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First Measurement of the Left-right Z Cross Section Asymmetry in Polarized E[sup +]e[sup [minus] Collisions at the SLC.

First Measurement of the Left-right Z Cross Section Asymmetry in Polarized E[sup +]e[sup [minus] Collisions at the SLC. PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages : 7

Book Description
The SLAC Linear Collider (SLC) has recently been upgraded to produce, accelerate, and collide a spin polarized electron beam. The average beam polarization during the 1992 run was (22.4 [plus minus] 0.7)%. The SLD Collaboration used the polarized beam to perform the first measurement of the left-right cross section asymmetry (A[sub LR]) for Z boson production by e[sup +]e[sup [minus]] collisions. The measurement was performed at a center-of-mass energy of 91.55 GeV with a sample of 10,224 Z decays. The measured value of A[sub LR] is 0.100 [plus minus] 0.044(stat.) [plus minus] O.004(syst.) which determines the effective weak mixing angle to be sin[sup 2][theta][sub W][sup eff] = 0.2378 [plus minus] 0.0056(stat.) [plus minus] 0.0005(syst.).

First Measurement of the Left-right Z Cross Section Asymmetry in Polarized E[sup +]e[sup [minus] Collisions at the SLC.

First Measurement of the Left-right Z Cross Section Asymmetry in Polarized E[sup +]e[sup [minus] Collisions at the SLC. PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages : 7

Book Description
The SLAC Linear Collider (SLC) has recently been upgraded to produce, accelerate, and collide a spin polarized electron beam. The average beam polarization during the 1992 run was (22.4 [plus minus] 0.7)%. The SLD Collaboration used the polarized beam to perform the first measurement of the left-right cross section asymmetry (A[sub LR]) for Z boson production by e[sup +]e[sup [minus]] collisions. The measurement was performed at a center-of-mass energy of 91.55 GeV with a sample of 10,224 Z decays. The measured value of A[sub LR] is 0.100 [plus minus] 0.044(stat.) [plus minus] O.004(syst.) which determines the effective weak mixing angle to be sin[sup 2][theta][sub W][sup eff] = 0.2378 [plus minus] 0.0056(stat.) [plus minus] 0.0005(syst.).

First Measurement of the Left-right Z Cross Section Asymmetry in Polarized Ee− Collisions at the SLC.

First Measurement of the Left-right Z Cross Section Asymmetry in Polarized Ee− Collisions at the SLC. PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages : 7

Book Description
The SLAC Linear Collider (SLC) has recently been upgraded to produce, accelerate, and collide a spin polarized electron beam. The average beam polarization during the 1992 run was (22.4 ± 0.7)%. The SLD Collaboration used the polarized beam to perform the first measurement of the left-right cross section asymmetry (A{sub LR}) for Z boson production by ee− collisions. The measurement was performed at a center-of-mass energy of 91.55 GeV with a sample of 10,224 Z decays. The measured value of A{sub LR} is 0.100 ± 0.044(stat.) ± O.004(syst.) which determines the effective weak mixing angle to be sin2?{sub W}{sup eff} = 0.2378 ± 0.0056(stat.) ± 0.0005(syst.).

A Measurement of the Left-right Cross Section Asymmetry in Z[sup 0] Production with Polarized E[sup +]e[sup [minus] Collisions

A Measurement of the Left-right Cross Section Asymmetry in Z[sup 0] Production with Polarized E[sup +]e[sup [minus] Collisions PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

Book Description
The Stanford Linear Collider at SLAC is an e[sup +]e[sup [minus]] collider running at [radical]s [approx] M[sub Z] and has provided an electron beam with longitudinal polarization at the SLC interaction point. The 1992 polarized run data were taken with the SLD detector. The author presents here the measurement of the left-right cross section asymmetry (A[sub LR]) for the 1992 run. The polarized run began in May and ended in September of 1992 at a mean center-of-mass energy of 91.56 GeV. Tower hit information of the liquid argon calorimeter and endcap warm iron calorimeter pads were used for selecting hadronic Z[sup 0] or tau pair events. The SLD detector collected about 11,000 events during this run. The magnitude of the longitudinal polarization of the electron beam was continuously measured by a polarimeter based on Compton scattering, and was monitored by a polarimeter based on Moller scattering. The luminosity-weighted average longitudinal polarization during the 1992 run was measured as 22.4 [+-] 0.6 (syst.)%. From these data, the value of A[sub LR] has been measured to be 0.102 [+-] 0.044 (stat.) [+-] 0.003 (syst.), corresponding to an effective electroweak mixing angle (sin[sup 2][theta][sub w][sup eff]) of 0.2375 [+-] 0.0056 (stat.) [+-] 0.0004 (syst.). The error is dominated by the statistical error. This value of sin[sup 2][theta][sub w][sup eff] is in good agreement with existing measurements from other experiments. Studies of improvements in A[sub LR] event selection for future high-statistics runs are also discussed.

