Cross Section Measurement of the Process [gamma Gamma->p Pbar] in Untagged Events at [sqrt](s)


Book Description

Le collisioneur LEP au CERN est utilisé pour étudier les collisions de deux photons quasi-réels e+e−->e+e−[gamma gamma]->e+e−X. L'échantillon de données pour la réaction e+e−->e+e−[gamma gamma]->e+e− [p pbar] a été collecté par le détecteur OPAL à une énergie dans le centre de masse de [sqrt](s)=183 et 189 GeV. Le processus [gamma gamma]->[p pbar] permet de tester les prédictions fournies par QED et QCD. Les mesures de section efficace obtenues par OPAL couvrent une région du centre de masse de deux photons, "W", entre 2.15 GeV"W"3.95 GeV et l'angle polaire dans le centre de masse du système [gamma gamma]-[p pbar] est restreint à I(cos theta*)I













A Measurement of the Differential Cross Section for the Reaction $\gamma N \to \pi^{-} P$ from Deuterium


Book Description

We report a measurement of the differential cross section for the $\gamma n \to \pi^- p$ process from the CLAS detector at Jefferson Lab in Hall B for photon energies between 1.0 and 3.5 GeV and pion center-of-mass (c.m.) angles ($\theta_{c.m.}$) between 50$^\circ$ and 115$^\circ$. We confirm a previous indication of a broad enhancement around a c.m. energy ($\sqrt{s}$) of 2.2 GeV at $\theta_{c.m.}=90^\circ$ in the scaled differential cross section, $s^7 {\frac{d\sigma}{dt}}$. Our data show the angular dependence of this enhancement as the scaling region is approached in the kinematic region from 70$^\circ$ to 105$^\circ$.










Evidence for $t\bar{t}\gamma$ Production and Measurement of $\sigma_t\bar{t}\gamma


Book Description

Using data corresponding to 6.0 fb−1 of p{bar p} collisions at √s = 1.96 TeV collected by the CDF II detector, we present a cross section measurement of top-quark pair production with an additional radiated photon, t{bar t}[gamma]. The events are selected by looking for a lepton (l), a photon ([gamma]), significant transverse momentum imbalance (E{sub T}), large total transverse energy, and three or more jets, with at least one identified as containing a b quark (b). The t{bar t}[gamma] sample requires the photon to have 10 GeV or more of transverse energy, and to be in the central region. Using an event selection optimized for the t{bar t}[gamma] candidate sample we measure the production cross section of t{bar t} ([sigma]{sub t{bar t}}), and the ratio of cross sections of the two samples. Control samples in the dilepton+photon and lepton+photon+E{sub T}, channels are constructed to aid in decay product identification and background measurements. We observe 30 t{bar t}[gamma] candidate events compared to the standard model expectation of 26.9 ± 3.4 events. We measure the t{bar t}[gamma] cross section ([sigma]{sub t{bar t}}) to be 0.18 ± 0.08 pb, and the ratio of [sigma]{sub t{bar t}[gamma]} to [sigma]{sub t{bar t}} to be 0.024 ± 0.009. Assuming no t{bar t}[gamma] production, we observe a probability of 0.0015 of the background events alone producing 30 events or more, corresponding to 3.0 standard deviations.




Measurement of The[gamma] Cross Section at D0 Using Dimuons


Book Description

The D0 experiment has measured the[gamma] differential cross section in p[bar p] collisions at[radical]s= 1.8 TeV for[vert-bar]y[sup[gamma]][vert-bar]0.7. We find the measured cross section to be a factor of five larger than the O([alpha][sub s][sup 3]) QCD prediction for p[sub T][sup[gamma]] 5 GeV/c.




Measurement of the Z Gamma ---] Nu Anti-nu Gamma Cross Section and Limits on Anomalous Z Z Gamma and Z Gamma Gamma Couplings in P Anti-p Collisions at S**1/2


Book Description

We present the first observation of the Z[gamma] →[nu]{bar [nu]}[gamma] process at the Tevatron at 5.1 standard deviations significance, based on 3.6 fb−1 of integrated luminosity collected with the D0 detector at the Fermilab Tevatron p{bar p} Collider at √s = 1.96 TeV. The measured Z[gamma] cross section multiplied by the branching fraction of Z → {nu}{bar {nu}} is 32 ± 9(stat. + syst.) ± 2(lumi.) fb for the photon E{sub T} > 90 GeV. It is in agreement with the standard model prediction of 39 ± 4 fb. We set the most restrictive limits on anomalous trilinear Z[gamma][gamma] and ZZ[gamma] gauge boson couplings at a hadron collider to date, with three constraints being the world's strongest.