List of Observables
The following is a list of observables that is available in EOS v1.0.21.
Observables in (semi)leptonic \(b\)-hadron decays
Observables in \(B^-\to \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(B_c^- \to \ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B^- \to \ell^-\bar\nu)\) |
The option “l” selects the charged lepton flavor.
Observables in \(B^-\to \ell^-\bar\nu\ell'^+\ell'^-\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_{\mathrm{FB}}(B^- \to e^-\bar\nu\mu^+\mu^-)\) |
|
|
\(\mathcal{B}(B^- \to e^-\bar\nu\mu^+\mu^-)\) |
|
|
n/a |
|
|
n/a |
|
|
\(\frac{d\mathcal{B}(B^- \to e^-\bar\nu\mu^+\mu^-)}{dq^2/dk^2}\) |
|
|
\(A_{\mathrm{FB}}(B^- \to \mu^-\bar\nu e^+e^-)\) |
|
|
\(\mathcal{B}(B^- \to \mu^-\bar\nu e^+e^-)\) |
|
|
n/a |
|
|
n/a |
|
|
\(\frac{d\mathcal{B}(B^- \to \mu^-\bar\nu e^+e^-)}{dq^2/dk^2}\) |
|
|
\(A_{\mathrm{FB}}(B^- \to \tau^-\bar\nu e^+e^-)\) |
|
|
\(\mathcal{B}(B^- \to \tau^-\bar\nu e^+e^-)\) |
|
|
\(\frac{d\mathcal{B}(B^- \to \tau^-\bar\nu e^+e^-)}{dq^2/dk^2}\) |
|
|
\(A_{\mathrm{FB}}(B^- \to \tau^-\bar\nu\mu^+\mu^-)\) |
|
|
\(\mathcal{B}(B^- \to \tau^-\bar\nu\mu^+\mu^-)\) |
|
|
\(\frac{d\mathcal{B}(B^- \to \tau^-\bar\nu\mu^+\mu^-)}{dq^2/dk^2}\) |
|
The option “l” selects the charged lepton flavour coming out of the weak current, “lprime” selects the lepton flavour coming out of the photon.
Observables in \(B\to \pi \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_{\mathrm{FB}}(B\to \pi\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{FB}}(B\to \pi\ell^-\bar\nu)(q^2)\) |
|
|
n/a |
|
|
\(\mathcal{B}(B\to\pi\ell^-\bar\nu)\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(dP(B\to\pi\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(P(B\to\pi\ell^-\bar\nu)\) |
|
|
\(R_{\pi}\) |
|
|
\(R_{\pi}(q^2)\) |
|
|
\(R_{\pi, 0}\) |
|
|
\(R_{\pi, P}\) |
|
|
n/a |
|
|
n/a |
|
|
\(d\mathcal{B}(B\to\pi\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(d^2\mathcal{B}(B\to\pi\ell^-\bar\nu)/dq^2/d\cos(\theta_l)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\Gamma(B\to\pi\ell^-\bar\nu)\) |
|
|
\(\Gamma(B\to\pi\ell^-\bar\nu)_0\) |
|
|
\(\Gamma(B\to\pi\ell^-\bar\nu)_p\) |
|
|
n/a |
|
The option “l” selects the charged lepton flavor. The option “q” selects the spectator quark flavor. The option “form-factors” selects the form factor parametrization.
Observables in \(\bar{B}\to D \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_{\mathrm{FB}}(\bar{B}\to D\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{FB}}(\bar{B}\to D\ell^-\bar\nu)(q^2)\) |
|
|
n/a |
|
|
\(\mathcal{B}(\bar{B}\to D\ell^-\bar\nu)\) |
|
|
\(\Gamma(\bar{B}\to D\ell^-\bar\nu)\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(R_D\) |
|
|
\(R_D(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(d\mathcal{B}(\bar{B}\to D\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(d\Gamma(\bar{B}\to D\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(d^2\mathcal{B}(\bar{B}\to D\ell^-\bar\nu)/dq^2/d\cos(\theta_l)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
n/a |
|
|
\(\Gamma(\bar{B}\to D\ell^-\bar\nu)_{|V_{cb}|=1}\) |
|
|
n/a |
|
|
n/a |
|
The option “l” selects the charged lepton flavor. The option “q” selects the spectator quark flavor. The option “form-factors” selects the form factor parametrization.
Observables in \(B^- \to \eta \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_{\mathrm{FB}}(B^- \to\eta\ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B^- \to \eta \ell^-\bar\nu)\) |
|
|
n/a |
|
|
n/a |
|
|
\(dP(B^- \to \eta \ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(P(B^- \to \eta \ell^-\bar\nu)\) |
|
|
n/a |
|
|
n/a |
|
|
\(d\mathcal{B}(B^- \to \eta \ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
n/a |
|
|
n/a |
|
The option “l” selects the charged lepton flavor.The option “form-factors” selects the form factor parametrization.
Observables in \(B^- \to \eta^\prime \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_{\mathrm{FB}}(B^- \to\eta^prime \ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B^- \to \eta^\prime \ell^-\bar\nu)\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(d\mathcal{B}(B^- \to \eta^\prime \ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
n/a |
|
|
n/a |
|
The option “l” selects the charged lepton flavor.The option “form-factors” selects the form factor parametrization.
Observables in \(B_s\to \bar{K} \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(\bar{B}_s\to K\ell^-\bar\nu)\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(d\mathcal{B}(\bar{B}_s\to K\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
n/a |
|
|
n/a |
|
The option “l” selects the charged lepton flavor.The option “form-factors” selects the form factor parametrization.
Observables in \(\bar{B}_s\to D_s \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_{\mathrm{FB}}(\bar{B}_s\to D_s\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{FB}}(\bar{B}_s\to D_s\ell^-\bar\nu)(q^2)\) |
|
|
n/a |
|
|
\(\mathcal{B}(\bar{B}_s\to D_s\ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(\bar{B}_s\to D_s\ell^-\bar\nu)({k_\perp}_\textrm{min},{k_\perp}_\textrm{max})\, \left[ \textrm{GeV}^{-1} \right]\) |
|
|
\(\Gamma(\bar{B}_s\to D_s\ell^-\bar\nu)\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(R_{D_s}\) |
|
|
\(R_{D_s}(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(d\mathcal{B}(\bar{B}_s\to D_s\ell^-\bar\nu)/dk_\perp\, \left[ \textrm{GeV}^{-1} \right]\) |
|
|
\(d\mathcal{B}(\bar{B}_s\to D_s\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(d\Gamma(\bar{B}_s\to D_s\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
n/a |
|
|
\(\Gamma(\bar{B}_s\to D_s\ell^-\bar\nu)_{|V_{cb}|=1}\) |
|
|
n/a |
|
|
n/a |
|
The option “l” selects the charged lepton flavor.The option “form-factors” selects the form factor parametrization.
Observables in \(B\to \omega \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(B\to\omega\ell^-\bar\nu)\) |
|
|
\(d\mathcal{B}(B\to\omega\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
The option “l” selects the charged lepton flavor. The option “q” selects the spectator quark flavor. The option “form-factors” selects the form factor parametrization.
Observables in \(B\to \rho \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(B\to\rho\ell^-\bar\nu)\) |
|
|
\(d\mathcal{B}(B\to\rho\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
The option “l” selects the charged lepton flavor. The option “q” selects the spectator quark flavor. The option “form-factors” selects the form factor parametrization.
Observables in \(\bar{B}\to D^* \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_{1c}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(A_{1s}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(A_{2c}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(A_{2s}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(A_3(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(A_4(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(A_5(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(A_{6c}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(A_{6s}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(A_7(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(A_8(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(A_9(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{C}}^1(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{C}}^2(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{C}}^3(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{FB}}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{FB}}(\bar{B}\to D^*\ell^-\bar\nu)(q^2)\) |
|
|
\(A_{\mathrm{FB}}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
n/a |
|
|
n/a |
|
|
\(A_{\mathrm{T}}^1(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{T}}^2(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{T}}^3(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(\bar{A}_{\mathrm{FB}}(\bar{B}\to D^*\ell^-\bar\nu)_{\ell=e,\mu}\) |
|
|
\(\bar{\mathcal{B}}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(\bar{B}\to D^*\ell^-\bar\nu)_{\ell=e,\mu}\) |
|
|
n/a |
|
|
\(\Delta\mathcal{B}(\bar{B}\to D^*\ell^-\bar\nu)_{\ell=e,\mu}\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(F_{\mathrm{L}}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(F_{\mathrm{L}}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(\bar{F}_{\mathrm{L}}(\bar{B}\to D^*\ell^-\bar\nu)_{\ell=e,\mu}\) |
|
|
\(\tilde{F}_{\mathrm{L}}(\bar{B}\to D^*\ell^-\bar\nu)\) |
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\(\tilde{F}_{\mathrm{L}}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(\bar{\tilde{F}}_{\mathrm{L}}(\bar{B}\to D^*\ell^-\bar\nu)_{\ell=e,\mu}\) |
|
|
\(\bar{\Gamma}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(\Gamma(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(J_{1c}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(J_{1c}(\bar{B}\to D^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{1s}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(J_{1s}(\bar{B}\to D^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{2c}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(J_{2c}(\bar{B}\to D^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{2s}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(J_{2s}(\bar{B}\to D^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{3}(\bar{B}\to D^*\ell^-\bar\nu)\) |
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\(J_{3}(\bar{B}\to D^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{4}(\bar{B}\to D^*\ell^-\bar\nu)\) |
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\(J_{4}(\bar{B}\to D^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{5}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(J_{5}(\bar{B}\to D^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{6c}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(J_{6c}(\bar{B}\to D^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{6s}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(J_{6s}(\bar{B}\to D^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{7}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(J_{7}(\bar{B}\to D^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{8}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(J_{8}(\bar{B}\to D^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{9}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(J_{9}(\bar{B}\to D^*\ell^-\bar\nu)(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(R_{D^*}\) |
|
|
\(R_{D^*}^{e/\mu}(q^2)\) |
|
|
\(R_{D^*}^{\tau/\mu}(q^2)\) |
|
|
\(S_{1c}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(S_{1s}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(S_{2c}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(S_{2s}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(S_3(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(S_4(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(S_5(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(S_{6c}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(S_{6s}(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(S_7(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(S_8(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
\(S_9(\bar{B}\to D^*\ell^-\bar\nu)\) |
|
|
n/a |
|
|
n/a |
|
|
\(d\mathcal{B}(\bar{B}\to D^*\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(d\Gamma(\bar{B}\to D^*\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
n/a |
|
|
\(\bar{\Gamma}(\bar{B}\to D^*\ell^-\bar\nu)_{|V_{cb}|=1}\) |
|
|
\(\Gamma(\bar{B}\to D^*\ell^-\bar\nu)_{|V_{cb}|=1}\) |
|
|
n/a |
|
|
n/a |
|
The option “l” selects the charged lepton flavor. The option “q” selects the spectator quark flavor. The option “form-factors” selects the form factor parametrization.
Observables in \(B_u \to \gamma \ell \nu_{\ell}\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_{\mathrm{FB}}(B^- \to \gamma \ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B^- \to \gamma \ell^-\bar\nu)\) |
|
|
n/a |
|
|
n/a |
|
The option “form-factors” selects the form factor parametrization.
