assume any liability for its * // * use. Please see the license in the file LICENSE and URL above * // * for the full disclaimer and the limitation of liability. * // * * // * This code implementation is the result of the scientific and * // * technical work of the GEANT4 collaboration. * // * By using, copying, modifying or distributing the software (or * // * any work based on the software) you agree to acknowledge its * // * use in resulting scientific publications, and indicate your * // * acceptance of all terms of the Geant4 Software license. * // ******************************************************************** // // // $Id: G4CookPairingCorrections.cc,v 1.7 2010/11/15 16:09:46 vnivanch Exp $ // GEANT4 tag $Name: geant4-09-04-ref-00 $ // // Hadronic Process: Nuclear De-excitations // by V. Lara #include "G4CookPairingCorrections.hh" // Data comes from: // J.L. Cook, H. Ferguson and A.R.de L. Musgrove, Aust. J. Phys., 20, 477(1967) // P(Z) 68 values from Z = 28 to Z = 95 const G4double G4CookPairingCorrections::PairingZTable [G4CookPairingCorrections::ZTableSize] = { 1.28, 0.26, 0.88, 0.19, 1.35, -0.05, 1.52, -0.09, 1.17, 0.04, 1.24, 0.29, 1.09, 0.26, 1.17, 0.23, 1.15, -0.08, 1.35, 0.34, 1.05, 0.28, 1.27, 0.00, 1.05, 0.00, 1.00, 0.09, 1.20, 0.20, 1.40, 0.93, 1.00, -0.20, 1.19, 0.09, 0.97, 0.00, 0.92, 0.11, 0.68, 0.05, 0.68, -0.22, 0.79, 0.09, 0.69, 0.01, 0.72, 0.00, 0.40, 0.16, 0.73, 0.00, 0.46, 0.17, 0.89, 0.00, 0.79, 0.00, 0.89, 0.00, 0.81, -0.06, 0.69, -0.20, 0.71, -0.12 }; // P(N) 118 values from N = 33 to N = 150 const G4double G4CookPairingCorrections::PairingNTable [G4CookPairingCorrections::NTableSize] = { 0.08, 1.41, -0.08, 1.50, -0.05, 2.24, -0.47, 1.43, -0.15, 1.44, 0.06, 1.56, 0.25, 1.57, -0.16, 1.46, 0.00, 0.93, 0.01, 0.62, -0.50, 1.42, 0.13, 1.52, -0.65, 0.80, -0.08, 1.29, -0.47, 1.25, -0.44, 0.97, 0.08, 1.65, -0.11, 1.26, -0.46, 1.06, 0.22, 1.55, -0.07, 1.37, 0.10, 1.20, -0.27, 0.92, -0.35, 1.19, 0.00, 1.05, -0.25, 1.61, -0.21, 0.90, -0.21, 0.74, -0.38, 0.72, -0.34, 0.92, -0.26, 0.94, 0.01, 0.65, -0.36, 0.83, 0.11, 0.67, 0.05, 1.00, 0.51, 1.04, 0.33, 0.68, -0.27, 0.81, 0.09, 0.75, 0.17, 0.86, 0.14, 1.10, -0.22, 0.84, -0.47, 0.48, 0.02, 0.88, 0.24, 0.52, 0.27, 0.41, -0.05, 0.38, 0.15, 0.67, 0.00, 0.61, 0.00, 0.78, 0.00, 0.67, 0.00, 0.67, 0.00, 0.79, 0.00, 0.60, 0.04, 0.64, -0.06, 0.45, 0.05, 0.26, -0.22, 0.39, 0.00, 0.39 }; G4CookPairingCorrections* G4CookPairingCorrections::theInstance = 0; G4CookPairingCorrections::G4CookPairingCorrections() {;} G4CookPairingCorrections::~G4CookPairingCorrections() {;} G4CookPairingCorrections* G4CookPairingCorrections::GetInstance() { if (!theInstance) { static G4CookPairingCorrections theCorrections; theInstance = &theCorrections; } return theInstance; }