Precise Measurement of the Left-right Cross Section Asymmetry in Z Boson Production by Esup +esup Minus Collisions

Precise Measurement of the Left-right Cross Section Asymmetry in Z Boson Production by Esup +esup Minus Collisions PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

Book Description


A Measurement of the Left-right Cross Section Asymmetry in Z° Production with Polarized Ee− Collisions

A Measurement of the Left-right Cross Section Asymmetry in Z° Production with Polarized Ee− Collisions PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages : 153

Book Description
The Stanford Linear Collider at SLAC is an ee− collider running at √s ≈ M{sub Z} and has provided an electron beam with longitudinal polarization at the SLC interaction point. The 1992 polarized run data were taken with the SLD detector. The author presents here the measurement of the left-right cross section asymmetry (A{sub LR}) for the 1992 run. The polarized run began in May and ended in September of 1992 at a mean center-of-mass energy of 91.56 GeV. Tower hit information of the liquid argon calorimeter and endcap warm iron calorimeter pads were used for selecting hadronic Z° or tau pair events. The SLD detector collected about 11,000 events during this run. The magnitude of the longitudinal polarization of the electron beam was continuously measured by a polarimeter based on Compton scattering, and was monitored by a polarimeter based on Moller scattering. The luminosity-weighted average longitudinal polarization during the 1992 run was measured as 22.4 ± 0.6 (syst.)%. From these data, the value of A{sub LR} has been measured to be 0.102 ± 0.044 (stat.) ± 0.003 (syst.), corresponding to an effective electroweak mixing angle (sin2?{sub w}{sup eff}) of 0.2375 ± 0.0056 (stat.) ± 0.0004 (syst.). The error is dominated by the statistical error. This value of sin2?{sub w}{sup eff} is in good agreement with existing measurements from other experiments. Studies of improvements in A{sub LR} event selection for future high-statistics runs are also discussed.

Measuring the Left-right Cross Section Asymmetry in Z Boson Production by Esup +esup Minus Collisions at the SLC.

Measuring the Left-right Cross Section Asymmetry in Z Boson Production by Esup +esup Minus Collisions at the SLC. PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

Book Description


First Measurement of the Left-right Cross Section Asymmetry in Z Boson Production at E{sub Cm}

First Measurement of the Left-right Cross Section Asymmetry in Z Boson Production at E{sub Cm} PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages : 8

Book Description
The left-right cross section asymmetry for Z boson production in e[sup +]e[sup -] annihilation (A[sub LR]) has been measured at E[sub cm] = 91.55 GeV with the SLD detector at the SLAC Linear Collider (SLC) using a longitudinally polarized electron beam. The electron polarization was continually monitored with a Compton scattering polarimeter, and was typically 22%. We have accumulated a sample of [approximately]10,200 Z events. We find that A[sup LR] = 0.100 [plus minus] 0.044 [plus minus] 0.003 where the first error is statistical and the second is systematic. From this measurement, we determine the weak mixing angle defined at the Z boson pole to be sin[sup 2][theta](lept/w) = 0.2378 [plus minus] 0.0056.

The First Measurement of the Left-Right Cross Section Asymmetry in Z Boson Production

The First Measurement of the Left-Right Cross Section Asymmetry in Z Boson Production PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

Book Description
The first measurement of the left-right cross section asymmetry (A[sub LR]) in Z[sup 0] boson production has been made with the SLAC Large Detector (SLD) at the SLAC Linear Collider (SLC). The measurement was performed at a center-of-mass energy (E[sub cm]) of 91.55 GeV with a longitudinally polarized electron beam. The average beam polarization was (22.4 [+-] 0.6)%. Using a sample of 10,224 Z[sup 0] decays, A[sub LR] is measured to be 0.102 [+-] 0.O44(stat) [+-] 0.003(syst), which determines the effective electroweak mixing angle to be sin[sup 2] [theta][sub W][sup eff] = 0.2375 [+-] 0.0056(stat) [+-] 0.0004(syst).

A Measurement of the Left-right Cross Section Asymmetry in Z P̊roduction with Polarized E+e- Collisions

A Measurement of the Left-right Cross Section Asymmetry in Z P̊roduction with Polarized E+e- Collisions PDF Author: Hwanbae Park
Publisher:
ISBN:
Category : Electron beams
Languages : en
Pages : 306

Book Description


Precise Measurement of the Left-right Cross Section Asymmetry in Z Boson Production by E[sup+]e[sup[minus] Collisions

Precise Measurement of the Left-right Cross Section Asymmetry in Z Boson Production by E[sup+]e[sup[minus] Collisions PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

Book Description
The authors present a precise measurement of the left-right cross section asymmetry (A[sub LR]) for Z boson production by e[sup+]e[sup[minus]] collisions. The measurement was performed at a center-of-mass energy of 91.26 GeV with the SLD detector at the SLAC Linear Collider (SLC). The luminosity-weighted average polarization of the SLC electron beam was (63.0[+-] 1.1)%. Using a sample of 49,392 Z decays, they measure A[sub LR] to be 0.1628[+-] 0.0071 (stat.)[+-] 0.0028(syst.) which determines the effective weak mixing angle to be sin[sup 2][theta][sub W][sup eff]= 0.2292[+-] 0.0009(stat.)[+-] 0.0004(syst.). They combine this result with the result obtained in 1992 and obtain sin[sup 2][theta][sub W][sup eff]= 0.2294[+-] 0.0010, which constitutes the best measurement of sin[sup 2][theta][sub W][sup eff] in a single experiment presently available.