Observables in \(B_s\to \bar{K}^* \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_{\mathrm{C}}^1(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{C}}^2(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{C}}^3(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{FB}}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{FB}}(B_s\to \bar{K}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(A_L(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(A_T(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{T}}^1(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{T}}^2(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{T}}^3(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(F_{\mathrm{L}}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(J_{1c}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(J_{1c}(B_s\to \bar{K}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{1s}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(J_{1s}(B_s\to \bar{K}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{2c}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(J_{2c}(B_s\to \bar{K}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{2s}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(J_{2s}(B_s\to \bar{K}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{3}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(J_{3}(B_s\to \bar{K}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{4}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(J_{4}(B_s\to \bar{K}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{5}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(J_{5}(B_s\to \bar{K}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{6c}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(J_{6c}(B_s\to \bar{K}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{6s}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(J_{6s}(B_s\to \bar{K}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{7}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(J_{7}(B_s\to \bar{K}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{8}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(J_{8}(B_s\to \bar{K}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{9}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(J_{9}(B_s\to \bar{K}^*\ell^-\bar\nu)(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(d\mathcal{B}(B_s\to \bar{K}^*\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
n/a |
|
|
\(d\mathcal{B}(B_s\to \bar{K}^*\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
The option “l” selects the charged lepton flavor. The option “form-factors” selects the form factor parametrization.
Observables in \(\bar{B}_s\to D_s^* \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_{\mathrm{C}}^1(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{C}}^2(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{C}}^3(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{FB}}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{FB}}(\bar{B}_s\to D_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(A_L(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(A_T(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{T}}^1(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{T}}^2(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{T}}^3(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(F_{\mathrm{L}}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(\Gamma(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(J_{1c}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(J_{1c}(\bar{B}_s\to D_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{1s}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(J_{1s}(\bar{B}_s\to D_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{2c}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(J_{2c}(\bar{B}_s\to D_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{2s}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(J_{2s}(\bar{B}_s\to D_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{3}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(J_{3}(\bar{B}_s\to D_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{4}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(J_{4}(\bar{B}_s\to D_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{5}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(J_{5}(\bar{B}_s\to D_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{6c}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(J_{6c}(\bar{B}_s\to D_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{6s}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(J_{6s}(\bar{B}_s\to D_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{7}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(J_{7}(\bar{B}_s\to D_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{8}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(J_{8}(\bar{B}_s\to D_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{9}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(J_{9}(\bar{B}_s\to D_s^*\ell^-\bar\nu)(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(R_{D_s^*}\) |
|
|
\(R_{D_s^*}(q^2)\) |
|
|
\(S_{1c}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(S_{1s}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(S_{2c}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(S_{2s}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(S_{3}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(S_{4}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(S_{5}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(S_{6c}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(S_{6s}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(S_{7}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(S_{8}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
\(S_{9}(\bar{B}_s\to D_s^*\ell^-\bar\nu)\) |
|
|
n/a |
|
|
\(d\mathcal{B}(\bar{B}_s\to D_s^*\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(d\Gamma(\bar{B}_s\to D_s^*\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
n/a |
|
|
\(\bar{\Gamma}(\bar{B}_s\to D_s^*\ell^-\bar\nu)_{|V_{cb}|=1}\) |
|
|
\(\Gamma(\bar{B}_s\to D_s^*\ell^-\bar\nu)_{|V_{cb}|=1}\) |
|
|
n/a |
|
|
n/a |
|
The option “l” selects the charged lepton flavor.The option “form-factors” selects the form factor parametrization.
Observables in \(\bar{B}_c\to J/\psi \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(\bar{B}_c\to J/\psi\ell^-\bar\nu)\) |
|
|
\(\Gamma(\bar{B}_c\to J/\psi\ell^-\bar\nu)\) |
|
|
\(d\mathcal{B}(\bar{B}_c\to J/\psi\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(d\Gamma(\bar{B}_c\to J/\psi\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\mathcal{B}(\bar{B}_c\to J/\psi\ell^-\bar\nu)_{|V_{cb}|=1}\) |
|
|
\(\Gamma(\bar{B}_c\to J/\psi\ell^-\bar\nu)_{|V_{cb}|=1}\) |
|
|
n/a |
|
|
n/a |
|
The option “l” selects the charged lepton flavor.The option “form-factors” selects the form factor parametrization.
Observables in \(B\to \pi\pi \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_{\mathrm{FB}}(B\to \pi\pi \ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{FB}}(B\to \pi\pi \ell^-\bar\nu)(q^2,k^2)\, \left[ \textrm{GeV}^{-4} \right]\) |
|
|
\(\mathcal{B}(B\to \pi\pi \ell^-\bar\nu)\) |
|
|
\(d^2\mathcal{B}(B\to \pi\pi \ell^-\bar\nu)/(dq^2\,dk^2)\, \left[ \textrm{GeV}^{-4} \right]\) |
|
|
n/a |
|
|
n/a |
|
|
\(\mathcal{A}^{(\pi)}_{FB}(B^-\to \pi^+\pi^- \ell^-\bar\nu)\) |
|
|
\(\mathcal{A}^{(\pi)}_{FB}(B^-\to \pi^+\pi^- \ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B^-\to \pi^+\pi^- \ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B^-\to \pi^+\pi^- \ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B^-\to \pi^+\pi^- \ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B^-\to \pi^+\pi^- \ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B^-\to \pi^+\pi^- \ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B^-\to \pi^+\pi^- \ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B^+\to (\pi^+\pi^-)_D \ell^+\nu)\) |
|
|
\(\mathcal{B}(B^-\to \pi^+\pi^- \ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B^-\to \pi^+\pi^- \ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B^-\to \pi^+\pi^- \ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B^+\to (\pi^+\pi^-)_P \ell^+\nu)\) |
|
|
\(\mathcal{B}(B^-\to \pi^+\pi^- \ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B^-\to \pi^+\pi^- \ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B^-\to \pi^+\pi^- \ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B^+\to (\pi^+\pi^-)_S \ell^+\nu)\) |
|
|
\(\mathcal{B}(B^-\to \pi^+\pi^- \ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B^-\to \pi^+\pi^- \ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B^-\to \pi^+\pi^- \ell^-\bar\nu)\) |
|
|
n/a |
|
|
n/a |
|
The option “l” selects the charged lepton flavor. The option “form-factors” selects the form factor parametrization.
Observables in \(\Lambda_b\to \Lambda_c \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_\mathrm{FB}(\Lambda_b\to\Lambda_c(2595) \ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(\Lambda_b\to\Lambda_c(2595) \ell^-\bar\nu)\) |
|
|
n/a |
|
|
\(R_{\Lambda_c(2595)}\) |
|
|
\(R_{\Lambda_c(2595)}(q^2)\) |
|
|
\(d\mathcal{B}/dq^2(\Lambda_b\to\Lambda_c(2595) \ell^-\bar\nu)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
n/a |
|
|
\(A_\mathrm{FB}(\Lambda_b\to\Lambda_c(2625) \ell^-\bar\nu)\) |
|
|
\(A_\mathrm{FB}(\Lambda_b\to\Lambda_c(2625) \ell^-\bar\nu)(q^2)\) |
|
|
\(\mathcal{B}(\Lambda_b\to\Lambda_c(2625) \ell^-\bar\nu)\) |
|
|
n/a |
|
|
n/a |
|
|
\(R_{\Lambda_c(2625)}\) |
|
|
\(R_{\Lambda_c(2625)}(q^2)\) |
|
|
n/a |
|
|
\(d\mathcal{B}/dq^2(\Lambda_b\to\Lambda_c(2625) \ell^-\bar\nu)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
n/a |
|
|
n/a |
|
|
\(A_{\mathrm{FB}}^{h\ell}(\Lambda_b\to\Lambda_c \ell^-\bar\nu)(q^2)\) |
|
|
n/a |
|
|
\(A_{\mathrm{FB}}^h(\Lambda_b\to\Lambda_c \ell^-\bar\nu)(q^2)\) |
|
|
n/a |
|
|
\(A_{\mathrm{FB}}^\ell(\Lambda_b\to\Lambda_c \ell^-\bar\nu)(q^2)\) |
|
|
\(\mathcal{B}(\Lambda_b\to\Lambda_c \ell^-\bar\nu)\) |
|
|
n/a |
|
|
\(F_0(\Lambda_b\to\Lambda_c \ell^-\bar\nu)(q^2)\) |
|
|
\(K_{1c}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{1cc}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{1ss}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{2c}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{2cc}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{2ss}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{3s}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{3sc}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{4s}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{4sc}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
n/a |
|
|
\(R(A_{\mathrm{FB}}^{\Lambda_c})\) |
|
|
\(R(A_{\mathrm{FB}}^{\Lambda_c})(q^2)\) |
|
|
\(R(\Lambda_c)\) |
|
|
n/a |
|
|
\(d\mathcal{B}(\Lambda_b\to\Lambda_c \ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
The option “l” selects the charged lepton flavor. The option “form-factors” selects the form factor parametrization.
Miscellaneous
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(M_{B^*} - M_B\, \left[ \textrm{GeV} \right]\) |
Class-I Nonleptonic Heavy-to-Heavy Decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(\bar{B}^0\to D^{*+}K^-)\) |
|
|
\(\mathcal{B}(\bar{B}^0\to D^+K^-)\) |
|
|
\(\mathcal{B}(\bar{B}_s^0\to D_s^{*+}\pi^-)\) |
|
|
\(\mathcal{B}(\bar{B}_s^0\to D_s^+\pi^-)\) |
Observables in (semi)leptonic \(c\)-hadron decays
Observables in \(D_q^{(*)+}\to \ell^+\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(D^+ \to \ell^+\nu)\) |
|
|
\(\mathcal{B}(D^{*+} \to \ell^+\nu)\) |
|
|
\(\mathcal{B}(D_s^+ \to \ell^+\nu)\) |
|
|
\(\mathcal{B}(D_s^{*+} \to \ell^+\nu)\) |
The option “l” selects the charged lepton flavor.
Observables in \(D\to K \ell^+ \nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(D\to K\ell^+ \nu)\) |
|
|
\(dP(D\to K\ell^+ \nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(P(D\to K\ell^+ \nu)\) |
|
|
\(d\mathcal{B}(D\to K\ell^+ \nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\Gamma(D\to K\ell^+ \nu)\) |
|
The option “l” selects the charged lepton flavor. The option “q” selects the spectator quark flavor. The option “form-factors” selects the form factor parametrization.
Observables in \(D_q\to\eta^{(\prime)}\ell^+ \nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_{\mathrm{FB}}(D\to\eta'\ell^+ \nu)\) |
|
|
\(\mathcal{B}(D\to\eta'\ell^+ \nu)\) |
|
|
\(dP(D\to\eta'\ell^+ \nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(P(D\to\eta'\ell^+ \nu)\) |
|
|
\(d\mathcal{B}(D\to\eta'\ell^+ \nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\Gamma(D\to\eta'\ell^+ \nu)\) |
|
|
\(A_{\mathrm{FB}}(D\to\eta\ell^+ \nu)\) |
|
|
\(\mathcal{B}(D\to\eta\ell^+ \nu)\) |
|
|
\(dP(D\to\eta\ell^+ \nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(P(D\to\eta\ell^+ \nu)\) |
|
|
\(d\mathcal{B}(D\to\eta\ell^+ \nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\Gamma(D\to\eta\ell^+ \nu)\) |
|
The option “l” selects the charged lepton flavor. The option “q” selects the spectator quark flavor. The option “form-factors” selects the form factor parametrization.
