This is an automatically generated list of all parameters defined in the default configuration of flavio. The first column contains the string name of the parameter.
| Name | Symbol | Description |
|---|---|---|
B+->K*+ deltaC7 a_+ Im |
$\text{Im}\,a^{\Delta_7}_+$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at low $q^2$ |
B+->K*+ deltaC7 a_+ Re |
$\text{Re}\,a^{\Delta_7}_+$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at low $q^2$ |
B+->K*+ deltaC7 a_- Im |
$\text{Im}\,a^{\Delta_7}_-$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at low $q^2$ |
B+->K*+ deltaC7 a_- Re |
$\text{Re}\,a^{\Delta_7}_-$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at low $q^2$ |
B+->K*+ deltaC7 a_0 Im |
$\text{Im}\,a^{\Delta_7}_0$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at low $q^2$ |
B+->K*+ deltaC7 a_0 Re |
$\text{Re}\,a^{\Delta_7}_0$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at low $q^2$ |
B+->K*+ deltaC7 b_+ Im |
$\text{Im}\,b^{\Delta_7}_+$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at low $q^2$ |
B+->K*+ deltaC7 b_+ Re |
$\text{Re}\,b^{\Delta_7}_+$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at low $q^2$ |
B+->K*+ deltaC7 b_- Im |
$\text{Im}\,b^{\Delta_7}_-$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at low $q^2$ |
B+->K*+ deltaC7 b_- Re |
$\text{Re}\,b^{\Delta_7}_-$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at low $q^2$ |
B+->K*+ deltaC7 b_0 Im |
$\text{Im}\,b^{\Delta_7}_0$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at low $q^2$ |
B+->K*+ deltaC7 b_0 Re |
$\text{Re}\,b^{\Delta_7}_0$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at low $q^2$ |
B+->K*+ deltaC7p a_+ Im |
$\text{Im}\,a^{\Delta_7^\prime}_+$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at low $q^2$ |
B+->K*+ deltaC7p a_+ Re |
$\text{Re}\,a^{\Delta_7^\prime}_+$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at low $q^2$ |
B+->K*+ deltaC7p b_+ Im |
$\text{Im}\,b^{\Delta_7^\prime}_+$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at low $q^2$ |
B+->K*+ deltaC7p b_+ Re |
$\text{Re}\,b^{\Delta_7^\prime}_+$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at low $q^2$ |
B+->K*+ deltaC9 a_0 Im |
$\text{Im}\,a^{\Delta_9}_0$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at low $q^2$ |
B+->K*+ deltaC9 a_0 Re |
$\text{Re}\,a^{\Delta_9}_0$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at low $q^2$ |
B+->K*+ deltaC9 b_0 Im |
$\text{Im}\,b^{\Delta_9}_0$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at low $q^2$ |
B+->K*+ deltaC9 b_0 Re |
$\text{Re}\,b^{\Delta_9}_0$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at low $q^2$ |
B+->K*+ deltaC9 c_+ Im |
$\text{Im}\,c^{\Delta_9}_+$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at high $q^2$ |
B+->K*+ deltaC9 c_+ Re |
$\text{Re}\,c^{\Delta_9}_+$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at high $q^2$ |
B+->K*+ deltaC9 c_- Im |
$\text{Im}\,c^{\Delta_9}_-$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at high $q^2$ |
B+->K*+ deltaC9 c_- Re |
$\text{Re}\,c^{\Delta_9}_-$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at high $q^2$ |
B+->K*+ deltaC9 c_0 Im |
$\text{Im}\,c^{\Delta_9}_0$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at high $q^2$ |
B+->K*+ deltaC9 c_0 Re |
$\text{Re}\,c^{\Delta_9}_0$ | Parameter for subleading hadronic effects in $B^+\to K^{*+}\ell^+\ell^-$ at high $q^2$ |
B+->K+ deltaC9 a Im |
$\text{Im}\,a^{\Delta_9}$ | Parameter for subleading hadronic effects in $B^+\to K^+\ell^+\ell^-$ at low $q^2$ |
B+->K+ deltaC9 a Re |
$\text{Re}\,a^{\Delta_9}$ | Parameter for subleading hadronic effects in $B^+\to K^+\ell^+\ell^-$ at low $q^2$ |
B+->K+ deltaC9 b Im |
$\text{Im}\,b^{\Delta_9}$ | Parameter for subleading hadronic effects in $B^+\to K^+\ell^+\ell^-$ at low $q^2$ |
B+->K+ deltaC9 b Re |
$\text{Re}\,b^{\Delta_9}$ | Parameter for subleading hadronic effects in $B^+\to K^+\ell^+\ell^-$ at low $q^2$ |
B+->K+ deltaC9 c Im |
$\text{Im}\,c^{\Delta_9}$ | Parameter for subleading hadronic effects in $B^+\to K^+\ell^+\ell^-$ at low $q^2$ |
B+->K+ deltaC9 c Re |
$\text{Re}\,c^{\Delta_9}$ | Parameter for subleading hadronic effects in $B^+\to K^+\ell^+\ell^-$ at high $q^2$ |
B->D BCL a0_f+ |
$a_0^{(+)}$ | BCL $B\to D$ form factor parametrization coefficient $a_0$ of $f_+$ |
B->D BCL a0_f0 |
$a_0^{(0)}$ | BCL $B\to D$ form factor parametrization coefficient $a_0$ of $f_0$ |
B->D BCL a1_f+ |
$a_1^{(+)}$ | BCL $B\to D$ form factor parametrization coefficient $a_1$ of $f_+$ |
B->D BCL a1_f0 |
$a_1^{(0)}$ | BCL $B\to D$ form factor parametrization coefficient $a_1$ of $f_0$ |
B->D BCL a2_f+ |
$a_2^{(+)}$ | BCL $B\to D$ form factor parametrization coefficient $a_2$ of $f_+$ |
B->D BCL a2_f0 |
$a_2^{(0)}$ | BCL $B\to D$ form factor parametrization coefficient $a_2$ of $f_0$ |
B->D BCL m+ |
$m_{B^*}^{f_+}$ | Resonance mass for the $B\to D$ vector and tensor form factors in BCL parametrization |
B->D BCL m0 |
$m_{B^*}^{f_0}$ | Resonance mass for the $B\to D$ scalar form factor in BCL parametrization |
B->D IW a_T |
$a_T^{B\to D}$ | Relative power correction to the $B\to D$ tensor form factor from the improved Isgur-Wise relation |
B->D* BCL m0 |
$m_{B^*}^{A_0}$ | Resonance mass for the $B\to D^*$ scalar form factor in BCL or BSZ parametrization |
B->D* BCL m1+ |
$m_{B^*}^{1^+}$ | Resonance mass for the $B\to D^*$ form factors $A_{12}$ and $T_{2,23}$ in BCL or BSZ parametrization |
B->D* BCL m1- |
$m_{B^*}^{1^-}$ | Resonance mass for the $B\to D^*$ form factors $V$ and $T_1$ in BCL or BSZ parametrization |
B->D* CLN R_0(1) |
$R_0(1)$ | Ratio of CLN form factors at $w=1$ |
B->D* CLN R_1(1) |
$R_1(1)$ | Ratio of CLN form factors at $w=1$ |
B->D* CLN R_2(1) |
$R_2(1)$ | Ratio of CLN form factors at $w=1$ |
B->D* CLN h_A1(1) |
$h_{A_1}(1)$ | Universal CLN form factor at $w=1$ |
B->D* CLN rho2 |
$\rho^2$ | Shape parameter in the CLN form factor parametrization |
B->D* IW a_T1 |
$a_{T_1}^{B\to D^*}$ | Relative power correction to the $B\to D^*$ tensor form factor $T_1$ from the improved Isgur-Wise relation |
B->D* IW a_T2 |
$a_{T_2}^{B\to D^*}$ | Relative power correction to the $B\to D^*$ tensor form factor $T_2$ from the improved Isgur-Wise relation |
B->D* IW a_T23 |
$a_{T_{23}}^{B\to D^*}$ | Relative power correction to the $B\to D^*$ tensor form factor $T_{23}$ from the improved Isgur-Wise relation |
B->K BCL a0_f+ |
$a_0^{(+)}$ | BCL $B\to K$ form factor parametrization coefficient $a_0$ of $f_+$ |
B->K BCL a0_f0 |
$a_0^{(0)}$ | BCL $B\to K$ form factor parametrization coefficient $a_0$ of $f_0$ |
B->K BCL a0_fT |
$a_0^{(T)}$ | BCL $B\to K$ form factor parametrization coefficient $a_0$ of $f_T$ |
B->K BCL a1_f+ |
$a_1^{(+)}$ | BCL $B\to K$ form factor parametrization coefficient $a_1$ of $f_+$ |
B->K BCL a1_f0 |
$a_1^{(0)}$ | BCL $B\to K$ form factor parametrization coefficient $a_1$ of $f_0$ |
B->K BCL a1_fT |
$a_1^{(T)}$ | BCL $B\to K$ form factor parametrization coefficient $a_1$ of $f_T$ |
B->K BCL a2_f+ |
$a_2^{(+)}$ | BCL $B\to K$ form factor parametrization coefficient $a_2$ of $f_+$ |
B->K BCL a2_f0 |
$a_2^{(0)}$ | BCL $B\to K$ form factor parametrization coefficient $a_2$ of $f_0$ |
B->K BCL a2_fT |
$a_2^{(T)}$ | BCL $B\to K$ form factor parametrization coefficient $a_2$ of $f_T$ |
B->K BCL m+ |
$m_{B^*}^{f_+}$ | Resonance mass for the $B\to K$ vector and tensor form factors in BCL parametrization |
B->K BCL m0 |
$m_{B^*}^{f_0}$ | Resonance mass for the $B\to K$ scalar form factor in BCL parametrization |
B->K* BCL m0 |
$m_{B^*}^{A_0}$ | Resonance mass for the $B\to K^*$ scalar form factor in BCL or BSZ parametrization |
B->K* BCL m1+ |
$m_{B^*}^{1^+}$ | Resonance mass for the $B\to K^*$ form factors $A_{12}$ and $T_{2,23}$ in BCL or BSZ parametrization |
B->K* BCL m1- |
$m_{B^*}^{1^-}$ | Resonance mass for the $B\to K^*$ form factors $V$ and $T_1$ in BCL or BSZ parametrization |
B->K* BSZ a0_A0 |
$a_0^{A_0}$ | BSZ form factor parametrization coefficient $a_0$ of $A_0$ |
B->K* BSZ a0_A1 |
$a_0^{A_1}$ | BSZ form factor parametrization coefficient $a_0$ of $A_1$ |
B->K* BSZ a0_T1 |
$a_0^{T_1}$ | BSZ form factor parametrization coefficient $a_0$ of $T_1$ |
B->K* BSZ a0_T23 |
$a_0^{T_{23}}$ | BSZ form factor parametrization coefficient $a_0$ of $T_{23}$ |
B->K* BSZ a0_V |
$a_0^{V}$ | BSZ form factor parametrization coefficient $a_0$ of $V$ |
B->K* BSZ a1_A0 |
$a_1^{A_0}$ | BSZ form factor parametrization coefficient $a_1$ of $A_0$ |
B->K* BSZ a1_A1 |
$a_1^{A_1}$ | BSZ form factor parametrization coefficient $a_1$ of $A_1$ |
B->K* BSZ a1_A12 |
$a_1^{A_{12}}$ | BSZ form factor parametrization coefficient $a_1$ of $A_{12}$ |
B->K* BSZ a1_T1 |
$a_1^{T_1}$ | BSZ form factor parametrization coefficient $a_1$ of $T_1$ |
B->K* BSZ a1_T2 |
$a_1^{T_2}$ | BSZ form factor parametrization coefficient $a_1$ of $T_2$ |
B->K* BSZ a1_T23 |
$a_1^{T_{23}}$ | BSZ form factor parametrization coefficient $a_1$ of $T_{23}$ |
B->K* BSZ a1_V |
$a_1^{V}$ | BSZ form factor parametrization coefficient $a_1$ of $V$ |
B->K* BSZ a2_A0 |
$a_2^{A_0}$ | BSZ form factor parametrization coefficient $a_2$ of $A_0$ |
B->K* BSZ a2_A1 |
$a_2^{A_1}$ | BSZ form factor parametrization coefficient $a_2$ of $A_1$ |
B->K* BSZ a2_A12 |
$a_2^{A_{12}}$ | BSZ form factor parametrization coefficient $a_2$ of $A_{12}$ |
B->K* BSZ a2_T1 |
$a_2^{T_1}$ | BSZ form factor parametrization coefficient $a_2$ of $T_1$ |
B->K* BSZ a2_T2 |
$a_2^{T_2}$ | BSZ form factor parametrization coefficient $a_2$ of $T_2$ |
B->K* BSZ a2_T23 |
$a_2^{T_{23}}$ | BSZ form factor parametrization coefficient $a_2$ of $T_{23}$ |
B->K* BSZ a2_V |
$a_2^{V}$ | BSZ form factor parametrization coefficient $a_2$ of $V$ |
B->gamma KM betaa |
$\beta_a$ | beta parameter for Fa form factor in KM parametrization |
B->gamma KM betata |
$\beta_{ta}$ | beta parameter for Fta form factor in KM parametrization |
B->gamma KM betatv |
$\beta_{tv}$ | beta parameter for Ftv form factor in KM parametrization |
B->gamma KM betav |
$\beta_v$ | beta parameter for Fv form factor in KM parametrization |
B->gamma KM deltaa |
$\Delta_a$ | Delta parameter for Fa form factor in KM parametrization |
B->gamma KM deltata |
$\Delta_{ta}$ | Delta parameter for Fta form factor in KM parametrization |
B->gamma KM deltatv |
