List of Observables
The following is a list of observables that is available in EOS v1.0.13.
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 |
|---|---|---|
|
\(A_{\mathrm{FB}}(B^- \to e^-\bar\nu\mu^+\mu^-)\) |
|
|
\(\mathcal{B}(B^- \to e^-\bar\nu\mu^+\mu^-)\) |
|
|
\(\frac{d\mathcal{B}(B^- \to e^-\bar\nu\mu^+\mu^-)}{dq^2/dk^2}\) |
|
|
\(A_{\mathrm{FB}}(B^- \to \mu^-\bar\nu e^+e^-)\) |
|
|
\(\mathcal{B}(B^- \to \mu^-\bar\nu e^+e^-)\) |
|
|
\(\frac{d\mathcal{B}(B^- \to \mu^-\bar\nu e^+e^-)}{dq^2/dk^2}\) |
|
|
\(A_{\mathrm{FB}}(B^- \to \tau^-\bar\nu e^+e^-)\) |
|
|
\(\mathcal{B}(B^- \to \tau^-\bar\nu e^+e^-)\) |
|
|
\(\frac{d\mathcal{B}(B^- \to \tau^-\bar\nu e^+e^-)}{dq^2/dk^2}\) |
|
|
\(A_{\mathrm{FB}}(B^- \to \tau^-\bar\nu\mu^+\mu^-)\) |
|
|
\(\mathcal{B}(B^- \to \tau^-\bar\nu\mu^+\mu^-)\) |
|
|
\(\frac{d\mathcal{B}(B^- \to \tau^-\bar\nu\mu^+\mu^-)}{dq^2/dk^2}\) |
|
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 |
|
|
\(dP(B\to\pi\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(P(B\to\pi\ell^-\bar\nu)\) |
|
|
\(R_{\pi}\) |
|
|
\(R_{\pi}(q^2)\) |
|
|
\(R_{\pi, 0}\) |
|
|
\(R_{\pi, P}\) |
|
|
\(d\mathcal{B}(B\to\pi\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(d^2\mathcal{B}(B\to\pi\ell^-\bar\nu)/dq^2/d\cos(\theta_l)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\Gamma(B\to\pi\ell^-\bar\nu)\) |
|
|
\(\Gamma(B\to\pi\ell^-\bar\nu)_0\) |
|
|
\(\Gamma(B\to\pi\ell^-\bar\nu)_p\) |
|
|
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 \(B\to \bar{D} \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_{\mathrm{FB}}(B\to \bar{D}\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{FB}}(B\to \bar{D}\ell^-\bar\nu)(q^2)\) |
|
|
n/a |
|
|
\(\mathcal{B}(B\to \bar{D}\ell^-\bar\nu)\) |
|
|
n/a |
|
|
n/a |
|
|
\(R_D\) |
|
|
\(R_D(q^2)\) |
|
|
\(d\mathcal{B}(B\to \bar{D}\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(d^2\mathcal{B}(B\to \bar{D}\ell^-\bar\nu)/dq^2/d\cos(\theta_l)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
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 \(B_s\to \bar{K} \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(\bar{B}_s\to K\ell^-\bar\nu)\) |
|
|
\(d\mathcal{B}(\bar{B}_s\to K\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
n/a |
|
|
n/a |
|
The option “l” selects the charged lepton flavor.The option “form-factors” selects the form factor parametrization.
Observables in \(B_s\to \bar{D_s} \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_{\mathrm{FB}}(B_s\to \bar{D}_s\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{FB}}(B_s\to \bar{D}_s\ell^-\bar\nu)(q^2)\) |
|
|
n/a |
|
|
\(\mathcal{B}(B_s\to \bar{D}_s\ell^-\bar\nu)\) |
|
|
n/a |
|
|
n/a |
|
|
\(R_{D_s}\) |
|
|
\(R_{D_s}(q^2)\) |
|
|
\(d\mathcal{B}(B_s\to \bar{D}_s\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
n/a |
|
|
n/a |
|
The option “l” selects the charged lepton flavor.The option “form-factors” selects the form factor parametrization.
