WL Ju, GL Wang, HF Fu… - Journal of High Energy …, 2015 - ui.adsabs.harvard.edu
The rare processes {B} _cto {D_ {(s)}^{(*)}} _Jμ overline {μ}, where D (s)(*) J stands for the final meson D s0*(2317), D s1 (2460, 2536), D s2*(2573), D 0*(2400), D 1 (2420, 2430) or D …
WL Ju, GL Wang, HF Fu, ZH Wang, Y Li - JHEP, 2015 - inspirehep.net
The rare processes ${B} _c\to {D_ {(s)}^{\left (*\right)}} _J\mu\overline {\mu} $, where D $ _ {(s} _ {)}^{(*) J} $ stands for the final meson D $ _ {s0}^{*} $(2317), D $ _ {s1} $(2460, 2536) …
WL Ju, GL Wang, HF Fu, ZH Wangc, Y Lid - core.ac.uk
The rare processes Bc→ D(∗)(s) J µµ, where D (∗)(s) J stands for the final meson D∗ s0 (2317), Ds1 (2460, 2536), D∗ s2 (2573), D∗ 0 (2400), D1 (2420, 2430) or D∗ 2 (2460), are …
WL Ju, GL Wang, HF Fu, ZH Wangc, Y Lid - s3.cern.ch
The rare processes Bc→ D(∗)(s) J µµ, where D (∗)(s) J stands for the final meson D∗ s0 (2317), Ds1 (2460, 2536), D∗ s2 (2573), D∗ 0 (2400), D1 (2420, 2430) or D∗ 2 (2460), are …
WL Ju, GL Wang, HF Fu, ZH Wang, Y Li - Journal of High Energy Physics, 2015 - infona.pl
The rare processes B c→ D s* J μ μ¯ $${B} _c\to {D_ {(s)}^{\left (*\right)}} _J\mu\overline {\mu} $$, where D (s)(*) J stands for the final meson Ds0*(2317), Ds1 (2460, 2536) …
WL Ju, GL Wang, HF Fu, ZH Wang, Y Li - 2015 - repo.scoap3.org
The rare processes Bc→ D(∗)(s) J µµ, where D (∗)(s) J stands for the final meson D∗ s0 (2317), Ds1 (2460, 2536), D∗ s2 (2573), D∗ 0 (2400), D1 (2420, 2430) or D∗ 2 (2460), are …