$\Delta_{tv}$ | Delta parameter for Ftv form factor in KM parametrization |
B->gamma KM deltav |
$\Delta_v$ | Delta parameter for Fv form factor in KM parametrization |
B->omega BCL m0 |
$m_{B^*}^{A_0}$ | Resonance mass for the $B\to \omega$ scalar form factor in BCL or BSZ parametrization |
B->omega BCL m1+ |
$m_{B^*}^{1^+}$ | Resonance mass for the $B\to \omega$ form factors $A_{12}$ and $T_{2,23}$ in BCL or BSZ parametrization |
B->omega BCL m1- |
$m_{B^*}^{1^-}$ | Resonance mass for the $B\to \omega$ form factors $V$ and $T_1$ in BCL or BSZ parametrization |
B->omega BSZ a0_A0 |
$a_0^{A_0}$ | BSZ form factor parametrization coefficient $a_0$ of $A_0$ |
B->omega BSZ a0_A1 |
$a_0^{A_1}$ | BSZ form factor parametrization coefficient $a_0$ of $A_1$ |
B->omega BSZ a0_T1 |
$a_0^{T_1}$ | BSZ form factor parametrization coefficient $a_0$ of $T_1$ |
B->omega BSZ a0_T23 |
$a_0^{T_{23}}$ | BSZ form factor parametrization coefficient $a_0$ of $T_{23}$ |
B->omega BSZ a0_V |
$a_0^{V}$ | BSZ form factor parametrization coefficient $a_0$ of $V$ |
B->omega BSZ a1_A0 |
$a_1^{A_0}$ | BSZ form factor parametrization coefficient $a_1$ of $A_0$ |
B->omega BSZ a1_A1 |
$a_1^{A_1}$ | BSZ form factor parametrization coefficient $a_1$ of $A_1$ |
B->omega BSZ a1_A12 |
$a_1^{A_{12}}$ | BSZ form factor parametrization coefficient $a_1$ of $A_{12}$ |
B->omega BSZ a1_T1 |
$a_1^{T_1}$ | BSZ form factor parametrization coefficient $a_1$ of $T_1$ |
B->omega BSZ a1_T2 |
$a_1^{T_2}$ | BSZ form factor parametrization coefficient $a_1$ of $T_2$ |
B->omega BSZ a1_T23 |
$a_1^{T_{23}}$ | BSZ form factor parametrization coefficient $a_1$ of $T_{23}$ |
B->omega BSZ a1_V |
$a_1^{V}$ | BSZ form factor parametrization coefficient $a_1$ of $V$ |
B->omega BSZ a2_A0 |
$a_2^{A_0}$ | BSZ form factor parametrization coefficient $a_2$ of $A_0$ |
B->omega BSZ a2_A1 |
$a_2^{A_1}$ | BSZ form factor parametrization coefficient $a_2$ of $A_1$ |
B->omega BSZ a2_A12 |
$a_2^{A_{12}}$ | BSZ form factor parametrization coefficient $a_2$ of $A_{12}$ |
B->omega BSZ a2_T1 |
$a_2^{T_1}$ | BSZ form factor parametrization coefficient $a_2$ of $T_1$ |
B->omega BSZ a2_T2 |
$a_2^{T_2}$ | BSZ form factor parametrization coefficient $a_2$ of $T_2$ |
B->omega BSZ a2_T23 |
$a_2^{T_{23}}$ | BSZ form factor parametrization coefficient $a_2$ of $T_{23}$ |
B->omega BSZ a2_V |
$a_2^{V}$ | BSZ form factor parametrization coefficient $a_2$ of $V$ |
B->pi BCL LMVD m+ |
$m_{B^*}^{f_+}$ | Resonance mass for the $B\to \pi$ vector and tensor form factors in BCL parametrization from LMVD |
B->pi BCL LMVD m0 |
$m_{B^*}^{f_0}$ | Resonance mass for the $B\to \pi$ scalar form factor in BCL parametrization from LMVD |
B->pi BCL LMVD m_B+ |
$m_{B^+}$ | B+ mass for the $B\to \pi$ form factors in BCL parametrization from LMVD |
B->pi BCL LMVD m_pi0 |
$m_{\pi^0}$ | pi0 mass for the $B\to \pi$ form factors in BCL parametrization from LMVD |
B->pi BCL a0_f+ |
$a_0^{(+)}$ | BCL $B\to \pi$ form factor parametrization coefficient $a_0$ of $f_+$ |
B->pi BCL a0_f0 |
$a_0^{(0)}$ | BCL $B\to \pi$ form factor parametrization coefficient $a_0$ of $f_0$ |
B->pi BCL a0_fT |
$a_0^{(T)}$ | BCL $B\to \pi$ form factor parametrization coefficient $a_0$ of $f_T$ |
B->pi BCL a1_f+ |
$a_1^{(+)}$ | BCL $B\to \pi$ form factor parametrization coefficient $a_1$ of $f_+$ |
B->pi BCL a1_f0 |
$a_1^{(0)}$ | BCL $B\to \pi$ form factor parametrization coefficient $a_1$ of $f_0$ |
B->pi BCL a1_fT |
$a_1^{(T)}$ | BCL $B\to \pi$ form factor parametrization coefficient $a_1$ of $f_T$ |
B->pi BCL a2_f+ |
$a_2^{(+)}$ | BCL $B\to \pi$ form factor parametrization coefficient $a_2$ of $f_+$ |
B->pi BCL a2_f0 |
$a_2^{(0)}$ | BCL $B\to \pi$ form factor parametrization coefficient $a_2$ of $f_0$ |
B->pi BCL a2_fT |
$a_2^{(T)}$ | BCL $B\to \pi$ form factor parametrization coefficient $a_2$ of $f_T$ |
B->pi BCL a3_f+ |
$a_3^{(+)}$ | BCL $B\to \pi$ form factor parametrization coefficient $a_3$ of $f_+$ |
B->pi BCL a3_f0 |
$a_3^{(0)}$ | BCL $B\to \pi$ form factor parametrization coefficient $a_3$ of $f_T$ |
B->pi BCL a3_fT |
$a_3^{(T)}$ | BCL $B\to \pi$ form factor parametrization coefficient $a_3$ of $f_T$ |
B->pi BCL b_+^1 |
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B->pi BCL b_+^2 |
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B->pi BCL b_+^3 |
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B->pi BCL b_0^1 |
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B->pi BCL b_0^2 |
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B->pi BCL b_0^3 |
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B->pi BCL b_0^4 |
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B->pi BCL b_T^1 |
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B->pi BCL b_T^2 |
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B->pi BCL b_T^3 |
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B->pi BCL f_+(0) |
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B->pi BCL f_T(0) |
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B->pi BCL m+ |
$m_{B^*}^{f_+}$ | Resonance mass for the $B\to \pi$ vector and tensor form factors in BCL parametrization |
B->pi BCL m0 |
$m_{B^*}^{f_0}$ | Resonance mass for the $B\to \pi$ scalar form factor in BCL parametrization |
B->pi IW a_T |
$a_T^{B\to \pi}$ | Relative power correction to the $B\to \pi$ tensor form factor from the improved Isgur-Wise relation |
B->rho BCL m0 |
$m_{B^*}^{A_0}$ | Resonance mass for the $B\to \rho$ scalar form factor in BCL or BSZ parametrization |
B->rho BCL m1+ |
$m_{B^*}^{1^+}$ | Resonance mass for the $B\to \rho$ form factors $A_{12}$ and $T_{2,23}$ in BCL or BSZ parametrization |
B->rho BCL m1- |
$m_{B^*}^{1^-}$ | Resonance mass for the $B\to \rho$ form factors $V$ and $T_1$ in BCL or BSZ parametrization |
B->rho BSZ a0_A0 |
$a_0^{A_0}$ | BSZ form factor parametrization coefficient $a_0$ of $A_0$ |
B->rho BSZ a0_A1 |
$a_0^{A_1}$ | BSZ form factor parametrization coefficient $a_0$ of $A_1$ |
B->rho BSZ a0_T1 |
$a_0^{T_1}$ | BSZ form factor parametrization coefficient $a_0$ of $T_1$ |
B->rho BSZ a0_T23 |
$a_0^{T_{23}}$ | BSZ form factor parametrization coefficient $a_0$ of $T_{23}$ |
B->rho BSZ a0_V |
$a_0^{V}$ | BSZ form factor parametrization coefficient $a_0$ of $V$ |
B->rho BSZ a1_A0 |
$a_1^{A_0}$ | BSZ form factor parametrization coefficient $a_1$ of $A_0$ |
B->rho BSZ a1_A1 |
$a_1^{A_1}$ | BSZ form factor parametrization coefficient $a_1$ of $A_1$ |
B->rho BSZ a1_A12 |
$a_1^{A_{12}}$ | BSZ form factor parametrization coefficient $a_1$ of $A_{12}$ |
B->rho BSZ a1_T1 |
$a_1^{T_1}$ | BSZ form factor parametrization coefficient $a_1$ of $T_1$ |
B->rho BSZ a1_T2 |
$a_1^{T_2}$ | BSZ form factor parametrization coefficient $a_1$ of $T_2$ |
B->rho BSZ a1_T23 |
$a_1^{T_{23}}$ | BSZ form factor parametrization coefficient $a_1$ of $T_{23}$ |
B->rho BSZ a1_V |
$a_1^{V}$ | BSZ form factor parametrization coefficient $a_1$ of $V$ |
B->rho BSZ a2_A0 |
$a_2^{A_0}$ | BSZ form factor parametrization coefficient $a_2$ of $A_0$ |
B->rho BSZ a2_A1 |
$a_2^{A_1}$ | BSZ form factor parametrization coefficient $a_2$ of $A_1$ |
B->rho BSZ a2_A12 |
$a_2^{A_{12}}$ | BSZ form factor parametrization coefficient $a_2$ of $A_{12}$ |
B->rho BSZ a2_T1 |
$a_2^{T_1}$ | BSZ form factor parametrization coefficient $a_2$ of $T_1$ |
B->rho BSZ a2_T2 |
$a_2^{T_2}$ | BSZ form factor parametrization coefficient $a_2$ of $T_2$ |
B->rho BSZ a2_T23 |
$a_2^{T_{23}}$ | BSZ form factor parametrization coefficient $a_2$ of $T_{23}$ |
B->rho BSZ a2_V |
$a_2^{V}$ | BSZ form factor parametrization coefficient $a_2$ of $V$ |
B0->K*0 deltaC7 a_+ Im |
$\text{Im}\,a^{\Delta_7}_+$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at low $q^2$ |
B0->K*0 deltaC7 a_+ Re |
$\text{Re}\,a^{\Delta_7}_+$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at low $q^2$ |
B0->K*0 deltaC7 a_- Im |
$\text{Im}\,a^{\Delta_7}_-$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at low $q^2$ |
B0->K*0 deltaC7 a_- Re |
$\text{Re}\,a^{\Delta_7}_-$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at low $q^2$ |
B0->K*0 deltaC7 a_0 Im |
$\text{Im}\,a^{\Delta_7}_0$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at low $q^2$ |
B0->K*0 deltaC7 a_0 Re |
$\text{Re}\,a^{\Delta_7}_0$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at low $q^2$ |
B0->K*0 deltaC7 b_+ Im |
$\text{Im}\,b^{\Delta_7}_+$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at low $q^2$ |
B0->K*0 deltaC7 b_+ Re |
$\text{Re}\,b^{\Delta_7}_+$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at low $q^2$ |
B0->K*0 deltaC7 b_- Im |
$\text{Im}\,b^{\Delta_7}_-$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at low $q^2$ |
B0->K*0 deltaC7 b_- Re |
$\text{Re}\,b^{\Delta_7}_-$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at low $q^2$ |
B0->K*0 deltaC7 b_0 Im |
$\text{Im}\,b^{\Delta_7}_0$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at low $q^2$ |
B0->K*0 deltaC7 b_0 Re |
$\text{Re}\,b^{\Delta_7}_0$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at low $q^2$ |
B0->K*0 deltaC7p a_+ Im |
$\text{Im}\,a^{\Delta_7^\prime}_+$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at low $q^2$ |
B0->K*0 deltaC7p a_+ Re |
$\text{Re}\,a^{\Delta_7^\prime}_+$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at low $q^2$ |
B0->K*0 deltaC7p b_+ Im |
$\text{Im}\,b^{\Delta_7^\prime}_+$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at low $q^2$ |
B0->K*0 deltaC7p b_+ Re |
$\text{Re}\,b^{\Delta_7^\prime}_+$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at low $q^2$ |
B0->K*0 deltaC9 a_0 Im |
$\text{Im}\,a^{\Delta_9}_0$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at low $q^2$ |
B0->K*0 deltaC9 a_0 Re |
$\text{Re}\,a^{\Delta_9}_0$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at low $q^2$ |
B0->K*0 deltaC9 b_0 Im |
$\text{Im}\,b^{\Delta_9}_0$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at low $q^2$ |
B0->K*0 deltaC9 b_0 Re |
$\text{Re}\,b^{\Delta_9}_0$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at low $q^2$ |
B0->K*0 deltaC9 c_+ Im |
$\text{Im}\,c^{\Delta_9}_+$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at high $q^2$ |
B0->K*0 deltaC9 c_+ Re |
$\text{Re}\,c^{\Delta_9}_+$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at high $q^2$ |
B0->K*0 deltaC9 c_- Im |