Observables in \(B\to \omega \ell^-\bar\nu\) 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 \(B\to \bar{D}^* \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_{1c}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(A_{1s}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(A_{2c}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(A_{2s}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(A_3(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(A_4(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(A_5(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(A_{6c}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(A_{6s}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(A_7(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(A_8(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(A_9(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{C}}^1(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{C}}^2(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{C}}^3(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{FB}}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{FB}}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(A_{\mathrm{FB}}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
n/a |
|
|
n/a |
|
|
\(A_{\mathrm{T}}^1(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{T}}^2(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{T}}^3(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(\bar{A}_{\mathrm{FB}}(B\to \bar{D}^*\ell^-\bar\nu)_{\ell=e,\mu}\) |
|
|
\(\bar{\mathcal{B}}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B\to \bar{D}^*\ell^-\bar\nu)_{\ell=e,\mu}\) |
|
|
n/a |
|
|
\(\Delta\mathcal{B}(B\to \bar{D}^*\ell^-\bar\nu)_{\ell=e,\mu}\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(F_{\mathrm{L}}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(F_{\mathrm{L}}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(\bar{F}_{\mathrm{L}}(B\to \bar{D}^*\ell^-\bar\nu)_{\ell=e,\mu}\) |
|
|
\(\tilde{F}_{\mathrm{L}}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(\tilde{F}_{\mathrm{L}}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(\bar{\tilde{F}}_{\mathrm{L}}(B\to \bar{D}^*\ell^-\bar\nu)_{\ell=e,\mu}\) |
|
|
\(J_{1c}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(J_{1c}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{1s}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(J_{1s}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{2c}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(J_{2c}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{2s}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(J_{2s}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{3}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(J_{3}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{4}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(J_{4}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{5}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(J_{5}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{6c}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(J_{6c}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{6s}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(J_{6s}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{7}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(J_{7}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{8}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(J_{8}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{9}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(J_{9}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(R_{D^*}\) |
|
|
\(R_{D^*}^{e/\mu}(q^2)\) |
|
|
\(R_{D^*}^{\tau/\mu}(q^2)\) |
|
|
\(S_{1c}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(S_{1s}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(S_{2c}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(S_{2s}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(S_3(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(S_4(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(S_5(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(S_{6c}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(S_{6s}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(S_7(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(S_8(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(S_9(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
n/a |
|
|
\(d\mathcal{B}(B\to \bar{D}^*\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
n/a |
|
|
\(\bar{\Gamma}(B\to \bar{D}^*\ell^-\bar\nu)_{|V_{cb}|=1}\) |
|
|
\(\Gamma(B\to \bar{D}^*\ell^-\bar\nu)_{|V_{cb}|=1}\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
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. The option “form-factors” selects the form factor parametrization.
Observables in \(B_u \to \gamma \ell \nu_{\ell}\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(A_{\mathrm{FB}}(B^- \to \gamma \ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B^- \to \gamma \ell^-\bar\nu)\) |
|
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 |
|
|
\(d\mathcal{B}(B_s\to \bar{K}^*\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
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 |
|---|---|---|
|
\(A_{\mathrm{C}}^1(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{C}}^2(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{C}}^3(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{FB}}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{FB}}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(A_L(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(A_T(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{T}}^1(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{T}}^2(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{T}}^3(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(F_{\mathrm{L}}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(J_{1c}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(J_{1c}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{1s}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(J_{1s}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{2c}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(J_{2c}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{2s}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(J_{2s}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{3}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(J_{3}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{4}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(J_{4}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{5}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(J_{5}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{6c}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(J_{6c}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{6s}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(J_{6s}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{7}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(J_{7}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{8}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(J_{8}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
|
|
\(J_{9}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(J_{9}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
|
|
n/a |
|
|
\(R_{D_s^*}\) |
|
|
\(R_{D_s^*}(q^2)\) |
|
|
\(d\mathcal{B}(B_s\to \bar{D}_s^*\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
n/a |
|
|
n/a |
|
The option “l” selects the charged lepton flavor.The option “form-factors” selects the form factor parametrization.
