| [4] | 1 | // -*- C++ -*-
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| 2 | // ---------------------------------------------------------------------------
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| 3 | //
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| 4 | // This file is a part of the CLHEP - a Class Library for High Energy Physics.
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| 5 | //
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| 6 | // This is part of the implementation of the HepLorentzVector class:
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| 7 | // Those methods which originated from ZOOM and which deal with relativistic
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| 8 | // kinematic properties.
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| 9 | //
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| 10 |
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| 11 | #ifdef GNUPRAGMA
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| 12 | #pragma implementation
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| 13 | #endif
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| 14 |
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| 15 | #include "CLHEP/Vector/defs.h"
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| 16 | #include "CLHEP/Vector/LorentzVector.h"
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| 17 | #include "CLHEP/Vector/ZMxpv.h"
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| 18 |
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| 19 | #include <cmath>
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| 20 |
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| 21 | namespace CLHEP {
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| 22 |
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| 23 | //-******************
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| 24 | // Metric flexibility
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| 25 | //-******************
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| 26 |
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| 27 | ZMpvMetric_t HepLorentzVector::setMetric( ZMpvMetric_t m ) {
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| 28 | ZMpvMetric_t oldMetric = (metric > 0) ? TimePositive : TimeNegative;
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| 29 | if ( m == TimeNegative ) {
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| 30 | metric = -1.0;
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| 31 | } else {
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| 32 | metric = 1.0;
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| 33 | }
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| 34 | return oldMetric;
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| 35 | }
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| 36 |
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| 37 | ZMpvMetric_t HepLorentzVector::getMetric() {
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| 38 | return ( (metric > 0) ? TimePositive : TimeNegative );
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| 39 | }
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| 40 |
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| 41 | //-********
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| 42 | // plus
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| 43 | // minus
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| 44 | //-********
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| 45 |
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| 46 | double HepLorentzVector::plus (const Hep3Vector & ref) const {
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| 47 | double r = ref.mag();
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| 48 | if (r == 0) {
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| 49 | ZMthrowA (ZMxpvZeroVector(
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| 50 | "A zero vector used as reference to LorentzVector plus-part"));
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| 51 | return ee;
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| 52 | }
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| 53 | return ee + pp.dot(ref)/r;
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| 54 | } /* plus */
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| 55 |
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| 56 | double HepLorentzVector::minus (const Hep3Vector & ref) const {
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| 57 | double r = ref.mag();
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| 58 | if (r == 0) {
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| 59 | ZMthrowA (ZMxpvZeroVector(
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| 60 | "A zero vector used as reference to LorentzVector minus-part"));
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| 61 | return ee;
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| 62 | }
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| 63 | return ee - pp.dot(ref)/r;
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| 64 | } /* plus */
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| 65 |
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| 66 | HepLorentzVector HepLorentzVector::rest4Vector() const {
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| 67 | return HepLorentzVector (0, 0, 0, (t() < 0.0 ? -m() : m()));
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| 68 | }
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| 69 |
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| 70 | //-********
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| 71 | // beta
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| 72 | // gamma
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| 73 | //-********
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| 74 |
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| 75 | double HepLorentzVector::beta() const {
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| 76 | if (ee == 0) {
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| 77 | if (pp.mag2() == 0) {
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| 78 | return 0;
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| 79 | } else {
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| 80 | ZMthrowA (ZMxpvInfiniteVector(
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| 81 | "beta computed for HepLorentzVector with t=0 -- infinite result"));
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| 82 | return 1./ee;
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| 83 | }
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| 84 | }
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| 85 | if (restMass2() <= 0) {
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| 86 | ZMthrowC (ZMxpvTachyonic(
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| 87 | "beta computed for a non-timelike HepLorentzVector"));
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| 88 | // result will make analytic sense but is physically meaningless
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| 89 | }
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| 90 | return sqrt (pp.mag2() / (ee*ee)) ;
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| 91 | } /* beta */
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| 92 |
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| 93 | double HepLorentzVector::gamma() const {
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| 94 | double v2 = pp.mag2();
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| 95 | double t2 = ee*ee;
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| 96 | if (ee == 0) {
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| 97 | if (pp.mag2() == 0) {
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| 98 | return 1;
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| 99 | } else {
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| 100 | ZMthrowC (ZMxpvInfiniteVector(
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| 101 | "gamma computed for HepLorentzVector with t=0 -- zero result"));
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| 102 | return 0;
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| 103 | }
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| 104 | }
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| 105 | if (t2 < v2) {
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| 106 | ZMthrowA (ZMxpvSpacelike(
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| 107 | "gamma computed for a spacelike HepLorentzVector -- imaginary result"));
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| 108 | // analytic result would be imaginary.
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| 109 | return 0;
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| 110 | } else if ( t2 == v2 ) {
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| 111 | ZMthrowA (ZMxpvInfinity(
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| 112 | "gamma computed for a lightlike HepLorentzVector -- infinite result"));
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| 113 | }
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| 114 | return 1./sqrt(1. - v2/t2 );
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| 115 | } /* gamma */
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| 116 |
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| 117 |
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| 118 | //-***************
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| 119 | // rapidity
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| 120 | // pseudorapidity
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| 121 | // eta
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| 122 | //-***************
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| 123 |
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| 124 | double HepLorentzVector::rapidity() const {
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| 125 | register double z = pp.getZ();
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| 126 | if (fabs(ee) == fabs(z)) {
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| 127 | ZMthrowA (ZMxpvInfinity(
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| 128 | "rapidity for 4-vector with |E| = |Pz| -- infinite result"));
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| 129 | }
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| 130 | if (fabs(ee) < fabs(z)) {
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| 131 | ZMthrowA (ZMxpvSpacelike(
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| 132 | "rapidity for spacelike 4-vector with |E| < |Pz| -- undefined"));
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| 133 | return 0;
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| 134 | }
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| 135 | double q = (ee + z) / (ee - z);
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| 136 | //-| This cannot be negative now, since both numerator
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| 137 | //-| and denominator have the same sign as ee.
