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).
| 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 |
| 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 |
| 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 |
| 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 |
flavio