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ATLAS Offline Software
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#include <vector>
#include <cmath>
#include <algorithm>
#include <array>
#include <cstdlib>
Go to the source code of this file.
Classes | |
class | DecodedPID |
Implementation of classification functions according to PDG2022. More... | |
Namespaces | |
SUSY | |
Functions | |
template<class T > | |
bool | isQuark (const T &p) |
PDG rule 2: Quarks and leptons are numbered consecutively starting from 1 and 11 respectively; to dothis they are first ordered by family and within families by weak isospin. More... | |
template<> | |
bool | isQuark (const int &p) |
template<> | |
bool | isQuark (const DecodedPID &p) |
template<class T > | |
bool | isStrange (const T &p) |
template<> | |
bool | isStrange (const int &p) |
template<class T > | |
bool | isCharm (const T &p) |
template<> | |
bool | isCharm (const int &p) |
template<class T > | |
bool | isBottom (const T &p) |
template<> | |
bool | isBottom (const int &p) |
template<class T > | |
bool | isTop (const T &p) |
template<> | |
bool | isTop (const int &p) |
template<class T > | |
bool | isLepton (const T &p) |
APID: the fourth generation leptons are leptons. More... | |
template<> | |
bool | isLepton (const int &p) |
template<> | |
bool | isLepton (const DecodedPID &p) |
template<class T > | |
bool | isSMLepton (const T &p) |
template<> | |
bool | isSMLepton (const int &p) |
template<> | |
bool | isSMLepton (const DecodedPID &p) |
template<class T > | |
bool | isChLepton (const T &p) |
APID: the fourth generation leptons are leptons. More... | |
template<> | |
bool | isChLepton (const int &p) |
template<class T > | |
bool | isElectron (const T &p) |
template<> | |
bool | isElectron (const int &p) |
template<class T > | |
bool | isMuon (const T &p) |
template<> | |
bool | isMuon (const int &p) |
template<class T > | |
bool | isTau (const T &p) |
template<> | |
bool | isTau (const int &p) |
template<class T > | |
bool | isNeutrino (const T &p) |
APID: the fourth generation neutrinos are neutrinos. More... | |
template<> | |
bool | isNeutrino (const int &p) |
template<class T > | |
bool | isSMNeutrino (const T &p) |
template<> | |
bool | isSMNeutrino (const int &p) |
template<class T > | |
bool | isGluon (const T &p) |
template<> | |
bool | isGluon (const int &p) |
template<class T > | |
bool | isPhoton (const T &p) |
template<> | |
bool | isPhoton (const int &p) |
template<class T > | |
bool | isZ (const T &p) |
template<> | |
bool | isZ (const int &p) |
template<class T > | |
bool | isW (const T &p) |
template<> | |
bool | isW (const int &p) |
template<class T > | |
bool | isDM (const T &p) |
PDG rule 11j: The nature of Dark Matter (DM) is not known, and therefore a definitive classificationis too early. More... | |
template<> | |
bool | isDM (const int &p) |
template<class T > | |
bool | isTrajectory (const T &p) |
PDG rule 8: The pomeron and odderon trajectories and a generic reggeon trajectory of states in QCD areassigned codes 990, 9990, and 110 respectively. More... | |
template<> | |
bool | isTrajectory (const int &p) |
template<class T > | |
bool | isHiggs (const T &p) |
APID: HIGGS boson is only one particle. More... | |
template<> | |
bool | isHiggs (const int &p) |
template<class T > | |
bool | isResonance (const T &p) |
template<class T > | |
bool | isGraviton (const T &p) |
template<> | |
bool | isGraviton (const int &p) |
template<class T > | |
bool | isLeptoQuark (const T &p) |
template<> | |
bool | isLeptoQuark (const int &p) |
template<class T > | |
bool | isSUSY (const T &p) |
template<class T > | |
bool | isTechnicolor (const T &p) |
template<class T > | |
bool | isExcited (const T &p) |
template<class T > | |
bool | isKK (const T &p) |
template<class T > | |
bool | isHiddenValley (const T &p) |
template<class T > | |
bool | isDiquark (const T &p) |