$\text{Im}\,c^{\Delta_9}_-$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at high $q^2$ |
B0->K*0 deltaC9 c_- Re |
$\text{Re}\,c^{\Delta_9}_-$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at high $q^2$ |
B0->K*0 deltaC9 c_0 Im |
$\text{Im}\,c^{\Delta_9}_0$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at high $q^2$ |
B0->K*0 deltaC9 c_0 Re |
$\text{Re}\,c^{\Delta_9}_0$ | Parameter for subleading hadronic effects in $B^0\to K^{*0}\ell^+\ell^-$ at high $q^2$ |
B0->K0 deltaC9 a Im |
$\text{Im}\,a^{\Delta_9}$ | Parameter for subleading hadronic effects in $B^0\to K^0\ell^+\ell^-$ at low $q^2$ |
B0->K0 deltaC9 a Re |
$\text{Re}\,a^{\Delta_9}$ | Parameter for subleading hadronic effects in $B^0\to K^0\ell^+\ell^-$ at low $q^2$ |
B0->K0 deltaC9 b Im |
$\text{Im}\,b^{\Delta_9}$ | Parameter for subleading hadronic effects in $B^0\to K^0\ell^+\ell^-$ at low $q^2$ |
B0->K0 deltaC9 b Re |
$\text{Re}\,b^{\Delta_9}$ | Parameter for subleading hadronic effects in $B^0\to K^0\ell^+\ell^-$ at low $q^2$ |
B0->K0 deltaC9 c Im |
$\text{Im}\,c^{\Delta_9}$ | Parameter for subleading hadronic effects in $B^0\to K^0\ell^+\ell^-$ at high $q^2$ |
B0->K0 deltaC9 c Re |
$\text{Re}\,c^{\Delta_9}$ | Parameter for subleading hadronic effects in $B^0\to K^0\ell^+\ell^-$ at high $q^2$ |
BR(B->Xcenu)_exp |
$\text{BR}(B\to X_ce\nu)_\text{exp}$ | Experimental branching ratio of $B\to X_ce\nu$ |
BR(Lambda(1520)->NKbar)_exp |
$\text{BR}(\Lambda(1520)\to N\bar{K})_\text{exp}$ | Experimental branching ratio of $\Lambda(1520)\to N\bar{K}$ |
BR(tau->enunu) |
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BR(tau->mununu) |
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BR(tau->rhonu) |
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BR_exp(J/psi->ee) |
$BR_{\rm exp}(J/\psi\to e^+ e^-)$ | measured branching ratio $J/\psi\to ee$ |
BR_exp(Upsilon(1S)->ee) |
$BR_{\rm exp}(\Upsilon(1S)\to e^+ e^-)$ | measured branching ratio $\Upsilon(1S)\to ee$ |
BR_exp(Upsilon(2S)->ee) |
$BR_{\rm exp}(\Upsilon(2S)\to e^+ e^-)$ | measured branching ratio $\Upsilon(2S)\to ee$ |
BR_exp(Upsilon(3S)->ee) |
$BR_{\rm exp}(\Upsilon(3S)\to e^+ e^-)$ | measured branching ratio $\Upsilon(3S)\to ee$ |
BR_exp(psi(2S)->ee) |
$BR_{\rm exp}(\psi(2S)\to e^+ e^-)$ | measured branching ratio $\psi(2S)\to ee$ |
Bs->K BCL a0_f+ |
$a_0^{(+)}$ | BCL $B_s\to K$ form factor parametrization coefficient $a_0$ of $f_+$ |
Bs->K BCL a0_f0 |
$a_0^{(0)}$ | BCL $B_s\to K$ form factor parametrization coefficient $a_0$ of $f_0$ |
Bs->K BCL a0_fT |
$a_0^{(T)}$ | BCL $B_s\to K$ form factor parametrization coefficient $a_0$ of $f_T$ |
Bs->K BCL a1_f+ |
$a_1^{(+)}$ | BCL $B_s\to K$ form factor parametrization coefficient $a_1$ of $f_+$ |
Bs->K BCL a1_f0 |
$a_1^{(0)}$ | BCL $B_s\to K$ form factor parametrization coefficient $a_1$ of $f_0$ |
Bs->K BCL a1_fT |
$a_1^{(T)}$ | BCL $B_s\to K$ form factor parametrization coefficient $a_1$ of $f_T$ |
Bs->K BCL a2_f+ |
$a_2^{(+)}$ | BCL $B_s\to K$ form factor parametrization coefficient $a_2$ of $f_+$ |
Bs->K BCL a2_f0 |
$a_2^{(0)}$ | BCL $B_s\to K$ form factor parametrization coefficient $a_2$ of $f_0$ |
Bs->K BCL a2_fT |
$a_2^{(T)}$ | BCL $B_s\to K$ form factor parametrization coefficient $a_2$ of $f_T$ |
Bs->K BCL m+ |
$m_{B^*}^{f_+}$ | Resonance mass for the $B_s\to K$ vector and tensor form factors in BCL parametrization |
Bs->K BCL m0 |
$m_{B^*}^{f_0}$ | Resonance mass for the $B_s\to K$ scalar form factor in BCL parametrization |
Bs->K* BCL m0 |
$m_{B^*}^{A_0}$ | Resonance mass for the $B_s\to K^*$ scalar form factor in BCL or BSZ parametrization |
Bs->K* BCL m1+ |
$m_{B^*}^{1^+}$ | Resonance mass for the $B_s\to K^*$ form factors $A_{12}$ and $T_{2,23}$ in BCL or BSZ parametrization |
Bs->K* BCL m1- |
$m_{B^*}^{1^-}$ | Resonance mass for the $B_s\to K^*$ form factors $V$ and $T_1$ in BCL or BSZ parametrization |
Bs->K* BSZ a0_A0 |
$a_0^{A_0}$ | BSZ form factor parametrization coefficient $a_0$ of $A_0$ |
Bs->K* BSZ a0_A1 |
$a_0^{A_1}$ | BSZ form factor parametrization coefficient $a_0$ of $A_1$ |
Bs->K* BSZ a0_T1 |
$a_0^{T_1}$ | BSZ form factor parametrization coefficient $a_0$ of $T_1$ |
Bs->K* BSZ a0_T23 |
$a_0^{T_{23}}$ | BSZ form factor parametrization coefficient $a_0$ of $T_{23}$ |
Bs->K* BSZ a0_V |
$a_0^{V}$ | BSZ form factor parametrization coefficient $a_0$ of $V$ |
Bs->K* BSZ a1_A0 |
$a_1^{A_0}$ | BSZ form factor parametrization coefficient $a_1$ of $A_0$ |
Bs->K* BSZ a1_A1 |
$a_1^{A_1}$ | BSZ form factor parametrization coefficient $a_1$ of $A_1$ |
Bs->K* BSZ a1_A12 |
$a_1^{A_{12}}$ | BSZ form factor parametrization coefficient $a_1$ of $A_{12}$ |
Bs->K* BSZ a1_T1 |
$a_1^{T_1}$ | BSZ form factor parametrization coefficient $a_1$ of $T_1$ |
Bs->K* BSZ a1_T2 |
$a_1^{T_2}$ | BSZ form factor parametrization coefficient $a_1$ of $T_2$ |
Bs->K* BSZ a1_T23 |
$a_1^{T_{23}}$ | BSZ form factor parametrization coefficient $a_1$ of $T_{23}$ |
Bs->K* BSZ a1_V |
$a_1^{V}$ | BSZ form factor parametrization coefficient $a_1$ of $V$ |
Bs->K* BSZ a2_A0 |
$a_2^{A_0}$ | BSZ form factor parametrization coefficient $a_2$ of $A_0$ |
Bs->K* BSZ a2_A1 |
$a_2^{A_1}$ | BSZ form factor parametrization coefficient $a_2$ of $A_1$ |
Bs->K* BSZ a2_A12 |
$a_2^{A_{12}}$ | BSZ form factor parametrization coefficient $a_2$ of $A_{12}$ |
Bs->K* BSZ a2_T1 |
$a_2^{T_1}$ | BSZ form factor parametrization coefficient $a_2$ of $T_1$ |
Bs->K* BSZ a2_T2 |
$a_2^{T_2}$ | BSZ form factor parametrization coefficient $a_2$ of $T_2$ |
Bs->K* BSZ a2_T23 |
$a_2^{T_{23}}$ | BSZ form factor parametrization coefficient $a_2$ of $T_{23}$ |
Bs->K* BSZ a2_V |
$a_2^{V}$ | BSZ form factor parametrization coefficient $a_2$ of $V$ |
Bs->phi BCL m0 |
$m_{B^*}^{A_0}$ | Resonance mass for the $B_s\to\phi$ scalar form factor in BCL or BSZ parametrization |
Bs->phi BCL m1+ |
$m_{B^*}^{1^+}$ | Resonance mass for the $B_s\to\phi$ form factors $A_{12}$ and $T_{2,23}$ in BCL or BSZ parametrization |
Bs->phi BCL m1- |
$m_{B^*}^{1^-}$ | Resonance mass for the $B_s\to\phi$ form factors $V$ and $T_1$ in BCL or BSZ parametrization |
Bs->phi BSZ a0_A0 |
$a_0^{A_0}$ | BSZ form factor parametrization coefficient $a_0$ of $A_0$ |
Bs->phi BSZ a0_A1 |
$a_0^{A_1}$ | BSZ form factor parametrization coefficient $a_0$ of $A_1$ |
Bs->phi BSZ a0_T1 |
$a_0^{T_1}$ | BSZ form factor parametrization coefficient $a_0$ of $T_1$ |
Bs->phi BSZ a0_T23 |
$a_0^{T_{23}}$ | BSZ form factor parametrization coefficient $a_0$ of $T_{23}$ |
Bs->phi BSZ a0_V |
$a_0^{V}$ | BSZ form factor parametrization coefficient $a_0$ of $V$ |
Bs->phi BSZ a1_A0 |
$a_1^{A_0}$ | BSZ form factor parametrization coefficient $a_1$ of $A_0$ |
Bs->phi BSZ a1_A1 |
$a_1^{A_1}$ | BSZ form factor parametrization coefficient $a_1$ of $A_1$ |
Bs->phi BSZ a1_A12 |
$a_1^{A_{12}}$ | BSZ form factor parametrization coefficient $a_1$ of $A_{12}$ |
Bs->phi BSZ a1_T1 |
$a_1^{T_1}$ | BSZ form factor parametrization coefficient $a_1$ of $T_1$ |
Bs->phi BSZ a1_T2 |
$a_1^{T_2}$ | BSZ form factor parametrization coefficient $a_1$ of $T_2$ |
Bs->phi BSZ a1_T23 |
$a_1^{T_{23}}$ | BSZ form factor parametrization coefficient $a_1$ of $T_{23}$ |
Bs->phi BSZ a1_V |
$a_1^{V}$ | BSZ form factor parametrization coefficient $a_1$ of $V$ |
Bs->phi BSZ a2_A0 |
$a_2^{A_0}$ | BSZ form factor parametrization coefficient $a_2$ of $A_0$ |
Bs->phi BSZ a2_A1 |
$a_2^{A_1}$ | BSZ form factor parametrization coefficient $a_2$ of $A_1$ |
Bs->phi BSZ a2_A12 |
$a_2^{A_{12}}$ | BSZ form factor parametrization coefficient $a_2$ of $A_{12}$ |
Bs->phi BSZ a2_T1 |
$a_2^{T_1}$ | BSZ form factor parametrization coefficient $a_2$ of $T_1$ |
Bs->phi BSZ a2_T2 |
$a_2^{T_2}$ | BSZ form factor parametrization coefficient $a_2$ of $T_2$ |
Bs->phi BSZ a2_T23 |
$a_2^{T_{23}}$ | BSZ form factor parametrization coefficient $a_2$ of $T_{23}$ |
Bs->phi BSZ a2_V |
$a_2^{V}$ | BSZ form factor parametrization coefficient $a_2$ of $V$ |
Bs->phi LCSR T10 |
$T_1(0)$ | Bs->phi T_1 parameter at q2=0 |
Bs->phi deltaC7 a_+ Im |
$\text{Im}\,a^{\Delta_7}_+$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at low $q^2$ |
Bs->phi deltaC7 a_+ Re |
$\text{Re}\,a^{\Delta_7}_+$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at low $q^2$ |
Bs->phi deltaC7 a_- Im |
$\text{Im}\,a^{\Delta_7}_-$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at low $q^2$ |
Bs->phi deltaC7 a_- Re |
$\text{Re}\,a^{\Delta_7}_-$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at low $q^2$ |
Bs->phi deltaC7 a_0 Im |
$\text{Im}\,a^{\Delta_7}_0$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at low $q^2$ |
Bs->phi deltaC7 a_0 Re |
$\text{Re}\,a^{\Delta_7}_0$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at low $q^2$ |
Bs->phi deltaC7 b_+ Im |
$\text{Im}\,b^{\Delta_7}_+$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at low $q^2$ |
Bs->phi deltaC7 b_+ Re |
$\text{Re}\,b^{\Delta_7}_+$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at low $q^2$ |
Bs->phi deltaC7 b_- Im |
$\text{Im}\,b^{\Delta_7}_-$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at low $q^2$ |
Bs->phi deltaC7 b_- Re |
$\text{Re}\,b^{\Delta_7}_-$ | |
Bs->phi deltaC7 b_0 Im |
$\text{Im}\,b^{\Delta_7}_0$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at low $q^2$ |
Bs->phi deltaC7 b_0 Re |
$\text{Re}\,b^{\Delta_7}_0$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at low $q^2$ |
Bs->phi deltaC7p a_+ Im |
$\text{Im}\,a^{\Delta_7^\prime}_+$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at low $q^2$ |
Bs->phi deltaC7p a_+ Re |
$\text{Re}\,a^{\Delta_7^\prime}_+$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at low $q^2$ |
Bs->phi deltaC7p b_+ Im |
$\text{Im}\,b^{\Delta_7^\prime}_+$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at low $q^2$ |
Bs->phi deltaC7p b_+ Re |
$\text{Re}\,b^{\Delta_7^\prime}_+$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at low $q^2$ |
Bs->phi deltaC9 a_0 Im |
$\text{Im}\,a^{\Delta_9}_0$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at low $q^2$ |
Bs->phi deltaC9 a_0 Re |
$\text{Re}\,a^{\Delta_9}_0$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at low $q^2$ |
Bs->phi deltaC9 b_0 Im |
$\text{Im}\,b^{\Delta_9}_0$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at low $q^2$ |
Bs->phi deltaC9 b_0 Re |
$\text{Re}\,b^{\Delta_9}_0$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at low $q^2$ |
