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Improved D0 W Boson Mass Determination

Improved D0 W Boson Mass Determination
Author:
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Total Pages:
Release: 2001
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ISBN:

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We present a measurement of the W boson mass in proton-antiproton collisions at[radical]s= 1.8 TeV based on a data sample of 82 pb[sup -1] integrated luminosity collected by the D0 detector at the Fermilab Tevatron. We utilize e[nu] events in which the electron shower is close to the phi edge of one of the 32 modules in the D0 central calorimeter. The electromagnetic calorimenter response and resolution in this region differs from that in the rest of the module and electrons in this region were not previously utilized. We determine the calorimeter response and resolution in this region using Z[yields] ee events. We extract the W boson mass by fitting to the transverse mass and to the electron and neutrino transverse momentum distributions. The result is combined with previous D0 results to obtain an improved measurement of the W boson mass: m[sub W]= 80.483[+-] 0.084 GeV.


Measurements of the $W$ Boson Mass with the D0 Detector

Measurements of the $W$ Boson Mass with the D0 Detector
Author:
Publisher:
Total Pages: 254
Release: 2013
Genre:
ISBN:

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In the first part, we describe what is the W boson mass in the context of the Standard Model. We discuss the prominent role this physical observable plays in the determination of the internal self consistency of the Electroweak Sector. We review measurements and calculation of the W boson mass done in past and argue about the importance and feasibility of improving the experimental determination. We give a description of the Fermilab Tevatron Collider and the D0 detector, highlighting the relevant parts for the measurement described in this Dissertation. In the second part, we give a detailed description of a measurement of the W boson mass using the D0 Central Calorimeter. The measurement uses 1.68 x 106 candidates from W → en decays, corresponding to 4.3 fb-1 of integrated luminosity collected from 2006 to 2009. We measure the mass using the transverse mass, electron transverse momentum, and missing transverse energy distributions. The transverse mass and electron transverse momentum measurements are the most precise and are combined to give MW = 80.367 ± 0.013(stat) ± 0.023 (syst) GeV = 80.367 ± 0.026 GeV. This is combined with an earlier D0 result determined using an independent 1 fb-1 data sample, also with central electrons only, to give MW = 80.375± 0.023 GeV. The uncertainty in the measurement is dominated by the determination of the calorimeter electron energy scale, the W sample size, the knowledge of the parton distribution function. In the third part, we discuss methods of reducing the dominant uncertainties in the W boson mass measurements. We show that introducing electrons detected in the End Calorimeters greatly reduce the measurement systematic uncertainty, especially the on related to the parton distribution functions. We describe a precise calibration of the End Calorimeter using Z → ee events corresponding to 4.3 fb-1 of integrated luminosity. The calibration is an important milestone in a measurement that explores a larger part of the D0 Calorimeter. We present parametrized models that describe the response of the End Calorimeters to electron showers and soft hadronic particles, giving special attention to the specific challenges of a measurement in the forward region: the inhomogeneity of the uninstrumented materials, the large hadronic energy flow in the calorimeter and the jet misidentification probability.


A Precision Measurement of the W Boson Mass at

A Precision Measurement of the W Boson Mass at
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Publisher:
Total Pages: 9
Release: 2009
Genre:
ISBN:

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I present the first measurement of the W boson mass in the electron decay channel using the Run II D0 detector at the Fermilab Tevatron Collider. The data used was collected from 2002 to 2006 and the integrated luminosity is 1 fb−1. The W boson mass was determined from the likelihood fit to the measured data distribution. The mass value is found to be 80.401 ± 0.023(stat) ± 0.037(syst) GeV = 80.401 ± 0.044 GeV using the transverse mass spectrum, which is the most precise measurement from one single experiment to date. This result puts tighter constraints on the mass of the standard model Higgs boson. I also present three other measurements that can help to reduce the theoretical uncertainties for the future W mass measurements.