Observables in \(B\to \pi\pi \ell^-\bar\nu\) 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 |
|
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 |
|
|
\(R_{\Lambda_c(2625)}\) |
|
|
\(R_{\Lambda_c(2625)}(q^2)\) |
|
|
\(d\mathcal{B}/dq^2(\Lambda_b\to\Lambda_c(2625) \ell^-\bar\nu)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
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 |
|
|
\(F_0(\Lambda_b\to\Lambda_c \ell^-\bar\nu)(q^2)\) |
|
|
\(K_{1c}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{1cc}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{1ss}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{2c}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{2cc}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{2ss}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{3s}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{3sc}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{4s}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{4sc}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(R(A_{\mathrm{FB}}^{\Lambda_c})\) |
|
|
\(R(A_{\mathrm{FB}}^{\Lambda_c})(q^2)\) |
|
|
\(R(\Lambda_c)\) |
|
|
\(d\mathcal{B}(\Lambda_b\to\Lambda_c \ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
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 \(\Lambda_c \to \Lambda \ell^+ \nu\) 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 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 |
|---|---|---|
|
\(A_\mathrm{CP}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(\bar A_\mathrm{FB}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(A_\mathrm{FB}(\bar{B}\to \bar{K}\ell^+\ell^-)(q^2)\) |
|
|
\(A_\mathrm{FB}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(\bar{\mathcal{B}}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(\mathcal{B}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(\bar F_\mathrm{H}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(F_\mathrm{H}(\bar{B}\to \bar{K}\ell^+\ell^-)(q^2)\) |
|
|
\(F_\mathrm{H}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(\Gamma(\bar{B}\to \bar{K}\ell^+\ell^-)\, \left[ \textrm{GeV} \right]\) |
|
|
\(\mathcal{B}(\bar{B}\to \bar{K}\ell^+\ell^-)/\mathcal{B}(\bar{B}\to \bar{K}J/\psi)\) |
|
|
\(R_K\) |
|
|
\(R_K(q^2)\) |
|
|
\(d\mathcal{B}(\bar{B}\to \bar{K}\ell^+\ell^-)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(d^2\mathcal{\Gamma(\bar{B}\to \bar{K}\ell^+\ell^-)}/(dq^2\, d\cos\theta_\ell)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
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 |
|
|
\(J_{1c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_{1c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_{1s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_{1s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_{2c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_{2c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_{2s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_{2s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_3(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_3(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(\bar{J}/\bar{\Gamma}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_3/\Gamma(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_4(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_4(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_5(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_5(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_{6c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_{6c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_{6s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_{6s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_7(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_7(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_8(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_8(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_9(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_9(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(\bar{J}/\bar{\Gamma}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_9/\Gamma(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(\mathcal{N}'_\mathrm{bin}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(\mathcal{B}(\bar{B}\to \bar{K}^*\ell^+\ell^-)/\mathcal{B}(\bar{B}\to \bar{K}^*J/\psi)\) |
|
|
\(P'_4(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P'_4(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q2)\) |
|
|
\(P'_4^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P'_5(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P'_5(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q2)\) |
|
|
\(P'_5^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P'_6(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P'_6(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q2)\) |
|
|
\(P'_6^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P'_8(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P'_8^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P_1(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P_1^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P_2(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P_2^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P_3(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P_3^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(R_{K^*}\) |
|
|
\(R_{K^*}(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(S_{1c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{1c}^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_{1c}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_{1c}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{1s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{1s}^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_{1s}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_{1s}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{2c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{2c}^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_{2c}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_{2c}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{2s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{2s}^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_{2s}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_{2s}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_3(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_3^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_3^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_3^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_4(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_4^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_4^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_4^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_5(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_5^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_5^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_5^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{6c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{6c}^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_{6c}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_{6c}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{6s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{6s}^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_{6s}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_{6s}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_7(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_7^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_7^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_7^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_8(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_8^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_8^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_8^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_9(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_9^{\bar{B}\to \bar{K}^*\ell^+\ell^-}(q^2)\) |
|
|
\(S_9^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(S_9^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(d\mathcal{B}/dq^2(\bar{B}\to \bar{K}^*\ell^+\ell^-)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
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 |
|---|---|---|
|
\(\mathcal{B}(\bar{B}\to \bar{K}\nu\bar\nu)\) |
|
|
\(d\mathcal{B}(\bar{B}\to \bar{K}\nu\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
Observables in \(B\to K^* \nu\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathcal{B}(\bar{B}\to \bar{K}^*\nu\bar\nu)\) |
|
|
\(F_L(\bar{B}\to \bar{K}^*\nu\bar\nu)\) |
|
|
\(F_L(\bar{B}\to \bar{K}^*\nu\bar\nu)(q^2)\) |
|
|
\(d\mathcal{B}(\bar{B}\to \bar{K}^*\nu\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
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 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 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 |
|
|
\(f_+^{'',B\to\pi}(q^2)\) |
|
|
\(f_+^{',B\to\pi}(q^2)\) |
|
|
\(f_+^{B\to\pi}(q^2)\) |
|
|
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 \(B\to K\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(F_T(q^2)/F_+(q^2)\) |
|
|
\(F_+^{B\to K}(q^2)\) |
|
|
\(F_T^{B\to K}(q^2)\) |
|
|
\(F_{+,T}(q^2)/F_+(q^2)\) |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_{T5}]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(f_+^{B\to K}(q^2)\) |
|
|
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 \(B_s\to \bar{K}\) transitions
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_{T5}]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(f_+^{B_s\to \bar{K}}(q^2)\) |
|
|
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 |
|---|---|---|
|
\(f_0(q^2_\mathrm{num})/f_+(q^2_\mathrm{denom})\) |
|
|
\(f_+^{B_s\to \bar{D}_s}(q^2)\) |
|
|
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.