Bs->phi deltaC9 c_+ Im |
$\text{Im}\,c^{\Delta_9}_+$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at high $q^2$ |
Bs->phi deltaC9 c_+ Re |
$\text{Re}\,c^{\Delta_9}_+$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at high $q^2$ |
Bs->phi deltaC9 c_- Im |
$\text{Im}\,c^{\Delta_9}_-$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at high $q^2$ |
Bs->phi deltaC9 c_- Re |
$\text{Re}\,c^{\Delta_9}_-$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at high $q^2$ |
Bs->phi deltaC9 c_0 Im |
$\text{Im}\,c^{\Delta_9}_0$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at high $q^2$ |
Bs->phi deltaC9 c_0 Re |
$\text{Re}\,c^{\Delta_9}_0$ | Parameter for subleading hadronic effects in $B_s\to \phi\ell^+\ell^-$ at high $q^2$ |
CLN c_xi |
$c_\xi$ | Parameter of leading Isgur-Wise function $\xi(w)=1-\rho^2\xi(w-1)+c\xi(w-1)^2+\ldots$ |
CLN l_1(1) |
$\ell_1(1)$ | $O(\epsilon_c^2)$ power correction to $B\to D^{(*)}$ HQET form factors |
CLN l_2(1) |
$\ell_2(1)$ | $O(\epsilon_c^2)$ power correction to $B\to D^{(*)}$ HQET form factors |
CLN l_3(1) |
$\ell_3(1)$ | $O(\epsilon_c^2)$ power correction to $B\to D^{(*)}$ HQET form factors |
CLN l_4(1) |
$\ell_4(1)$ | $O(\epsilon_c^2)$ power correction to $B\to D^{(*)}$ HQET form factors |
CLN l_5(1) |
$\ell_5(1)$ | $O(\epsilon_c^2)$ power correction to $B\to D^{(*)}$ HQET form factors |
CLN l_6(1) |
$\ell_6(1)$ | $O(\epsilon_c^2)$ power correction to $B\to D^{(*)}$ HQET form factors |
CLN lp_1(1) |
$\ell_1’(1)$ | $O(\epsilon_c^2)$ power correction to $B\to D^{(*)}$ HQET form factors |
CLN lp_2(1) |
$\ell_2’(1)$ | $O(\epsilon_c^2)$ power correction to $B\to D^{(*)}$ HQET form factors |
CLN lp_3(1) |
$\ell_3’(1)$ | $O(\epsilon_c^2)$ power correction to $B\to D^{(*)}$ HQET form factors |
CLN lp_4(1) |
$\ell_4’(1)$ | $O(\epsilon_c^2)$ power correction to $B\to D^{(*)}$ HQET form factors |
CLN lp_5(1) |
$\ell_5’(1)$ | $O(\epsilon_c^2)$ power correction to $B\to D^{(*)}$ HQET form factors |
CLN lp_6(1) |
$\ell_6’(1)$ | $O(\epsilon_c^2)$ power correction to $B\to D^{(*)}$ HQET form factors |
CLN rho2_xi |
$\rho^2_\xi$ | Slope parameter of leading Isgur-Wise function $\xi(w)=1-\rho^2_\xi(w-1)+\ldots$ |
CLN xi3 |
$\xi^{(3)}$ | Parameter of leading Isgur-Wise function $\xi(w)=1-\rho^2\xi(w-1)+c\xi(w-1)^2+\xi^{(3)}(w-1)^3/6$ |
C_BXlnu |
$C$ | |
D Al |
$D$ | Overlap integral corresponding to the photon/Z contribution |
D Au |
$D$ | Overlap integral corresponding to the photon/Z contribution |
D Ti |
$D$ | Overlap integral corresponding to the photon/Z contribution |
D->K BCL m+ |
$m_{D^*}^{f_+}$ | Resonance mass for the $D\to K$ vector and tensor form factors in BCL parametrization |
D->K BCL m0 |
$m_{D^*}^{f_0}$ | Resonance mass for the $D\to K$ scalar form factor in BCL parametrization |
D->K BSZ a0_f+ |
$a_0^{f_+}$ | BSZ form factor parametrization coefficient $a_0$ of $f_+$ |
D->K BSZ a0_fT |
$a_0^{f_T}$ | BSZ form factor parametrization coefficient $a_0$ of $f_T$ |
D->K BSZ a1_f+ |
$a_1^{f_+}$ | BSZ form factor parametrization coefficient $a_1$ of $f_+$ |
D->K BSZ a1_f0 |
$a_1^{f_0}$ | BSZ form factor parametrization coefficient $a_1$ of $f_0$ |
D->K BSZ a1_fT |
$a_1^{f_T}$ | BSZ form factor parametrization coefficient $a_1$ of $f_T$ |
D->K BSZ a2_f+ |
$a_2^{f_+}$ | BSZ form factor parametrization coefficient $a_2$ of $f_+$ |
D->K BSZ a2_f0 |
$a_2^{f_0}$ | BSZ form factor parametrization coefficient $a_2$ of $f_0$ |
D->K BSZ a2_fT |
$a_2^{f_T}$ | BSZ form factor parametrization coefficient $a_2$ of $f_T$ |
D->pi BCL m+ |
$m_{D^*}^{f_+}$ | Resonance mass for the $D\to \pi$ vector and tensor form factors in BCL parametrization |
D->pi BCL m0 |
$m_{D^*}^{f_0}$ | Resonance mass for the $D\to \pi$ scalar form factor in BCL parametrization |
D->pi BSZ a0_f+ |
$a_0^{f_+}$ | BSZ form factor parametrization coefficient $a_0$ of $f_+$ |
D->pi BSZ a0_fT |
$a_0^{f_T}$ | BSZ form factor parametrization coefficient $a_0$ of $f_T$ |
D->pi BSZ a1_f+ |
$a_1^{f_+}$ | BSZ form factor parametrization coefficient $a_1$ of $f_+$ |
D->pi BSZ a1_f0 |
$a_1^{f_0}$ | BSZ form factor parametrization coefficient $a_1$ of $f_0$ |
D->pi BSZ a1_fT |
$a_1^{f_T}$ | BSZ form factor parametrization coefficient $a_1$ of $f_T$ |
D->pi BSZ a2_f+ |
$a_2^{f_+}$ | BSZ form factor parametrization coefficient $a_2$ of $f_+$ |
D->pi BSZ a2_f0 |
$a_2^{f_0}$ | BSZ form factor parametrization coefficient $a_2$ of $f_0$ |
D->pi BSZ a2_fT |
$a_2^{f_T}$ | BSZ form factor parametrization coefficient $a_2$ of $f_T$ |
DeltaGamma/Gamma_B0 |
$\Delta \Gamma_d/\Gamma_d$ | Relative decay width difference in the $B_s$ system |
DeltaGamma/Gamma_Bs |
$\Delta \Gamma_s/\Gamma_s$ | Relative decay width difference in the $B_s$ system |
DeltaM_K0 |
$\Delta M_K$ | Mass difference in the $K^0$ system |
DeltaRA |
$\Delta_R^A$ | Relative radiative correction to the SM Gamow-Teller beta decay rate |
DeltaRV |
$\Delta_R^V$ | Relative radiative correction to the SM Fermi beta decay rate |
Delta_alpha_e_had |
$\Delta\alpha_{\rm had}^{(5)}(m_Z)$ | hadronic contribution to the running of the electromagnetic fine structure constant between 0 and $m_Z$ |
Delta_alpha_e_lep |
$\Delta\alpha_{\rm lep}(m_Z)$ | leptonic contribution to the running of the electromagnetic fine structure constant between 0 and $m_Z$ |
GF |
$G_F$ | Fermi constant |
Gamma12_B0_a |
$a$ | Coefficient in the approximate equality $\Delta \Gamma_d/M_{12}^d=10^{-4}[c+a\frac{\lambda_u}{\lambda_t}]$ |
Gamma12_B0_c |
$c$ | Coefficient in the approximate equality $\Delta \Gamma_d/M_{12}^d=10^{-4}[c+a\frac{\lambda_u}{\lambda_t}]$ |
Gamma12_Bs_a |
$a$ | Coefficient in the approximate equality $\Delta \Gamma_s/M_{12}^s=10^{-4}[c+a\frac{\lambda_u}{\lambda_t}]$ |
Gamma12_Bs_c |
$c$ | Coefficient in the approximate equality $\Delta \Gamma_s/M_{12}^s=10^{-4}[c+a\frac{\lambda_u}{\lambda_t}]$ |
Gamma12_D a_bb |
$a_{bb}$ | SM contribution to the absorptive part of the $D^0$-$\bar D^0$ mixing amplitude multiplied by $V_{ub}V_{cb}^\ast$ in inverse picoseconds |
Gamma12_D a_bs |
$a_{bb}$ | SM contribution to the absorptive part of the $D^0$-$\bar D^0$ mixing amplitude multiplied by $V_{ub}V_{cs}^\ast$ in inverse picoseconds |
Gamma12_D a_ss |
$a_{bb}$ | SM contribution to the absorptive part of the $D^0$-$\bar D^0$ mixing amplitude multiplied by $V_{us}V_{cs}^\ast$ in inverse picoseconds |
GammaCapture Al |
$\Gamma_\text{capture}(\phantom k^{27}_{13} \mathrm{Al})$ | Capture rate of $\mu$ in $\phantom k^{27}_{13} \mathrm{Al}$ |
GammaCapture Au |
$\Gamma_\text{capture}(\phantom k^{197}_{79} \mathrm{Au})$ | Capture rate of $\mu$ in $\phantom k^{197}_{79} \mathrm{Au}$ |
GammaCapture Ti |
$\Gamma_\text{capture}(\phantom k^{48}_{22} \mathrm{Ti})$ | Capture rate of $\mu$ in $\phantom k^{48}_{22} \mathrm{Ti}$ |
GammaW_had |
$\Gamma_W^\text{had}$ | Hadronic $W$ width in the SM |
GammaW_lep |
$\Gamma_W^\text{lep}$ | Leptonic $W$ width in the SM |
Gamma_phi |
$\Gamma_\phi$ | phi decay width |
K+e3 delta_EM |
$\delta_\text{em}^{K^+e}$ | Relative electromagnetic correction to $K^+\to\pi^0 e^+\bar\nu$ decay rate |
K+mu3 delta_EM |
$\delta_\text{em}^{K^+\mu}$ | Relative electromagnetic correction to $K^+\to\pi^0 \mu^+\bar\nu$ decay rate |
K->pi D |
$D$ | Parameter in the dispersive parametrization of the $K\to\pi$ form factors |
K->pi H1 |
$H_1$ | Parameter in the dispersive parametrization of the $K\to\pi$ form factors |
K->pi H2 |
$H_s$ | Parameter in the dispersive parametrization of the $K\to\pi$ form factors |
K->pi Lambda_+ |
$\Lambda_+$ | Parameter in the dispersive parametrization of the $K\to\pi$ form factors |
K->pi d |
$d$ | Parameter in the dispersive parametrization of the $K\to\pi$ form factors |
K->pi delta_K+pi0 |
$\delta_{SU(2)}^{K^+\pi^0}$ | Isospin breaking parameter in $K\to \pi\ell\nu$ decays |
K->pi f+(0) |
$f_+(0)$ | $K\to\pi$ form factor $f_+$ at $q^2=0$ |
K->pi fT(0) |
$f_T(0)$ | $K\to\pi$ form factor $f_T$ at $q^2=0$ |
K->pi k |
$k$ | Parameter in the dispersive parametrization of the $K\to\pi$ form factors |
K->pi ln(C) |
$\ln C$ | Parameter in the dispersive parametrization of the $K\to\pi$ form factors |
K->pi sT |
$s_T$ | Parameter in the pole parametrization of the $K\to\pi$ tensor form factor |
K0e3 delta_EM |
$\delta_\text{em}^{K^0e}$ | Relative electromagnetic correction to $K^0\to\pi^+ e^-\nu$ decay rate |
K0mu3 delta_EM |
$\delta_\text{em}^{K^0\mu}$ | Relative electromagnetic correction to $K^0\to\pi^+ \mu^-\nu$ decay rate |
Kpipi M0 3 |
$\langle Q_3 \rangle_0$ | $K\to (\pi\pi)_{I=0}$ matrix element of $Q_3$ |
Kpipi M0 4 |
$\langle Q_4 \rangle_0$ | $K\to (\pi\pi)_{I=0}$ matrix element of $Q_4$ |
Kpipi M0 5 |
$\langle Q_5 \rangle_0$ | $K\to (\pi\pi)_{I=0}$ matrix element of $Q_5$ |
Kpipi M0 6 |
$\langle Q_6 \rangle_0$ | $K\to (\pi\pi)_{I=0}$ matrix element of $Q_6$ |
Kpipi M0 7 |
$\langle Q_7 \rangle_0$ | $K\to (\pi\pi)_{I=0}$ matrix element of $Q_7$ |
Kpipi M0 8 |
$\langle Q_8 \rangle_0$ | $K\to (\pi\pi)_{I=0}$ matrix element of $Q_8$ |
Kpipi M0 9 |
$\langle Q_9 \rangle_0$ | $K\to (\pi\pi)_{I=0}$ matrix element of $Q_9$ |
Kpipi M0 SLL1_d |
$\langle Q_1^{\text{SLL},d} \rangle_0$ | $K\to (\pi\pi)_{I=0}$ matrix element of $Q_1^{\text{SLL},d}$ |
Kpipi M0 SLL1_u |
$\langle Q_1^{\text{SLL},u} \rangle_0$ | $K\to (\pi\pi)_{I=0}$ matrix element of $Q_1^{\text{SLL},u}$ |
Kpipi M0 SLL2_d |
$\langle Q_2^{\text{SLL},d} \rangle_0$ | $K\to (\pi\pi)_{I=0}$ matrix element of $Q_2^{\text{SLL},d}$ |
Kpipi M0 SLL2_u |
$\langle Q_2^{\text{SLL},u} \rangle_0$ | $K\to (\pi\pi)_{I=0}$ matrix element of $Q_2^{\text{SLL},u}$ |
Kpipi M0 SLL3_u |
$\langle Q_3^{\text{SLL},u} \rangle_0$ | $K\to (\pi\pi)_{I=0}$ matrix element of $Q_3^{\text{SLL},u}$ |
Kpipi M0 SLL4_u |
$\langle Q_4^{\text{SLL},u} \rangle_0$ | $K\to (\pi\pi)_{I=0}$ matrix element of $Q_4^{\text{SLL},u}$ |
Kpipi M0 SLR1_u |
$\langle Q_1^{\text{SLR},u} \rangle_0$ | $K\to (\pi\pi)_{I=0}$ matrix element of $Q_1^{\text{SLR},u}$ |
Kpipi M0 SLR2_u |
$\langle Q_2^{\text{SLR},u} \rangle_0$ | $K\to (\pi\pi)_{I=0}$ matrix element of $Q_2^{\text{SLR},u}$ |
Kpipi M0 g- |
$\langle Q_g^- \rangle_0$ | $K\to (\pi\pi)_{I=0}$ matrix element of $Q_g^-$ |
Kpipi M2 7 |
$\langle Q_7 \rangle_2$ | $K\to (\pi\pi)_{I=2}$ matrix element of $Q_7$ |
Kpipi M2 8 |
$\langle Q_8 \rangle_2$ | $K\to (\pi\pi)_{I=2}$ matrix element of $Q_8$ |