template<class T > | |
bool | isHadron (const T &p) |
template<class T > | |
bool | isMeson (const T &p) |
template<class T > | |
bool | isBaryon (const T &p) |
template<class T > | |
bool | isTetraquark (const T &p) |
template<class T > | |
bool | isPentaquark (const T &p) |
template<class T > | |
bool | isNucleus (const T &p) |
template<class T > | |
bool | isBSM (const T &p) |
template<class T > | |
bool | isValid (const T &p) |
template<> | |
bool | isValid (const DecodedPID &p) |
Av: we implement here an ATLAS-sepcific convention: all particles which are 99xxxxx are fine. More... | |
template<class T > | |
bool | isTransportable (const T &p) |
template<class T > | |
bool | isGenSpecific (const T &p) |
template<class T > | |
bool | isGeantino (const T &p) |
template<class T > | |
bool | isPythia8Specific (const T &p) |
template<> | |
bool | isPythia8Specific (const DecodedPID &p) |
template<> | |
bool | isGenSpecific (const int &p) |
Main Table for MC internal use 81–100,901–930,998-999,1901–1930,2901–2930, and 3901–3930. More... | |
template<> | |
bool | isGeantino (const int &p) |
template<> | |
bool | isSUSY (const DecodedPID &p) |
PDG rule 11d Fundamental supersymmetric particles are identified by adding a nonzeronto the par-ticle number. More... | |
template<> | |
bool | isTechnicolor (const DecodedPID &p) |
PDG rule 11e Technicolor states have n= 3, with technifermions treated like ordinary fermions. More... | |
template<> | |
bool | isTechnicolor (const int &p) |
template<> | |
bool | isExcited (const DecodedPID &p) |
PDG rule 11f Excited (composite) quarks and leptons are identified by setting n= 4 and nr= 0. More... | |
template<> | |
bool | isExcited (const int &p) |
template<> | |
bool | isKK (const DecodedPID &p) |
PDG rule 11h A black hole in models with extra dimensions has code 5000040. More... | |
template<> | |
bool | isKK (const int &p) |
template<> | |
bool | isHiddenValley (const DecodedPID &p) |
PDG rule 11k Hidden Valley particles have n= 4 and nr= 9, and trailing numbers in agreement with their nearest-analog standard particles, as far as possible. More... | |
template<> | |
bool | isHiddenValley (const int &p) |
template<> | |
bool | isDiquark (const DecodedPID &p) |
PDG rule 4 Diquarks have 4-digit numbers with nq1 >= nq2 and nq3 = 0 APID: the diquarks with fourth generation are not diquarks. More... | |
template<> | |
bool | isMeson (const DecodedPID &p) |
Table 43.1 PDG rule 5a: The numbers specifying the meson’s quark content conform to the convention nq1= 0 and nq2 >= nq3. More... | |
template<> | |
bool | isBaryon (const DecodedPID &p) |
Table 43.2. More... | |
template<> | |
bool | isPentaquark (const DecodedPID &p) |
PDG rule 15 The 9-digit penta-quark codes are±1nrnLnq1nq2nq3nq4nq5nJ, sorted such thatnq1≥nq2≥nq3≥nq4. More... | |
template<> | |
bool | isTetraquark (const DecodedPID &p) |
PDG rule 14 The 9-digit tetra-quark codes are±1nrnLnq1nq20nq3nq4nJ. More... | |
template<> | |
bool | isNucleus (const DecodedPID &p) |
PDG rule 16: Nuclear codes are given as 10-digit numbers±10LZZZAAAI. More... | |
template<> | |
bool | isBSM (const DecodedPID &p) |
APID: graviton and all Higgs extensions are BSM. More... | |
template<> | |
bool | isSUSY (const int &p) |
template<> | |
bool | isDiquark (const int &p) |
template<> | |
bool | isMeson (const int &p) |
template<> | |
bool | isBaryon (const int &p) |
template<> | |
bool | isTetraquark (const int &p) |
template<> | |
bool | isPentaquark (const int &p) |
template<> | |
bool | isNucleus (const int &p) |
template<> | |
bool | isBSM (const int &p) |
template<> | |
bool | isHadron (const DecodedPID &p) |
template<> | |
bool | isHadron (const int &p) |
template<> | |
bool | isTransportable (const DecodedPID &p) |
template<> | |
bool | isTransportable (const int &p) |
template<> | |
bool | isValid (const int &p) |
template<class T > | |
bool | hasQuark (const T &p, const int &q) |