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 |
|
|
\(\mathcal{F}_0^{B\to K^*}(q^2)\) |
|
|
\(\mathcal{F}_{0,T}^{B\to K^*}(q^2)\) |
|
|
\(\mathcal{F}_{0,T}(q^2)/\mathcal{F}_0(q^2)\) |
|
|
\(\mathcal{F}_\parallel^{B\to K^*}(q^2)\) |
|
|
\(\mathcal{F}_{\parallel,T}^{B\to K^*}(q^2)\) |
|
|
\(\mathcal{F}_{\parallel,T}(q^2)/\mathcal{F}_\parallel(q^2)\) |
|
|
\(\mathcal{F}_\perp^{B\to K^*}(q^2)\) |
|
|
\(\mathcal{F}_{\perp,T}^{B\to K^*}(q^2)\) |
|
|
\(\mathcal{F}_{\perp,T}(q^2)/\mathcal{F}_\perp(q^2)\) |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_{T5}]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(T_1^{B\to K^*}(q^2)\) |
|
|
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 |
|
|
\(T_1^{B\to D^*}(q^2)\) |
|
|
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 |
|
|
\(a_0^{A_1}\) |
|
|
\(a_0^{A_5}\) |
|
|
\(a_0^{F_1}\) |
|
|
\(a_0^{F_2}\) |
|
|
\(a_0^{P_1}\) |
|
|
\(a_0^{T_{23}}\) |
|
|
\(a_0^{T_2}\) |
|
|
\(a_0^{V_4}\) |
|
|
\(a_1^{A_1}/a_0^{A_1}\) |
|
|
\(a_1^{A_5}/a_0^{A_5}\) |
|
|
\(a_1^{P_1}/a_0^{P_1}\) |
|
|
\(a_1^{V_4}/a_0^{V_4}\) |
|
|
\(a_1^{A_1}\) |
|
|
\(a_1^{A_5}\) |
|
|
\(a_1^{P_1}\) |
|
|
\(a_1^{V_4}\) |
|
|
\(a_2^{A_1}/a_0^{A_1}\) |
|
|
\(a_2^{A_5}/a_0^{A_5}\) |
|
|
\(a_2^{P_1}/a_0^{P_1}\) |
|
|
\(a_2^{V_4}/a_0^{V_4}\) |
|
|
\(a_2^{A_1}\) |
|
|
\(a_2^{A_5}\) |
|
|
\(a_2^{P_1}\) |
|
|
\(a_2^{V_4}\) |
|
|
\(h_{A_1}^{\bar{B}\to D^*}(q^2)\) |
|
|
\(h_{A_2}^{\bar{B}\to D^*}(q^2)\) |
|
|
\(h_{A_3}^{\bar{B}\to D^*}(q^2)\) |
|
|
\(h_{T_1}^{\bar{B}\to D^*}(q^2)\) |
|
|
\(h_{T_2}^{\bar{B}\to D^*}(q^2)\) |
|
|
\(h_{T_3}^{\bar{B}\to D^*}(q^2)\) |
|
|
\(h_V^{\bar{B}\to D^*}(q^2)\) |
|
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 \(B_s\to \bar{K}^*\) 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 |
|
|
\(T_1^{B_s\to \bar{K}^*}(q^2)\) |
|
|
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 |
|
|
\(\mathcal{F}_0^{B_s\to \phi}(q^2)\) |
|
|
\(\mathcal{F}_{0,T}^{B_s\to \phi}(q^2)\) |
|
|
\(\mathcal{F}_{0,T}(q^2)/\mathcal{F}_0(q^2)\) |
|
|
\(\mathcal{F}_\parallel^{B_s\to \phi}(q^2)\) |
|
|
\(\mathcal{F}_{\parallel,T}^{B_s\to \phi}(q^2)\) |
|
|
\(\mathcal{F}_{\parallel,T}(q^2)/\mathcal{F}_\parallel(q^2)\) |
|
|
\(\mathcal{F}_\perp^{B_s\to \phi}(q^2)\) |
|
|
\(\mathcal{F}_{\perp,T}^{B_s\to \phi}(q^2)\) |
|
|
\(\mathcal{F}_{\perp,T}(q^2)/\mathcal{F}_\perp(q^2)\) |
|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_{T5}]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(T_1^{B_s\to \phi}(q^2)\) |
|
|
