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Measurement of the Diphoton Differential Cross Section in P Anti-p Collisions at {u221A}s

Measurement of the Diphoton Differential Cross Section in P Anti-p Collisions at {u221A}s
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Total Pages: 97
Release: 2007
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The diphoton differential cross-section as a function of mass up to 300 GeV/c2, qT up to 100 GeV/c, and opening angle over a range of 0 to ? radians is measured. The measurement is performed using 1046.19 pb-1 of data collected at Fermi National Accelerator Laboratory using the D0 detector. This analysis considers all direct diphoton states but attempts to suppress contributions due to fragmentation.


Measurement of the Diphoton Differential Cross Section in P Anti-p Collisions at S**1/2

Measurement of the Diphoton Differential Cross Section in P Anti-p Collisions at S**1/2
Author:
Publisher:
Total Pages: 97
Release: 2007
Genre:
ISBN:

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The diphoton differential cross-section as a function of mass up to 300 GeV/c2, q{sub T} up to 100 GeV/c, and opening angle over a range of 0 to [pi] radians is measured. The measurement is performed using 1046.19 pb−1 of data collected at Fermi National Accelerator Laboratory using the D0 detector. This analysis considers all direct diphoton states but attempts to suppress contributions due to fragmentation.


Measurement of Particle Production and Inclusive Differential Cross Sections in P Anti-p Collisions at S**1/2

Measurement of Particle Production and Inclusive Differential Cross Sections in P Anti-p Collisions at S**1/2
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Total Pages: 21
Release: 2009
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ISBN:

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We report a set of measurements of particle production in inelastic p{bar p} collisions collected with a minimum-bias trigger at the Tevatron Collider with the CDF II experiment. The inclusive charged particle transverse momentum differential cross section is measured, with improved precision, over a range about ten times wider than in previous measurements. The former modeling of the spectrum appears to be incompatible with the high particle momenta observed. The dependence of the charged particle transverse momentum on the event particle multiplicity is analyzed to study the various components of hadron interactions. This is one of the observable variables most poorly reproduced by the available Monte Carlo generators. A first measurement of the event transverse energy sum differential cross section is also reported. A comparison with a PYTHIA prediction at the hadron level is performed. The inclusive charged particle differential production cross section is fairly well reproduced only in the transverse momentum range available from previous measurements. At higher momentum the agreement is poor. The transverse energy sum is poorly reproduced over the whole spectrum. The dependence of the charged particle transverse momentum on the particle multiplicity needs the introduction of more sophisticated particle production mechanisms, such as multiple parton interactions, in order to be better explained.


Measurement of the B Meson Differential Cross-section in P[bar P] Collisions At[radical]

Measurement of the B Meson Differential Cross-section in P[bar P] Collisions At[radical]
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Release: 2001
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This paper presents a direct measurement of the differential[ital B][sup+] and[ital B][sup 0] cross sections, [ital d[sigma]/dp[sub T]] in[ital p][ital[anti p]] collisions at[radical]s= 1.8 TeV using a sample of 74[ital pb][sup -1] accumulated by the Collider Detector at Fermilab (CDF). The cross sections are measured in the central pseudorapidity region[vert-bar][eta][vert-bar][lt] 1 for[ital p[sub T]]([ital B])[gt] 6.0 GeV/c by fully reconstructing the[ital B] meson decays[ital B][sup+][r-arrow][ital J/[psi]K[sup+]] and[ital B][sup 0][r-arrow][ital J/[psi]K[sup*0]](892), where[ital J/[psi]][r-arrow][mu][sup+][mu][sup -] and[ital K][sup*0][r-arrow][ital K][sup+][pi][sup -]. The prediction of next-to- leading order QCD is consistent with the shape of the differential cross section but is low by a factor of 2.1[+-]0.2[+-]0.3. The integrated[ital B] meson cross section for[ital p[sub T]]([ital B])[gt] 6.0 GeV/c is determined to be[sigma]([ital B][sup -]= 3. 54[+-]0.22[+-]0.53[mu][ital b].


Measurement of the Double Differential Diject Mass Cross Section in P$\bar{p}$ Collisions at {u221A}(s)

Measurement of the Double Differential Diject Mass Cross Section in P$\bar{p}$ Collisions at {u221A}(s)
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Total Pages: 176
Release: 2009
Genre:
ISBN:

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This thesis presents the analysis of the double differential dijet mass cross section, measured at the D0 detector in Batavia, IL, using p$ar{p}$ collisions at a center of mass energy of √s = 1.96 TeV. The dijet mass was calculated using the two highest pT jets in the event, with approximately 0.7 fb-1 of data collected between 2004 and 2005. The analysis was presented in bins of dijet mass (MJJ) and rapidity (y), and extends the measurement farther in MJJ and y than any previous measurement. Corrections due to detector effects were calculated using a Monte Carlo simulation and applied to data. The errors on the measurement consist of statistical and systematic errors, of which the Jet Energy Scale was the largest. The final result was compared to next-to-leading order theory and good agreement was found. These results may be used in the determination of the proton parton distribution functions and to set limits on new physics.


Measurement of the Isolated Photon Cross Section in P Anti-p Collisions at S**ư

Measurement of the Isolated Photon Cross Section in P Anti-p Collisions at S**ư
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Total Pages: 7
Release: 2005
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ISBN:

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The cross section for the inclusive production of isolated photons has been measured in p anti-p collisions at √s = 1.96 TeV with the D0 detector at the Fermilab Tevatron Collider. The photons span transverse momenta 23 to 300 GeV and have pseudorapidity ?


Measurement of the Cross Section for Production of Prompt Diphoton in Proton Anti-proton Collisions at {u221A}s

Measurement of the Cross Section for Production of Prompt Diphoton in Proton Anti-proton Collisions at {u221A}s
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Total Pages: 147
Release: 2004
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This thesis presents the measurement of prompt diphoton production rate in proton-antiproton collisions at a center-of-mass energy of 1.96 TeV using the upgraded Collider Detector at Fermilab (CDF II). This process deserves some attention for the following reasons. The H → ?? decay mode is an important channel for the Standard Model (SM) Higgs boson searches in the low mass region (MH 130 GeV) at the forth coming LHC. In many models involving physics beyond the SM, cascade decays of heavy new particles generate a ?? signature. Some examples are supersymmetry with a light gravitino, radiative decays to a higgsino-LSP and models with large symmetry groups. The QCD production of prompt photon pairs with large invariant mass is the irreducible background to these searches. The rate is huge and requires to be quantitatively evaluated prior to any of the possible discoveries. In a hadronic collider environment such as LHC, prompt photon signals are contaminated by the production of neutral mesons which decay to multiple collinear photons. The experience of classifying background of neutral meson is very important. The process can be used to test the Next-to-Leading Order (NLO) calculation of Quantum Chromodynamics (QCD). The 4-momentum of particles in the di-photon final state can be precisely determined due to the fine energy resolution of the electromagnetic calorimeters. The imbalance in the transverse momentum of the two photons reflects the transverse motion of the colliding partons. At collider energies, most of the transverse momentum of the incoming partons can be attributed to multiple soft gluon emissions prior to the collision, of which the effect to di-photon production can be resummed by Collins-Soper-Sterman (CSS) formalism. The Tevatron data can be used to test the resummation formalisms. They have used 207 pbsup-1