List of Observables
The following is a list of observables that is available in EOS v1.0.
Observables in (semi)leptonic \(b\)-hadron decays
Observables in \(B^-\to \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
---|---|---|
|
\(\mathcal{B}(B^- \to \ell^-\bar\nu)\) |
The option “l” selects the charged lepton flavor.
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 |
|
|
\(dP(B\to\pi\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(P(B\to\pi\ell^-\bar\nu)\) |
|
|
\(R_{\pi}\) |
|
|
\(R_{\pi}(q^2)\) |
|
|
\(R_{\pi, 0}\) |
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|
\(R_{\pi, P}\) |
|
|
\(d\mathcal{B}(B\to\pi\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(\Gamma(B\to\pi\ell^-\bar\nu)\) |
|
|
\(\Gamma(B\to\pi\ell^-\bar\nu)_0\) |
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|
\(\Gamma(B\to\pi\ell^-\bar\nu)_p\) |
|
|
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 |
|
|
\(R_D\) |
|
|
\(R_D(q^2)\) |
|
|
\(d\mathcal{B}(B\to \bar{D}\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
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 \(B_s\to \bar{D_s} \ell^-\bar\nu\) 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 |
---|---|---|
|
\(A_{1c}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(A_{1s}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(A_{2c}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(A_{2s}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(A_{3}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(A_{4}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(A_{5}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(A_{6c}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(A_{6s}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(A_{7}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(A_{8}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(A_{9}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(A_{\mathrm{C}}^1(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(A_{\mathrm{C}}^2(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(A_{\mathrm{C}}^3(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(A_{\mathrm{FB}}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{FB}}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(A_{\mathrm{T}}^1(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
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\(A_{\mathrm{T}}^2(B\to \bar{D}^*\ell^-\bar\nu)\) |
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|
\(A_{\mathrm{T}}^3(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
n/a |
|
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\(\mathcal{B}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(\mathcal{B}(B\to \bar{D}^*\ell^-\bar\nu)_{\ell=e,\mu}\) |
|
|
n/a |
|
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\(\Delta\mathcal{B}(B\to \bar{D}^*\ell^-\bar\nu)_{\ell=e,\mu}\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(F_{\mathrm{L}}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
n/a |
|
|
\(\tilde{F}_{\mathrm{L}}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
n/a |
|
|
\(J_{1c}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(J_{1c}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
|
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\(J_{1s}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(J_{1s}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
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\(J_{2c}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(J_{2c}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
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\(J_{2s}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(J_{2s}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
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\(J_{3}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(J_{3}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
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\(J_{4}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(J_{4}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
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\(J_{5}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(J_{5}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
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\(J_{6c}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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|
\(J_{6c}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
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|
\(J_{6s}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(J_{6s}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
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\(J_{7}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(J_{7}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
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\(J_{8}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(J_{8}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
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\(J_{9}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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|
\(J_{9}(B\to \bar{D}^*\ell^-\bar\nu)(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(R_{D^*}\) |
|
|
\(R_{D^*}^{e/\mu}(q^2)\) |
|
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\(R_{D^*}^{\tau/\mu}(q^2)\) |
|
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\(S_{1c}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
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\(S_{1s}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
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\(S_{2c}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(S_{2s}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(S_{3}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(S_{4}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(S_{5}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(S_{6c}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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|
\(S_{6s}(B\to \bar{D}^*\ell^-\bar\nu)\) |
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\(S_{7}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
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\(S_{8}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
\(S_{9}(B\to \bar{D}^*\ell^-\bar\nu)\) |
|
|
n/a |
|
|
\(d\mathcal{B}(B\to \bar{D}^*\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
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n/a |
|
|
n/a |
|
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n/a |
|
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n/a |
|
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n/a |
|
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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 \(B_s\to \bar{K}^* \ell^-\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
---|---|---|
|
\(A_\mathrm{FB}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
|
|
\(A_\mathrm{FB}(B_s\to \bar{K}^*\ell^-\bar\nu)(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
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n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(\mathcal{B}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
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\(F_L(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
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\(F_L(B_s\to \bar{K}^*\ell^-\bar\nu)(q^2)\) |
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\(F_T(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
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\(F_T(B_s\to \bar{K}^*\ell^-\bar\nu)(q^2)\) |
|
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n/a |
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n/a |
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n/a |