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 |
|
|
\(T_1^{B_s\to D_s^*}(q^2)\) |
|
|
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 |
|
|
\(h_{A_1}^{\bar{B}_s\to D_s^*}(q^2)\) |
|
|
\(h_{A_2}^{\bar{B}_s\to D_s^*}(q^2)\) |
|
|
\(h_{A_3}^{\bar{B}_s\to D_s^*}(q^2)\) |
|
|
\(h_{T_1}^{\bar{B}_s\to D_s^*}(q^2)\) |
|
|
\(h_{T_2}^{\bar{B}_s\to D_s^*}(q^2)\) |
|
|
\(h_{T_3}^{\bar{B}_s\to D_s^*}(q^2)\) |
|
|
\(h_V^{\bar{B}_s\to D_s^*}(q^2)\) |
|
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 |
|---|---|---|
|
\(\mathrm{Im}\,F_0^{B\to \pi\pi}(q^2,k^2,z)\) |
|
|
\(\mathrm{Im}\,F_\parallel^{B\to \pi\pi}(q^2,k^2,z)\) |
|
|
\(\mathrm{Im}\,F_\perp^{B\to \pi\pi}(q^2,k^2,z)\) |
|
|
\(\mathrm{Im}\,F_t^{B\to \pi\pi}(q^2,k^2,z)\) |
|
|
\(\mathrm{Res}\,\mathrm{Im}\,F_0^{B\to \pi\pi}(q^2,k^2,z)\) |
|
|
\(\mathrm{Res}\,\mathrm{Im}\,F_\parallel^{B\to \pi\pi}(q^2,k^2,z)\) |
|
|
\(\mathrm{Res}\,\mathrm{Im}\,F_\perp^{B\to \pi\pi}(q^2,k^2,z)\) |
|
|
\(\mathrm{Res}\,\mathrm{Im}\,F_t^{B\to \pi\pi}(q^2,k^2,z)\) |
|
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 |
|---|---|---|
|
\(\textrm{Saturation}[0^+_V]\) |
|
|
\(\textrm{Saturation}[0^-_A]\) |
|
|
\(\textrm{Saturation}[1^+_{A,0}]\) |
|
|
\(\textrm{Saturation}[1^+_{A,\parallel}]\) |
|
|
\(\textrm{Saturation}[1^+_{A,\perp}]\) |
|
|
\(\textrm{Saturation}[1^+_A]\) |
|
|
\(\textrm{Saturation}[1^+_{T5,0}]\) |
|
|
\(\textrm{Saturation}[1^+_{T5,\parallel}]\) |
|
|
\(\textrm{Saturation}[1^+_{T5,\perp}]\) |
|
|
\(\textrm{Saturation}[1^+_{T5}]\) |
|
|
\(\textrm{Saturation}[1^-_{T,0}]\) |
|
|
\(\textrm{Saturation}[1^-_{T,\parallel}]\) |
|
|
\(\textrm{Saturation}[1^-_{T,\perp}]\) |
|
|
\(\textrm{Saturation}[1^-_T]\) |
|
|
\(\textrm{Saturation}[1^-_{V,0}]\) |
|
|
\(\textrm{Saturation}[1^-_{V,\parallel}]\) |
|
|
\(\textrm{Saturation}[1^-_{V,\perp}]\) |
|
|
\(\textrm{Saturation}[1^-_V]\) |
|
|
\(f_0^{A,\Lambda_c\to\Lambda}(q^2)\) |
|
|
\(f_0^{T,\Lambda_c\to\Lambda}(q^2)\) |
|
|
\(f_0^{T5,\Lambda_c\to\Lambda}(q^2)\) |
|
|
\(f_0^{V,\Lambda_c\to\Lambda}(q^2)\) |
|
|
\(f_\perp^{A,\Lambda_c\to\Lambda}(q^2)\) |
|
|
\(f_\perp^{T,\Lambda_c\to\Lambda}(q^2)\) |
|
|
\(f_\perp^{T5,\Lambda_c\to\Lambda}(q^2)\) |
|
|
\(f_\perp^{V,\Lambda_c\to\Lambda}(q^2)\) |
|
|
\(f_t^{A,\Lambda_c\to\Lambda}(q^2)\) |
|
|
\(f_t^{V,\Lambda_c\to\Lambda}(q^2)\) |
|
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 \(\Lambda_b \to \Lambda^*\) 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 |
|---|---|---|
|
\(\textrm{Saturation}_{B_{s,0}}[0^+_V]\) |