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| 138 | return .5 * log(q);
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| 139 | } /* rapidity */
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| 140 |
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| 141 | double HepLorentzVector::rapidity(const Hep3Vector & ref) const {
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| 142 | register double r = ref.mag2();
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| 143 | if (r == 0) {
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| 144 | ZMthrowA (ZMxpvZeroVector(
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| 145 | "A zero vector used as reference to LorentzVector rapidity"));
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| 146 | return 0;
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| 147 | }
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| 148 | register double vdotu = pp.dot(ref)/sqrt(r);
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| 149 | if (fabs(ee) == fabs(vdotu)) {
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| 150 | ZMthrowA (ZMxpvInfinity(
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| 151 | "rapidity for 4-vector with |E| = |Pu| -- infinite result"));
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| 152 | }
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| 153 | if (fabs(ee) < fabs(vdotu)) {
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| 154 | ZMthrowA (ZMxpvSpacelike(
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| 155 | "rapidity for spacelike 4-vector with |E| < |P*ref| -- undefined "));
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| 156 | return 0;
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| 157 | }
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| 158 | double q = (ee + vdotu) / (ee - vdotu);
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| 159 | return .5 * log(q);
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| 160 | } /* rapidity(ref) */
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| 161 |
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| 162 | double HepLorentzVector::coLinearRapidity() const {
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| 163 | register double v = pp.mag();
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| 164 | if (fabs(ee) == fabs(v)) {
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| 165 | ZMthrowA (ZMxpvInfinity(
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| 166 | "co-Linear rapidity for 4-vector with |E| = |P| -- infinite result"));
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| 167 | }
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| 168 | if (fabs(ee) < fabs(v)) {
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| 169 | ZMthrowA (ZMxpvSpacelike(
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| 170 | "co-linear rapidity for spacelike 4-vector -- undefined"));
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| 171 | return 0;
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| 172 | }
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| 173 | double q = (ee + v) / (ee - v);
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| 174 | return .5 * log(q);
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| 175 | } /* rapidity */
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| 176 |
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| 177 | //-*************
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| 178 | // invariantMass
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| 179 | //-*************
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| 180 |
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| 181 | double HepLorentzVector::invariantMass(const HepLorentzVector & w) const {
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| 182 | double m2 = invariantMass2(w);
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| 183 | if (m2 < 0) {
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| 184 | // We should find out why:
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| 185 | if ( ee * w.ee < 0 ) {
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| 186 | ZMthrowA (ZMxpvNegativeMass(
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| 187 | "invariant mass meaningless: \n"
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| 188 | "a negative-mass input led to spacelike 4-vector sum" ));
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| 189 | return 0;
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| 190 | } else if ( (isSpacelike() && !isLightlike()) ||
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| 191 | (w.isSpacelike() && !w.isLightlike()) ) {
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| 192 | ZMthrowA (ZMxpvSpacelike(
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| 193 | "invariant mass meaningless because of spacelike input"));
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| 194 | return 0;
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| 195 | } else {
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| 196 | // Invariant mass squared for a pair of timelike or lightlike vectors
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| 197 | // mathematically cannot be negative. If the vectors are within the
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| 198 | // tolerance of being lightlike or timelike, we can assume that prior
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| 199 | // or current roundoffs have caused the negative result, and return 0
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| 200 | // without comment.
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| 201 | return 0;
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| 202 | }
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| 203 | }
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| 204 | return (ee+w.ee >=0 ) ? sqrt(m2) : - sqrt(m2);
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| 205 | } /* invariantMass */
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| 206 |
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| 207 | //-***************
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| 208 | // findBoostToCM
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| 209 | //-***************
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| 210 |
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| 211 | Hep3Vector HepLorentzVector::findBoostToCM() const {
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| 212 | return -boostVector();
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| 213 | } /* boostToCM() */
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| 214 |
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| 215 | Hep3Vector HepLorentzVector::findBoostToCM (const HepLorentzVector & w) const {
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| 216 | double t = ee + w.ee;
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| 217 | Hep3Vector v = pp + w.pp;
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| 218 | if (t == 0) {
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| 219 | if (v.mag2() == 0) {
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| 220 | return Hep3Vector(0,0,0);
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| 221 | } else {
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| 222 | ZMthrowA (ZMxpvInfiniteVector(
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| 223 | "boostToCM computed for two 4-vectors with combined t=0 -- "
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| 224 | "infinite result"));
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| 225 | return Hep3Vector(v*(1./t)); // Yup, 1/0 -- that is how we return infinity
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| 226 | }
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| 227 | }
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| 228 | if (t*t - v.mag2() <= 0) {
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| 229 | ZMthrowC (ZMxpvTachyonic(
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| 230 | "boostToCM computed for pair of HepLorentzVectors with non-timelike sum"));
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| 231 | // result will make analytic sense but is physically meaningless
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| 232 | }
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| 233 | return Hep3Vector(v * (-1./t));
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| 234 | } /* boostToCM(w) */
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| 235 |
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| 236 | } // namespace CLHEP
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| 237 |
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