Measurement of the $W$ Boson Mass with the D0 Detector

Measurement of the $W$ Boson Mass with the D0 Detector
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Total Pages:
Release: 2014
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ISBN:

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We give a detailed description of the measurement of the $W$ boson mass, $M_W$, performed on an integrated luminosity of 4.3 fb$^{-1}$, which is based on similar techniques as used for our previous measurement done on an independent data set of 1 fb$^{-1}$ of data. The data were collected using the D0 detector at the Fermilab Tevatron Collider. This data set yields $1.68\times 10^6$ $W\rightarrow e\nu$ candidate events. We measure the mass using the transverse mass, electron transverse momentum, and missing transverse energy distributions. The $M_W$ measurements using the transverse mass and the electron transverse momentum distributions are the most precise of these three and are combined to give $M_W$ = 80.367 $\pm$ 0.013 (stat) $\pm$ 0.022 (syst) GeV = 80.367 $\pm$ 0.026 GeV. When combined with our earlier measurement on 1 fb$^{-1}$ of data, we obtain $M_W$ = 80.375 $\pm$ 0.023 GeV.


The Measurement of the W Boson Mass from CDF.

The Measurement of the W Boson Mass from CDF.
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Publisher:
Total Pages: 12
Release: 1994
Genre:
ISBN:

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Recent results from LEP experiments have substantially improved the knowledge of the Z boson. However, hadron colliders remain the only source of direct measurements of the W boson. There have been measurements of the W boson mass from the UA2 and CDF collaborations. The W mass continues to be a subject of great interest in testing the Standard Model. Here, the authors have made a preliminary determination of the W boson mass M{sub W} = 80.38 ± 0.23 GeV/c2 from a combined analysis of W → e[nu] and W → [mu][nu] in {anti p}p collisions at √s = 1.8 TeV. The electron data alone yields M{sub W} = 80.47 ± 0.15(stat.) ± 0.25(syst.) GeV/c2, while the muon data gives M{sub W} = 80.29 ± 0.20(stat.) ± 0.24(syst.) GeV/c2.


A New Measurement of the W Boson Mass at D-Zero

A New Measurement of the W Boson Mass at D-Zero
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Total Pages:
Release: 2000
Genre:
ISBN:

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We present a new measurement of the W mass using the W [yields] e[nu] data from the D0 forward detectors at the Fermilab Tevatron p[anti p] Collider. This is the first measurement of the W mass with electron candidates in the range 1.5


Measuring the Mass of the W Boson with the Last 3.7 Fb−1 of Tevatron Data

Measuring the Mass of the W Boson with the Last 3.7 Fb−1 of Tevatron Data
Author: Michelle Brochmann
Publisher:
Total Pages: 204
Release: 2017
Genre:
ISBN:

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This thesis presents the results of an analysis of the 3.7 {fb}^{-1} of Tevatron proton-antiproton data collected with the DZero (D0) Detector at Fermilab during the ``RunIIb34'' period, with the goal of extracting an improved measurement of the $W$ boson mass, which is currently measured to a precision of approx 20,{MeV}. The measurement is performed on events with one W boson which decays to an electron and a neutrino. Using a template technique, the mass is measured from three distributions that are correlated with the W boson mass: the transverse electron momentum, p_T^e, the transverse W mass, m_T$ and the neutrino momentum, which appears as missing transverse energy, {E}_T. A test measurement using this technique is successfully performed on a mock dataset generated with a Monte Carlo simulation. In the data, we find unexpected azimuthally dependent inconsistencies between the early and late parts of the data taking period. Implications for the completion of the data measurement are discussed.


W Boson Mass Measurement at CDF.

W Boson Mass Measurement at CDF.
Author:
Publisher:
Total Pages: 10
Release: 2017
Genre:
ISBN:

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This is the closeout report for the grant for experimental research at the energy frontier in high energy physics. The report describes the precise measurement of the W boson mass at the CDF experiment at Fermilab, with an uncertainty of ≈ 12 MeV, using the full dataset of ≈ 9 fb-1 collected by the experiment up to the shutdown of the Tevatron in 2011. In this analysis, the statistical and most of the experimental systematic uncertainties have been reduced by a factor of two compared to the previous measurement with 2.2 fb-1 of CDF data. This research has been the culmination of the PI's track record of producing world-leading measurements of the W boson mass from the Tevatron. The PI performed the first and only measurement to date of the W boson mass using high-rapidity leptons using the D0 endcap calorimeters in Run 1. He has led this measurement in Run 2 at CDF, publishing two world-leading measurements in 2007 and 2012 with total uncertainties of 48 MeV and 19 MeV respectively. The analysis of the final dataset is currently under internal review in CDF. Upon approval of the internal review, the result will be available for public release.