template<> | |
bool | hasQuark (const DecodedPID &p, const int &q) |
template<> | |
bool | hasQuark (const int &p, const int &q) |
template<class T > | |
int | leadingQuark (const T &p) |
template<> | |
int | leadingQuark (const DecodedPID &p) |
template<> | |
int | leadingQuark (const int &p) |
template<class T > | |
bool | hasStrange (const T &p) |
template<class T > | |
bool | hasCharm (const T &p) |
template<class T > | |
bool | hasBottom (const T &p) |
template<class T > | |
bool | hasTop (const T &p) |
template<class T > | |
bool | isLightHadron (const T &p) |
template<class T > | |
bool | isHeavyHadron (const T &p) |
template<class T > | |
bool | isStrangeHadron (const T &p) |
template<class T > | |
bool | isCharmHadron (const T &p) |
template<class T > | |
bool | isBottomHadron (const T &p) |
template<class T > | |
bool | isTopHadron (const T &p) |
template<class T > | |
bool | isLightMeson (const T &p) |
template<class T > | |
bool | isHeavyMeson (const T &p) |
template<class T > | |
bool | isStrangeMeson (const T &p) |
template<class T > | |
bool | isCharmMeson (const T &p) |
template<class T > | |
bool | isBottomMeson (const T &p) |
template<class T > | |
bool | isTopMeson (const T &p) |
template<class T > | |
bool | isCCbarMeson (const T &p) |
template<> | |
bool | isCCbarMeson (const DecodedPID &p) |
template<> | |
bool | isCCbarMeson (const int &p) |
template<class T > | |
bool | isBBbarMeson (const T &p) |
template<> | |
bool | isBBbarMeson (const DecodedPID &p) |
template<> | |
bool | isBBbarMeson (const int &p) |
template<class T > | |
bool | isLightBaryon (const T &p) |
template<class T > | |
bool | isHeavyBaryon (const T &p) |
template<class T > | |
bool | isStrangeBaryon (const T &p) |
template<class T > | |
bool | isCharmBaryon (const T &p) |
template<class T > | |
bool | isBottomBaryon (const T &p) |
template<class T > | |
bool | isTopBaryon (const T &p) |
template<class T > | |
int | charge3 (const T &p) |
template<class T > | |
double | charge (const T &p) |
template<class T > | |
double | threeCharge (const T &p) |
template<class T > | |
bool | isCharged (const T &p) |
template<class T > | |
bool | isNeutral (const T &p) |
template<> | |
int | charge3 (const DecodedPID &p) |
template<> | |
int | charge3 (const int &p) |
template<class T > | |
bool | isEMInteracting (const T &p) |
template<> | |
bool | isEMInteracting (const int &p) |
template<class T > | |
bool | isStrongInteracting (const T &p) |
template<> | |
bool | isStrongInteracting (const int &p) |
template<class T > | |
bool | isParton (const T &p) |
template<class T > | |
bool | SUSY::isRGlueball (const T &p) |
template<> | |
bool | SUSY::isRGlueball (const DecodedPID &p) |
template<> | |
bool | SUSY::isRGlueball (const int &p) |
template<class T > | |
bool | SUSY::isRHadron (const T &p) |
template<> | |
bool | SUSY::isRHadron (const DecodedPID &p) |
template<> | |
bool | SUSY::isRHadron (const int &p) |
template<class T > | |
bool | SUSY::isRMeson (const T &p) |
template<> | |
bool | SUSY::isRMeson (const DecodedPID &p) |
template<> | |
bool | SUSY::isRMeson (const int &p) |
template<class T > | |
bool | SUSY::isRBaryon (const T &p) |
template<> | |
bool | SUSY::isRBaryon (const DecodedPID &p) |
template<> | |
bool | SUSY::isRBaryon (const int &p) |
template<class T > | |
bool | SUSY::isRBottomHadron (const T &p) |
template<> | |
bool | SUSY::isRBottomHadron (const DecodedPID &p) |
template<> | |
bool | SUSY::isRBottomHadron (const int &p) |
template<class T > | |
bool | SUSY::isRTopHadron (const T &p) |
template<> | |
bool | SUSY::isRTopHadron (const DecodedPID &p) |
template<> | |
bool | SUSY::isRTopHadron (const int &p) |
template<class T > | |
bool | SUSY::isSLepton (const T &p) |
template<> | |
bool | SUSY::isSLepton (const DecodedPID &p) |
template<> | |
bool | SUSY::isSLepton (const int &p) |
template<class T > | |
bool | SUSY::isSTopHadron (const T &p) |
