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Title: A measurement of the Z 0 hadronic branching fraction to bottom quarks and the charged multiplicity of bottom quark events using precision vertex detectors at E cm = 91 GeV

Abstract

Using the precision vertex detectors of the Mark 2 at the SLC, an impact parameter tag was developed to select a sample of hadronic Z° decays enriched in its fraction of bottom quark events. The nominal tagging method requires that there be at least three tracks whose impact parameters are inconsistent with the track having originated at the electron-position interaction point. A tagging efficiency for b$$\bar{b}$$ events of 50% with a enriched sample purity of 85% was achieved. This impact parameter tag was used to measure the fraction hadronic Z° decays which produce b$$\bar{b}$$ events, F b. It is found that F b = 0.232$$+0.053\atop{-0.045}$$ (stat) $$+0.025\atop{-0.021}$$ (syst). This result is consistent with those found using other tagging methods as well as the Standard Model prediction of 0.217. The b b-enriched event sample was also used to measure the difference between the average charged multiplicity of b$$\bar{b}$$ events and that of all hadronic Z° decays, δ$$\bar{n}$$ b = 2.11 ± 1.82(stat) ± 0.57(syst). Using previous measurements of the total hadronic charged multiplicity, the corresponding total multiplicity for b$$\bar{b}$$ events is $$\bar{n}$$ b=23.05 ± 1.82 (stat) ± 0.60 (syst). Subtracting the contribution to the multiplicity from B hadron decays yields the multiplicity of the b$$\bar{b}$$ non-leading system, $$\bar{n}$$$\bar{nl}$$ = 12.04 ± 1.82 (stat) ± 0.63(syst). Comparing this non-leading multiplicity to the total hadronic multiplicity data at lower energy supports the hypothesis that the non-leading particle production is independent of the flavor of the initial quarks.

Authors:
 [1]
  1. Stanford Univ., CA (United States)
Publication Date:
Research Org.:
Stanford Linear Accelerator Center, Menlo Park, CA (United States)
Sponsoring Org.:
USDOE
OSTI Identifier:
10164831
Report Number(s):
SLAC-396
ON: DE92018236
DOE Contract Number:
AC03-76SF00515
Resource Type:
Thesis/Dissertation
Resource Relation:
Other Information: TH: Thesis (Ph.D.); PBD: Jun 1992
Country of Publication:
United States
Language:
English
Subject:
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS; Z NEUTRAL BOSONS; HADRONIC PARTICLE DECAY; BRANCHING RATIO; BEAUTY PARTICLES; MULTIPLICITY; EXPERIMENTAL DATA; STANFORD LINEAR COLLIDER DETECTOR; STANDARD MODEL; MONTE CARLO METHOD; PERFORMANCE; QUARKS; 662380; DECAYS OF INTERMEDIATE BOSONS