Kpipi M2 9 |
$\langle Q_9 \rangle_2$ | $K\to (\pi\pi)_{I=2}$ matrix element of $Q_9$ |
Kpipi M2 SLL1_d |
$\langle Q_1^{\text{SLL},d} \rangle_2$ | $K\to (\pi\pi)_{I=2}$ matrix element of $Q_1^{\text{SLL},d}$ |
Kpipi M2 SLL2_d |
$\langle Q_2^{\text{SLL},d} \rangle_2$ | $K\to (\pi\pi)_{I=2}$ matrix element of $Q_2^{\text{SLL},d}$ |
Lambda->p f_1(0) |
$f_1(0)$ | $\Lambda\to p$ vector form factor $f_1$ at $q^2=0$ |
Lambda->p g_1(0) |
$g_1(0)$ | $\Lambda\to p$ axial vector form factor $g_1$ at $q^2=0$ |
Lambda->ppi alpha_- |
$\alpha_-$ | $\Lambda\to p \pi^-$ decay parameter |
Lambdab->Lambda SSE a0_fA0 |
$a_0^{f^A_0}$ | SSE form factor parametrization coefficient $a_0$ of $f^A_0$ |
Lambdab->Lambda SSE a0_fAt |
$a_0^{f^A_t}$ | SSE form factor parametrization coefficient $a_0$ of $f^A_t$ |
Lambdab->Lambda SSE a0_fT0 |
$a_0^{f^T_0}$ | SSE form factor parametrization coefficient $a_0$ of $f^T_0$ |
Lambdab->Lambda SSE a0_fT50 |
$a_0^{f^{T5}_0}$ | SSE form factor parametrization coefficient $a_0$ of $f^{T5}_0$ |
Lambdab->Lambda SSE a0_fTperp |
$a_0^{f^T_\perp}$ | SSE form factor parametrization coefficient $a_0$ of $f^T_\perp$ |
Lambdab->Lambda SSE a0_fV0 |
$a_0^{f^V_0}$ | SSE form factor parametrization coefficient $a_0$ of $f^V_0$ |
Lambdab->Lambda SSE a0_fVperp |
$a_0^{f^V_\perp}$ | SSE form factor parametrization coefficient $a_0$ of $f^V_\perp$ |
Lambdab->Lambda SSE a0_fVt |
$a_0^{f^V_t}$ | SSE form factor parametrization coefficient $a_0$ of $f^V_t$ |
Lambdab->Lambda SSE a1_fA0 |
$a_1^{f^A_0}$ | SSE form factor parametrization coefficient $a_1$ of $f^A_0$ |
Lambdab->Lambda SSE a1_fAperp |
$a_1^{f^A_\perp}$ | SSE form factor parametrization coefficient $a_1$ of $f^A_\perp$ |
Lambdab->Lambda SSE a1_fAt |
$a_1^{f^A_t}$ | SSE form factor parametrization coefficient $a_1$ of $f^A_t$ |
Lambdab->Lambda SSE a1_fT0 |
$a_1^{f^T_0}$ | SSE form factor parametrization coefficient $a_1$ of $f^T_0$ |
Lambdab->Lambda SSE a1_fT50 |
$a_1^{f^{T5}_0}$ | SSE form factor parametrization coefficient $a_1$ of $f^{T5}_0$ |
Lambdab->Lambda SSE a1_fT5perp |
$a_1^{f^{T5}_\perp}$ | SSE form factor parametrization coefficient $a_1$ of $f^{T5}_\perp$ |
Lambdab->Lambda SSE a1_fTperp |
$a_1^{f^T_\perp}$ | SSE form factor parametrization coefficient $a_1$ of $f^T_\perp$ |
Lambdab->Lambda SSE a1_fV0 |
$a_1^{f^V_0}$ | SSE form factor parametrization coefficient $a_1$ of $f^V_0$ |
Lambdab->Lambda SSE a1_fVperp |
$a_1^{f^V_\perp}$ | SSE form factor parametrization coefficient $a_1$ of $f^V_\perp$ |
Lambdab->Lambda SSE a1_fVt |
$a_1^{f^V_t}$ | SSE form factor parametrization coefficient $a_1$ of $f^V_t$ |
Lambdab->Lambda SSE a2_fA0 |
$a_2^{f^A_0}$ | SSE form factor parametrization coefficient $a_2$ of $f^A_0$ |
Lambdab->Lambda SSE a2_fAperp |
$a_2^{f^A_\perp}$ | SSE form factor parametrization coefficient $a_2$ of $f^A_\perp$ |
Lambdab->Lambda SSE a2_fAt |
$a_2^{f^A_t}$ | SSE form factor parametrization coefficient $a_2$ of $f^A_t$ |
Lambdab->Lambda SSE a2_fT0 |
$a_2^{f^T_0}$ | SSE form factor parametrization coefficient $a_2$ of $f^T_0$ |
Lambdab->Lambda SSE a2_fT50 |
$a_2^{f^{T5}_0}$ | SSE form factor parametrization coefficient $a_2$ of $f^{T5}_0$ |
Lambdab->Lambda SSE a2_fT5perp |
$a_2^{f^{T5}_\perp}$ | SSE form factor parametrization coefficient $a_2$ of $f^{T5}_\perp$ |
Lambdab->Lambda SSE a2_fTperp |
$a_2^{f^T_\perp}$ | SSE form factor parametrization coefficient $a_2$ of $f^T_\perp$ |
Lambdab->Lambda SSE a2_fV0 |
$a_2^{f^V_0}$ | SSE form factor parametrization coefficient $a_2$ of $f^V_0$ |
Lambdab->Lambda SSE a2_fVperp |
$a_2^{f^V_\perp}$ | SSE form factor parametrization coefficient $a_2$ of $f^V_\perp$ |
Lambdab->Lambda SSE a2_fVt |
$a_2^{f^V_t}$ | SSE form factor parametrization coefficient $a_2$ of $f^V_t$ |
Lambdab->Lambda deltaC7 a_para0 Im |
$\text{Im}\,a^{\Delta_7}_{\parallel_0}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC7 a_para0 Re |
$\text{Re}\,a^{\Delta_7}_{\parallel_0}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC7 a_para1 Im |
$\text{Im}\,a^{\Delta_7}_{\parallel_1}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC7 a_para1 Re |
$\text{Re}\,a^{\Delta_7}_{\parallel_1}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC7 a_perp0 Im |
$\text{Im}\,a^{\Delta_7}_{\perp_0}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC7 a_perp0 Re |
$\text{Re}\,a^{\Delta_7}_{\perp_0}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC7 a_perp1 Im |
$\text{Im}\,a^{\Delta_7}_{\perp_1}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC7 a_perp1 Re |
$\text{Re}\,a^{\Delta_7}_{\perp_1}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC7 b_para0 Im |
$\text{Im}\,b^{\Delta_7}_{\parallel_0}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC7 b_para0 Re |
$\text{Re}\,b^{\Delta_7}_{\parallel_0}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC7 b_para1 Im |
$\text{Im}\,b^{\Delta_7}_{\parallel_1}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC7 b_para1 Re |
$\text{Re}\,b^{\Delta_7}_{\parallel_1}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC7 b_perp0 Im |
$\text{Im}\,b^{\Delta_7}_{\perp_0}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC7 b_perp0 Re |
$\text{Re}\,b^{\Delta_7}_{\perp_0}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC7 b_perp1 Im |
$\text{Im}\,b^{\Delta_7}_{\perp_1}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC7 b_perp1 Re |
$\text{Re}\,b^{\Delta_7}_{\perp_1}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC9 c_para0 Im |
$\text{Im}\,c^{\Delta_9}_{\parallel_0}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC9 c_para0 Re |
$\text{Re}\,c^{\Delta_9}_{\parallel_0}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC9 c_para1 Im |
$\text{Im}\,c^{\Delta_9}_{\parallel_1}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC9 c_para1 Re |
$\text{Re}\,c^{\Delta_9}_{\parallel_1}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC9 c_perp0 Im |
$\text{Im}\,c^{\Delta_9}_{\perp_0}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC9 c_perp0 Re |
$\text{Re}\,c^{\Delta_9}_{\perp_0}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC9 c_perp1 Im |
$\text{Im}\,c^{\Delta_9}_{\perp_1}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda deltaC9 c_perp1 Re |
$\text{Re}\,c^{\Delta_9}_{\perp_1}$ | Parameter for subleading hadronic effects in $\Lambda_b\to\Lambda\ell^+\ell^-$ at low $q^2$ |
Lambdab->Lambda(1520) F1 a0 |
$a_0^{F1}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) F1 a2 |
$a_2^{F1}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) F1 a4 |
$a_4^{F1}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) F2 a0 |
$a_0^{F2}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) F2 a2 |
$a_2^{F2}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) F2 a4 |
$a_4^{F2}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) F3 a0 |
$a_0^{F3}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) F3 a2 |
$a_2^{F3}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) F3 a4 |
$a_4^{F3}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) F4 a0 |
$a_0^{F4}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) F4 a2 |
$a_2^{F4}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) F4 a4 |
$a_4^{F4}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) G1 a0 |
$a_0^{G1}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) G1 a2 |
$a_2^{G1}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) G1 a4 |
$a_4^{G1}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) G2 a0 |
$a_0^{G2}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) G2 a2 |
$a_2^{G2}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) G2 a4 |
$a_4^{G2}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) G3 a0 |
$a_0^{G3}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) G3 a2 |
$a_2^{G3}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) G3 a4 |
$a_4^{G3}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) G4 a0 |
$a_0^{G4}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) G4 a2 |
$a_2^{G4}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) G4 a4 |
$a_4^{G4}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) H1 a0 |
$a_0^{H1}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) H1 a2 |
$a_2^{H1}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) H1 a4 |
$a_4^{H1}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) H2 a0 |
$a_0^{H2}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) H2 a2 |
$a_2^{H2}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) H2 a4 |
$a_4^{H2}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) H3 a0 |
$a_0^{H3}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) H3 a2 |
$a_2^{H3}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) H3 a4 |
$a_4^{H3}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) H4 a0 |
$a_0^{H4}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) H4 a2 |
$a_2^{H4}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) H4 a4 |
$a_4^{H4}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) H5 a0 |
$a_0^{H5}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) H5 a2 |
$a_2^{H5}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) H5 a4 |
$a_4^{H5}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) H6 a0 |
$a_0^{H6}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) H6 a2 |
$a_2^{H6}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) H6 a4 |
$a_4^{H6}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) alpha_Lambda(1520) |
$\alpha_{\Lambda(1520)}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) alpha_Lambdab |
$\alpha_{\Lambda b}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) f0 A |
$F^{f_{0}}$ | Slope of the parametrization of the form factor $f_{0}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) f0 F |
$F^{f_{0}}$ | Constant of the parametrization of the form factor $f_{0}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) fA0 uncertainty |
$\Delta_{fA0}$ | Uncertainty applied on the form factor fA0 |
Lambdab->Lambda(1520) fAg uncertainty |
$\Delta_{fAg}$ | Uncertainty applied on the form factor fAg |
Lambdab->Lambda(1520) fAperp uncertainty |
$\Delta_{fAperp}$ | Uncertainty applied on the form factor fAperp |
Lambdab->Lambda(1520) fAt uncertainty |
$\Delta_{fAt}$ | Uncertainty applied on the form factor fAt |