template<> | |
bool | SUSY::isSTopHadron (const DecodedPID &p) |
template<> | |
bool | SUSY::isSTopHadron (const int &p) |
template<class T > | |
bool | SUSY::isSBaryon (const T &p) |
template<> | |
bool | SUSY::isSBaryon (const DecodedPID &p) |
template<> | |
bool | SUSY::isSBaryon (const int &p) |
template<class T > | |
bool | SUSY::isSMeson (const T &p) |
template<> | |
bool | SUSY::isSMeson (const DecodedPID &p) |
template<> | |
bool | SUSY::isSMeson (const int &p) |
template<class T > | |
bool | SUSY::isSBottomHadron (const T &p) |
template<> | |
bool | SUSY::isSBottomHadron (const DecodedPID &p) |
template<> | |
bool | SUSY::isSBottomHadron (const int &p) |
template<class T > | |
bool | SUSY::isSTopMeson (const T &p) |
template<> | |
bool | SUSY::isSTopMeson (const DecodedPID &p) |
template<> | |
bool | SUSY::isSTopMeson (const int &p) |
template<class T > | |
bool | SUSY::isSBottomMeson (const T &p) |
template<> | |
bool | SUSY::isSBottomMeson (const DecodedPID &p) |
template<> | |
bool | SUSY::isSBottomMeson (const int &p) |
template<class T > | |
bool | SUSY::isSTopBaryon (const T &p) |
template<> | |
bool | SUSY::isSTopBaryon (const DecodedPID &p) |
template<> | |
bool | SUSY::isSTopBaryon (const int &p) |
template<class T > | |
bool | SUSY::isSBottomBaryon (const T &p) |
template<> | |
bool | SUSY::isSBottomBaryon (const DecodedPID &p) |
template<> | |
bool | SUSY::isSBottomBaryon (const int &p) |
template<class T > | |
bool | SUSY::spin (const T &p) |
template<> | |
bool | SUSY::spin (const int &p) |
std::vector< int > | SUSY::containedQuarks (int p) |
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Definition at line 494 of file AtlasPID.h.
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Definition at line 501 of file AtlasPID.h.
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Definition at line 493 of file AtlasPID.h.
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Definition at line 120 of file AtlasPID.h.
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Definition at line 465 of file AtlasPID.h.
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Definition at line 472 of file AtlasPID.h.
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Definition at line 140 of file AtlasPID.h.
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PDG rule 4 Diquarks have 4-digit numbers with nq1 >= nq2 and nq3 = 0 APID: the diquarks with fourth generation are not diquarks.
Definition at line 276 of file AtlasPID.h.
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Definition at line 404 of file AtlasPID.h.
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Definition at line 206 of file AtlasPID.h.
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Definition at line 181 of file AtlasPID.h.
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PDG rule 11j: The nature of Dark Matter (DM) is not known, and therefore a definitive classificationis too early.
Candidates within specific scenarios are classified therein, such as 1000022 for the lightest neutralino. Generic fundamental states can be given temporary codes in the range 51 - 60, with 51, 52 and 53 reserved for spin 0, 1/2 and 1 ones (this could also be an axion state). Generic mediators of s-channel DM pair creation of annihilationcan be given codes 54 and 55 for spin 0 or 1 ones. Separate antiparticles, with negativecodes, may or may not exist. More elaborate new scenarios should be constructed with n= 5 and nr = 9. APID: Only the 51-60 range is considered DM. The antiparticles are assumed to be existing.
Definition at line 180 of file AtlasPID.h.
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Definition at line 143 of file AtlasPID.h.
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Definition at line 142 of file AtlasPID.h.
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Definition at line 203 of file AtlasPID.h.
