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Observation of the time dependence of B(d)0 - anti-B(d)0 mixing

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Observation of the time dependence of B(d)0 - anti-B(d)0 mixing. / ALEPH Collaboration.
In: Physics Letters B, Vol. 313, No. 3-4, 1993, p. 498-508.

Research output: Contribution to Journal/Magazine › Journal article › peer-review

Harvard

ALEPH Collaboration 1993, 'Observation of the time dependence of B(d)0 - anti-B(d)0 mixing', Physics Letters B, vol. 313, no. 3-4, pp. 498-508. https://doi.org/10.1016/0370-2693(93)90025-D

APA

ALEPH Collaboration (1993). Observation of the time dependence of B(d)0 - anti-B(d)0 mixing. Physics Letters B, 313(3-4), 498-508. https://doi.org/10.1016/0370-2693(93)90025-D

Vancouver

ALEPH Collaboration. Observation of the time dependence of B(d)0 - anti-B(d)0 mixing. Physics Letters B. 1993;313(3-4):498-508. doi: 10.1016/0370-2693(93)90025-D

Author

ALEPH Collaboration. / Observation of the time dependence of B(d)0 - anti-B(d)0 mixing. In: Physics Letters B. 1993 ; Vol. 313, No. 3-4. pp. 498-508.

Bibtex

@article{1bbc28b1dd824189aaae72b6f6d58f14,
title = "Observation of the time dependence of B(d)0 - anti-B(d)0 mixing",
abstract = "The time dependence of oscillations has been observed using events with a d∗, decaying into a D0π+, and a lepton in opposite hemispheres. The time dependence of the oscillations is derived from the displacement of the D0 vertex and the D∗-lepton charge correlation. From a fit for the oscillation frequency the mass difference of the B0d states is measured: Δm = [3.44+0.65−0.70(stat.)+0.26−0.20(syst.)] × 10−4 eV/c2.",
author = "D. Buskulic and Alexander Finch and {ALEPH Collaboration}",
year = "1993",
doi = "10.1016/0370-2693(93)90025-D",
language = "English",
volume = "313",
pages = "498--508",
journal = "Physics Letters B",
issn = "0370-2693",
publisher = "ELSEVIER SCIENCE BV",
number = "3-4",

}

RIS

TY - JOUR

T1 - Observation of the time dependence of B(d)0 - anti-B(d)0 mixing

AU - Buskulic, D.

AU - Finch, Alexander

AU - ALEPH Collaboration

PY - 1993

Y1 - 1993

N2 - The time dependence of oscillations has been observed using events with a d∗, decaying into a D0π+, and a lepton in opposite hemispheres. The time dependence of the oscillations is derived from the displacement of the D0 vertex and the D∗-lepton charge correlation. From a fit for the oscillation frequency the mass difference of the B0d states is measured: Δm = [3.44+0.65−0.70(stat.)+0.26−0.20(syst.)] × 10−4 eV/c2.

AB - The time dependence of oscillations has been observed using events with a d∗, decaying into a D0π+, and a lepton in opposite hemispheres. The time dependence of the oscillations is derived from the displacement of the D0 vertex and the D∗-lepton charge correlation. From a fit for the oscillation frequency the mass difference of the B0d states is measured: Δm = [3.44+0.65−0.70(stat.)+0.26−0.20(syst.)] × 10−4 eV/c2.

U2 - 10.1016/0370-2693(93)90025-D

DO - 10.1016/0370-2693(93)90025-D

M3 - Journal article

VL - 313

SP - 498

EP - 508

JO - Physics Letters B

JF - Physics Letters B

SN - 0370-2693

IS - 3-4

ER -