Lambdab->Lambda(1520) fT0 uncertainty |
$\Delta_{fT0}$ | Uncertainty applied on the form factor fT0 |
Lambdab->Lambda(1520) fT50 uncertainty |
$\Delta_{fT50}$ | Uncertainty applied on the form factor fT50 |
Lambdab->Lambda(1520) fT5g uncertainty |
$\Delta_{fT5g}$ | Uncertainty applied on the form factor fT5g |
Lambdab->Lambda(1520) fT5perp uncertainty |
$\Delta_{fT5perp}$ | Uncertainty applied on the form factor fT5perp |
Lambdab->Lambda(1520) fT5t uncertainty |
$\Delta_{fT5t}$ | Uncertainty applied on the form factor fT5t |
Lambdab->Lambda(1520) fTg uncertainty |
$\Delta_{fTg}$ | Uncertainty applied on the form factor fTg |
Lambdab->Lambda(1520) fTperp uncertainty |
$\Delta_{fTperp}$ | Uncertainty applied on the form factor fTperp |
Lambdab->Lambda(1520) fTt uncertainty |
$\Delta_{fTt}$ | Uncertainty applied on the form factor fTt |
Lambdab->Lambda(1520) fV0 uncertainty |
$\Delta_{fV0}$ | Uncertainty applied on the form factor fV0 |
Lambdab->Lambda(1520) fVg uncertainty |
$\Delta_{fVg}$ | Uncertainty applied on the form factor fVg |
Lambdab->Lambda(1520) fVperp uncertainty |
$\Delta_{fVperp}$ | Uncertainty applied on the form factor fVperp |
Lambdab->Lambda(1520) fVt uncertainty |
$\Delta_{fVt}$ | Uncertainty applied on the form factor fVt |
Lambdab->Lambda(1520) fperp A |
$F^{f_{\perp}}$ | Slope of the parametrization of the form factor $f_{\perp}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) fperp F |
$F^{f_{\perp}}$ | Constant of the parametrization of the form factor $f_{\perp}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) fperpPrim A |
$F^{f_{\perp^{\prime}}}$ | Slope of the parametrization of the form factor $f_{\perp^{\prime}}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) fperpPrim F |
$F^{f_{\perp^{\prime}}}$ | Constant of the parametrization of the form factor $f_{\perp^{\prime}}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) fplus A |
$F^{f_{+}}$ | Slope of the parametrization of the form factor $f_{+}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) fplus F |
$F^{f_{+}}$ | Constant of the parametrization of the form factor $f_{+}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) g0 A |
$F^{g_{0}}$ | Slope of the parametrization of the form factor $g_{0}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) g0 F |
$F^{g_{0}}$ | Constant of the parametrization of the form factor $g_{0}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) gperp A |
$F^{g_{\perp}}$ | Slope of the parametrization of the form factor $g_{\perp}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) gperp F |
$F^{g_{\perp}}$ | Constant of the parametrization of the form factor $g_{\perp}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) gperpPrim A |
$F^{g_{\perp^{\prime}}}$ | Slope of the parametrization of the form factor $g_{\perp^{\prime}}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) gperpPrim F |
$F^{g_{\perp^{\prime}}}$ | Constant of the parametrization of the form factor $g_{\perp^{\prime}}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) gplus A |
$F^{g_{+}}$ | Slope of the parametrization of the form factor $g_{+}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) gplus F |
$F^{g_{+}}$ | Constant of the parametrization of the form factor $g_{+}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) hTperp A |
$F^{\tilde{h}_{\perp}}$ | Slope of the parametrization of the form factor $\tilde{h}_{\perp}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) hTperp F |
$F^{\tilde{h}_{\perp}}$ | Constant of the parametrization of the form factor $\tilde{h}_{\perp}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) hTperpPrim A |
$F^{\tilde{h}_{\perp^{\prime}}}$ | Slope of the parametrization of the form factor $\tilde{h}_{\perp^{\prime}}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) hTperpPrim F |
$F^{\tilde{h}_{\perp^{\prime}}}$ | Constant of the parametrization of the form factor $\tilde{h}_{\perp^{\prime}}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) hTplus A |
$F^{\tilde{h}_{+}}$ | Slope of the parametrization of the form factor $\tilde{h}_{+}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) hTplus F |
$F^{\tilde{h}_{+}}$ | Constant of the parametrization of the form factor $\tilde{h}_{+}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) hperp A |
$F^{h_{\perp}}$ | Slope of the parametrization of the form factor $h_{\perp}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) hperp F |
$F^{h_{\perp}}$ | Constant of the parametrization of the form factor $h_{\perp}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) hperpPrim A |
$F^{h_{\perp^{\prime}}}$ | Slope of the parametrization of the form factor $h_{\perp^{\prime}}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) hperpPrim F |
$F^{h_{\perp^{\prime}}}$ | Constant of the parametrization of the form factor $h_{\perp^{\prime}}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) hplus A |
$F^{h_{+}}$ | Slope of the parametrization of the form factor $h_{+}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) hplus F |
$F^{h_{+}}$ | Constant of the parametrization of the form factor $h_{+}$ from lattice QCD in high q2 region as in arXiv:2009.09313 |
Lambdab->Lambda(1520) m_q |
$m_q^{model}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
Lambdab->Lambda(1520) m_s |
$m_s^{model}$ | Parameter for the form factor calculation of $\Lambda_b\to\Lambda(1520)\ell^+\ell^-$ using the quark model as in arXiv 1108.6129 |
M12_D a_bb |
$a_{bb}$ | SM contribution to the dispersive part of the $D^0$-$\bar D^0$ mixing amplitude multiplied by $V_{ub}V_{cb}^\ast$ in inverse picoseconds |
M12_D a_bs |
$a_{bb}$ | SM contribution to the dispersive part of the $D^0$-$\bar D^0$ mixing amplitude multiplied by $V_{ub}V_{cs}^\ast$ in inverse picoseconds |
M12_D a_ss |
$a_{bb}$ | SM contribution to the dispersive part of the $D^0$-$\bar D^0$ mixing amplitude multiplied by $V_{us}V_{cs}^\ast$ in inverse picoseconds |
Omegahat_eff |
$\hat \Omega_\text{eff}$ | Parameter for isospin breaking corrections to $\epsilon'/\epsilon$ |
PDFmembers avg=0 replicas=1-100 |
$\text{mem}_{\text{PDF}}$ | member ID of PDF set where mem=0 is average on replicas and mem=1-100 are PDF replicas |
ReA0(K->pipi) |
$\text{Re}A_0$ | Real part of the $K\to(\pi\pi)_{I=0}$ isospin amplitude from experiment |
ReA2(K->pipi) |
$\text{Re}A_2$ | Real part of the $K\to(\pi\pi)_{I=2}$ isospin amplitude from experiment |
Sn Al |
$S^{(n)}$ | Scalar overlap integral with neutron distribution |
Sn Au |
$S^{(n)}$ | Scalar overlap integral with neutron distribution |
Sn Ti |
$S^{(n)}$ | Scalar overlap integral with neutron distribution |
Sp Al |
$S^{(p)}$ | Scalar overlap integral with proton distribution |
Sp Au |
$S^{(p)}$ | Scalar overlap integral with proton distribution |
Sp Ti |
$S^{(p)}$ | Scalar overlap integral with proton distribution |
Vcb |
$V_{cb}$ | CKM element $V_{cb}$ |
Vn Al |
$V^{(n)$ | Vector overlap integral with neutron distribution |
Vn Au |
$V^{(n)$ | Vector overlap integral with neutron distribution |
Vn Ti |
$V^{(n)$ | Vector overlap integral with neutron distribution |
Vp Al |
$V^{(p)}$ | Vector overlap integral with proton distribution |
Vp Au |
$V^{(p)}$ | Vector overlap integral with proton distribution |
Vp Ti |
$V^{(p)}$ | Vector overlap integral with proton distribution |
Vub |
$\vert V_{ub}\vert$ | Absolute value of the CKM element $V_{ub}$ |
Vus |
$V_{us}$ | CKM element $V_{us}$ |
Xt_di->djnunu |
$X_t^{d_i\to d_j\nu\bar\nu}$ | Loop function for the CL_SM Wilson coefficient of $d_i\to d_j\nu\bar\nu$ |
a1_para_K*+ |
$a_1^{K^{*+}_\parallel}$ | First Gegenbauer moment of the parallely polarized $K^{*+}$ LCDA at 1 GeV |
a1_para_K*0 |
$a_1^{K^{*0}_\parallel}$ | First Gegenbauer moment of the parallely polarized $K^{*0}$ LCDA at 1 GeV |
a1_para_omega |
$a_1^{\omega_\parallel}$ | First Gegenbauer moment of the parallely polarized $\omega$ LCDA at 1 GeV |
a1_para_phi |
$a_1^{\phi_\parallel}$ | First Gegenbauer moment of the parallely polarized $\phi$ LCDA at 1 GeV |
a1_para_rho+ |
$a_1^{\rho^{+}_\parallel}$ | First Gegenbauer moment of the parallely polarized $\rho^{+}$ LCDA at 1 GeV |
a1_para_rho0 |
$a_1^{\rho^{0}_\parallel}$ | First Gegenbauer moment of the parallely polarized $\rho^{0}$ LCDA at 1 GeV |
a1_perp_K*+ |
$a_1^{K^{*+}_\perp}$ | First Gegenbauer moment of the transversely polarized $K^{*+}$ LCDA at 1 GeV |
a1_perp_K*0 |
$a_1^{K^{*0}_\perp}$ | First Gegenbauer moment of the transversely polarized $K^{*0}$ LCDA at 1 GeV |
a1_perp_omega |
$a_1^{\omega_\perp}$ | First Gegenbauer moment of the transversely polarized $\omega$ LCDA at 1 GeV |
a1_perp_phi |
$a_1^{\phi_\perp}$ | First Gegenbauer moment of the transversely polarized $\phi$ LCDA at 1 GeV |
a1_perp_rho+ |
$a_1^{\rho^{+}_\perp}$ | First Gegenbauer moment of the transversely polarized $\rho^{+}$ LCDA at 1 GeV |
a1_perp_rho0 |
$a_1^{\rho^{0}_\perp}$ | First Gegenbauer moment of the transversely polarized $\rho^{0}$ LCDA at 1 GeV |
a2_para_K*+ |
$a_2^{K^{*+}_\parallel}$ | Second Gegenbauer moment of the parallely polarized $K^{*+}$ LCDA at 1 GeV |
a2_para_K*0 |
$a_2^{K^{*0}_\parallel}$ | Second Gegenbauer moment of the parallely polarized $K^{*0}$ LCDA at 1 GeV |
a2_para_omega |
$a_2^{\omega_\parallel}$ | Second Gegenbauer moment of the parallely polarized $\omega$ LCDA at 1 GeV |
a2_para_phi |
$a_2^{\phi_\parallel}$ | Second Gegenbauer moment of the parallely polarized $\phi$ LCDA at 1 GeV |
a2_para_rho+ |
$a_2^{\rho^{+}_\parallel}$ | Second Gegenbauer moment of the parallely polarized $\rho^{+}$ LCDA at 1 GeV |
a2_para_rho0 |
$a_2^{\rho^{0}_\parallel}$ | Second Gegenbauer moment of the parallely polarized $\rho^{0}$ LCDA at 1 GeV |
a2_perp_K*+ |
$a_2^{K^{*+}_\perp}$ | Second Gegenbauer moment of the transversely polarized $K^{*+}$ LCDA at 1 GeV |
a2_perp_K*0 |
$a_2^{K^{*0}_\perp}$ | Second Gegenbauer moment of the transversely polarized $K^{*0}$ LCDA at 1 GeV |
a2_perp_omega |
$a_2^{\omega_\perp}$ | Second Gegenbauer moment of the transversely polarized $\omega$ LCDA at 1 GeV |
a2_perp_phi |
$a_2^{\phi_\perp}$ | Second Gegenbauer moment of the transversely polarized $\phi$ LCDA at 1 GeV |
a2_perp_rho+ |
$a_2^{\rho^{+}_\perp}$ | Second Gegenbauer moment of the transversely polarized $\rho^{+}$ LCDA at 1 GeV |
