Observables / Higgs production and decay / $h\to ff$

The tables below have been generated automatically from the observables currently implemented in flavio. The first column is the string name that must be used when calling functions such as flavio.sm_prediction. The last column lists the arguments the observable depends on (which can also be empty in case of a scalar observable).

$h \to \mu^+\mu^-$

Name Symbol Description Arguments
mu_VBF(h->mumu) $\mu_{\text{VBF}}(h \to \mu^+\mu^-)$ Signal strength of $h \to \mu^+\mu^-$ from weak boson fusion  
mu_Vh(h->mumu) $\mu_{Vh}(h \to \mu^+\mu^-)$ Signal strength of $h \to \mu^+\mu^-$ from $Z$ or $W$ boson associated production  
mu_Wh(h->mumu) $\mu_{Wh}(h \to \mu^+\mu^-)$ Signal strength of $h \to \mu^+\mu^-$ from $W$ boson associated production  
mu_Zh(h->mumu) $\mu_{Zh}(h \to \mu^+\mu^-)$ Signal strength of $h \to \mu^+\mu^-$ from $Z$ boson associated production  
mu_gg(h->mumu) $\mu_{gg}(h \to \mu^+\mu^-)$ Signal strength of $h \to \mu^+\mu^-$ from gluon fusion production  
mu_tth(h->mumu) $\mu_{t\bar t h}(h \to \mu^+\mu^-)$ Signal strength of $h \to \mu^+\mu^-$ from top pair associated production  

$h \to \tau^+\tau^-$

Name Symbol Description Arguments
mu_VBF(h->tautau) $\mu_{\text{VBF}}(h \to \tau^+\tau^-)$ Signal strength of $h \to \tau^+\tau^-$ from weak boson fusion  
mu_Vh(h->tautau) $\mu_{Vh}(h \to \tau^+\tau^-)$ Signal strength of $h \to \tau^+\tau^-$ from $Z$ or $W$ boson associated production  
mu_Wh(h->tautau) $\mu_{Wh}(h \to \tau^+\tau^-)$ Signal strength of $h \to \tau^+\tau^-$ from $W$ boson associated production  
mu_Zh(h->tautau) $\mu_{Zh}(h \to \tau^+\tau^-)$ Signal strength of $h \to \tau^+\tau^-$ from $Z$ boson associated production  
mu_gg(h->tautau) $\mu_{gg}(h \to \tau^+\tau^-)$ Signal strength of $h \to \tau^+\tau^-$ from gluon fusion production  
mu_tth(h->tautau) $\mu_{t\bar t h}(h \to \tau^+\tau^-)$ Signal strength of $h \to \tau^+\tau^-$ from top pair associated production  

$h \to b\bar b$

Name Symbol Description Arguments
mu_VBF(h->bb) $\mu_{\text{VBF}}(h \to b\bar b)$ Signal strength of $h \to b\bar b$ from weak boson fusion  
mu_Vh(h->bb) $\mu_{Vh}(h \to b\bar b)$ Signal strength of $h \to b\bar b$ from $Z$ or $W$ boson associated production  
mu_Wh(h->bb) $\mu_{Wh}(h \to b\bar b)$ Signal strength of $h \to b\bar b$ from $W$ boson associated production  
mu_Zh(h->bb) $\mu_{Zh}(h \to b\bar b)$ Signal strength of $h \to b\bar b$ from $Z$ boson associated production  
mu_gg(h->bb) $\mu_{gg}(h \to b\bar b)$ Signal strength of $h \to b\bar b$ from gluon fusion production  
mu_tth(h->bb) $\mu_{t\bar t h}(h \to b\bar b)$ Signal strength of $h \to b\bar b$ from top pair associated production  

$h \to c\bar c$

Name Symbol Description Arguments
mu_VBF(h->cc) $\mu_{\text{VBF}}(h \to c\bar c)$ Signal strength of $h \to c\bar c$ from weak boson fusion  
mu_Vh(h->cc) $\mu_{Vh}(h \to c\bar c)$ Signal strength of $h \to c\bar c$ from $Z$ or $W$ boson associated production  
mu_Wh(h->cc) $\mu_{Wh}(h \to c\bar c)$ Signal strength of $h \to c\bar c$ from $W$ boson associated production  
mu_Zh(h->cc) $\mu_{Zh}(h \to c\bar c)$ Signal strength of $h \to c\bar c$ from $Z$ boson associated production  
mu_gg(h->cc) $\mu_{gg}(h \to c\bar c)$ Signal strength of $h \to c\bar c$ from gluon fusion production  
mu_tth(h->cc) $\mu_{t\bar t h}(h \to c\bar c)$ Signal strength of $h \to c\bar c$ from top pair associated production