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|
n/a |
|
|
n/a |
|
|
n/a |
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n/a |
|
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n/a |
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n/a |
|
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n/a |
|
|
n/a |
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n/a |
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n/a |
|
|
\(\hat{S}_{1c}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
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\(\hat{S}_{1s}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
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\(\hat{S}_{2c}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
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\(\hat{S}_{2s}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
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\(\hat{S}_3(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
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\(\hat{S}_4(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
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\(\hat{S}_5(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
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\(\hat{S}_{6s}(B_s\to \bar{K}^*\ell^-\bar\nu)\) |
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|
\(d\mathcal{B}(B_s\to \bar{K}^*\ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
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 |
---|---|---|
|
\(A_{\mathrm{C}}^1(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{C}}^2(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
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\(A_{\mathrm{C}}^3(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
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|
\(A_{\mathrm{FB}}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
|
\(A_{\mathrm{FB}}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
|
|
n/a |
|
|
n/a |
|
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\(A_{\mathrm{T}}^1(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
|
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\(A_{\mathrm{T}}^2(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
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\(A_{\mathrm{T}}^3(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
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\(\mathcal{B}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
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\(F_{\mathrm{L}}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
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\(J_{1c}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
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\(J_{1c}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
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\(J_{1s}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
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\(J_{1s}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
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\(J_{2c}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
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\(J_{2c}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
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|
\(J_{2s}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
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\(J_{2s}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
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\(J_{3}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
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\(J_{3}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
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|
\(J_{4}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
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\(J_{4}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
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|
\(J_{5}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
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\(J_{5}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
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\(J_{6c}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
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\(J_{6c}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
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|
\(J_{6s}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
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\(J_{6s}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
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|
\(J_{7}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
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\(J_{7}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
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\(J_{8}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
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\(J_{8}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
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\(J_{9}(B_s\to \bar{D}_s^*\ell^-\bar\nu)\) |
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\(J_{9}(B_s\to \bar{D}_s^*\ell^-\bar\nu)(q^2)\) |
|
|
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 \(B\to K \nu\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
---|---|---|
|
\(\mathcal{B}(\bar{B}\to \bar{K}\nu\bar\nu)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(d\mathcal{B}(\bar{B}\to \bar{K}\nu\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
Observables in \(B\to K^* \nu\bar\nu\) decays
Qualified Name |
Description |
Kinematic Variables |
---|---|---|
|
\(\mathcal{B}(\bar{B}\to \bar{K}^*\nu\bar\nu)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(d\mathcal{B}(\bar{B}\to \bar{K}^*\nu\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
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 |
|
|
\(A_\mathrm{FB}(\Lambda_b\to\Lambda_c(2625) \ell^-\bar\nu)\) |
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|
\(A_\mathrm{FB}(\Lambda_b\to\Lambda_c(2625) \ell^-\bar\nu)(q^2)\) |
|
|
\(\mathcal{B}(\Lambda_b\to\Lambda_c(2625) \ell^-\bar\nu)\) |
|
|
n/a |
|
|
\(R_{\Lambda_c(2625)}\) |
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|
\(R_{\Lambda_c(2625)}(q^2)\) |
|
|
\(d\mathcal{B}/dq^2(\Lambda_b\to\Lambda_c(2625) \ell^-\bar\nu)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
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 |
|
|
\(F_0(\Lambda_b\to\Lambda_c \ell^-\bar\nu)(q^2)\) |
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\(K_{1c}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
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|
\(K_{1cc}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
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|
\(K_{1ss}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{2c}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{2cc}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
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|
\(K_{2ss}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
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|
\(K_{3s}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{3sc}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
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|
\(K_{4s}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(K_{4sc}(\Lambda_b\to\Lambda_c(\to \Lambda\pi)\ell^-\bar\nu)\) |
|
|
\(R(A_{\mathrm{FB}}^{\Lambda_c})\) |
|
|
\(R(A_{\mathrm{FB}}^{\Lambda_c})(q^2)\) |
|
|
\(R(\Lambda_c)\) |
|
|
\(d\mathcal{B}(\Lambda_b\to\Lambda_c \ell^-\bar\nu)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
The option “l” selects the charged lepton flavor. The option “form-factors” selects the form factor parametrization.