Observables in \(\Lambda_c \to \Lambda \ell^+ \nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(\Lambda_c^+ \to \Lambda \ell^+ \nu)\) |
|
|
\(d\mathcal{B}/dq^2(\Lambda_c^+ \to \Lambda \ell^+ \nu)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
The option “l” selects the charged lepton flavor.
Observables in \(\Lambda_c \to n \ell^+ \nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(\Lambda_c^+ \to n \ell^+ \nu)\) |
|
|
\(d\mathcal{B}/dq^2(\Lambda_c^+ \to n \ell^+ \nu)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
The option “l” selects the charged lepton flavor.
Observables in rare (semi)leptonic and radiative \(b\)-hadron decays
Observables in \(B_q \to \ell^+\ell^-\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{A}_{\Delta\Gamma}(B_q \to \ell^+\ell^-)\) |
|
|
\(\mathcal{B}(B_q \to \ell^+\ell^-)\) |
|
|
\(\left\langle\mathcal{B}(B_q \to \ell^+\ell^-)\right\rangle\) |
|
|
\(\mathcal{S}(B_q \to \ell^+\ell^-)\) |
|
|
\(\langle\tau\rangle(B_q \to \ell^+\ell^-)\) |
The option “l” selects the charged lepton flavor. The option “q” selects the spectator quark flavor.
Observables in \(B_q \to P \psi\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(\bar{B} \to \bar{K}\psi)\) |
|
|
n/a |
The option “q” selects the spectator quark flavor.
Observables in \(B_q \to V \psi\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(\bar{B} \to \bar{K}^*\psi)\) |
|
|
\(S_{1c}(\bar{B} \to \bar{K}^*\psi)\) |
|
|
\(S_{1s}(\bar{B} \to \bar{K}^*\psi)\) |
|
|
\(S_{3}(\bar{B} \to \bar{K}^*\psi)\) |
|
|
\(S_{4}(\bar{B} \to \bar{K}^*\psi)\) |
|
|
\(S_{8}(\bar{B} \to \bar{K}^*\psi)\) |
|
|
\(S_{9}(\bar{B} \to \bar{K}^*\psi)\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(\mathcal{B}(\bar{B}_s \to \phi\psi)\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
The option “q” selects the spectator quark flavor.
Observables in \(B_q \to V \gamma\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_\mathrm{CP}(\bar{B}\to \bar{K}^*\gamma)\) |
|
|
\(A_\mathrm{I}(\bar{B}\to \bar{K}^*\gamma)\) |
|
|
\(\bar{\mathcal{B}}(\bar{B}\to \bar{K}^*\gamma)\) |
|
|
\(\mathcal{B}(\bar{B}\to \bar{K}^*\gamma)\) |
|
|
\(C_{K^*\gamma}\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(S_{K^*\gamma}\) |
The option “l” selects the charged lepton flavor. The option “q” selects the spectator quark flavor.
Observables in \(B_q \to P \ell^+\ell^-\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_\mathrm{CP}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(\bar A_\mathrm{FB}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(A_\mathrm{FB}(\bar{B}\to \bar{K}\ell^+\ell^-)(q^2)\) |
|
|
\(A_\mathrm{FB}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(\bar{\mathcal{B}}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(\mathcal{B}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(\bar F_\mathrm{H}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(F_\mathrm{H}(\bar{B}\to \bar{K}\ell^+\ell^-)(q^2)\) |
|
|
\(F_\mathrm{H}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(\Gamma(\bar{B}\to \bar{K}\ell^+\ell^-)\, \left[ \textrm{GeV} \right]\) |
|
|
n/a |
|
|
\(\mathcal{B}(\bar{B}\to \bar{K}\ell^+\ell^-)/\mathcal{B}(\bar{B}\to \bar{K}J/\psi)\) |
|
|
\(R_K\) |
|
|
\(R_K(q^2)\) |
|
|
n/a |
|
|
\(d\mathcal{B}(\bar{B}\to \bar{K}\ell^+\ell^-)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(d^2\mathcal{\Gamma(\bar{B}\to \bar{K}\ell^+\ell^-)}/(dq^2\, d\cos\theta_\ell)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
The option “l” selects the charged lepton flavor. The option “q” selects the spectator quark flavor.
Observables in \(B_q \to V \ell^+\ell^-\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_{1c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(A_{1s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(A_{2c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(A_{2s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(A_3(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(A_4(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(A_5(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(A_{6c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(A_{6s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(A_7(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(A_8(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(A_9(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(\bar{A}_\mathrm{CP}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(\bar{A}_\mathrm{FB}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(A_\mathrm{FB}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(A_\mathrm{FB}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(A_\mathrm{FB}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(A_\mathrm{FB}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(\bar{A}_T^2(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
n/a |
|
|
n/a |
|
|
\(A_T^3(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
n/a |
|
|
\(A_T^4(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
n/a |
|
|
\(A_T^5(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
n/a |
|
|
\(\mathrm{Im}A_T(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
n/a |
|
|
\(\mathrm{Re}A_T(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
n/a |
|
|
n/a |
|
|
\(\bar{\mathcal{B}}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(\mathcal{B}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(\bar{F}_L(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(F_L(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(F_L(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(\bar{T}_L(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(F_T(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(F_T(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(\Gamma(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(\Gamma^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(H_T^1(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
n/a |
|
|
\(H_T^2(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
n/a |
|
|
\(H_T^3(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
n/a |
|
|
\(H_T^4(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
n/a |
|
|
\(H_T^5(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(J_{1c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_{1c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_{1s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_{1s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_{2c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_{2c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_{2s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_{2s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_3(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_3(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(\bar{J}/\bar{\Gamma}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_3/\Gamma(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_4(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_4(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_5(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_5(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_{6c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_{6c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_{6s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_{6s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_7(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_7(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_8(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_8(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_9(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_9(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(\bar{J}/\bar{\Gamma}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_9/\Gamma(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(\mathcal{N}'_\mathrm{bin}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
n/a |
|
|
\(\mathcal{B}(\bar{B}\to \bar{K}^*\ell^+\ell^-)/\mathcal{B}(\bar{B}\to \bar{K}^*J/\psi)\) |
|
|
\(P'_4(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P'_4(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\({P'_4}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P'_5(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P'_5(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\({P'_5}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P'_6(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P'_6(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\({P'_6}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P'_8(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\({P'_8}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P_1(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P_1^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P_2(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P_2^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P_3(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P_3^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(R_{K^*}\) |
|
|
\(R_{K^*}(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(S_{1c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{1c}^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_{1c}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_{1c}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{1s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{1s}^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_{1s}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_{1s}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{2c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{2c}^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_{2c}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_{2c}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{2s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{2s}^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_{2s}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_{2s}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_3(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_3^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_3^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_3^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_4(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_4^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_4^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_4^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_5(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_5^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_5^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_5^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{6c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{6c}^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_{6c}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_{6c}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{6s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{6s}^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_{6s}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_{6s}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_7(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_7^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_7^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_7^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_8(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_8^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_8^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_8^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_9(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_9^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_9^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_9^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
n/a |
|
|
\(d\mathcal{B}/dq^2(\bar{B}\to \bar{K}^*\ell^+\ell^-)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
n/a |
|
|
n/a |
|
|
\(A_{1c}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(A_{1s}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(A_{2c}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(A_{2s}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(A_3(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(A_4(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(A_5(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(A_{6c}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(A_{6s}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(A_7(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(A_8(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(A_9(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(A_\mathrm{FB}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(A_\mathrm{FB}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(A_\mathrm{FB}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(A_\mathrm{FB}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(\bar{\mathcal{B}}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(\mathcal{B}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(F_L(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(F_L(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(\Gamma(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(\Gamma(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(H_{1c}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(H_{1s}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(H_{2c}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(H_{2s}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
n/a |
|
|
n/a |
|
|
\(J_{1c}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(J_{1c}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(J_{1s}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(J_{1s}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(J_{2c}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(J_{2c}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(J_{2s}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(J_{2s}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(J_3(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(J_3(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(J_4(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(J_4(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(J_5(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(J_5(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(J_{6c}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(J_{6c}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(J_{6s}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(J_{6s}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(J_7(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(J_7(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(J_8(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(J_8(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(J_9(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(J_9(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(\mathcal{B}(\bar{B}_s\to \phi\ell^+\ell^-)/\mathcal{B}(\bar{B}_s\to\phi J/\psi)\) |
|
|
\(\langle\mathcal{B}\rangle(B_s->\phi\ell\ell)/\mathcal{B}(B_s->\phi J/\psi)\) |
|
|
\(R_\phi\) |
|
|
\(R_{\phi}(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(S_{1c}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_{1c}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_{1c}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_{1c}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_{1s}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_{1s}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_{1s}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_{1s}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_{2c}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_{2c}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_{2c}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_{2c}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_{2s}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_{2s}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_{2s}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_{2s}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_3(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_3(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_3^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_3^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_4(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_4(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_4^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_4^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_5(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_5(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_5^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_5^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_{6c}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_{6c}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_{6c}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_{6c}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_{6s}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_{6s}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_{6s}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_{6s}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_7(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_7(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_7^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_7^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_8(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_8(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_8^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_8^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_9(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_9(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_9^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(S_9^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(d\mathcal{B}/dq^2(\bar{B}_s\to \phi\ell^+\ell^-)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
n/a |
|
|
\(\langle\mathcal{B}\rangle(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
The option “l” selects the charged lepton flavor. The option “q” selects the spectator quark flavor.
Observables in \(\Lambda_b \to \Lambda\ell^+\ell^-\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
n/a |
|
|
n/a |
|
|
\(A_\mathrm{FB}^{h,\ell}(\Lambda_b\to\Lambda\ell^+\ell^-)\) |
|
|
\(A_\mathrm{FB}^{h,\ell}(\Lambda_b\to\Lambda\ell^+\ell^-)\) |
|
|
n/a |
|
|
n/a |
|
|
\(A_\mathrm{FB}^h(\Lambda_b\to\Lambda\ell^+\ell^-)\) |
|
|
\(A_\mathrm{FB}^h(\Lambda_b\to\Lambda\ell^+\ell^-)\) |
|
|
n/a |
|
|
n/a |
|
|
\(A_\mathrm{FB}^\ell(\Lambda_b\to\Lambda\ell^+\ell^-)\) |
|
|
\(A_\mathrm{FB}^\ell(\Lambda_b\to\Lambda\ell^+\ell^-)\) |
|
|
\(\mathcal{B}(\Lambda_b\to\Lambda\ell^+\ell^-)\) |
|
|
\(\mathcal{B}(\Lambda_b\to\Lambda\ell^+\ell^-)\) |
|
|
n/a |
|
|
n/a |
|
|
\(F_0(\Lambda_b\to\Lambda\ell^+\ell^-)\) |
|
|
\(F_0(\Lambda_b\to\Lambda\ell^+\ell^-)\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(M_{10}\) |
|
|
\(M_{11}\) |
|
|
\(M_{12}\) |
|
|
\(M_{13}\) |
|
|
\(M_{14}\) |
|
|
\(M_{15}\) |
|
|
\(M_{16}\) |
|
|
\(M_{17}\) |
|
|
\(M_{18}\) |
|
|
\(M_{19}\) |
|
|
\(M_1\) |
|
|
\(M_{20}\) |
|
|
\(M_{21}\) |
|
|
\(M_{22}\) |
|
|
\(M_{23}\) |
|
|
\(M_{24}\) |
|
|
\(M_{25}\) |
|
|
\(M_{26}\) |
|
|
\(M_{27}\) |
|
|
\(M_{28}\) |
|
|
\(M_{29}\) |
|
|
\(M_2\) |
|
|
\(M_{30}\) |
|
|
\(M_{31}\) |
|
|
\(M_{32}\) |
|
|
\(M_{33}\) |
|
|
\(M_{34}\) |
|
|
\(M_3\) |
|
|
\(M_4\) |
|
|
\(M_5\) |
|
|
\(M_6\) |
|
|
\(M_7\) |
|
|
\(M_8\) |
|
|
\(M_9\) |
|
|
\(R_{\Lambda}\) |
|
|
\(d\mathcal{B}(\Lambda_b\to\Lambda\ell^+\ell^-)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(d\mathcal{B}(\Lambda_b\to\Lambda\ell^+\ell^-)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
The option “l” selects the charged lepton flavor.
