Light-cone sum rules for $B \to π$ form factors revisited
| dc.creator | Duplancic, G. | |
| dc.creator | Khodjamirian, A. | |
| dc.creator | Mannel, Th. | |
| dc.creator | Melic, B. | |
| dc.creator | Offen, N. | |
| dc.date | 2008-01-11 | |
| dc.date | 2008-04-03 | |
| dc.date.accessioned | 2026-07-07T12:24:08Z | |
| dc.date.available | 2026-07-07T12:24:08Z | |
| dc.description | We reconsider and update the QCD light-cone sum rules for $B\to π$ form factors. The gluon radiative corrections to the twist-2 and twist-3 terms in the correlation functions are calculated. The $\bar{MS}$ $b$-quark mass is employed, instead of the one-loop pole mass used in the previous analyses. The light-cone sum rule for $f^+_{Bπ}(q^2)$ is fitted to the measured $q^2$-distribution in $B\to πl ν_l$, fixing the input parameters with the largest uncertainty: the Gegenbauer moments of the pion distribution amplitude. For the $B\to π$ vector form factor at zero momentum transfer we predict $f^+_{Bπ}(0)= 0.26^{+0.04}_{-0.03}$. Combining it with the value of the product $|V_{ub}f^+_{Bπ}(0)|$ extracted from experiment, we obtain $|V_{ub}|=(3.5\pm 0.4\pm 0.2\pm 0.1) \times 10^{-3}$. In addition, the scalar and penguin $B\to π$ form factors $f^0_{Bπ}(q^2)$ and $f^T_{Bπ}(q^2)$ are calculated. | |
| dc.description | 33 pages, 7 figures, one figure and a few comments added, version to appear in JHEP | |
| dc.identifier | https://arxiv.org/abs/0801.1796 | |
| dc.identifier | http://arxiv.org/abs/0801.1796 | |
| dc.identifier | JHEP 0804:014,2008 | |
| dc.identifier | doi:10.1088/1126-6708/2008/04/014 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/214225 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | Light-cone sum rules for $B \to π$ form factors revisited | |
| dc.type | text |