Miscellaneous
Qualified Name |
Description |
Kinematic Variables |
---|---|---|
|
\(M_{B^*} - M_B\, \left[ \textrm{GeV} \right]\) |
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 \(B_q \to P \ell^+\ell^-\) decays
Qualified Name |
Description |
Kinematic Variables |
---|---|---|
|
\(A_\mathrm{CP}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(A_\mathrm{FB}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(A_\mathrm{FB}(\bar{B}\to \bar{K}\ell^+\ell^-)(q^2)\) |
|
|
\(\bar A_\mathrm{FB}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(\mathcal{B}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(\bar{\mathcal{B}}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(F_\mathrm{H}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(F_\mathrm{H}(\bar{B}\to \bar{K}\ell^+\ell^-)(q^2)\) |
|
|
\(\bar F_\mathrm{H}(\bar{B}\to \bar{K}\ell^+\ell^-)\) |
|
|
\(\Gamma(\bar{B}\to \bar{K}\ell^+\ell^-)\, \left[ \textrm{GeV} \right]\) |
|
|
\(R_K\) |
|
|
\(R_K(q^2)\) |
|
|
\(d\mathcal{B}(\bar{B}\to \bar{K}\ell^+\ell^-)/dq^2\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
\(d^2\mathcal{\Gamma(\bar{B}\to \bar{K}\ell^+\ell^-)}/(dq^2\, d\cos\theta_\ell)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
The option “l” selects the charged lepton flavor. The option “q” selects the spectator quark flavor.
Observables in \(B_q \to V \gamma\) decays
Qualified Name |
Description |
Kinematic Variables |
---|---|---|
|
\(A_\mathrm{CP}(\bar{B}\to \bar{K}^*\gamma)\) |
|
|
\(A_\mathrm{I}(\bar{B}\to \bar{K}^*\gamma)\) |
|
|
\(\mathcal{B}(\bar{B}\to \bar{K}^*\gamma)\) |
|
|
\(\bar{\mathcal{B}}(\bar{B}\to \bar{K}^*\gamma)\) |
|
|
n/a |
|
|
n/a |
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 |
---|---|---|
|
\(A_9(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(\bar{A}_\mathrm{CP}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(A_\mathrm{FB}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(A_\mathrm{FB}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(A_\mathrm{FB}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(\bar{A}_\mathrm{FB}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
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 |
|
|
\(\mathcal{B}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(\bar{\mathcal{B}}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(F_L(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(F_L(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(\bar{F}_L(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(F_T(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(F_T(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(\bar{T}_L(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(\Gamma(\bar{B}\to \bar{K}^*\ell^+\ell^-)\, \left[ \textrm{GeV} \right]\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(J_{1c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_{1c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_{1s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_{1s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_{2c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_{2c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_{2s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_{2s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_3(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_3(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(J_4(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_4(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_5(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_5(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_{6c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_{6c}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_{6s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_{6s}(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_7(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_7(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_8(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_8(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(J_9(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(J_9(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
\(\mathcal{B}(\bar{B}\to \bar{K}^*\ell^+\ell^-)/\mathcal{B}(\bar{B}\to \bar{K}^*J/\psi)\) |
|
|
\(P'_4(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P'_4(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(P'_5(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P'_5(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(P'_6(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(P'_6(\bar{B}\to \bar{K}^*\ell^+\ell^-)(q^2)\) |
|
|
\(R_{K^*}\) |
|
|
\(R_{K^*}(q^2)\) |
|
|