Observables in \(\Lambda_b \to \Lambda(1520))\ell^+\ell^-\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_\mathrm{FB}^\ell(\bar{\Lambda}_b\to\bar{\Lambda}(1520)\ell^+\ell^-)\) |
|
|
n/a |
|
|
\(\mathcal{B}(\bar{\Lambda}_b\to\bar{\Lambda}(1520)\ell^+\ell^-)\) |
|
|
\(\Gamma(\bar{\Lambda}_b\to\bar{\Lambda}(1520)\ell^+\ell^-)\) |
|
|
\(\Gamma(\bar{\Lambda}_b\to\bar{\Lambda}(1520)\ell^+\ell^-)(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(L_{1cc}(\bar{\Lambda}_b\to\bar{\Lambda}(1520)\ell^+\ell^-)\) |
|
|
\(L_{1cc}(\bar{\Lambda}_b\to\bar{\Lambda}(1520)\ell^+\ell^-)(q^2)\) |
|
|
\(S_{1cc}(\Lambda_b\to\Lambda(1520)\ell^+\ell^-)\) |
|
|
\(S_{1cc}(\Lambda_b\to\Lambda(1520)\ell^+\ell^-)(q^2)\) |
|
|
\(d\mathcal{B}(\bar{\Lambda}_b\to\bar{\Lambda}(1520)\ell^+\ell^-)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
The option “l” selects the charged lepton flavor.
Observables in \(\Lambda_b \to \Lambda(1520)) \gamma\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(\Lambda_b\to\Lambda(1520)\gamma)\) |
Observables in \(B \to X_s \lbrace \gamma, \ell^+\ell^-\rbrace\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
The option “l” selects the charged lepton flavor. The option “q” selects the spectator quark flavor.
Observables in \(B\to K \nu\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(\bar{B}\to \bar{K}\nu\bar\nu)\) |
|
|
n/a |
|
|
n/a |
|
|
\(d\mathcal{B}(\bar{B}\to \bar{K}\nu\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
Observables in \(B_s\to \eta \nu\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(\bar{B}_s\to\bar{\eta_prime}\nu\bar\nu)\) |
|
|
\(d\mathcal{B}(\bar{B}_s\to\bar{\eta_prime}\nu\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\mathcal{B}(\bar{B}_s\to\bar{\eta}\nu\bar\nu)\) |
|
|
\(d\mathcal{B}(\bar{B}_s\to\bar{\eta}\nu\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
Observables in \(B\to K^* \nu\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(\bar{B}\to \bar{K}^*\nu\bar\nu)\) |
|
|
\(F_L(\bar{B}\to \bar{K}^*\nu\bar\nu)\) |
|
|
\(F_L(\bar{B}\to \bar{K}^*\nu\bar\nu)(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(d\mathcal{B}(\bar{B}\to \bar{K}^*\nu\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
Observables in \(B_s\to\phi\nu\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(\bar{B}_s\to\phi\nu\bar\nu)\) |
|
|
\(F_L(\bar{B}_s\to\phi\nu\bar\nu)\) |
|
|
\(F_L(\bar{B}_s\to\phi\nu\bar\nu)(q^2)\) |
|
|
\(d\mathcal{B}(\bar{B}_s\to\phi\nu\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
Observables in \(\Lambda_b\to\Lambda\nu\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(\bar{\Lambda}_b\to\Lambda\nu\bar\nu)\) |
|
|
\(F_L(\bar{\Lambda}_b\to\Lambda\nu\bar\nu)\) |
|
|
\(F_L(\bar{\Lambda}_b\to\Lambda\nu\bar\nu)(q^2)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(d\mathcal{B}(\bar{\Lambda}_b\to\Lambda\nu\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
Observables in rare \(c\)-hadron decays
Observables in \(\Lambda_c \to p \ell^+ \ell^-\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\langle A_{\mathrm{FB}}^\ell(\Lambda_c^+ \to p \ell^+ \ell^-)\rangle\) |
|
|
\(A_{\mathrm{FB}}^\ell(q^2)(\Lambda_c^+ \to p \ell^+ \ell^-)\) |
|
|
\(\Gamma \cdot \langle A_{\mathrm{FB}}^\ell(\Lambda_c^+ \to p \ell^+ \ell^-)\rangle\, \left[ \textrm{GeV} \right]\) |
|
|
\(\mathcal{B}(\Lambda_c^+ \to p \ell^+ \ell^-)\) |
|
|
\(\Delta\langle A_{\mathrm{FB}}^\ell(\Lambda_c^+ \to p \ell^+ \ell^-)\rangle\) |
|
|
\(\langle F_{\mathrm{L}}(\Lambda_c^+ \to p \ell^+ \ell^-)\rangle\) |
|
|
\(F_{\mathrm{L}}(q^2)(\Lambda_c^+ \to p \ell^+ \ell^-)\) |
|
|
\(\Gamma \cdot \langle F_{\mathrm{L}}(\Lambda_c^+ \to p \ell^+ \ell^-)\rangle\, \left[ \textrm{GeV} \right]\) |
|
|
\(\Gamma(\Lambda_c^+ \to p \ell^+ \ell^-)\, \left[ \textrm{GeV} \right]\) |
|
|
\(\Sigma\langle A_{\mathrm{FB}}^\ell(\Lambda_c^+ \to p \ell^+ \ell^-)\rangle\) |
|
|
\(d\mathcal{B}(\Lambda_c^+ \to p \ell^+ \ell^-)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(d^2\Gamma(\Lambda_c^+ \to p \ell^+ \ell^-)/dq^2 d\cos(\theta_\ell)\, \left[ \textrm{GeV}^{-1} \right]\) |
|
- The option “l” selects the charged lepton flavor. The option
“cp-conjugate” selects between the decay and its CP-conjugate. The option “model” selects the model for the Wilson coefficients. The option “form-factors” selects the form factor parameterization.
Observables in neutral meson mixing
Observables in \(B_s\)–\(\bar{B}_s\) mixing
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\Delta M_s(B_s\leftrightarrow \bar{B}_s)\, \left[ \textrm{ps}^{-1} \right]\) |
Pseudo-observables in nonleptonic amplitudes
Pseudo-observables for the non-local form factors
Observables in \(B_q \to P\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(|\mathcal{H}_0^{B \to K}(q^2)|\) |
|
|
\(|\hat{\mathcal{H}}_0^{B \to K}(q^2)|\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(\mathrm{Im}\mathcal{H}_0^{B \to K}(q^2)\) |
|
|
\(\mathrm{Im}\hat{\mathcal{H}}_0^{B \to K}(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(\mathrm{Re}\mathcal{H}_0^{B \to K}(q^2)\) |
|
|
\(\mathrm{Re}\hat{\mathcal{H}}_0^{B \to K}(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
The option “q” selects the spectator quark flavor.
Observables in \(B_q \to V\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(|\mathcal{H}_0^{B \to K^*}(q^2)|\) |
|
|
\(|\mathcal{H}_\parallel^{B \to K^*}(q^2)|\) |
|
|
\(|\mathcal{H}_\perp^{B \to K^*}(q^2)|\) |
|
|
\(|\hat{\mathcal{H}}_0^{B \to K^*}(q^2)|\) |
|
|
\(|\hat{\mathcal{H}}_\parallel^{B \to K^*}(q^2)|\) |
|
|
\(|\hat{\mathcal{H}}_\perp^{B \to K^*}(q^2)|\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(\mathrm{Im}\mathcal{H}_0^{B \to K^*}(q^2)\) |
|
|
\(\mathrm{Im}\mathcal{H}_\parallel^{B \to K^*}(q^2)\) |
|
|
\(\mathrm{Im}\mathcal{H}_\perp^{B \to K^*}(q^2)\) |
|
|
\(\mathrm{Im}\hat{\mathcal{H}}_0^{B \to K^*}(q^2)\) |
|
|
\(\mathrm{Im}\hat{\mathcal{H}}_\parallel^{B \to K^*}(q^2)\) |
|
|
\(\mathrm{Im}\hat{\mathcal{H}}_\perp^{B \to K^*}(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(\mathrm{Re}\mathcal{H}_0^{B \to K^*}(q^2)\) |
|
|
\(\mathrm{Re}\mathcal{H}_\parallel^{B \to K^*}(q^2)\) |
|
|
\(\mathrm{Re}\mathcal{H}_\perp^{B \to K^*}(q^2)\) |
|
|
\(\mathrm{Re}\hat{\mathcal{H}}_0^{B \to K^*}(q^2)\) |
|
|
\(\mathrm{Re}\hat{\mathcal{H}}_\parallel^{B \to K^*}(q^2)\) |
|
|
\(\mathrm{Re}\hat{\mathcal{H}}_\perp^{B \to K^*}(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(|\mathcal{H}_0^{B_s \to \phi}(q^2)|\) |
|
|
\(|\mathcal{H}_\parallel^{B_s \to \phi}(q^2)|\) |
|
|
\(|\mathcal{H}_\perp^{B_s \to \phi}(q^2)|\) |
|
|
\(|\hat{\mathcal{H}}_0^{B_s \to \phi}(q^2)|\) |
|
|
\(|\hat{\mathcal{H}}_\parallel^{B_s \to \phi}(q^2)|\) |
|
|
\(|\hat{\mathcal{H}}_\perp^{B_s \to \phi}(q^2)|\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(\mathrm{Im}\mathcal{H}_0^{B_s \to \phi}(q^2)\) |
|
|
\(\mathrm{Im}\mathcal{H}_\parallel^{B_s \to \phi}(q^2)\) |
|
|
\(\mathrm{Im}\mathcal{H}_\perp^{B_s \to \phi}(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(\mathrm{Re}\mathcal{H}_0^{B_s \to \phi}(q^2)\) |
|
|
\(\mathrm{Re}\mathcal{H}_\parallel^{B_s \to \phi}(q^2)\) |
|
|
\(\mathrm{Re}\mathcal{H}_\perp^{B_s \to \phi}(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
The option “q” selects the spectator quark flavor.
