TY  - JOUR
AU  - Albertus, C.
AU  - Hernandez, E.
AU  - Nieves, J.
PY  - 2014
DA  - 2014//
TI  - B -> rho semileptonic decays and vertical bar V-ub vertical bar
T2  - Phys. Rev. D
JO  - Physical Review D
SP  - 013017
EP  - 11pp
VL  - 90
IS  - 1
PB  - Amer Physical Soc
AB  - We reevaluate the B -> rho l(+) nu(l) decay width as a full B. pi pi iota(+)nu iota four-particle decay, in which the two final pions are produced via an intermediate. meson. The decay width can be written as a convolution of the B -> rho l(+) nu(l) decay width, for an off-shell., with the.. pp line shape. This allows us to fully incorporate the effects of the finite. meson width and a better comparison with actual experiments. We use an Omn s representation to provide the dependence of the B.. semileptonic form factors on q2. The Omn s subtraction constants and the overall normalization parameter jVubj are fitted to light cone sum rules and lattice QCD theoretical form-factor calculations, in the low and high q2 regions, respectively, together to the CLEO, BABAR, and Belle experimental partial branching fraction distributions. The extracted value from this global fit is jVubj d3.40 +/- 0.15_ x 10-3, in agreement with jVubj extracted using all other inputs in Cabibbo-Kobayashi-Maskawa fits and the exclusive semileptonic B. p channel, but showing a clear disagreement with jVubj extracted from inclusive semileptonic b. u decays. As estimated by [U.-G. Mei beta ner andW. Wang, J. High Energy Phys. 01 (2014) 107], taking into account the. meson width effects and the actual acceptance of the experiments is essential to render the jVubj determinations from exclusive B. p and B.. decays totally compatible.
SN  - 1550-7998
UR  - http://arxiv.org/abs/arXiv:1406.7782
UR  - https://doi.org/10.1103/PhysRevD.90.013017
DO  - 10.1103/PhysRevD.90.013017
LA  - English
N1  - WOS:000339482900002
ID  - Albertus_etal2014
ER  -