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Definition at line 233 of file AtlasPID.h.
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Definition at line 218 of file AtlasPID.h.
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Main Table for MC internal use 81–100,901–930,998-999,1901–1930,2901–2930, and 3901–3930.
Definition at line 223 of file AtlasPID.h.
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Definition at line 217 of file AtlasPID.h.
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Definition at line 159 of file AtlasPID.h.
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Definition at line 486 of file AtlasPID.h.
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Definition at line 463 of file AtlasPID.h.
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Definition at line 470 of file AtlasPID.h.
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PDG rule 11k Hidden Valley particles have n= 4 and nr= 9, and trailing numbers in agreement with their nearest-analog standard particles, as far as possible.
Thus 4900021 is the gauge boson gv of a confining gauge field, 490000 nqv and 490001 nlv fundamental constituents charged or not under this, 4900022 is the γv of a non-confining field, and 4900 nqv1 nqv2 nJ a Hidden Valley meson.
Definition at line 270 of file AtlasPID.h.
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Definition at line 271 of file AtlasPID.h.
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Definition at line 205 of file AtlasPID.h.
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Definition at line 191 of file AtlasPID.h.
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APID: HIGGS boson is only one particle.
Definition at line 190 of file AtlasPID.h.
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PDG rule 11h A black hole in models with extra dimensions has code 5000040.
Kaluza-Klein excitations in models with extra dimensions have n= 5 or n= 6, to distinguish excitations of left-or right-handed fermions or, in case of mixing, the lighter or heavier state (cf. 11d). The non zero nr digit gives the radial excitation number, in scenarios where the level spacing allows these to be distinguished. Should the model also contain supersymmetry, excited SUSY states would be denoted by a nnr>0, with n= 1 or 2 as usual. Should some colored states be long-lived enough that hadrons would form around them, the coding strategy of 11g applies, with the initial two nnr digits preserved in the combined code.
Definition at line 262 of file AtlasPID.h.
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Definition at line 263 of file AtlasPID.h.
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Definition at line 204 of file AtlasPID.h.
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Definition at line 132 of file AtlasPID.h.
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Definition at line 131 of file AtlasPID.h.
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APID: the fourth generation leptons are leptons.
Definition at line 130 of file AtlasPID.h.
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Definition at line 198 of file AtlasPID.h.
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Definition at line 485 of file AtlasPID.h.
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Definition at line 462 of file AtlasPID.h.
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Definition at line 469 of file AtlasPID.h.
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Table 43.1 PDG rule 5a: The numbers specifying the meson’s quark content conform to the convention nq1= 0 and nq2 >= nq3.
The special case K0L is the sole exception to this rule. PDG rule 5C: The special numbers 310 and 130 are given to the K0S and K0L respectively. APID: The special code K0 is used when a generator uses K0S/K0L
Definition at line 291 of file AtlasPID.h.
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Definition at line 153 of file AtlasPID.h.
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PDG rule 16: Nuclear codes are given as 10-digit numbers±10LZZZAAAI.
For a (hyper)nucleus consistingofnpprotons,nnneutrons andnΛΛ’s,A=np+nn+nΛgives the total baryon number, Z=np the total charge andL=nΛthe total number of strange quarks.Igives the isomerlevel, withI= 0corresponding to the ground state andI >0to excitations, see [2], wherestates denotedm,n,p,qtranslate toI= 1–4. As examples, the deuteron is 1000010020 and 235U is
Definition at line 384 of file AtlasPID.h.
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Definition at line 409 of file AtlasPID.h.
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Definition at line 212 of file AtlasPID.h.
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PDG rule 15 The 9-digit penta-quark codes are±1nrnLnq1nq2nq3nq4nq5nJ, sorted such thatnq1≥nq2≥nq3≥nq4.
In the particle the first four are quarks and the fifth an antiquark while t heopposite holds in the antiparticle, which is given with a negative sign. Thenr,nL, andnJnumbers have the same meaning as for ordinary hadrons.
Definition at line 357 of file AtlasPID.h.
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Definition at line 219 of file AtlasPID.h.
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Definition at line 115 of file AtlasPID.h.
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Definition at line 114 of file AtlasPID.h.