Pseudo-observables for Non-local Matrix Elements
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
Form factors
Form factors for \(B\to \pi\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_T5]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(f_+^{'',B\to\pi}(q^2)\) |
|
|
\(f_+^{',B\to\pi}(q^2)\) |
|
|
\(f_+^{B\to\pi}(q^2)\) |
|
|
n/a |
|
|
\(f_-^{B\to\pi}(q^2)\) |
|
|
\(f_0^{B\to\pi}(q^2)\) |
|
|
\(f_0(q^2)/f_+(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(f_T^{B\to\pi}(q^2)\) |
|
|
n/a |
|
Pseudo observables representing the full basis of \(B\to \pi\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(B\to \eta\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_{T5}]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(f_+^{B\to\eta}(q^2)\) |
|
|
\(f_0^{B\to\eta}(q^2)\) |
|
|
\(f_T^{B\to\eta}(q^2)\) |
|
|
\(f_+^{B\to\eta'}(q^2)\) |
|
|
\(f_0^{B\to\eta'}(q^2)\) |
|
|
\(f_T^{B\to\eta'}(q^2)\) |
|
Pseudo observables representing the full basis of \(B\to \eta\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(B\to K\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(F_T(q^2)/F_+(q^2)\) |
|
|
\(F_+^{B\to K}(q^2)\) |
|
|
\(F_T^{B\to K}(q^2)\) |
|
|
\(F_{+,T}(q^2)/F_+(q^2)\) |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_{T5}]\) |
|
|
\(\textrm{Saturation}[1^+_T5]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(f_+^{B\to K}(q^2)\) |
|
|
n/a |
|
|
\(\hat{f}_+^{B\to K}(q^2)\) |
|
|
\(\hat{f}_+^{\prime B\to K}(q^2)\) |
|
|
\(f_-^{B\to K}(q^2)\) |
|
|
\(f_0^{B\to K}(q^2)\) |
|
|
n/a |
|
|
\(\hat{f}_0^{B\to K}(q^2)\) |
|
|
\(\hat{f}_0^{\prime B\to K}(q^2)\) |
|
|
\(f_T^{B\to K}(q^2)\) |
|
|
n/a |
|
|
\(\hat{f}_T^{B\to K}(q^2)\) |
|
|
\(\hat{f}_T^{\prime B\to K}(q^2)\) |
|
Pseudo observables representing the full basis of \(B\to K\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(B_s\to \eta^{(\prime)}\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(f_+^{B_s\to\eta}(q^2)\) |
|
|
\(f_0^{B_s\to\eta}(q^2)\) |
|
|
\(f_T^{B_s\to\eta}(q^2)\) |
|
|
\(f_+^{B_s\to\eta'}(q^2)\) |
|
|
\(f_0^{B_s\to\eta'}(q^2)\) |
|
|
\(f_T^{B_s\to\eta'}(q^2)\) |
|
Pseudo observables representing the full basis of \(B_s\to \eta^{(\prime)}\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(B_s\to \bar{K}\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_{T5}]\) |
|
|
\(\textrm{Saturation}[1^+_T5]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(f_+^{B_s\to \bar{K}}(q^2)\) |
|
|
n/a |
|
|
\(f_-^{B_s\to \bar{K}}(q^2)\) |
|
|
\(f_0^{B_s\to \bar{K}}(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(f_T^{B_s\to \bar{K}}(q^2)\) |
|
|
n/a |
|
Pseudo observables representing the full basis of \(B_s\to \bar{K}\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(B_s\to \bar{D_s}\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(f_0(q^2_\mathrm{num})/f_+(q^2_\mathrm{denom})\) |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_{T5}]\) |
|
|
\(\textrm{Saturation}[1^+_T5]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(a_0^{S_1}\) |
|
|
\(a_0^{V_1}\) |
|
|
\(a_0^{f_T}\) |
|
|
\(a_1^{S_1}/a_0^{S_1}\) |
|
|
\(a_1^{V_1}/a_0^{V_1}\) |
|
|
\(a_1^{f_T}/a_0^{f_T}\) |
|
|
\(a_1^{S_1}\) |
|
|
\(a_1^{V_1}\) |
|
|
\(a_1^{f_T}\) |
|
|
\(a_2^{S_1}/a_0^{S_1}\) |
|
|
\(a_2^{V_1}/a_0^{V_1}\) |
|
|
\(a_2^{f_T}/a_0^{f_T}\) |
|
|
\(a_2^{S_1}\) |
|
|
\(a_2^{V_1}\) |
|
|
\(a_2^{f_T}\) |
|
|
\(f_+^{B_s\to \bar{D}_s}(q^2)\) |
|
|
n/a |
|
|
\(f_-^{B_s\to \bar{D}_s}(q^2)\) |
|
|
\(f_0^{B_s\to \bar{D}_s}(q^2)\) |
|
|
n/a |
|
|
\(f_T^{B_s\to \bar{D}_s}(q^2)\) |
|
|
\(f_T(q^2)/f_+(q^2)\) |
|
|
n/a |
|
Pseudo observables representing the full basis of \(B_s\to\bar{D}_s\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(B \to \gamma^*\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\text{Abs}\,F_1^{B\to \gamma^*}(q^2,k^2)\) |
|
|
\(\text{Abs}\,F_2^{B\to \gamma^*}(q^2,k^2)\) |
|
|
\(\text{Abs}\,F_3^{B\to \gamma^*}(q^2,k^2)\) |
|
|
\(\text{Abs}\,F_4^{B\to \gamma^*}(q^2,k^2)\) |
|
|
\(\text{Arg}\,F_1^{B\to \gamma^*}(q^2,k^2)\) |
|
|
\(\text{Arg}\,F_2^{B\to \gamma^*}(q^2,k^2)\) |
|
|
\(\text{Arg}\,F_3^{B\to \gamma^*}(q^2,k^2)\) |
|
|
\(\text{Arg}\,F_4^{B\to \gamma^*}(q^2,k^2)\) |
|
Pseudo observables representing the \(B \to \gamma^*\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(B\to \gamma\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(F_A^{B\to \gamma}(E_\gamma)\) |
|
|
\(F_V^{B\to \gamma}(E_\gamma)\) |
|
Pseudo observables representing the full basis of \(B\to \gamma\) form factors. The FLvD2022QCDF form factors implement [BBJW:2018A], Eq. (5.1). Option lcda-model selects the model of the \(B\)-meson LCDAs, FLvD2022 (default), FLvD2022+profile, or exponential; they differ by more than RG evolution, since their three-particle LCDAs differ. FLvD2022+profile uses the same \(\phi_+\) as FLvD2022 but models the three-particle LCDAs from it by the profile-function ansatz of [BBJW:2018A], so its twist-3,4 soft term carries an unquantifiable modelling error and violates the ansatz’s own equation-of-motion relation away from a codimension-one surface in coefficient space; it is a separate model, not a completion of FLvD2022. Option contributions selects the terms of Eq. (5.1), one value per term plus two composites: none, ht, soft-nlo, soft-tw-3+4, soft-tw-5+6, soft (the three soft terms), and all (default). The twist-3,4 soft term requires the three-particle LCDAs, which [FLvD:2022A] does not parametrise, so naming it explicitly under FLvD2022 is rejected, while soft and all deliver what the selected model supports and therefore mean one term less under FLvD2022. The twist-5,6 soft term needs only \(\phi_-^{WW}\) and \(1/\lambda_B\) and is available for all models. Option evolution-order accepts NLL (default) and LL. EOS reproduces every published equation of [BBJW:2018A] that can be checked in isolation. Compared against the curves of their Fig. 7 (lower) at their own inputs — Table 1, \(\hat\sigma_1 = 0\), LCDA defined at \(\mu_0 = 1\,\text{GeV}\) and evolved to \(\mu = 1.5\,\text{GeV}\) — FLvD2022+profile, the only model here carrying both that evolution and all four terms of Eq. (5.1), gives an \(F_V\) that is 2.6-3.0% low for \(\lambda_B = 0.20\ldots0.50\,\text{GeV}\), near-uniformly in \(E_\gamma\); almost all of that residual sits in the leading-power term rather than in the soft corrections. exponential instead lies 9-15% high, because it omits the RG evolution that [BBJW:2018A] apply.