\(S_{1c}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{1s}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{2c}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{2s}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_3(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_3^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_4(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_4^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_5(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_5^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{6c}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_{6s}^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_7(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_7^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_8(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_8^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_9(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(S_9^\mathrm{LHCb}(\bar{B}\to \bar{K}^*\ell^+\ell^-)\) |
|
|
\(d\mathcal{B}/dq^2(\bar{B}\to \bar{K}^*\ell^+\ell^-)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
n/a |
|
|
n/a |
|
|
\(A_5(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(A_{6s}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(A_8(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(A_9(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(A_\mathrm{FB}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(A_\mathrm{FB}(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(A_\mathrm{FB}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(\mathcal{B}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(F_L(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(F_L(\bar{B}_s\to \phi\ell^+\ell^-)(q^2)\) |
|
|
\(\Gamma(\bar{B}_s\to \phi\ell^+\ell^-)\, \left[ \textrm{GeV} \right]\) |
|
|
\(\mathcal{B}(\bar{B}_s\to \phi\ell^+\ell^-)/\mathcal{B}(\bar{B}_s\to\phi J/\psi)\) |
|
|
\(R_\phi\) |
|
|
\(R_{\phi}(q^2)\) |
|
|
\(S_{1c}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_{1s}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_{2c}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_{2s}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_3(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_3^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_4(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_4^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_5(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_5^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_{6c}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_{6s}^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_7(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_7^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_8(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_8^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_9(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(S_9^\mathrm{LHCb}(\bar{B}_s\to \phi\ell^+\ell^-)\) |
|
|
\(d\mathcal{B}/dq^2(\bar{B}_s\to \phi\ell^+\ell^-)\, \left[ \textrm{GeV}^{-2} \right]\) |
|
|
n/a |
|
The option “l” selects the charged lepton flavor. The option “q” selects the spectator quark flavor.
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 |
|
|
\(\mathrm{Im}\mathcal{H}_0^{B \to K}(q^2)\) |
|
|
\(\mathrm{Im}\hat{\mathcal{H}}_0^{B \to K}(q^2)\) |
|
|
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 |
|
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 |
|
|
\(\mathrm{Im}\mathcal{H}_0^{B \to K^*}(q^2)\) |
|
|
\(\mathrm{Im}\mathcal{H}_\parallel^{B \to K^*}(q^2)\) |
|
|
\(\mathrm{Im}\mathcal{H}_\perp^{B \to K^*}(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
|
\(\mathrm{Re}\mathcal{H}_0^{B \to K^*}(q^2)\) |
|
|
\(\mathrm{Re}\mathcal{H}_\parallel^{B \to K^*}(q^2)\) |
|
|
\(\mathrm{Re}\mathcal{H}_\perp^{B \to K^*}(q^2)\) |
|
|
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 |
|
|
\(\mathrm{Re}\mathcal{H}_0^{B_s \to \phi}(q^2)\) |
|
|
\(\mathrm{Re}\mathcal{H}_\parallel^{B_s \to \phi}(q^2)\) |
|
|
\(\mathrm{Re}\mathcal{H}_\perp^{B_s \to \phi}(q^2)\) |
|
|
n/a |
|
|
n/a |
|
|
n/a |
|
The option “q” selects the spectator quark flavor.
Observables in \(B_q \to P \psi\) decays
Qualified Name |
Description |
Kinematic Variables |
---|---|---|
|
\(\mathcal{B}(\bar{B} \to \bar{K}\psi)\) |
The option “q” selects the spectator quark flavor.
Observables in \(B_q \to V \psi\) decays
Qualified Name |
Description |
Kinematic Variables |
---|---|---|
|
\(\mathcal{B}(\bar{B} \to \bar{K}^*\psi)\) |
|
|
\(S_{1c}(\bar{B} \to \bar{K}^*\psi)\) |
|
|
\(S_{1s}(\bar{B} \to \bar{K}^*\psi)\) |
|
|
\(S_{3}(\bar{B} \to \bar{K}^*\psi)\) |
|
|
\(S_{4}(\bar{B} \to \bar{K}^*\psi)\) |
|
|
\(S_{8}(\bar{B} \to \bar{K}^*\psi)\) |
|
|
\(S_{9}(\bar{B} \to \bar{K}^*\psi)\) |
|
|
\(\mathcal{B}(\bar{B}_s \to \phi\psi)\) |
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 \(B \to X_s \lbrace \gamma, \ell^+\ell^-\rbrace\) 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.