|
|
\(\textrm{Saturation}_{B_{s,1}}[1^+_{A,0}]\) |
|
|
\(\textrm{Saturation}_{B_{s,1}}[1^+_{A,\parallel}]\) |
|
|
\(\textrm{Saturation}_{B_{s,1}}[1^+_{A,\perp}]\) |
|
|
\(\textrm{Saturation}_{B_{s,1}}[1^+_A]\) |
|
|
\(\textrm{Saturation}_{B_{s,1}}[1^+_{T_5,0}]\) |
|
|
\(\textrm{Saturation}_{B_{s,1}}[1^+_{T_5,\parallel}]\) |
|
|
\(\textrm{Saturation}_{B_{s,1}}[1^+_{T_5,\perp}]\) |
|
|
\(\textrm{Saturation}_{B_{s,1}}[1^+_{T_5}]\) |
|
|
\(\textrm{Saturation}_{B_s^0}[0^-_A]\) |
|
|
\(\textrm{Saturation}_{B_s^*}[1^-_{T,0}]\) |
|
|
\(\textrm{Saturation}_{B_s^*}[1^-_{T,\parallel}]\) |
|
|
\(\textrm{Saturation}_{B_s^*}[1^-_{T,\perp}]\) |
|
|
\(\textrm{Saturation}_{B_s^*}[1^-_T]\) |
|
|
\(\textrm{Saturation}_{B_s^*}[1^-_{V,0}]\) |
|
|
\(\textrm{Saturation}_{B_s^*}[1^-_{V,\perp}]\) |
|
|
\(\textrm{Saturation}_{B_s^*}[1^-_{V,\parallel}]\) |
|
|
\(\textrm{Saturation}_{B_s^*}[1^-_V]\) |
|
|
\(\textrm{Saturation}_{B_{s,0}}[0^+_V]\) |
|
|
\(\textrm{Saturation}_{B_{s,1}}[1^+_{A,0}]\) |
|
|
\(\textrm{Saturation}_{B_{s,1}}[1^+_{A,\parallel}]\) |
|
|
\(\textrm{Saturation}_{B_{s,1}}[1^+_{A,\perp}]\) |
|
|
\(\textrm{Saturation}_{B_{s,1}}[1^+_A]\) |
|
|
\(\textrm{Saturation}_{B_{s,1}}[1^+_{T_5,0}]\) |
|
|
\(\textrm{Saturation}_{B_{s,1}}[1^+_{T_5,\parallel}]\) |
|
|
\(\textrm{Saturation}_{B_{s,1}}[1^+_{T_5,\perp}]\) |
|
|
\(\textrm{Saturation}_{B_{s,1}}[1^+_{T_5}]\) |
|
|
\(\textrm{Saturation}_{D_s^0}[0^-_A]\) |
|
|
\(\textrm{Saturation}_{D_s^*}[1^-_{T,0}]\) |
|
|
\(\textrm{Saturation}_{D_s^*}[1^-_{T,\parallel}]\) |
|
|
\(\textrm{Saturation}_{D_s^*}[1^-_{T,\perp}]\) |
|
|
\(\textrm{Saturation}_{D_s^*}[1^-_T]\) |
|
|
\(\textrm{Saturation}_{D_s^*}[1^-_{V,0}]\) |
|
|
\(\textrm{Saturation}_{D_s^*}[1^-_{V,\perp}]\) |
|
|
\(\textrm{Saturation}_{D_s^*}[1^-_{V,\parallel}]\) |
|
|
\(\textrm{Saturation}_{D_s^*}[1^-_V]\) |
|
|
\(B^{b\to c}_{0^+}\) |
|
|
\(B^{b\to c}_{0^+}\) |
|
|
\(B^{b\to c}_{0^+}\) |
|
|
\(B^{b\to c}_{0^-}\) |
|
|
\(B^{b\to c}_{0^-}\) |
|
|
\(B^{b\to c}_{0^-}\) |
|
|
\(B^{b\to c}_{1^+,T}\) |
|
|
\(B^{b\to c}_{1^+}\) |
|
|
\(B^{b\to c}_{1^+}\) |
|
|
\(B^{b\to c}_{1^+}\) |
|
|
\(B^{b\to c}_{1^-,T}\) |
|
|
\(B^{b\to c}_{1^-}\) |
|
|
\(B^{b\to c}_{1^-}\) |
|
|
\(B^{b\to c}_{1^-}\) |
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 \(0 \to \pi \pi\) 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.
Observables in scattering processes
Observables in \(ee \to c\bar{c}\) processes
Qualified Name |
Description |
Kinematic Variables |
|---|---|---|
|