Form factors for \(B\to \omega\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_0^{B\to \omega}(q^2)\) |
|
|
\(A_1^{B\to \omega}(q^2)\) |
|
|
\(A_{12}^{B\to \omega}(q^2)\) |
|
|
\(A_2^{B\to \omega}(q^2)\) |
|
|
\(T_1^{B\to \omega}(q^2)\) |
|
|
\(T_2^{B\to \omega}(q^2)\) |
|
|
\(T_{23}^{B\to \omega}(q^2)\) |
|
|
\(T_3^{B\to \omega}(q^2)\) |
|
|
\(V^{B\to \omega}(q^2)\) |
|
Pseudo observables representing the full basis of \(B\to \omega\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(B\to \rho\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_0^{B\to \rho}(q^2)\) |
|
|
\(A_1^{B\to \rho}(q^2)\) |
|
|
\(A_{12}^{B\to \rho}(q^2)\) |
|
|
\(A_{12}(q^2)/A_1(q^2)\) |
|
|
n/a |
|
|
\(A_2^{B\to \rho}(q^2)\) |
|
|
\(A_2(q^2)/A_1(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(T_1^{B\to \rho}(q^2)\) |
|
|
n/a |
|
|
\(T_2^{B\to \rho}(q^2)\) |
|
|
\(T_{23}^{B\to \rho}(q^2)\) |
|
|
\(T_{23}(q^2)/T_2(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(T_3^{B\to \rho}(q^2)\) |
|
|
\(V^{B\to \rho}(q^2)\) |
|
|
\(V(q^2)/A_1(q^2)\) |
|
|
n/a |
|
Pseudo observables representing the full basis of \(B\to \rho\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(B\to K^*\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_0^{B\to K^*}(q^2)\) |
|
|
\(A_1^{B\to K^*}(q^2)\) |
|
|
\(A_{12}^{B\to K^*}(q^2)\) |
|
|
\(A_{12}(q^2)/A_1(q^2)\) |
|
|
n/a |
|
|
\(A_2^{B\to K^*}(q^2)\) |
|
|
\(A_2(q^2)/A_1(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(\mathcal{F}_0^{B\to K^*}(q^2)\) |
|
|
\(\mathcal{F}_{0,T}^{B\to K^*}(q^2)\) |
|
|
\(\mathcal{F}_{0,T}(q^2)/\mathcal{F}_0(q^2)\) |
|
|
\(\mathcal{F}_\parallel^{B\to K^*}(q^2)\) |
|
|
\(\mathcal{F}_{\parallel,T}^{B\to K^*}(q^2)\) |
|
|
\(\mathcal{F}_{\parallel,T}(q^2)/\mathcal{F}_\parallel(q^2)\) |
|
|
\(\mathcal{F}_\perp^{B\to K^*}(q^2)\) |
|
|
\(\mathcal{F}_{\perp,T}^{B\to K^*}(q^2)\) |
|
|
\(\mathcal{F}_{\perp,T}(q^2)/\mathcal{F}_\perp(q^2)\) |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_{T5}]\) |
|
|
\(\textrm{Saturation}[1^+_T5]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(T_1^{B\to K^*}(q^2)\) |
|
|
n/a |
|
|
\(T_2^{B\to K^*}(q^2)\) |
|
|
\(T_{23}^{B\to K^*}(q^2)\) |
|
|
\(T_{23}(q^2)/T_2(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(T_3^{B\to K^*}(q^2)\) |
|
|
\(V^{B\to K^*}(q^2)\) |
|
|
\(V(q^2)/A_1(q^2)\) |
|
|
n/a |
|
Pseudo observables representing the full basis of \(B\to K^*\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(B\to \bar{D}^*\) transitions and related pseudo-observables
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_0^{B\to D^*}(q^2)\) |
|
|
\(A_1^{B\to D^*}(q^2)\) |
|
|
\(A_{12}^{B\to D^*}(q^2)\) |
|
|
\(A_{12}(q^2)/A_1(q^2)\) |
|
|
n/a |
|
|
\(A_2^{B\to D^*}(q^2)\) |
|
|
\(A_2(q^2)/A_1(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_{T5}]\) |
|
|
\(\textrm{Saturation}[1^+_T5]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(T_1^{B\to D^*}(q^2)\) |
|
|
n/a |
|
|
\(T_2^{B\to D^*}(q^2)\) |
|
|
\(T_{23}^{B\to D^*}(q^2)\) |
|
|
\(T_{23}(q^2)/T_2(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(T_3^{B\to D^*}(q^2)\) |
|
|
\(V^{B\to D^*}(q^2)\) |
|
|
\(V(q^2)/A_1(q^2)\) |
|
|
n/a |
|
|
\(a_0^{A_1}\) |
|
|
\(a_0^{A_5}\) |
|
|
\(a_0^{F_1}\) |
|
|
\(a_0^{F_2}\) |
|
|
\(a_0^{P_1}\) |
|
|
\(a_0^{T_1}\) |
|
|
\(a_0^{T_{23}}\) |
|
|
\(a_0^{T_{23}}\) |
|
|
\(a_0^{T_2}\) |
|
|
\(a_0^{T_2}\) |
|
|
\(a_0^{V_4}\) |
|
|
\(a_1^{A_1}/a_0^{A_1}\) |
|
|
\(a_1^{A_5}/a_0^{A_5}\) |
|
|
\(a_1^{P_1}/a_0^{P_1}\) |
|
|
\(a_1^{T_1}/a_0^{T_1}\) |
|
|
\(a_1^{T_{23}}/a_0^{T_{23}}\) |
|
|
\(a_1^{T_2}/a_0^{T_2}\) |
|
|
\(a_1^{V_4}/a_0^{V_4}\) |
|
|
\(a_1^{A_1}\) |
|
|
\(a_1^{A_5}\) |
|
|
\(a_1^{P_1}\) |
|
|
\(a_1^{T_1}\) |
|
|
\(a_1^{T_{23}}\) |
|
|
\(a_1^{T_2}\) |
|
|
\(a_1^{V_4}\) |
|
|
\(a_2^{A_1}/a_0^{A_1}\) |
|
|
\(a_2^{A_5}/a_0^{A_5}\) |
|
|
\(a_2^{P_1}/a_0^{P_1}\) |
|
|
\(a_2^{T_1}/a_0^{T_1}\) |
|
|
\(a_2^{T_{23}}/a_0^{T_{23}}\) |
|
|
\(a_2^{T_2}/a_0^{T_2}\) |
|
|
\(a_2^{V_4}/a_0^{V_4}\) |
|
|
\(a_2^{A_1}\) |
|
|
\(a_2^{A_5}\) |
|
|
\(a_2^{P_1}\) |
|
|
\(a_2^{T_1}\) |
|
|
\(a_2^{T_{23}}\) |
|
|
\(a_2^{T_2}\) |
|
|
\(a_2^{V_4}\) |
|
|
\(h_{A_1}^{\bar{B}\to D^*}(q^2)\) |
|
|
\(h_{A_2}^{\bar{B}\to D^*}(q^2)\) |
|
|
\(h_{A_3}^{\bar{B}\to D^*}(q^2)\) |
|
|
\(h_{T_1}^{\bar{B}\to D^*}(q^2)\) |
|
|
\(h_{T_2}^{\bar{B}\to D^*}(q^2)\) |
|
|
\(h_{T_3}^{\bar{B}\to D^*}(q^2)\) |
|
|
\(h_V^{\bar{B}\to D^*}(q^2)\) |
|
Pseudo observables representing the full basis of \(B\to \bar{D}^*\) form factors. For most pseudo-observables, the specific parametrization can be chosen via the “form-factors” option.
Form factors for \(B_c\to J/\psi\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_0^{B_c\to J/\psi}(q^2)\) |
|
|
\(A_1^{B_c\to J/\psi}(q^2)\) |
|
|
\(A_{12}^{B_c\to J/\psi}(q^2)\) |
|
|
\(A_2^{B_c\to J/\psi}(q^2)\) |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_{T5}]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(T_1^{B_c\to J/\psi}(q^2)\) |
|
|
\(T_2^{B_c\to J/\psi}(q^2)\) |
|
|
\(T_{23}^{B_c\to J/\psi}(q^2)\) |
|
|
\(T_3^{B_c\to J/\psi}(q^2)\) |
|
|
\(V^{B_c\to J/\psi}(q^2)\) |
|
Pseudo observables representing the full basis of \(B_c\to J/\psi\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(B_s\to \bar{K}^*\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_0^{B_s\to \bar{K}^*}(q^2)\) |
|
|
\(A_1^{B_s\to \bar{K}^*}(q^2)\) |
|
|
\(A_{12}^{B_s\to \bar{K}^*}(q^2)\) |
|
|
\(A_{12}(q^2)/A_1(q^2)\) |
|
|
n/a |
|
|
\(A_2^{B_s\to \bar{K}^*}(q^2)\) |
|
|
\(A_2(q^2)/A_1(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_T5]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(T_1^{B_s\to \bar{K}^*}(q^2)\) |
|
|
n/a |
|
|
\(T_2^{B_s\to \bar{K}^*}(q^2)\) |
|
|
\(T_{23}^{B_s\to \bar{K}^*}(q^2)\) |
|
|
\(T_{23}(q^2)/T_2(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(T_3^{B_s\to \bar{K}^*}(q^2)\) |
|
|
\(V^{B_s\to \bar{K}^*}(q^2)\) |
|
|
\(V(q^2)/A_1(q^2)\) |
|
|
n/a |
|
Pseudo observables representing the full basis of \(B_s\to \bar{K}^*\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(B_s\to \phi\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_0^{B_s\to \phi}(q^2)\) |
|
|
\(A_1^{B_s\to \phi}(q^2)\) |
|
|
\(A_{12}^{B_s\to \phi}(q^2)\) |
|
|
\(A_{12}(q^2)/A_1(q^2)\) |
|
|
n/a |
|
|
\(A_2^{B_s\to \phi}(q^2)\) |
|
|
\(A_2(q^2)/A_1(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(\mathcal{F}_0^{B_s\to \phi}(q^2)\) |
|
|
\(\mathcal{F}_{0,T}^{B_s\to \phi}(q^2)\) |
|
|
\(\mathcal{F}_{0,T}(q^2)/\mathcal{F}_0(q^2)\) |
|
|
\(\mathcal{F}_\parallel^{B_s\to \phi}(q^2)\) |
|
|
\(\mathcal{F}_{\parallel,T}^{B_s\to \phi}(q^2)\) |
|
|
\(\mathcal{F}_{\parallel,T}(q^2)/\mathcal{F}_\parallel(q^2)\) |
|
|
\(\mathcal{F}_\perp^{B_s\to \phi}(q^2)\) |
|
|
\(\mathcal{F}_{\perp,T}^{B_s\to \phi}(q^2)\) |
|
|
\(\mathcal{F}_{\perp,T}(q^2)/\mathcal{F}_\perp(q^2)\) |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_{T5}]\) |
|
|
\(\textrm{Saturation}[1^+_T5]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(T_1^{B_s\to \phi}(q^2)\) |
|
|
n/a |
|
|
\(T_2^{B_s\to \phi}(q^2)\) |
|
|
\(T_{23}^{B_s\to \phi}(q^2)\) |
|
|
\(T_{23}(q^2)/T_2(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(T_3^{B_s\to \phi}(q^2)\) |
|
|
\(V^{B_s\to \phi}(q^2)\) |
|
|
\(V(q^2)/A_1(q^2)\) |
|
|
n/a |
|
Pseudo observables representing the full basis of \(B_s\to \phi\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(B_s\to \bar{D}_s^*\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_0^{B_s\to D_s^*}(q^2)\) |
|
|
\(A_1^{B_s\to D_s^*}(q^2)\) |
|
|
\(A_{12}^{B_s\to D_s^*}(q^2)\) |
|
|
\(A_{12}(q^2)/A_1(q^2)\) |
|
|
n/a |
|
|
\(A_2^{B_s\to D_s^*}(q^2)\) |
|
|
\(A_2(q^2)/A_1(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_{T5}]\) |
|
|
\(\textrm{Saturation}[1^+_T5]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(T_1^{B_s\to D_s^*}(q^2)\) |
|
|
n/a |
|
|
\(T_2^{B_s\to D_s^*}(q^2)\) |
|
|
\(T_{23}^{B_s\to D_s^*}(q^2)\) |