Citation Formats

Koetke, Dale Steven. A measurement of the Z0 hadronic branching fraction to bottom quarks and the charged multiplicity of bottom quark events using precision vertex detectors at Ecm = 91 GeV. United States: N. p., 1992. Web. doi:10.2172/10164831.
Koetke, Dale Steven. A measurement of the Z0 hadronic branching fraction to bottom quarks and the charged multiplicity of bottom quark events using precision vertex detectors at Ecm = 91 GeV. United States. doi:10.2172/10164831.
Koetke, Dale Steven. Mon . "A measurement of the Z0 hadronic branching fraction to bottom quarks and the charged multiplicity of bottom quark events using precision vertex detectors at Ecm = 91 GeV". United States. doi:10.2172/10164831. https://www.osti.gov/servlets/purl/10164831.
@article{osti_10164831,
title = {A measurement of the Z0 hadronic branching fraction to bottom quarks and the charged multiplicity of bottom quark events using precision vertex detectors at Ecm = 91 GeV},
author = {Koetke, Dale Steven},
abstractNote = {Using the precision vertex detectors of the Mark 2 at the SLC, an impact parameter tag was developed to select a sample of hadronic Z° decays enriched in its fraction of bottom quark events. The nominal tagging method requires that there be at least three tracks whose impact parameters are inconsistent with the track having originated at the electron-position interaction point. A tagging efficiency for b$\bar{b}$ events of 50% with a enriched sample purity of 85% was achieved. This impact parameter tag was used to measure the fraction hadronic Z° decays which produce b$\bar{b}$ events, Fb. It is found that Fb = 0.232$+0.053\atop{-0.045}$ (stat) $+0.025\atop{-0.021}$ (syst). This result is consistent with those found using other tagging methods as well as the Standard Model prediction of 0.217. The bb-enriched event sample was also used to measure the difference between the average charged multiplicity of b$\bar{b}$ events and that of all hadronic Z° decays, δ$\bar{n}$b = 2.11 ± 1.82(stat) ± 0.57(syst). Using previous measurements of the total hadronic charged multiplicity, the corresponding total multiplicity for b$\bar{b}$ events is $\bar{n}$b=23.05 ± 1.82 (stat) ± 0.60 (syst). Subtracting the contribution to the multiplicity from B hadron decays yields the multiplicity of the b$\bar{b}$ non-leading system, $\bar{n}$$\bar{nl}$ = 12.04 ± 1.82 (stat) ± 0.63(syst). Comparing this non-leading multiplicity to the total hadronic multiplicity data at lower energy supports the hypothesis that the non-leading particle production is independent of the flavor of the initial quarks.},
doi = {10.2172/10164831},
journal = {},
number = ,
volume = ,
place = {United States},
year = {Mon Jun 01 00:00:00 EDT 1992},
month = {Mon Jun 01 00:00:00 EDT 1992}
}