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PDG rule 2: Quarks and leptons are numbered consecutively starting from 1 and 11 respectively; to dothis they are first ordered by family and within families by weak isospin.
APID: the fourth generation quarks are quarks.
Definition at line 113 of file AtlasPID.h.
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Definition at line 136 of file AtlasPID.h.
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Definition at line 135 of file AtlasPID.h.
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Definition at line 134 of file AtlasPID.h.
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Definition at line 156 of file AtlasPID.h.
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Definition at line 155 of file AtlasPID.h.
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Definition at line 118 of file AtlasPID.h.
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Definition at line 117 of file AtlasPID.h.
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Definition at line 487 of file AtlasPID.h.
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Definition at line 464 of file AtlasPID.h.
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Definition at line 471 of file AtlasPID.h.
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Definition at line 538 of file AtlasPID.h.
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PDG rule 11d Fundamental supersymmetric particles are identified by adding a nonzeronto the par-ticle number.
T he superpartner of a boson or a left-handed fermion hasn= 1whilethe superpartner of a right-handed fermion hasn= 2. When mixing occurs, such asbetween the winos and charged Higgsinos to give charginos, or between left and rightsfermions, the lighter physical state is given the smaller basis state number.
Definition at line 240 of file AtlasPID.h.
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Definition at line 403 of file AtlasPID.h.
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Definition at line 201 of file AtlasPID.h.
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Definition at line 149 of file AtlasPID.h.
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Definition at line 148 of file AtlasPID.h.
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PDG rule 11e Technicolor states have n= 3, with technifermions treated like ordinary fermions.
States which are ordinary color singlets have nr= 0. Color octets have nr= 1. If a state has non-trivial quantum numbers under the topcolor groups SU(3)1×SU(3)2, the quantum numbers are specified by tech, ij, where i and j are 1 or 2. nLis then 2i+j. The coloron V8, is a heavy gluon color octet and thus is 3100021
Definition at line 247 of file AtlasPID.h.
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Definition at line 248 of file AtlasPID.h.
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Definition at line 202 of file AtlasPID.h.
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PDG rule 14 The 9-digit tetra-quark codes are±1nrnLnq1nq20nq3nq4nJ.
For the particleq1q2is a diquarkand ̄q3 ̄q4an antidiquark, sorted such thatnq1≥nq2,nq3≥nq4,nq1≥nq3, andnq2≥nq4ifnq1=nq3. For the antiparticle, given with a negative sign, ̄q1 ̄q2is an antidiquark andq3q4a diquark, with the same sorting except that eithernq1> nq3ornq2> nq4(so thatflavour-diagonal states are particles). Thenr,nL, andnJnumbers have the same meaningas for ordinary hadrons.
Definition at line 368 of file AtlasPID.h.
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Definition at line 407 of file AtlasPID.h.
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Definition at line 210 of file AtlasPID.h.
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Definition at line 127 of file AtlasPID.h.
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Definition at line 126 of file AtlasPID.h.
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Definition at line 490 of file AtlasPID.h.
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Definition at line 467 of file AtlasPID.h.
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Definition at line 474 of file AtlasPID.h.
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Definition at line 187 of file AtlasPID.h.
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PDG rule 8: The pomeron and odderon trajectories and a generic reggeon trajectory of states in QCD areassigned codes 990, 9990, and 110 respectively.
Definition at line 186 of file AtlasPID.h.
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Definition at line 421 of file AtlasPID.h.
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Definition at line 422 of file AtlasPID.h.
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Definition at line 216 of file AtlasPID.h.
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Av: we implement here an ATLAS-sepcific convention: all particles which are 99xxxxx are fine.
Definition at line 424 of file AtlasPID.h.
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Definition at line 425 of file AtlasPID.h.
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Definition at line 214 of file AtlasPID.h.
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Definition at line 168 of file AtlasPID.h.
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Definition at line 167 of file AtlasPID.h.
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Definition at line 165 of file AtlasPID.h.
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Definition at line 164 of file AtlasPID.h.
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Definition at line 445 of file AtlasPID.h.
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Definition at line 455 of file AtlasPID.h.
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Definition at line 444 of file AtlasPID.h.
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Definition at line 495 of file AtlasPID.h.