|
|
\(T_{23}(q^2)/T_2(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(T_3^{B_s\to D_s^*}(q^2)\) |
|
|
\(V^{B_s\to D_s^*}(q^2)\) |
|
|
\(V(q^2)/A_1(q^2)\) |
|
|
n/a |
|
|
\(a_0^{A_1}\) |
|
|
\(a_0^{A_5}\) |
|
|
\(a_0^{P_1}\) |
|
|
\(a_0^{T_1}\) |
|
|
\(a_0^{T_{23}}\) |
|
|
\(a_0^{T_2}\) |
|
|
\(a_0^{V_4}\) |
|
|
\(a_1^{A_1}/a_0^{A_1}\) |
|
|
\(a_1^{A_5}/a_0^{A_5}\) |
|
|
\(a_1^{P_1}/a_0^{P_1}\) |
|
|
\(a_1^{T_1}/a_0^{T_1}\) |
|
|
\(a_1^{T_{23}}/a_0^{T_{23}}\) |
|
|
\(a_1^{T_2}/a_0^{T_2}\) |
|
|
\(a_1^{V_4}/a_0^{V_4}\) |
|
|
\(a_1^{A_1}\) |
|
|
\(a_1^{A_5}\) |
|
|
\(a_1^{P_1}\) |
|
|
\(a_1^{T_1}\) |
|
|
\(a_1^{T_{23}}\) |
|
|
\(a_1^{T_2}\) |
|
|
\(a_1^{V_4}\) |
|
|
\(a_2^{A_1}/a_0^{A_1}\) |
|
|
\(a_2^{A_5}/a_0^{A_5}\) |
|
|
\(a_2^{P_1}/a_0^{P_1}\) |
|
|
\(a_2^{T_1}/a_0^{T_1}\) |
|
|
\(a_2^{T_{23}}/a_0^{T_{23}}\) |
|
|
\(a_2^{T_2}/a_0^{T_2}\) |
|
|
\(a_2^{V_4}/a_0^{V_4}\) |
|
|
\(a_2^{A_1}\) |
|
|
\(a_2^{A_5}\) |
|
|
\(a_2^{P_1}\) |
|
|
\(a_2^{T_1}\) |
|
|
\(a_2^{T_{23}}\) |
|
|
\(a_2^{T_2}\) |
|
|
\(a_2^{V_4}\) |
|
|
\(h_{A_1}^{\bar{B}_s\to D_s^*}(q^2)\) |
|
|
\(h_{A_2}^{\bar{B}_s\to D_s^*}(q^2)\) |
|
|
\(h_{A_3}^{\bar{B}_s\to D_s^*}(q^2)\) |
|
|
\(h_{T_1}^{\bar{B}_s\to D_s^*}(q^2)\) |
|
|
\(h_{T_2}^{\bar{B}_s\to D_s^*}(q^2)\) |
|
|
\(h_{T_3}^{\bar{B}_s\to D_s^*}(q^2)\) |
|
|
\(h_V^{\bar{B}_s\to D_s^*}(q^2)\) |
|
Pseudo observables representing the full basis of \(B_s\to \bar{D}_s^*\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(B \to \pi \pi\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathrm{Im}\,F_0^{B\to \pi\pi}(q^2,k^2,z)\) |
|
|
\(\mathrm{Im}\,F_\parallel^{B\to \pi\pi}(q^2,k^2,z)\) |
|
|
\(\mathrm{Im}\,F_\perp^{B\to \pi\pi}(q^2,k^2,z)\) |
|
|
\(\mathrm{Im}\,F_t^{B\to \pi\pi}(q^2,k^2,z)\) |
|
|
\(\mathrm{Res}\,\mathrm{Im}\,F_0^{B\to \pi\pi}(q^2,k^2,z)\) |
|
|
\(\mathrm{Res}\,\mathrm{Im}\,F_0^{B\to \pi\pi}(q^2,k^2,z)\) |
|
|
\(\mathrm{Res}\,\mathrm{Im}\,F_\parallel^{B\to \pi\pi}(q^2,k^2,z)\) |
|
|
\(\mathrm{Res}\,\mathrm{Im}\,F_\parallel^{B\to \pi\pi}(q^2,k^2,z)\) |
|
|
\(\mathrm{Res}\,\mathrm{Im}\,F_\perp^{B\to \pi\pi}(q^2,k^2,z)\) |
|
|
\(\mathrm{Res}\,\mathrm{Im}\,F_\perp^{B\to \pi\pi}(q^2,k^2,z)\) |
|
|
\(\mathrm{Res}\,\mathrm{Im}\,F_t^{B\to \pi\pi}(q^2,k^2,z)\) |
|
|
\(\mathrm{Res}\,\mathrm{Im}\,F_t^{B\to \pi\pi}(q^2,k^2,z)\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
Pseudo observables representing the \(B \to \pi \pi\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(\Lambda_b \to \Lambda\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_{T_5}]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(f_0^{A,\Lambda_b\to\Lambda}(q^2)\) |
|
|
\(f_0^{T,\Lambda_b\to\Lambda}(q^2)\) |
|
|
\(f_0^{T5,\Lambda_b\to\Lambda}(q^2)\) |
|
|
\(f_0^{V,\Lambda_b\to\Lambda}(q^2)\) |
|
|
\(f_\perp^{A,\Lambda_b\to\Lambda}(q^2)\) |
|
|
\(f_\perp^{T,\Lambda_b\to\Lambda}(q^2)\) |
|
|
\(f_\perp^{T5,\Lambda_b\to\Lambda}(q^2)\) |
|
|
\(f_\perp^{V,\Lambda_b\to\Lambda}(q^2)\) |
|
|
\(f_t^{A,\Lambda_b\to\Lambda}(q^2)\) |
|
|
\(f_t^{V,\Lambda_b\to\Lambda}(q^2)\) |
|
Pseudo observables representing the full basis of \(\Lambda_b \to \Lambda\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(\Lambda_b \to \Lambda_c\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(f_0^{A,\Lambda_b\to\Lambda_c}(q^2)\) |
|
|
\(f_0^{T,\Lambda_b\to\Lambda_c}(q^2)\) |
|
|
\(f_0^{T5,\Lambda_b\to\Lambda_c}(q^2)\) |
|
|
\(f_0^{V,\Lambda_b\to\Lambda_c}(q^2)\) |
|
|
\(f_\perp^{A,\Lambda_b\to\Lambda_c}(q^2)\) |
|
|
\(f_\perp^{T,\Lambda_b\to\Lambda_c}(q^2)\) |
|
|
\(f_\perp^{T5,\Lambda_b\to\Lambda_c}(q^2)\) |
|
|
\(f_\perp^{V,\Lambda_b\to\Lambda_c}(q^2)\) |
|
|
\(f_t^{A,\Lambda_b\to\Lambda_c}(q^2)\) |
|
|
\(f_t^{V,\Lambda_b\to\Lambda_c}(q^2)\) |
|
Pseudo observables representing the full basis of \(\Lambda_b \to \Lambda_c\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(\Lambda_c \to \Lambda\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_{T5}]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(f_0^{A,\Lambda_c\to\Lambda}(q^2)\) |
|
|
\(f_0^{T,\Lambda_c\to\Lambda}(q^2)\) |
|
|
\(f_0^{T5,\Lambda_c\to\Lambda}(q^2)\) |
|
|
\(f_0^{V,\Lambda_c\to\Lambda}(q^2)\) |
|
|
\(f_\perp^{A,\Lambda_c\to\Lambda}(q^2)\) |
|
|
\(f_\perp^{T,\Lambda_c\to\Lambda}(q^2)\) |
|
|
\(f_\perp^{T5,\Lambda_c\to\Lambda}(q^2)\) |
|
|
\(f_\perp^{V,\Lambda_c\to\Lambda}(q^2)\) |
|
|
\(f_t^{A,\Lambda_c\to\Lambda}(q^2)\) |
|
|
\(f_t^{V,\Lambda_c\to\Lambda}(q^2)\) |
|
Pseudo observables representing the full basis of \(\Lambda_c \to \Lambda\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(\Lambda_c \to n\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_{T5}]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(f_0^{A,\Lambda_c\to n}(q^2)\) |
|
|
\(f_0^{T,\Lambda_c\to n}(q^2)\) |
|
|
\(f_0^{T5,\Lambda_c\to n}(q^2)\) |
|
|
\(f_0^{V,\Lambda_c\to n}(q^2)\) |
|
|
\(f_\perp^{A,\Lambda_c\to n}(q^2)\) |
|
|
\(f_\perp^{T,\Lambda_c\to n}(q^2)\) |
|
|
\(f_\perp^{T5,\Lambda_c\to n}(q^2)\) |
|
|
\(f_\perp^{V,\Lambda_c\to n}(q^2)\) |
|
|
\(f_t^{A,\Lambda_c\to n}(q^2)\) |
|
|
\(f_t^{V,\Lambda_c\to n}(q^2)\) |
|
Pseudo observables representing the full basis of \(\Lambda_c \to n\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(\Lambda_c \to p\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(f_0^{A,\Lambda_c\to p}(q^2)\) |
|
|
\(f_0^{T,\Lambda_c\to p}(q^2)\) |
|
|
\(f_0^{T5,\Lambda_c\to p}(q^2)\) |
|
|
\(f_0^{V,\Lambda_c\to p}(q^2)\) |
|
|
\(f_\perp^{A,\Lambda_c\to p}(q^2)\) |
|
|
\(f_\perp^{T,\Lambda_c\to p}(q^2)\) |
|
|
\(f_\perp^{T5,\Lambda_c\to p}(q^2)\) |
|
|
\(f_\perp^{V,\Lambda_c\to p}(q^2)\) |
|
|
\(f_t^{A,\Lambda_c\to p}(q^2)\) |
|
|
\(f_t^{V,\Lambda_c\to p}(q^2)\) |
|
Pseudo observables representing the full basis of \(\Lambda_c \to p\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(\Lambda_b \to \Lambda^*\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_{T_5}]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(f_0^{A,\Lambda_b\to\Lambda(1520)}(q^2)\) |
|
|
\(f_0^{T,\Lambda_b\to\Lambda(1520)}(q^2)\) |
|
|
\(f_0^{T5,\Lambda_b\to\Lambda(1520)}(q^2)\) |
|
|
\(f_0^{V,\Lambda_b\to\Lambda(1520)}(q^2)\) |
|
|
\(f_\perp^{A,\Lambda_b\to\Lambda(1520)}(q^2)\) |
|
|
\(f_\perp^{T,\Lambda_b\to\Lambda(1520)}(q^2)\) |
|
|
\(f_\perp^{T5,\Lambda_b\to\Lambda(1520)}(q^2)\) |
|
|
\(f_\perp^{V,\Lambda_b\to\Lambda(1520)}(q^2)\) |
|
|
\(f_{\perp'}^{A,\Lambda_b\to\Lambda(1520)}(q^2)\) |
|
|
\(f_{\perp'}^{T,\Lambda_b\to\Lambda(1520)}(q^2)\) |
|
|
\(f_{\perp'}^{T5,\Lambda_b\to\Lambda(1520)}(q^2)\) |
|
|
\(f_{\perp'}^{V,\Lambda_b\to\Lambda(1520)}(q^2)\) |
|
|
\(f_t^{A,\Lambda_b\to\Lambda(1520)}(q^2)\) |
|
|
\(f_t^{V,\Lambda_b\to\Lambda(1520)}(q^2)\) |
|
Pseudo observables representing the full basis of \(\Lambda_b \to \Lambda^*\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Unitarity Bounds
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\textrm{Saturation}_{B_{s,0}}[0^+_V]\) |
|
|
\(\textrm{Saturation}_{B_{s,1}}[1^+_A]\) |
|
|
\(\textrm{Saturation}_{B_{s,1}}[1^+_{T_5}]\) |
|
|
\(\textrm{Saturation}_{B_s^0}[0^-_A]\) |
|
|
\(\textrm{Saturation}_{B_s^*}[1^-_T]\) |
|
|
\(\textrm{Saturation}_{B_s^*}[1^-_V]\) |
|
|
\(\textrm{Saturation}_{B_u}[0^-_A]\) |
|
|
\(\textrm{Saturation}_{B_u^*}[1^-_{V}]\) |
|
|
\(\textrm{Saturation}_{D_{s,0}}[0^+_V]\) |
|
|
\(\textrm{Saturation}_{D_{s,1}}[1^+_A]\) |
|
|
\(\textrm{Saturation}_{D_{s,1}}[1^+_{T_5}]\) |
|
|
\(\textrm{Saturation}_{D_s^0}[0^-_A]\) |
|
|
\(\textrm{Saturation}_{D_s^*}[1^-_T]\) |
|
|
\(\textrm{Saturation}_{D_s^*}[1^-_V]\) |
|
|
\(B^{b\to c}_{0^+}\) |
|
|
\(B^{b\to c}_{0^+}\) |
|
|
\(B^{b\to c}_{0^-}\) |
|
|
\(B^{b\to c}_{0^-}\) |
|
|
\(B^{b\to c}_{1^+,T}\) |
|
|
\(B^{b\to c}_{1^+}\) |
|
|
\(B^{b\to c}_{1^+}\) |
|
|
\(B^{b\to c}_{1^-,T}\) |
|
|
\(B^{b\to c}_{1^-}\) |
|
|
\(B^{b\to c}_{1^-}\) |
Pseudo observables arising in the various unitarity bounds of semileptonic form factors.