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 |
|
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 |
---|---|---|
|
\(F_T(q^2)/F_+(q^2)\) |
|
|
\(F_+^{B\to K}(q^2)\) |
|
|
\(F_T^{B\to K}(q^2)\) |
|
|
\(F_{+,T}(q^2)/F_+(q^2)\) |
|
|
\(f_+^{B\to K}(q^2)\) |
|
|
n/a |
|
|
\(f_-^{B\to K}(q^2)\) |
|
|
\(f_0^{B\to K}(q^2)\) |
|
|
n/a |
|
|
\(f_T^{B\to K}(q^2)\) |
|
|
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 \(B_s\to \bar{K}\) transitions
Qualified Name |
Description |
Kinematic Variables |
---|---|---|
|
\(f_+^{B_s\to \bar{K}}(q^2)\) |
|
|
n/a |
|
|
\(f_-^{B_s\to \bar{K}}(q^2)\) |
|
|
\(f_0^{B_s\to \bar{K}}(q^2)\) |
|
|
n/a |
|
|
\(f_T^{B_s\to \bar{K}}(q^2)\) |
|
|
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 \(B\to \omega\) 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 |
|
|
\(\mathcal{F}_0^{B\to K^*}(q^2)\) |
|
|
\(\mathcal{F}_{0,T}^{B\to K^*}(q^2)\) |
|
|
\(\mathcal{F}_{0,T}(q^2)/\mathcal{F}_0(q^2)\) |
|
|
\(\mathcal{N} \mathcal{F}_{0,T}(q^2)/\mathcal{F}_0(q^2)\) |
|
|
n/a |
|
|
\(\mathcal{F}_\parallel^{B\to K^*}(q^2)\) |
|
|
\(\mathcal{F}_{\parallel,T}^{B\to K^*}(q^2)\) |
|
|
\(\mathcal{F}_{\parallel,T}(q^2)/\mathcal{F}_\parallel(q^2)\) |
|
|
\(\mathcal{F}_\perp^{B\to K^*}(q^2)\) |
|
|
\(\mathcal{F}_{\perp,T}^{B\to K^*}(q^2)\) |
|
|
\(\mathcal{F}_{\perp,T}(q^2)/\mathcal{F}_\perp(q^2)\) |
|
|
\(T_1^{B\to K^*}(q^2)\) |
|
|
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 |
---|---|---|
|
\(V^{B\to D^*}(q^2)\) |
|
|
\(A_1^{B\to D^*}(q^2)\) |
|
|
\(A_{12}^{B\to D^*}(q^2)\) |
|
|
\(A_{12}(q^2)/A_1(q^2)\) |
|
|
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 |
|
|
\(a_0^{A_1}\) |
|
|
\(a_0^{A_5}\) |
|
|
\(a_0^{P_1}\) |
|
|
\(a_0^{V_4}\) |
|
|
\(a_1^{A_1}/a_0^{A_1}\) |
|
|
\(a_1^{A_5}/a_0^{A_5}\) |
|
|
\(a_1^{P_1}/a_0^{P_1}\) |
|
|
\(a_1^{V_4}/a_0^{V_4}\) |
|
|
\(a_1^{A_1}\) |
|
|
\(a_1^{A_5}\) |
|
|
\(a_1^{P_1}\) |
|
|
\(a_1^{V_4}\) |
|
|
\(a_2^{A_1}/a_0^{A_1}\) |
|
|
\(a_2^{A_5}/a_0^{A_5}\) |
|
|
\(a_2^{P_1}/a_0^{P_1}\) |
|
|
\(a_2^{V_4}/a_0^{V_4}\) |
|
|
\(a_2^{A_1}\) |
|
|
\(a_2^{A_5}\) |
|
|
\(a_2^{P_1}\) |
|
|
\(a_2^{V_4}\) |
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 |
