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 |
---|---|---|---|
BR(W->enu) |
$\text{BR}(W^\pm\to e^\pm\nu)$ | Branching ratio of $W^\pm\to e^\pm\nu$, summed over neutrino flavours | |
GammaW |
$\Gamma_W$ | Total width of the $W^\pm$ boson | |
Rmue(W->lnu) |
$\text{R}_{\mu e}(W^\pm\to \ell^\pm\nu)$ | Ratio of branching ratio of $W^\pm\to \mu^\pm\nu$ and $W^\pm\to e^\pm\nu$, individually summed over neutrino flavours | |
Rtaue(W->lnu) |
$\text{R}_{\tau e}(W^\pm\to \ell^\pm\nu)$ | Ratio of branching ratio of $W^\pm\to \tau^\pm\nu$ and $W^\pm\to e^\pm\nu$, individually summed over neutrino flavours |
Name | Symbol | Description | Arguments |
---|---|---|---|
BR(W->munu) |
$\text{BR}(W^\pm\to \mu^\pm\nu)$ | Branching ratio of $W^\pm\to \mu^\pm\nu$, summed over neutrino flavours | |
GammaW |
$\Gamma_W$ | Total width of the $W^\pm$ boson | |
Rmue(W->lnu) |
$\text{R}_{\mu e}(W^\pm\to \ell^\pm\nu)$ | Ratio of branching ratio of $W^\pm\to \mu^\pm\nu$ and $W^\pm\to e^\pm\nu$, individually summed over neutrino flavours | |
Rtaumu(W->lnu) |
$\text{R}_{\tau \mu}(W^\pm\to \ell^\pm\nu)$ | Ratio of branching ratio of $W^\pm\to \tau^\pm\nu$ and $W^\pm\to \mu^\pm\nu$, individually summed over neutrino flavours |
Name | Symbol | Description | Arguments |
---|---|---|---|
BR(W->taunu) |
$\text{BR}(W^\pm\to \tau^\pm\nu)$ | Branching ratio of $W^\pm\to \tau^\pm\nu$, summed over neutrino flavours | |
GammaW |
$\Gamma_W$ | Total width of the $W^\pm$ boson | |
Rtaue(W->lnu) |
$\text{R}_{\tau e}(W^\pm\to \ell^\pm\nu)$ | Ratio of branching ratio of $W^\pm\to \tau^\pm\nu$ and $W^\pm\to e^\pm\nu$, individually summed over neutrino flavours | |
Rtaumu(W->lnu) |
$\text{R}_{\tau \mu}(W^\pm\to \ell^\pm\nu)$ | Ratio of branching ratio of $W^\pm\to \tau^\pm\nu$ and $W^\pm\to \mu^\pm\nu$, individually summed over neutrino flavours |