\(B\)-meson LCDAs
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(L_0\, \left[ \textrm{GeV}^{-1} \right]\) |
|
|
\(L_1\, \left[ \textrm{GeV}^{-1} \right]\) |
|
|
\(L_2\, \left[ \textrm{GeV}^{-1} \right]\) |
|
|
\(\tilde\phi_{B,+}(-i \tau, \mu)\) |
|
|
\(-i \tau \, \tilde\phi^{\prime}_{B,+}(-i \tau, \mu)\) |
|
|
\(-\tau^2 \, \tilde\phi^{\prime\prime}_{B,+}(-i \tau, \mu)\) |
|
Pseudo observables arising in the description of \(B\)-meson Light-Cone Distribution Amplitudes (LCDAs).
Form factors for \(D \to K\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(F_T(q^2)/F_+(q^2)\) |
|
|
\(F_+^{D \to K}(q^2)\) |
|
|
\(F_T^{D \to K}(q^2)\) |
|
|
\(F_{+,T}(q^2)/F_+(q^2)\) |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_{T5}]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(f_+^{D \to K}(q^2)\) |
|
|
\(\hat{f}_+^{D \to K}(q^2)\) |
|
|
\(\hat{f}_+^{\prime D \to K}(q^2)\) |
|
|
\(f_-^{D \to K}(q^2)\) |
|
|
\(f_0^{D \to K}(q^2)\) |
|
|
\(\hat{f}_0^{D \to K}(q^2)\) |
|
|
\(\hat{f}_0^{\prime D \to K}(q^2)\) |
|
|
\(f_T^{D \to K}(q^2)\) |
|
|
\(\hat{f}_T^{D \to K}(q^2)\) |
|
|
\(\hat{f}_T^{\prime D \to K}(q^2)\) |
|
Pseudo observables representing the full basis of \(D \to K\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(D\to \eta^{(\prime)}\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(f_+^{D\to\eta}(q^2)\) |
|
|
\(f_0^{D\to\eta}(q^2)\) |
|
|
\(f_T^{D\to\eta}(q^2)\) |
|
|
\(f_+^{D\to\eta'}(q^2)\) |
|
|
\(f_0^{D\to\eta'}(q^2)\) |
|
|
\(f_T^{D\to\eta'}(q^2)\) |
|
Pseudo observables representing the full basis of \(D\to \eta^{(\prime)}\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(D_s\to \eta^{(\prime)}\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(f_+^{D_s\to\eta}(q^2)\) |
|
|
\(f_0^{D_s\to\eta}(q^2)\) |
|
|
\(f_T^{D_s\to\eta}(q^2)\) |
|
|
\(f_+^{D_s\to\eta'}(q^2)\) |
|
|
\(f_0^{D_s\to\eta'}(q^2)\) |
|
|
\(f_T^{D_s\to\eta'}(q^2)\) |
|
Pseudo observables representing the full basis of \(D_s\to \eta^{(\prime)}\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(0 \to \pi \pi\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(|f_+^{0\to \pi\pi}(q^2)|^2\) |
|
|
\(\textrm{arg}(f_+^{0\to\pi\pi}(q^2))\) |
|
|
\(\textrm{Im}\,\textrm{Res}_{q^2} (M_\rho^2)\,f_+^{0\to\pi\pi}\) |
|
|
\(\textrm{Im}\,\textrm{Res}_{z} (M_\rho^2)\,f_+^{0\to\pi\pi}\) |
|
|
\(\textrm{Im}(f_+^{0\to\pi\pi}(q^2))\) |
|
|
\(\textrm{Re}\,\textrm{Res}_{q^2} (M_\rho^2)\,f_+^{0\to\pi\pi}\) |
|
|
\(\textrm{Re}\,\textrm{Res}_{z} (M_\rho^2)\,f_+^{0\to\pi\pi}\) |
|
|
\(\textrm{Re}(f_+^{0\to\pi\pi}(q^2))\) |
|
|
\(\textrm{Saturation}\) |
|
|
\(b_0^{0 \to \pi\pi}\) |
|
|
\(b_1^{0 \to \pi\pi}\) |
|
|
\(\langle r_\pi^2 \rangle\, \left[ \textrm{fm}^2 \right]\) |
Pseudo observables representing the full basis of \(0 \to \pi \pi\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Form factors for \(0 \to K \pi\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(|f_+^{0\to K\pi}(q^2)|^2\) |
|
|
\(|f_0^{0\to K\pi}(q^2)|^2\) |
|
|
\(\textrm{arg}(f_+^{0\to K\pi}(q^2))\) |
|
|
\(\textrm{arg}(f_0^{0\to K\pi}(q^2))\) |
|
|
\(\Delta_{\textrm{CT}}\) |
|
|
\(\Delta_{\widetilde{\textrm{CT}}}\) |
|
|
\(\textrm{Im}(f_+^{0\to K\pi}(q^2))\) |
|
|
\(\textrm{Im}(f_0^{0\to K\pi}(q^2))\) |
|
|
\(\textrm{Re}(f_+^{0\to K\pi}(q^2))\) |
|
|
\(\textrm{Re}(f_0^{0\to K\pi}(q^2))\) |
|
|
\(\textrm{Saturation}[1^-]\) |
|
|
\(\textrm{Saturation}[0^+]\) |
|
|
\(b_0^{+, 0 \to K\pi}\) |
|
|
\(b_0^{0, 0 \to K\pi}\) |
|
|
\(f_+^{0 \to K\pi}(0)\) |
|
|
\(\lambda_+^{\prime\prime, K \to \pi}\) |
|
|
\(\lambda_0^{\prime\prime, K \to \pi}\) |
|
|
\(\lambda_+^{(\prime), K \to \pi}\) |
|
|
\(\lambda_0^{(\prime), K \to \pi}\) |
Pseudo observables representing the full basis of \(0 \to K \pi\) form factors. The specific parametrization can be chosen via the “form-factors” option.
Observables in scattering processes
Observables in \(ee \to c\bar{c}\) processes
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathrm{Re}\rho_{D^+D^-}(E))\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\mathrm{Re}\rho_{D^0 \bar{D}^0}(E))\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\Gamma(J/\psi \to ee)\, \left[ \textrm{GeV} \right]\) |
|
|
\(\Gamma(J/\psi \to \textrm{eff})\, \left[ \textrm{GeV} \right]\) |
|
|
\(\Gamma_{J/\psi}\, \left[ \textrm{GeV} \right]\) |
|
|
\(\mathrm{Im}T^{II}(e^+e^- \to D^+ D^-)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\mathrm{Re}T^{II}(e^+e^- \to D^+ D^-)\, \left[ \textrm{GeV}^{-2} \right]\) |
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\(\sigma(e^+e^- \to D^+ D^-)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
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\(\sigma(e^+e^- \to D^+ D^-)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\mathrm{Im}T^{II}(e^+e^- \to D^0 \bar{D}^0)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\mathrm{Re}T^{II}(e^+e^- \to D^0 \bar{D}^0)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\sigma(e^+e^- \to D^0 \bar{D}^0)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
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\(\sigma(e^+e^- \to D^0 \bar{D}^0)\, \left[ \textrm{GeV}^{-2} \right]\) |
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\(R\) |
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\(\mathrm{Im}T^{II}(e^+e^- \to e^+e^-)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
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\(\mathrm{Re}T^{II}(e^+e^- \to e^+e^-)\, \left[ \textrm{GeV}^{-2} \right]\) |
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\(\sigma(e^+e^- \to e^+e^-)|_{s\textrm{-channel}}\, \left[ \textrm{GeV}^{-2} \right]\) |
|
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\(\sigma(e^+e^- \to e^+e^-)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\mathrm{Im}T^{II}(e^+e^- \to \mathrm{eff})\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\mathrm{Re}T^{II}(e^+e^- \to \mathrm{eff})\, \left[ \textrm{GeV}^{-2} \right]\) |
|
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\(\sigma(e^+e^- \to \textrm{eff})\, \left[ \textrm{GeV}^{-2} \right]\) |
|
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\(\mathrm{Re}\rho_{e^+e^-}(E))\, \left[ \textrm{GeV}^{-2} \right]\) |
|
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\(\mathrm{Re}\rho_{e^+e^-}(E))\, \left[ \textrm{GeV}^{-2} \right]\) |
|
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\(\Gamma(\psi(2S) \to ee)\, \left[ \textrm{GeV} \right]\) |
|
|
\(\Gamma(\psi(2S) \to \textrm{eff})\, \left[ \textrm{GeV} \right]\) |
|
|
\(\Gamma_{\psi(2S)}\, \left[ \textrm{GeV} \right]\) |
|
|
\(\Gamma(\psi(3770) \to D^+ D^-)\, \left[ \textrm{GeV} \right]\) |
|
|
\(\Gamma(\psi(3770) \to D^0\bar{D}^0)\, \left[ \textrm{GeV} \right]\) |
|
|
\(\Gamma(\psi(3770) \to \textrm{eff})\, \left[ \textrm{GeV} \right]\) |
|
|
\(\textrm{spect}_{\psi(3770)}(E)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\Gamma_{\psi(3770)}\, \left[ \textrm{GeV} \right]\) |
The “assume_isospin” option equalises the couplings of isospin-related channels.
Observables in (semi)leptonic \(s\)-hadron decays
Observables in \(K \to \ell^-\bar{\nu}_\ell\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(K^- \to \ell^-\bar{\nu}_\ell)\) |
The option “l” selects the charged lepton flavor.
Observables in \(K \to \pi \ell^+ \bar{\nu}_\ell\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(K_L \to \pi^+ \ell^- \bar{\nu}_\ell)\) |
|
|
\(\mathcal{B}(K_S \to \pi^+ \ell^- \bar{\nu}_\ell)\) |
|
|
\(\mathcal{B}(K^- \to \pi^0 \ell^- \bar{\nu}_\ell)\) |
The option “l” selects the charged lepton flavor.The option “form-factors” selects the form factor parametrization.
Observables in \(\tau\) decays
Observables in \(\tau \to K^- \nu_\tau\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(\tau^- \to K^- \nu)\) |
Observables in \(\tau \to K \pi^- \nu_\tau\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(\tau^- \to K^- \pi^0 \nu_\tau)\) |
|
|
\(d^2\Gamma(\tau^- \to K^- \pi^0 \nu_\tau)/dq^2/d\cos\theta_K\, \left[ \textrm{GeV}^{-1} \right]\) |
|
|
\(\mathcal{B}(\tau^- \to K_S \pi^- \nu_\tau)\) |
|
|
\(dP(\tau^- \to K_S \pi^- \nu_\tau)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(P(\tau^-\to K_S \pi^- \nu_\tau)\) |
|
|
\(d^2\Gamma(\tau^- \to K_S \pi^- \nu_\tau)/dq^2/d\cos\theta_K\, \left[ \textrm{GeV}^{-1} \right]\) |
|
|
\(d\mathcal{B}(\tau^- \to K_S \pi^- \nu_\tau)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(d\Gamma(\tau^- \to K_S \pi^- \nu_\tau)/dq^2\, \left[ \textrm{GeV}^{-1} \right]\) |
|