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Measurement of |Vub| using b hadron semileptonic decay

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Measurement of |Vub| using b hadron semileptonic decay. / OPAL Collaboration.
In: European Physical Journal C: Particles and Fields, Vol. 21, No. 3, 07.2001, p. 399-410.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

OPAL Collaboration 2001, 'Measurement of |Vub| using b hadron semileptonic decay', European Physical Journal C: Particles and Fields, vol. 21, no. 3, pp. 399-410. https://doi.org/10.1007/s100520100764

APA

OPAL Collaboration (2001). Measurement of |Vub| using b hadron semileptonic decay. European Physical Journal C: Particles and Fields, 21(3), 399-410. https://doi.org/10.1007/s100520100764

Vancouver

OPAL Collaboration. Measurement of |Vub| using b hadron semileptonic decay. European Physical Journal C: Particles and Fields. 2001 Jul;21(3):399-410. doi: 10.1007/s100520100764

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OPAL Collaboration. / Measurement of |Vub| using b hadron semileptonic decay. In: European Physical Journal C: Particles and Fields. 2001 ; Vol. 21, No. 3. pp. 399-410.

Bibtex

@article{4833b41e0a8642f290054b4498fae015,
title = "Measurement of |Vub| using b hadron semileptonic decay",
abstract = "The magnitude of the CKM matrix element |Vub| is determined by measuring the inclusive charmless semileptonic branching fraction of beauty hadrons at OPAL based on b→Xuℓν event topology and kinematics. This analysis uses OPAL data collected between 1991 and 1995, which correspond to about four million hadronic Z decays. We measure Br( b→Xuℓν) to be (1.63±0.53+0.55−0.62)×10−3. The first uncertainty is the statistical error and the second is the systematic error. From this analysis, |Vub| is determined to be:|Vub| = (4.00 ± 0.65(stat)+0.67−0.76(sys) ± 0.19(HQE)) × 10−3.The last error represents the theoretical uncertainties related to the extraction of |Vub| from Br( b→Xuℓν) using the Heavy Quark Expansion.",
author = "Bailey, {Ian Richard} and Vakhtang Kartvelishvili and {OPAL Collaboration}",
year = "2001",
month = jul,
doi = "10.1007/s100520100764",
language = "English",
volume = "21",
pages = "399--410",
journal = "European Physical Journal C: Particles and Fields",
issn = "1434-6044",
publisher = "SPRINGER",
number = "3",

}

RIS

TY - JOUR

T1 - Measurement of |Vub| using b hadron semileptonic decay

AU - Bailey, Ian Richard

AU - Kartvelishvili, Vakhtang

AU - OPAL Collaboration

PY - 2001/7

Y1 - 2001/7

N2 - The magnitude of the CKM matrix element |Vub| is determined by measuring the inclusive charmless semileptonic branching fraction of beauty hadrons at OPAL based on b→Xuℓν event topology and kinematics. This analysis uses OPAL data collected between 1991 and 1995, which correspond to about four million hadronic Z decays. We measure Br( b→Xuℓν) to be (1.63±0.53+0.55−0.62)×10−3. The first uncertainty is the statistical error and the second is the systematic error. From this analysis, |Vub| is determined to be:|Vub| = (4.00 ± 0.65(stat)+0.67−0.76(sys) ± 0.19(HQE)) × 10−3.The last error represents the theoretical uncertainties related to the extraction of |Vub| from Br( b→Xuℓν) using the Heavy Quark Expansion.

AB - The magnitude of the CKM matrix element |Vub| is determined by measuring the inclusive charmless semileptonic branching fraction of beauty hadrons at OPAL based on b→Xuℓν event topology and kinematics. This analysis uses OPAL data collected between 1991 and 1995, which correspond to about four million hadronic Z decays. We measure Br( b→Xuℓν) to be (1.63±0.53+0.55−0.62)×10−3. The first uncertainty is the statistical error and the second is the systematic error. From this analysis, |Vub| is determined to be:|Vub| = (4.00 ± 0.65(stat)+0.67−0.76(sys) ± 0.19(HQE)) × 10−3.The last error represents the theoretical uncertainties related to the extraction of |Vub| from Br( b→Xuℓν) using the Heavy Quark Expansion.

U2 - 10.1007/s100520100764

DO - 10.1007/s100520100764

M3 - Journal article

VL - 21

SP - 399

EP - 410

JO - European Physical Journal C: Particles and Fields

JF - European Physical Journal C: Particles and Fields

SN - 1434-6044

IS - 3

ER -