LEP2ThObservable.h

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/* 
 * Copyright (C) 2012 HEPfit Collaboration
 *
 *
 * For the licensing terms see doc/COPYING.
 */
 
#ifndef LEP2THOBSERVABLE_H
#define LEP2THOBSERVABLE_H
 
#include <stdexcept>
#include <cstring>
#include <ThObservable.h>
//#include <NPSTUVWXY.h>
#include <StandardModel.h>
#include "LEP2test.h"
#include "std_make_vector.h"
 
// TEST: use the Zfitter outputs defined in LEP2test class for SM predictions
//#define LEP2TEST
 
class LEP2ThObservable : public ThObservable  {
public:
 
    // Radiative Corrections for the LEP2 observables
//    enum LEP2RCs {Weak=0, WeakBox, ISR, QEDFSR, QCDFSR, NUMofLEP2RCs};
        
    LEP2ThObservable(const StandardModel& SM_i, const double sqrt_s_i) 
            : ThObservable(SM_i),sqrt_s(sqrt_s_i), s(sqrt_s_i*sqrt_s_i)
    {
        // SM intrinsic (relative) error. Assumed the same for all energies
        // Different for cross sections and asymmetries.
        // Same for muon and tau final states. Not implemented for electrons
        // For hadronic final states, only implemented for total cross section
        setParametersForObservable(make_vector<std::string>() << "errSMint_xseellLEP2"<< "errSMint_AFBeellLEP2"
                << "errSMint_xseejjLEP2");   
    }
 
    const LEP2test myTEST;
    const double sqrt_s, s;
    
    
private:   
      
};
 
 
class LEP2ThDiffObservable : public ThObservable  {
public:
        
    LEP2ThDiffObservable(const StandardModel& SM_i, const double sqrt_s_i, const double cos_i) 
            : ThObservable(SM_i),sqrt_s(sqrt_s_i), s(sqrt_s_i*sqrt_s_i), cos(cos_i)
    {
        // SM intrinsic (relative) error. Assumed the same for all energies/angles
        // Same for muon and tau final states but different than for electrons
        setParametersForObservable(make_vector<std::string>() << "errSMint_deeeedcosLEP2"<< "errSMint_deelldcosLEP2");                
    }
 
    const LEP2test myTEST;
    const double sqrt_s, s, cos;
    
    
private:   
      
};
 
 
class LEP2ThDiffObservableBin : public ThObservable  {
public:
        
    LEP2ThDiffObservableBin(const StandardModel& SM_i, const double sqrt_s_i, const double cos_i, const double cosmin_i, const double cosmax_i) 
            : ThObservable(SM_i),sqrt_s(sqrt_s_i), s(sqrt_s_i*sqrt_s_i), cos(cos_i), cosmin(cosmin_i), cosmax(cosmax_i)
    {
        // SM intrinsic (relative) error. Assumed the same for all energies/angles
        // Same for muon and tau final states but different than for electrons
        setParametersForObservable(make_vector<std::string>() << "errSMint_deeeedcosLEP2"<< "errSMint_deelldcosLEP2");                
    }
 
    const LEP2test myTEST;
    const double sqrt_s, s, cos, cosmin, cosmax;
    
    
private:   
      
};
 
 
class eeffThObservable : public ThObservable  {
public:
        
    eeffThObservable(const StandardModel& SM_i, const double pol_e_i, const double pol_p_i, const double sqrt_s_i) 
            : ThObservable(SM_i), pol_e(pol_e_i), pol_p(pol_p_i), sqrt_s(sqrt_s_i), s(sqrt_s_i*sqrt_s_i)
    {                
        // SM intrinsic (relative) error. Assumed the same for all energies
        // Different for cross sections, asymmetries and ratios with the hadronic cross section.
        // Same for muon and tau final states but different than for electrons.
        // Separate uncertainties for b-hadrons and light jets
        setParametersForObservable(make_vector<std::string>() << "errSMint_xseeee"<< "errSMint_AFBeeee"<< "errSMint_Reeee" << "errSMint_xseell"<< "errSMint_AFBeell"<< "errSMint_Reell"
                << "errSMint_xseebb"<< "errSMint_AFBeebb"<< "errSMint_Reebb" << "errSMint_xseejj"<< "errSMint_AFBeejj"<< "errSMint_Reejj");                  
    }
 
    const double pol_e, pol_p, sqrt_s, s;
     
private:   
      
};
 
 
#endif  /* LEP2THOBSERVABLE_H */