Herwig 7.3.0
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The bornVVKinematics class is used to store information on the the kinematics of the real emission processes needed for the evaluation of matrix elements in the real part of the NLO process. More...
#include <VVKinematics.h>
Leading order momentum fractions and associated etabar's: | |
Invariants required for the evaluation of 2-> 2 next-to-leading order quantities (Frixione et al. NPB.383 WZ production at colliders). | |
double | x1b_ |
Leading order momentum fraction for first particle. | |
double | eta1b_ |
Leading order etabar for first particle. | |
double | x2b_ |
Leading order momentum fraction for second particle. | |
double | eta2b_ |
Leading order etabar for second particle. | |
double | x1b () const |
Leading order momentum fraction for first particle. | |
double | eta1b () const |
Leading order etabar for first particle. | |
double | x2b () const |
Leading order momentum fraction for second particle. | |
double | eta2b () const |
Leading order etabar for second particle. | |
The Born momenta according to the notation of the FMNR papers, | |
in the diboson centre of mass frame: | |
Lorentz5Momentum | p1b_ |
Momentum \(p_1\). | |
Lorentz5Momentum | p2b_ |
Momentum \(p_2\). | |
Lorentz5Momentum | k1b_ |
Momentum \(k_1\). | |
Lorentz5Momentum | k2b_ |
Momentum \(k_2\). | |
Lorentz5Momentum | p1b () const |
Momentum \(p_1\). | |
Lorentz5Momentum | p2b () const |
Momentum \(p_2\). | |
Lorentz5Momentum | k1b () const |
Momentum \(k_1\). | |
Lorentz5Momentum | k2b () const |
Momentum \(k_2\). | |
The diboson invariant mass / shat, that and uhat: | |
Energy2 | sb_ |
\(\hat s\) | |
Energy2 | tb_ |
\(\hat t\) | |
Energy2 | ub_ |
\(\hat u\) | |
double | Yb_ |
The diboson rapidity: Note Yb_ = + lastY() if flipped = false but Yb_ = - lastY() if flipped = true. | |
Energy2 | sb () const |
\(\hat s\) | |
Energy2 | tb () const |
\(\hat t\) | |
Energy2 | ub () const |
\(\hat u\) | |
double | Yb () const |
The diboson rapidity: Note Yb_ = + lastY() if flipped = false but Yb_ = - lastY() if flipped = true. | |
Masses of the final state bosons: | |
Energy2 | k12b_ |
Mass squared og the first boson. | |
Energy2 | k22b_ |
Mass squared og the second boson. | |
double | theta1b_ |
Polar angle of the dibosons in their rest frame: | |
Energy2 | k12b () const |
Mass squared og the first boson. | |
Energy2 | k22b () const |
Mass squared og the second boson. | |
double | theta1b () const |
Polar and azimuthal angles of the dibosons in their rest frame: | |
void | sanityCheck () const |
A check to make sure that the momenta calculated from the energies and angles are equal to those of meMomenta(). | |
The bornVVKinematics class is used to store information on the the kinematics of the real emission processes needed for the evaluation of matrix elements in the real part of the NLO process.
Definition at line 18 of file VVKinematics.h.
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Leading order etabar for first particle.
Definition at line 54 of file VVKinematics.h.
References eta1b_.
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Leading order etabar for second particle.
Definition at line 64 of file VVKinematics.h.
References eta2b_.
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Polar and azimuthal angles of the dibosons in their rest frame:
Definition at line 139 of file VVKinematics.h.
References theta1b_.
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Leading order momentum fraction for first particle.
Definition at line 49 of file VVKinematics.h.
References x1b_.
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Leading order momentum fraction for second particle.
Definition at line 59 of file VVKinematics.h.
References x2b_.
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The diboson rapidity: Note Yb_ = + lastY() if flipped = false but Yb_ = - lastY() if flipped = true.
Yb_ is always defined with the quark travelling in the +z direction!
Definition at line 119 of file VVKinematics.h.
References Yb_.
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Leading order etabar for first particle.
Definition at line 166 of file VVKinematics.h.
Referenced by eta1b().
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Leading order etabar for second particle.
Definition at line 176 of file VVKinematics.h.
Referenced by eta2b().
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Mass squared og the first boson.
Definition at line 240 of file VVKinematics.h.
Referenced by k12b().
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Mass squared og the second boson.
Definition at line 245 of file VVKinematics.h.
Referenced by k22b().
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Polar angle of the dibosons in their rest frame:
Definition at line 251 of file VVKinematics.h.
Referenced by theta1b().
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Leading order momentum fraction for first particle.
Definition at line 161 of file VVKinematics.h.
Referenced by x1b().
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Leading order momentum fraction for second particle.
Definition at line 171 of file VVKinematics.h.
Referenced by x2b().
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The diboson rapidity: Note Yb_ = + lastY() if flipped = false but Yb_ = - lastY() if flipped = true.
Yb_ is always defined with the quark travelling in the +z direction!
Definition at line 231 of file VVKinematics.h.
Referenced by Yb().