\(\mathrm{Re}\rho_{D^+D^-}(E))\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\mathrm{Re}\rho_{D^0 \bar{D}^0}(E))\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\Gamma(J/\psi \to ee)\, \left[ \textrm{GeV} \right]\) |
|
|
\(\Gamma(J/\psi \to \textrm{eff})\, \left[ \textrm{GeV} \right]\) |
|
|
\(\Gamma_{J/\psi}\, \left[ \textrm{GeV} \right]\) |
|
|
\(\mathrm{Im}T^{II}(e^+e^- \to D^+ D^-)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\mathrm{Re}T^{II}(e^+e^- \to D^+ D^-)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\sigma(e^+e^- \to D^+ D^-)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\sigma(e^+e^- \to D^+ D^-)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\mathrm{Im}T^{II}(e^+e^- \to D^0 \bar{D}^0)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\mathrm{Re}T^{II}(e^+e^- \to D^0 \bar{D}^0)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\sigma(e^+e^- \to D^0 \bar{D}^0)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\sigma(e^+e^- \to D^0 \bar{D}^0)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(R\) |
|
|
\(\mathrm{Im}T^{II}(e^+e^- \to e^+e^-)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\mathrm{Re}T^{II}(e^+e^- \to e^+e^-)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\sigma(e^+e^- \to e^+e^-)|_{s\textrm{-channel}}\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\sigma(e^+e^- \to e^+e^-)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\mathrm{Im}T^{II}(e^+e^- \to \mathrm{eff})\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\mathrm{Re}T^{II}(e^+e^- \to \mathrm{eff})\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\sigma(e^+e^- \to \textrm{eff})\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\mathrm{Re}\rho_{e^+e^-}(E))\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\mathrm{Re}\rho_{e^+e^-}(E))\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\Gamma(\psi(2S) \to ee)\, \left[ \textrm{GeV} \right]\) |
|
|
\(\Gamma(\psi(2S) \to \textrm{eff})\, \left[ \textrm{GeV} \right]\) |
|
|
\(\Gamma_{\psi(2S)}\, \left[ \textrm{GeV} \right]\) |
|
|
\(\Gamma(\psi(3770) \to D^+ D^-)\, \left[ \textrm{GeV} \right]\) |
|
|
\(\Gamma(\psi(3770) \to D^0\bar{D}^0)\, \left[ \textrm{GeV} \right]\) |
|
|
\(\Gamma(\psi(3770) \to \textrm{eff})\, \left[ \textrm{GeV} \right]\) |
|
|
\(\textrm{spect}_{\psi(3770)}(E)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\Gamma_{\psi(3770)}\, \left[ \textrm{GeV} \right]\) |
The “assume_isospin” option equalises the couplings of isospin-related channels.