a2_perp_rho0 |
$a_2^{\rho^{0}_\perp}$ | Second Gegenbauer moment of the transversely polarized $\rho^{0}$ LCDA at 1 GeV |
a_chi_b0(1P) |
$a_{\chi_{b0}(1P)}$ | $\chi_{b0}(1P)$ anomaly decay constant |
a_chi_b0(2P) |
$a_{\chi_{b0}(2P)}$ | $\chi_{b0}(2P)$ anomaly decay constant |
a_chi_c0(1P) |
$a_{\chi_{c0}(1P)}$ | $\chi_{c0}(1P)$ anomaly decay constant |
a_e SM |
$a_e^\text{SM}$ | SM prediction for the anomalous magnetic moment of the electron |
a_eta_b(1S) |
$a_{\eta_b(1S)}$ | $\eta_b(1S)$ anomaly decay constant |
a_eta_c(1S) |
$a_{\eta_c(1S)}$ | $\eta_c(1S)$ anomaly decay constant |
a_mu SM |
$a_\mu^\text{SM}$ | SM prediction for the anomalous magnetic moment of the muon |
a_tau SM |
$a_\tau^\text{SM}$ | SM prediction for the anomalous magnetic moment of the tau |
alpha_CS(HfF) |
$\alpha_{C_S}^\text{HfF}$ | Coefficient of the scalar coupling contribution to the Hafnium fluoride energy shift |
alpha_CS(ThO) |
$\alpha_{C_S}^\text{ThO}$ | Coefficient of the scalar coupling contribution to the Thorium monoxide energy shift |
alpha_CS(Tl) |
$\alpha_{C_S}^\text{Tl}$ | Coefficient of the scalar coupling contribution to the Thallium EDM |
alpha_CS(YbF) |
$\alpha_{C_S}^\text{YbF}$ | Coefficient of the scalar coupling contribution to the Ytterbium fluoride energy shift |
alpha_de(HfF) |
$\alpha_{d_e}^\text{HfF}$ | Coefficient of the electron EDM contribution to the Hafnium fluoride energy shift |
alpha_de(ThO) |
$\alpha_{d_e}^\text{ThO}$ | Coefficient of the electron EDM contribution to the Thorium monoxide energy shift |
alpha_de(Tl) |
$\alpha_{d_e}^\text{Tl}$ | Coefficient of the electron EDM contribution to the Thallium EDM |
alpha_de(YbF) |
$\alpha_{d_e}^\text{YbF}$ | Coefficient of the electron EDM contribution to the Ytterbium fluoride energy shift |
alpha_e |
$\alpha_e(m_Z)$ | electromagnetic fine structure constant in the $\overline{\text{MS}}$ scheme at the scale $m_Z$ |
alpha_s |
$\alpha_s(m_Z)$ | strong coupling constant in the $\overline{\text{MS}}$ scheme at the scale $m_Z$ |
bag_B0_1 |
$B_1^{(d)}$ | $B^0$ bag parameter of $O_1$ in the $\overline{\text{MS}}$ scheme at $m_b$ |
bag_B0_2 |
$B_2^{(d)}$ | $B^0$ bag parameter of $O_2$ in the $\overline{\text{MS}}$ scheme at $m_b$ |
bag_B0_3 |
$B_3^{(d)}$ | $B^0$ bag parameter of $O_3$ in the $\overline{\text{MS}}$ scheme at $m_b$ |
bag_B0_4 |
$B_4^{(d)}$ | $B^0$ bag parameter of $O_4$ in the $\overline{\text{MS}}$ scheme at $m_b$ |
bag_B0_5 |
$B_5^{(d)}$ | $B^0$ bag parameter of $O_5$ in the $\overline{\text{MS}}$ scheme at $m_b$ |
bag_Bs_1 |
$B_1^{(s)}$ | $B_s$ bag parameter of $O_1$ in the $\overline{\text{MS}}$ scheme at $m_b$ |
bag_Bs_2 |
$B_2^{(s)}$ | $B_s$ bag parameter of $O_2$ in the $\overline{\text{MS}}$ scheme at $m_b$ |
bag_Bs_3 |
$B_3^{(s)}$ | $B_s$ bag parameter of $O_3$ in the $\overline{\text{MS}}$ scheme at $m_b$ |
bag_Bs_4 |
$B_4^{(s)}$ | $B_s$ bag parameter of $O_4$ in the $\overline{\text{MS}}$ scheme at $m_b$ |
bag_Bs_5 |
$B_5^{(s)}$ | $B_s$ bag parameter of $O_5$ in the $\overline{\text{MS}}$ scheme at $m_b$ |
bag_D0_1 |
$B_1^{(D)}$ | $D^0$ bag parameter of $O_1$ in the $\overline{\text{MS}}$ scheme at 2 GeV |
bag_D0_2 |
$B_2^{(D)}$ | $D^0$ bag parameter of $O_2$ in the $\overline{\text{MS}}$ scheme at 2 GeV |
bag_D0_3 |
$B_3^{(D)}$ | $D^0$ bag parameter of $O_3$ in the $\overline{\text{MS}}$ scheme at 2 GeV |
bag_D0_4 |
$B_4^{(D)}$ | $D^0$ bag parameter of $O_4$ in the $\overline{\text{MS}}$ scheme at 2 GeV |
bag_D0_5 |
$B_5^{(D)}$ | $D^0$ bag parameter of $O_5$ in the $\overline{\text{MS}}$ scheme at 2 GeV |
bag_K0_1 |
$B_1^{(K)}$ | $K^0$ bag parameter of $O_1$ in the $\overline{\text{MS}}$ scheme at 2 GeV |
bag_K0_2 |
$B_2^{(K)}$ | $K^0$ bag parameter of $O_2$ in the $\overline{\text{MS}}$ scheme at 2 GeV |
bag_K0_3 |
$B_3^{(K)}$ | $K^0$ bag parameter of $O_3$ in the $\overline{\text{MS}}$ scheme at 2 GeV |
bag_K0_4 |
$B_4^{(K)}$ | $K^0$ bag parameter of $O_4$ in the $\overline{\text{MS}}$ scheme at 2 GeV |
bag_K0_5 |
$B_5^{(K)}$ | $K^0$ bag parameter of $O_5$ in the $\overline{\text{MS}}$ scheme at 2 GeV |
c1_K+lnu |
$c_1^{(K)}$ | Chiral perturbation theory coefficient in $K^+\to\ell^+\nu$ |
c1_pi+lnu |
$c_1^{(\pi)}$ | Chiral perturbation theory coefficient in $\pi^+\to\ell^+\nu$ |
c2_K+lnu |
$c_2^{(K)}$ | Chiral perturbation theory coefficient in $K^+\to\ell^+\nu$ |
c2_pi+lnu |
$c_2^{(\pi)}$ | Chiral perturbation theory coefficient in $\pi^+\to\ell^+\nu$ |
c2t_K+lnu |
$\tilde{c}_2^{(K)}$ | Chiral perturbation theory coefficient in $K^+\to\ell^+\nu$ |
c2t_pi+lnu |
$\tilde{c}_2^{(\pi)}$ | Chiral perturbation theory coefficient in $\pi^+\to\ell^+\nu$ |
c3_K+lnu |
$c_3^{(K)}$ | Chiral perturbation theory coefficient in $K^+\to\ell^+\nu$ |
c3_pi+lnu |
$c_3^{(\pi)}$ | Chiral perturbation theory coefficient in $\pi^+\to\ell^+\nu$ |
c4_K+munu |
$c_4^{(K)}(m_\mu)$ | Chiral perturbation theory coefficient in $K^+\to\mu^+\nu$ |
c4_pi+munu |
$c_4^{(\pi)}(m_\mu)$ | Chiral perturbation theory coefficient in $\pi^+\to\mu^+\nu$ |
chi_2(1) |
$\chi_2(1)$ | Subleading Isgur-Wise function $\chi_2$ at $w=1$ |
chi_2p(1) |
$\chi_2'(1)$ | Derivative of subleading Isgur-Wise function $\chi_2$ at $w=1$ |
chi_2pp(1) |
$\chi_2''(1)$ | 2nd derivative of subleading Isgur-Wise function $\chi_2$ at $w=1$ |
chi_3p(1) |
$\chi_3'(1)$ | Derivative of subleading Isgur-Wise function $\chi_3$ at $w=1$ |
chi_3pp(1) |
$\chi_3''(1)$ | 3rd derivative of subleading Isgur-Wise function $\chi_3$ at $w=1$ |
chi_disp(KL->gammagamma) |
$\chi_\text{disp}$ | Dispersive part of the $K_L\to\gamma\gamma$ amplitude |
deltaPcu |
$\delta P_{c,u}$ | Contributions to the $K^+\to\pi^+\nu\bar\nu$ amplitude not described by the dimension-6 effective Hamiltonian. |
deltaRp_n |
$\delta R^\prime$ | Long-distance radiative correction to neutron beta decay |
delta_BXdee high |
$\delta_{bdee}^\text{high}$ | Quantity parametrizing the remaining theory uncertainty due to higher orders and non-perturbative effects in $B\to X_de^+e^-$ at high $q^2$. The relative uncertainty is $1+\delta$. |
delta_BXdee low |
$\delta_{bdee}^\text{low}$ | Quantity parametrizing the remaining theory uncertainty due to higher orders and non-perturbative effects in $B\to X_de^+e^-$ at low $q^2$. The relative uncertainty is $1+\delta$. |
delta_BXdgamma |
$\delta_{bd\gamma}$ | Quantity parametrizing the remaining theory uncertainty due to higher orders, interpolation, and non-perturbative effects in $B\to X_d\gamma$. The relative uncertainty is $1+\delta$. |
delta_BXdmumu high |
$\delta_{bd\mu\mu}^\text{high}$ | Quantity parametrizing the remaining theory uncertainty due to higher orders and non-perturbative effects in $B\to X_d\mu^+\mu^-$ at high $q^2$. The relative uncertainty is $1+\delta$. |
delta_BXdmumu low |
$\delta_{bd\mu\mu}^\text{low}$ | Quantity parametrizing the remaining theory uncertainty due to higher orders and non-perturbative effects in $B\to X_d\mu^+\mu^-$ at low $q^2$. The relative uncertainty is $1+\delta$. |
delta_BXdtautau high |
$\delta_{bd\tau\tau}^\text{high}$ | Quantity parametrizing the remaining theory uncertainty due to higher orders and non-perturbative effects in $B\to X_d\tau^+\tau^-$ at high $q^2$. The relative uncertainty is $1+\delta$. |
delta_BXlnu |
$\delta_{BX\ell\nu}$ | Quantity parametrizing the remaining theory uncertainty due to higher orders $B\to X_c\ell\nu$. |
delta_BXsee high |
$\delta_{bsee}^\text{high}$ | Quantity parametrizing the remaining theory uncertainty due to higher orders and non-perturbative effects in $B\to X_se^+e^-$ at high $q^2$. The relative uncertainty is $1+\delta$. |
delta_BXsee low |
$\delta_{bsee}^\text{low}$ | Quantity parametrizing the remaining theory uncertainty due to higher orders and non-perturbative effects in $B\to X_se^+e^-$ at low $q^2$. The relative uncertainty is $1+\delta$. |
delta_BXsgamma |
$\delta_{bs\gamma}$ | Quantity parametrizing the remaining theory uncertainty due to higher orders, interpolation, and non-perturbative effects in $B\to X_s\gamma$. The relative uncertainty is $1+\delta$. |
delta_BXsmumu high |
$\delta_{bs\mu\mu}^\text{high}$ | Quantity parametrizing the remaining theory uncertainty due to higher orders and non-perturbative effects in $B\to X_s\mu^+\mu^-$ at high $q^2$. The relative uncertainty is $1+\delta$. |
delta_BXsmumu low |
$\delta_{bs\mu\mu}^\text{low}$ | Quantity parametrizing the remaining theory uncertainty due to higher orders and non-perturbative effects in $B\to X_s\mu^+\mu^-$ at low $q^2$. The relative uncertainty is $1+\delta$. |
delta_BXstautau high |
$\delta_{bs\tau\tau}^\text{high}$ | Quantity parametrizing the remaining theory uncertainty due to higher orders and non-perturbative effects in $B\to X_s\tau^+\tau^-$ at high $q^2$. The relative uncertainty is $1+\delta$. |
delta_BsKstarmumu |
$\delta_{B_s^0 \to \bar{K}^{\ast 0} \mu \mu}$ | relative uncertainty on the $B_s^0 \to \bar{K}^{\ast 0} \mu \mu$ branching ratio inside the resonant region |
delta_Gammab |
$\delta_{\Gamma_b} $ | Uncertainty in the SM $Z$ partial width to bottom quarks in GeV |
delta_Gammac |
$\delta_{\Gamma_c}$ | Uncertainty in the SM $Z$ partial width to charm quarks in GeV |
delta_Gammad,s |
$\delta_{\Gamma_s}$ | Uncertainty in the SM $Z$ partial width to strange quarks in GeV |
delta_Gammae,mu |
$\delta_{\Gamma_{e,\mu}}$ | Uncertainty in the SM $Z$ partial width to light leptons in GeV |
delta_Gammanu |
$\delta_{\Gamma_\nu}$ | Uncertainty in the SM $Z$ partial width to neutrinos in GeV |
delta_Gammatau |
$\delta_{\Gamma_\tau}$ | Uncertainty in the SM $Z$ partial width to tau leptons in GeV |
delta_Gammau |
$\delta_{\Gamma_u}$ | Uncertainty in the SM $Z$ partial width to up quarks in GeV |
delta_deltaNS,A |
$\delta(\delta_{NS,A}$ | Uncertainty on the nuclear structure dependent corrections from quenching in nuclei |
delta_deltaNS,E_QEC |
$\delta(\delta_{NS,E} / Q_{EC}$ | Uncertainty on the nuclear structure dependent corrections from nuclear polarizabilities divided by $Q_{EC}$ |
delta_deltaRp_Z2 |
$\delta(\delta R^\prime) / Z^2$ | Uncertainty on the structure-independent radiative correction to beta decay divided by $Z^2$ |
delta_mN |
$\delta m_N$ | QCD contribution to the neutron-proton mass difference |
eps_K |
$|\epsilon_K|$ | Measured value of $|\epsilon_K|$ |
epsp a |
