Repository logo
Log in(current)
Repository logoMIT Open ScholarshipDSpace@MIT
  1. Home
  2. MIT Open Access Articles
  3. MIT Open Access Articles
  4. Angular analysis of B 0 → D ∗ − D s ∗ + $$ {B}^0\to {D}^{\ast -}{D}_s^{\ast +} $$ with D s ∗ + → D s + γ $$ {D}_s^{\ast +}\to {D}_s^{+}\gamma $$ decays

Angular analysis of B 0 → D ∗ − D s ∗ + $$ {B}^0\to {D}^{\ast -}{D}_s^{\ast +} $$ with D s ∗ + → D s + γ $$ {D}_s^{\ast +}\to {D}_s^{+}\gamma $$ decays

Thumbnail Image
Download
Name

13130_2021_Article_16089.pdf

Size

1.74 MB

Format

Adobe PDF

Checksum (MD5)

dbf25ce77cd933bb74fb263ef8946dcd

Download all files submitted through automated deposit
art_9075073926462202552.zip (1.26 MB)
Author(s)
Aaij, R.
•
Abellán Beteta, C.
•
Ackernley, T.
•
Adeva, B.
•
Adinolfi, M.
•
Afsharnia, H.
•
Aidala, C. A.
•
Aiola, S.
•
Ajaltouni, Z.
•
Akar, S.
more
Date Issued
June 29, 2021
Publisher
Springer Berlin Heidelberg
Citation
Journal of High Energy Physics. 2021 Jun 29;2021(6):177
Version
Final published version
Abstract
Abstract The first full angular analysis of the B 0 → D ∗ − D s ∗ + $$ {B}^0\to {D}^{\ast -}{D}_s^{\ast +} $$ decay is performed using 6 fb−1 of pp collision data collected with the LHCb experiment at a centre-of-mass energy of 13 TeV. The D s ∗ + → D s + γ $$ {D}_s^{\ast +}\to {D}_s^{+}\gamma $$ and D*− → D ¯ 0 π − $$ {\overline{D}}^0{\pi}^{-} $$ vector meson decays are used with the subsequent D s + $$ {D}_s^{+} $$ → K+K−π+ and D ¯ 0 $$ {\overline{D}}^0 $$ → K+π− decays. All helicity amplitudes and phases are measured, and the longitudinal polarisation fraction is determined to be fL = 0.578 ± 0.010 ± 0.011 with world-best precision, where the first uncertainty is statistical and the second is systematic. The pattern of helicity amplitude magnitudes is found to align with expectations from quark-helicity conservation in B decays. The ratio of branching fractions [ℬ( B 0 → D ∗ − D s ∗ + $$ {B}^0\to {D}^{\ast -}{D}_s^{\ast +} $$ ) × ℬ( D s ∗ + → D s + γ $$ {D}_s^{\ast +}\to {D}_s^{+}\gamma $$ )]/ℬ(B0 → D*− D s + $$ {D}_s^{+} $$ ) is measured to be 2.045 ± 0.022 ± 0.071 with world-best precision. In addition, the first observation of the Cabibbo-suppressed Bs → D*− D s + $$ {D}_s^{+} $$ decay is made with a significance of seven standard deviations. The branching fraction ratio ℬ(Bs → D*− D s + $$ {D}_s^{+} $$ )/ℬ(B0 → D*− D s + $$ {D}_s^{+} $$ ) is measured to be 0.049 ± 0.006 ± 0.003 ± 0.002, where the third uncertainty is due to limited knowledge of the ratio of fragmentation fractions.
MIT Department
Massachusetts Institute of Technology. Department of Physics
Terms of Use
Creative Commons Attribution
https://creativecommons.org/licenses/by/4.0/
Persistent DSpace Link
https://hdl.handle.net/1721.1/136739
DOI of Published Version
https://doi.org/10.1007/JHEP06(2021)177
Repository logo
PrivacyPermissionsAccessibilityContact us
Repository logo
Notify us about copyright concerns.