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Search for violations of Lorentz invariance and CPT symmetry in B0(s) mixing

MPS-Authors
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Aquines Gutierrez,  O.
Division Prof. Dr. Werner Hofmann, MPI for Nuclear Physics, Max Planck Society;

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Blouw,  Johan
Division Prof. Dr. Werner Hofmann, MPI for Nuclear Physics, Max Planck Society;

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Britsch,  Markward
Division Prof. Dr. Werner Hofmann, MPI for Nuclear Physics, Max Planck Society;

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Fontana,  Marianna
Division Prof. Dr. Werner Hofmann, MPI for Nuclear Physics, Max Planck Society;

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Popov,  Dmitry
Division Prof. Dr. Werner Hofmann, MPI for Nuclear Physics, Max Planck Society;

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Schmelling,  Michael
Division Prof. Dr. Werner Hofmann, MPI for Nuclear Physics, Max Planck Society;

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Zavertyaev,  Mikhail
Division Prof. Dr. Werner Hofmann, MPI for Nuclear Physics, Max Planck Society;

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1603.04804.pdf
(Preprint), 537KB

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Citation

LHCb Collaboration, Aaij, R., Abellán Beteta, C., Adeva, B., Adinolfi, M., Ajaltouni, Z., et al. (2016). Search for violations of Lorentz invariance and CPT symmetry in B0(s) mixing. Physical Review Letters, 116(24): 241601. doi:10.1103/PhysRevLett.116.241601.


Cite as: https://hdl.handle.net/11858/00-001M-0000-002B-2070-1
Abstract
Violations of $ CPT$ symmetry and Lorentz invariance are searched for by
studying interference effects in $ B^0$ mixing and in $ B^0_s$ mixing. Samples
of $ B^0\to J/\psi K^0_{\mathrm{S}}$ and $ B^0_s\to J/\psi K^+ K^-$ decays are
recorded by the LHCb detector in proton--proton collisions at centre-of-mass
energies of 7 and 8 TeV, corresponding to an integrated luminosity of 3
fb$^{-1}$. No periodic variations of the particle-antiparticle mass differences
are found, consistent with Lorentz invariance and $ CPT$ symmetry. Results are
expressed in terms of the Standard Model Extension parameter $\Delta a_{\mu}$
with precisions of $ \mathcal{O}(10^{-15})$ and $ \mathcal{O}(10^{-14})$ GeV
for the $ B^0$ and $ B^0_s$ systems, respectively. With no assumption on
Lorentz (non-)invariance, the $ CPT$-violating parameter $z$ in the $ B^0_s$
system is measured for the first time and found to be $ \mathcal{R}e(z) =
-0.022 \pm 0.033 \pm 0.005$ and $ \mathcal{I}m(z) = 0.004 \pm 0.011\pm 0.002$,
where the first uncertainties are statistical and the second systematic.