FORWARD-BACKWARD ASYMMETRIES
The forward-backward assymmetry is defined as A$_{FB}$ = [ N(q$_{FB}>$ 0) $−$ N(q$_{FB}<$ 0)] $/$ [N(q$_{FB}>$ 0) + N(q$_{FB}<$ 0) ], where q$_{FB}$ = $−$ q$_{B}\cdot{}$sgn(${{\mathit \eta}_{{{B}}}}$) with q$_{B}$ as the ${{\mathit B}}$ hadron electric charge, ${{\mathit \eta}_{{{B}}}}$ as its pseudorapidity, and sgn(${{\mathit \eta}_{{{B}}}}$) as a sign function of ${{\mathit \eta}_{{{B}}}}$.
A$_{P}({{\mathit B}^{+}}$) = [${\mathit \sigma (}{{\mathit B}^{-}}{)}$ $−$ ${\mathit \sigma (}{{\mathit B}^{+}}{)}$] $/$ [${\mathit \sigma (}{{\mathit B}^{-}}{)}$ $+$ ${\mathit \sigma (}{{\mathit B}^{+}}{)}$]
INSPIRE search
Production asymmetries
S041A03 |
$\bf{
-5.7 \pm1.7}$
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OUR AVERAGE
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$-7.0$ $\pm0.8$ $\pm3.1$ |
1 |
|
LHCB |
$-4.1$ $\pm4.9$ $\pm1.0$ |
2 |
|
LHCB |
$-5.3$ $\pm3.1$ $\pm1.0$ |
2 |
|
LHCB |
$-2.3$ $\pm2.4$ $\pm3.7$ |
3 |
|
LHCB |
$-7.4$ $\pm1.5$ $\pm3.2$ |
3 |
|
LHCB |
1
The second error includes the uncertainties from $\mathit A_{CP}$( ${{\mathit B}^{+}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit K}^{+}}$) = $0.0018$ $\pm0.0030$.
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2
AAIJ 2017AP uses ${{\mathit B}^{+}}$ $\rightarrow$ ${{\overline{\mathit D}}^{0}}{{\mathit \pi}^{+}}$ decays with ${{\mathit B}^{+}}$ transverse momenta $p_T$ and rapidities y in the region of 2 $<$ $p_T$ $<$ 30 GeV/c and 2.1 $<$ y $<$ 4.5.
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3
AAIJ 2017BF uses ${{\mathit B}^{+}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit K}^{+}}$ decays with ${{\mathit B}^{+}}$ transverse momenta $p_T$ and rapidities y in the region of 0 $<$ $p_T$ $<$ 30 GeV/c and 2.1 $<$ y $<$ 4.5.
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References: |
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PR D108 012008
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Direct violation in charmless three-body decays of mesons |
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PR D95 052005
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Measurement of the ${{\mathit B}^{\pm}}$ Production Asymmetry and the $\mathit CP$ Asymmetry in ${{\mathit B}^{\pm}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit K}^{\pm}}$ Decays |
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PL B774 139
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Measurement of ${{\mathit B}^{0}}$, ${{\mathit B}_{{{s}}}^{0}}$, ${{\mathit B}^{+}}$ and ${{\mathit \Lambda}_{{{b}}}^{0}}$ Production Asymmetries in 7 and 8 TeV Proton-Proton Collisions |
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