$a$ | Parameter for isospin breaking corrections to $\epsilon'/\epsilon$ |
eta(1) |
$\eta(1)$ | Subleading Isgur-Wise function $\eta$ at $w=1$ |
eta_cc_K0 |
$\eta_{cc}$ | SM QCD correction factor for the charm contribution to $K^0$ mixing |
eta_ct_K0 |
$\eta_{ct}$ | SM QCD correction factor for the top-charm contribution to $K^0$ mixing |
eta_tt_B0 |
$\eta_B$ | SM QCD correction factor for $B^0$ mixing |
eta_tt_Bs |
$\eta_B$ | SM QCD correction factor for $B_s$ mixing |
eta_tt_K0 |
$\eta_{tt}$ | SM QCD correction factor for the top contribution to $K^0$ mixing |
eta_tt_K0_ut |
$\eta_{tt,c}$ | SM QCD correction factor for the top contribution to $K^0$ mixing using u-t unitarity |
eta_ut_K0_ut |
$\eta_{ut,ut}$ | SM QCD correction factor for the top-up contribution to $K^0$ mixing using u-t unitarity |
eta_uu_K0_ut |
$\eta_{uu,ut}$ | SM QCD correction factor for the up contribution to $K^0$ mixing using u-t unitarity |
etap(1) |
$\eta'(1)$ | Derivative of subleading Isgur-Wise function $\eta$ at $w=1$ |
etapp(1) |
$\eta''(1)$ | 2nd derivative of subleading Isgur-Wise function $\eta$ at $w=1$ |
fT_J/psi |
$f_{J/\psi}^T$ | $J/\psi$ tensor decay constant |
fT_Upsilon(1S) |
$f_{\Upsilon(1S)}^T$ | $\Upsilon(1S)$ tensor decay constant |
fT_Upsilon(2S) |
$f_{\Upsilon(2S)}^T$ | $\Upsilon(2S)$ tensor decay constant |
fT_Upsilon(3S) |
$f_{\Upsilon(3S)}^T$ | $\Upsilon(3S)$ tensor decay constant |
fT_psi(2S) |
$f_{\psi(2S)}^T$ | $\psi(2S)$ tensor decay constant |
f_B+ |
$f_{B^\pm}$ | $B^\pm$ decay constant |
f_B0 |
$f_{B^0}$ | $B^0$ decay constant |
f_Bc |
$f_{B_c}$ | $B_c$ decay constant |
f_Bs |
$f_{B_s}$ | $B_s$ decay constant |
f_D+ |
$f_{D^\pm}$ | $D^\pm$ decay constant |
f_D0 |
$f_{D^0}$ | $D^0$ decay constant |
f_Ds |
$f_{D_s}$ | $D_s$ decay constant |
f_J/psi |
$f_{J/\psi}$ | $J/\psi$ decay constant |
f_K*+ |
$f_{K^{*\pm}}$ | $K^{*\pm}$ decay constant |
f_K*0 |
$f_{K^{*0}}$ | $K^{*0}$ decay constant |
f_K+ |
$f_{K^\pm}$ | Charged kaon decay constant |
f_K0 |
$f_{K^0}$ | Neutral kaon decay constant |
f_Upsilon(1S) |
$f_{\Upsilon(1S)}$ | $\Upsilon(1S)$ decay constant |
f_Upsilon(2S) |
$f_{\Upsilon(2S)}$ | $\Upsilon(2S)$ decay constant |
f_Upsilon(3S) |
$f_{\Upsilon(3S)}$ | $\Upsilon(3S)$ decay constant |
f_chi_b0(1P) |
$f_{\chi_{b0}(1P)}$ | $\chi_{b0}(1P)$ decay constant |
f_chi_b0(2P) |
$f_{\chi_{b0}(2P)}$ | $\chi_{b0}(2P)$ decay constant |
f_chi_c0(1P) |
$f_{\chi_{c0}(1P)}$ | $\chi_{c0}(1P)$ decay constant |
f_eta_b(1S) |
$f_{\eta_b(1S)}$ | $\eta_b(1S)$ decay constant |
f_eta_c(1S) |
$f_{\eta_c(1S)}$ | $\eta_c(1S)$ decay constant |
f_n |
$f_n$ | Statistical rate function for neutron beta decay |
f_omega |
$f_{\omega}$ | $\omega$ decay constant |
f_perp_K*+ |
$f^\perp_{K^{\pm}}$ | Transverse $K^{*\pm}$ decay constant at 2 GeV in the 3-flavour scheme |
f_perp_K*0 |
$f^\perp_{K^{*0}}$ | Transverse $K^{*0}$ decay constant at 2 GeV in the 3-flavour scheme |
f_perp_omega |
$f^\perp_\omega$ | Transverse $\omega$ decay constant at 2 GeV in the 3-flavour scheme |
f_perp_phi |
$f^\perp_\phi$ | Transverse $\phi$ decay constant at 2 GeV in the 3-flavour scheme |
f_perp_rho+ |
$f^\perp_{\rho^{\pm}}$ | Transverse $\rho^{\pm}$ decay constant at 2 GeV in the 3-flavour scheme |
f_perp_rho0 |
$f^\perp_{\rho^{0}}$ | Transverse $\rho^{0}$ decay constant at 2 GeV in the 3-flavour scheme |
f_phi |
$f_{\phi}$ | $\phi$ decay constant |
f_pi+ |
$f_{\pi^\pm}$ | Charged pion decay constant |
f_pi0 |
$f_{\pi^0}$ | Neutral pion decay constant |
f_psi(2S) |
$f_{\psi(2S)}$ | $\psi(2S)$ decay constant |
f_rho0 |
$f_{\rho^0}$ | $\rho^0$ decay constant |
gA_s |
$g_A^s$ | Proton strange quark axial charge |
gS_u-d |
$g_S^{u-d}$ | Nucleon isovector scalar charge |
gT_d |
$g_T^d$ | Proton down quark tensor charge |
gT_s |
$g_T^s$ | Proton strange quark tensor charge |
gT_u |
$g_T^u$ | Proton up quark tensor charge |
g_A |
$g_A^{u-d}$ | Nucleon isovector axial charge |
gamma |
$\gamma$ | CKM Unitarity Triangle angle $\gamma$ in radians |
kappa_L_tilde |
$\tilde{\kappa}_L$ | Parameter $\kappa_L$ containing the hadronic form factor information needed for the $K_L\to\pi^0\nu\bar\nu$ branching ratio, determined assuming $V_{us}\equiv0.225$ |
kappa_epsilon |
$\kappa_\epsilon$ | Correction factor for $\epsilon_K$ |
kappa_plus_tilde |
$\tilde{\kappa}_+$ | Parameter $\kappa_+$ containing the hadronic form factor information needed for the $K^+\to\pi^+\nu\bar\nu$ branching ratio, determined assuming $V_{us}\equiv0.225$ |
lambda_1 |
$\lambda_1$ | Matrix element of $B$ meson kinetic energy operator |
lambda_2 |
$\lambda_2$ | Matrix element of $B$ meson magnetic moment operator |
m_B*+ |
$m_{B^{*+}}$ | $B^{*+}$ mass |
m_B*0 |
$m_{B^{*0}}$ | $B^{*0}$ mass |
m_B+ |
$m_{B^{+}}$ | $B^{+}$ mass |
m_B0 |
$m_{B^{0}}$ | $B^{0}$ mass |
m_Bc |
$m_{B_{c}}$ | $B_{c}$ mass |
m_Bs |
$m_{B_{s}}$ | $B_{s}$ mass |
m_Bs* |
$m_{B_{s}^{*}}$ | $B_{s}^{*}$ mass |
m_D*+ |
$m_{D^{*+}}$ | $D^{*+}$ mass |
m_D*0 |
$m_{D^{*0}}$ | $D^{*0}$ mass |
m_D+ |
$m_{D^{+}}$ | $D^{+}$ mass |
m_D0 |
$m_{D^{0}}$ | $D^{0}$ mass |
m_Ds |
$m_{D_{s}}$ | $D_{s}$ mass |
m_Ds* |
$m_{D_{s}^{*}}$ | $D_{s}^{*}$ mass |
m_J/psi |
$m_{J/\psi}$ | $J/\psi$ mass |
m_K*+ |
$m_{K^{*+}}$ | $K^{*+}$ mass |
m_K*0 |
$m_{K^{*0}}$ | $K^{*0}$ mass |
m_K+ |
$m_{K^{+}}$ | $K^{+}$ mass |
m_K0 |
$m_{K^{0}}$ | $K^{0}$ mass |
m_KL |
$m_{K_{L}}$ | $K_{L}$ mass |
m_KS |
$m_{K_{S}}$ | $K_{S}$ mass |
m_Lambda |
$m_{\Lambda}$ | $\Lambda$ mass |
m_Lambda(1520) |
$m_{\Lambda}$ | $\Lambda$ mass |
m_Lambdab |
$m_{\Lambda_{b}}$ | $\Lambda_{b}$ mass |
m_Lambdac |
$m_{\Lambda_{c}}$ | $\Lambda_{c}$ mass |
m_Upsilon(1S) |
$m_{\Upsilon_{1S}}$ | $\Upsilon_{1S}$ mass |
m_Upsilon(2S) |
$m_{\Upsilon_{2S}}$ | $\Upsilon_{2S}$ mass |
m_Upsilon(3S) |
$m_{\Upsilon_{3S}}$ | $\Upsilon_{3S}$ mass |
m_W |
$m_{W}$ | $W$ mass |
m_Z |
$m_{Z}$ | $Z$ mass |
m_b |
$m_{b}(m_{b})$ | $b$ quark mass in the $\overline{\text{MS}}$ scheme at the scale $m_b$ |
m_c |
$m_{c}(m_{c})$ | $c$ quark mass in the $\overline{\text{MS}}$ scheme at the scale $m_c$ |
m_c BVgamma |
$m_c$ | Charm quark mass entering $O(\alpha_s)$ corrections to matrix elements in exclusive radiative $B$ decays. Uncertainty contains scheme ambiguity at $O(\alpha_s)$. |
m_chi_b0(1P) |
$m_{\chi_{b0}}$ | $\chi_{b0}$ mass |
m_chi_b0(2P) |
$m_{\chi_{b0}}$ | $\chi_{b0}$ mass |
m_chi_c0(1P) |
$m_{\chi_{c0}}$ | $\chi_{c0}$ mass |
m_d |
$m_{d}(2\,\text{GeV})$ | $d$ quark mass in the $\overline{\text{MS}}$ scheme at 2 GeV |
m_e |
$m_{e}$ | $e$ mass |
m_eta |
$m_{\eta}$ | $\eta$ mass |
m_eta_b(1S) |
$m_{\eta_b(1S)}$ | $\eta_b(1S)$ mass |
m_eta_c(1S) |
$m_{\eta_{c}}$ | $\eta_{c}$ mass |
m_f0 |
$m_{f_{0}}$ | $f_{0}$ mass |
m_h |
$m_{H}$ | $H$ mass |
m_mu |
$m_{\mu}$ | $\mu$ mass |
m_n |
$m_{n}$ | $n$ mass |
m_omega |
$m_{\omega}$ | $\omega$ mass |
m_p |
$m_{p}$ | $p$ mass |
m_phi |
$m_{\phi}$ | $\phi$ mass |
m_pi+ |
$m_{\pi^{+}}$ | $\pi^{+}$ mass |
m_pi0 |
$m_{\pi^{0}}$ | $\pi^{0}$ mass |
m_psi(2S) |
$m_{\psi_{2S}}$ | $\psi_{2S}$ mass |
m_rho+ |
$m_{\rho^{+}}$ | $\rho^{+}$ mass |
m_rho0 |
$m_{\rho^{0}}$ | $\rho^{0}$ mass |
m_s |
$m_{s}(2\,\text{GeV})$ | $s$ quark mass in the $\overline{\text{MS}}$ scheme at 2 GeV |
m_t |
$m_{t}$ | $t$ quark pole mass |
m_tau |
$m_{\tau}$ | $\tau$ mass |
m_u |
$m_{u}$ | $u$ mass |
mu_G^2 |
$\mu_G^2$ | |
mu_pi^2 |
$\mu_\pi^2$ | |
nEDM beta_G |
$\beta_G$ | coefficient of the three-gluon Weinberg operator contribution to the neutron EDM |
nEDM ~rho_d |
$\tilde \rho_d$ | coefficient of the down quark CEDM contribution to the neutron EDM |
nEDM ~rho_s |
$\tilde \rho_s$ | coefficient of the strange quark CEDM contribution to the neutron EDM |
nEDM ~rho_u |
$\tilde \rho_u$ | coefficient of the up quark CEDM contribution to the neutron EDM |
omega+ |
$\omega_+$ | |
rho_D^3 |
$\rho_D^3$ | |
rho_LS^3 |
$\rho_{LS}^3$ | |
s2w |
$\sin^2 \hat\theta_w(m_Z)$ | sine squared of the weak mixing angle in the $\overline{\text{MS}}$ scheme at the scale $m_Z$ |
sigma_piN |
$\sigma_{\pi N}$ | Pion-nucleon $\sigma$ term |
sigma_s |
$\sigma_s$ | Nuclean strange quark $\sigma$ term |
tau_B+ |
$\tau_{B^{+}}$ | $B^{+}$ lifetime |
tau_B0 |
$\tau_{B^{0}}$ | $B^{0}$ lifetime |
tau_Bc |
$\tau_{B_{c}}$ | $B_{c}$ lifetime |
tau_Bc_SM |
$\tau_{B_c}^\text{SM}$ | Standard Model prediction for the $B_c$ lifetime |
tau_Bs |
$\tau_{B_{s}}$ | $B_{s}$ lifetime |
tau_D*+ |
$\tau_{D^{*+}}$ | $D^{*+}$ lifetime |
tau_D+ |
$\tau_{D^{+}}$ | $D^{+}$ lifetime |
tau_D0 |
$\tau_{D^{0}}$ | $D^{0}$ lifetime |
tau_Ds |
$\tau_{D_{s}}$ | $D_{s}$ lifetime |
tau_J/psi |
$\tau_{J/\psi}$ | $J/\psi$ lifetime |
tau_K*+ |
$\tau_{K^{*+}}$ | $K^{*+}$ lifetime |
tau_K*0 |
$\tau_{K^{*0}}$ | $K^{*0}$ lifetime |
tau_K+ |
$\tau_{K^{+}}$ | $K^{+}$ lifetime |
tau_KL |
$\tau_{K_{L}}$ | $K_{L}$ lifetime |
tau_KS |
$\tau_{K_{S}}$ | $K_{S}$ lifetime |
tau_Lambda |
$\tau_{\Lambda}$ | $\Lambda$ lifetime |
tau_Lambda(1520) |
$\tau_{\Lambda}$ | $\Lambda$ lifetime |
tau_Lambdab |
$\tau_{\Lambda_{b}}$ | $\Lambda_{b}$ lifetime |
tau_Lambdac |
$\tau_{\Lambda_{c}}$ | $\Lambda_{c}$ lifetime |
tau_Upsilon(1S) |
$\tau_{\Upsilon_{1S}}$ | $\Upsilon_{1S}$ lifetime |
tau_Upsilon(2S) |
$\tau_{\Upsilon_{2S}}$ | $\Upsilon_{2S}$ lifetime |
tau_Upsilon(3S) |
$\tau_{\Upsilon_{3S}}$ | $\Upsilon_{3S}$ lifetime |
tau_W |
$\tau_{W}$ | $W$ lifetime |
tau_Z |
$\tau_{Z}$ | $Z$ lifetime |
tau_chi_b0(1P) |
$\tau_{\chi_{b0}(1P)}$ | lifetime of $\chi_{b0}(1P)$ |
tau_chi_b0(2P) |
$\tau_{\chi_{b0}(2P)}$ | lifetime of $\chi_{b0}(2P)$ |
tau_chi_c0(1P) |
$\tau_{\chi_{c0}}$ | $\chi_{c0}$ lifetime |
tau_eta |
$\tau_{\eta}$ | $\eta$ lifetime |
tau_eta_b(1S) |
$\tau_{\eta_b(1S)}$ | $\eta_b(1S)$ lifetime |
tau_eta_c(1S) |
$\tau_{\eta_{c}}$ | $\eta_{c}$ lifetime |
tau_f0 |
$\tau_{f_{0}}$ | $f_{0}$ lifetime |
tau_h |
$\tau_{H}$ | $H$ lifetime |
tau_mu |
$\tau_{\mu}$ | $\mu$ lifetime |
tau_n |
$\tau_{n}$ | $n$ lifetime |
tau_omega |
$\tau_{\omega}$ | $\omega$ lifetime |
tau_phi |
$\tau_{\phi}$ | $\phi$ lifetime |
tau_pi+ |
$\tau_{\pi^{+}}$ | $\pi^{+}$ lifetime |
tau_pi0 |
$\tau_{\pi^{0}}$ | $\pi^{0}$ lifetime |
tau_psi(2S) |
$\tau_{\psi_{2S}}$ | $\psi_{2S}$ lifetime |
tau_rho+ |
$\tau_{\rho^{+}}$ | $\rho^{+}$ lifetime |
tau_rho0 |
$\tau_{\rho^{0}}$ | $\rho^{0}$ lifetime |
tau_t |
$\tau_{t}$ | $t$ lifetime |
tau_tau |
$\tau_{\tau}$ | $\tau$ lifetime |
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