Thesis/Dissertation:
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  • Using the precision vertex detectors of the Mark II at the SLC, an impact parameter tag was developed to select a sample of hadronic Z[sup 0] decays enriched in its fraction of bottom quark events. The nominal tagging method requires that there be at least three tracks whose impact parameters are inconsistent with the track having originated at the electron-position interaction point. A tagging efficiency for b[bar b] events of 50% with an enriched sample purity of 85% was achieved. This impact parameter tag was used to measure the fraction hadronic Z[sup 0] decays which produce b[bar b] events, F[submore » b]. It is found that F[sub b] = 0.232[sub [minus]0.045][sup +0.053](stat) [sub [minus]0.021][sup +0.025](syst). This result is consistent with those found using other tagging methods as well as the Standard Model prediction of 0.217. The b[bar b]-enriched event sample was also used to measure the difference between the average charged multiplicity of b[bar b] events and that of all hadronic Z[sup 0] decays, [delta][bar n][sub b] = 2.11 [+-] 1.82 (stat) [+-] 0.57 (syst). Using previous measurements of the total hadronic charged multiplicity, the corresponding total multiplicity for b[bar b] events in [bar n][sub b] = 23.05[+-]1.82 (stat) [+-] 0.60 (syst). Subtracting the contribution to the multiplicity from B hadron decays yields the multiplicity of the b[bar b] non-leading system, [bar n][sub nl] = 12.04 [+-] 1.82 (stat) [+-] 0.63 (syst). Comparing this non-leading multiplicity to the total hadronic multiplicity data at lower energy supports the hypothesis that the non-leading particle production is independent of the flavor of the initial quarks. This also yields a determination of the average energy fraction of bottom hadrons in Z[sup 0] decays of [l angle]x[sub E][r angle][sub b] = 0.619[sub [minus].107[sup +.096]] (stat) [sub [minus].045[sup +.043]] (syst).« less
  • Using the precision vertex detectors of the Mark 2 at the SLC, an impact parameter tag was developed to select a sample of hadronic Z{degree} decays enriched in its fraction of bottom quark events. The nominal tagging method requires that there be at least three tracks whose impact parameters are inconsistent with the track having originated at the electron-position interaction point. A tagging efficiency for b{bar b} events of 50% with a enriched sample purity of 85% was achieved. This impact parameter tag was used to measure the fraction hadronic Z{degree} decays which produce b{bar b} events, F{sub b}. Itmore » is found that F{sub b} = 0.232{sub {minus}0.045}{sup +0.053} (stat) {sub {minus}0.021}{sup +0.025} (syst). This result is consistent with those found using other tagging methods as well as the Standard Model prediction of 0.217. The b{bar b}-enriched event sample was also used to measure the difference between the average charged multiplicity of b{bar b} events and that of all hadronic Z{degree} decays, {delta}{bar n}{sub b} = 2.11 {plus minus} 1.82(stat) {plus minus} 0.57(syst). Using previous measurements of the total hadronic charged multiplicity, the corresponding total multiplicity for b{bar b} events is {bar n}{sub b}=23.05 {plus minus} 1.82 (stat) {plus minus} 0.60 (syst). Subtracting the contribution to the multiplicity from B hadron decays yields the multiplicity of the b{bar b} non-leading system, {bar n}{sub nl} = 12.04 {plus minus} 1.82 (stat) {plus minus} 0.63(syst). Comparing this non-leading multiplicity to the total hadronic multiplicity data at lower energy supports the hypothesis that the non-leading particle production is independent of the flavor of the initial quarks.« less
  • This thesis describes a measurement of the branching fraction Br (B 0 s → D s*D s*) made using a data sample collected from proton-antiproton collisions at a centre-of-mass energy of 1.96 TeV, corresponding to approximately 1.3 fb -1 of integrated luminosity collected in 2002--2006 by the D0 detector at the Fermilab Tevatron Collider. One D* s meson was partially reconstructed in the decay D s → Φμv, and the other D* s meson was identified using the decay D s → Φπ where no attempt was made to distinguish D s and D* s states. The resulting measurement is Br (B 0 s → D s*D s*) = 0.039 +0.019 -0.017(stat) +0.016 -0.015(syst). This was subsequently used to estimate the width difference ΔΓ CP s in the B 0 s-more » $$\bar{B}$$ 0 s system: ΔΓ CP ss = 0.079 +0.038 -0.035(stat) +0.031 -0.030(syst), and is currently one of the most precise estimates of this quantity and consistent with the Standard Model.« less
  • The authors measure the time-dependent CP asymmetry parameters in B 0 → K +K -K 0 based on a data sample of approximately 277 million B-meson pairs recorded at the Y(4S) resonance with the BABAR detector at the PEP-II B-meson Factory at SLAC. They reconstruct two-body B 0 decays to Φ(1020)Kmore » $$0\atop{S}$$ and Φ(1020)K$$0\atop{L}$$. Using a time-dependent maximum-likelihood fit, they measure sin2β eff(ΦK 0) = 0.48 ± 0.28 ± 0.10, and C(ΦK 0) = 0.16 ± 0.25 ± 0.09, where the first error is statistical, and the second is systematic. They also present measurements of the CP-violating asymmetries in the decay B 0 → f 0(→ {pi} +π -)K$$0\atop{S}$$. The results are obtained from a data sample of 209 x 10{sup 6} Y(4S) → B$$\bar{B}$$ decays, also collected with the BABAR detector at the PEP-II asymmetric-energy B Factory at SLAC. From a time-dependent maximum-likelihood fit they measure the mixing-induced CP violation parameter S(f 0(980)K$$0\atop{S}$$) = - sin 2β efff 0(980)K$$0\atop{S}$$ = -0.95$$+0.32\atop{-0.23}$$ ± 0.10 and the direct CP violation parameter C(f 0(980)K$$0\atop{S}$$) = - 0.24 ± 0.31 ± 0.15, where the first errors are statistical and the second systematic. Finally, they present a measurement of the branching fraction of the decay B 0 → f 0(→ π +π -)K$$0\atop{S}$$. From a time-dependent maximum likelihood fit to a data sample of 123 x 10 6 Y(4S) → B$$\bar{B}$$ decays they find 93.6 ± 13.6 ± 6.4 signal events corresponding to a branching fraction of β(B 0 → f 0(980)(→ π +π -)K 0) = (6.0 ± 0.9 ± 0.6 ± 1.2) x 10 -6, where the first error is statistical, the second systematic, and the third due to model uncertainties.« less