|
|
\(\mathcal{F}_0^{B_s\to \phi}(q^2)\) |
|
|
\(\mathcal{F}_{0,T}^{B_s\to \phi}(q^2)\) |
|
|
\(\mathcal{F}_{0,T}(q^2)/\mathcal{F}_0(q^2)\) |
|
|
\(\mathcal{N} \mathcal{F}_{0,T}(q^2)/\mathcal{F}_0(q^2)\) |
|
|
n/a |
|
|
\(\mathcal{F}_\parallel^{B_s\to \phi}(q^2)\) |
|
|
\(\mathcal{F}_{\parallel,T}^{B_s\to \phi}(q^2)\) |
|
|
\(\mathcal{F}_{\parallel,T}(q^2)/\mathcal{F}_\parallel(q^2)\) |
|
|
\(\mathcal{F}_\perp^{B_s\to \phi}(q^2)\) |
|
|
\(\mathcal{F}_{\perp,T}^{B_s\to \phi}(q^2)\) |
|
|
\(\mathcal{F}_{\perp,T}(q^2)/\mathcal{F}_\perp(q^2)\) |
|
|
\(T_1^{B_s\to \phi}(q^2)\) |
|
|
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 |
|
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 |
---|---|---|
|
\(f_0^{A,\Lambda_b\to\Lambda}(q^2)\) |
|
|
\(f_0^{T,\Lambda_b\to\Lambda}(q^2)\) |
|
|
\(f_0^{T5,\Lambda_b\to\Lambda}(q^2)\) |
|
|
\(f_0^{V,\Lambda_b\to\Lambda}(q^2)\) |
|
|
\(f_\perp^{A,\Lambda_b\to\Lambda}(q^2)\) |
|
|
\(f_\perp^{T,\Lambda_b\to\Lambda}(q^2)\) |
|
|
\(f_\perp^{T5,\Lambda_b\to\Lambda}(q^2)\) |
|
|
\(f_\perp^{V,\Lambda_b\to\Lambda}(q^2)\) |
|
|
\(f_t^{A,\Lambda_b\to\Lambda}(q^2)\) |
|
|
\(f_t^{V,\Lambda_b\to\Lambda}(q^2)\) |
|
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.
Unitarity Bounds
Qualified Name |
Description |
Kinematic Variables |
---|---|---|
|
\(B^{b\to c}_{0^+}\) |
|
|
\(B^{b\to c}_{0^+}\) |
|
|
\(B^{b\to c}_{0^+}\) |
|
|
\(B^{b\to c}_{0^-}\) |
|
|
\(B^{b\to c}_{0^-}\) |
|
|
\(B^{b\to c}_{0^-}\) |
|
|
\(B^{b\to c}_{1^+}\) |
|
|
\(B^{b\to c}_{1^+}\) |
|
|
\(B^{b\to c}_{1^+}\) |
|
|
\(B^{b\to c}_{1^-}\) |
|
|
\(B^{b\to c}_{1^-}\) |
|
|
\(B^{b\to c}_{1^-}\) |
|
|
\(B^{b\to c}_{0^+}\) |
|
|
\(B^{b\to c}_{0^+}\) |
|
|
\(B^{b\to c}_{0^-}\) |
|
|
\(B^{b\to c}_{0^-}\) |
|
|
\(B^{b\to c}_{1^+}\) |
|
|
\(B^{b\to c}_{1^+}\) |
|
|
\(B^{b\to c}_{1^-}\) |
|
|
\(B^{b\to c}_{1^-}\) |
Pseudo observables arising in the various unitarity bounds for \(b\to c\) semileptonic form factors.
Observables in neutral meson mixing
Observables in \(B_s\)–\(\bar{B}_s\) mixing
Qualified Name |
Description |
Kinematic Variables |
---|---|---|
|
\(\Delta M_s(B_s\leftrightarrow \bar{B}_s)\, \left[ \textrm{ps}^{-1} \right]\) |