Study of double parton scattering using W+2-jet events in proton-proton collisions at √s=7 TeV

Peer reviewe

Jet and underlying event properties as a function of charged-particle multiplicity in proton-proton collisions at √s=7 TeV

This is the pre-print version of the final published paper that is available from the link belowCharacteristics of multi-particle production in proton-proton collisions at √s=7 TeV are studied as a function of the charged-particle multiplicity, N. The produced particles are separated into two classes: those belonging to jets and those belonging to the underlying event. Charged particles are measured with pseudorapidity |η|0.25 GeV/c. Jets are reconstructed from charged-particles only and required to have p>5 GeV/c. The distributions of jet p, average p of charged particles belonging to the underlying event or to jets, jet rates, and jet shapes are presented as functions of N and compared to the predictions of the pythia and herwig event generators. Predictions without multi-parton interactions fail completely to describe the N-dependence observed in the data. For increasing N, pythia systematically predicts higher jet rates and harder p spectra than seen in the data, whereas herwig shows the opposite trends. At the highest multiplicity, the data-model agreement is worse for most observables, indicating the need for further tuning and/or new model ingredients

Measurement of the inclusive production cross sections for forward jets and for dijet events with one forward and one central jet in pp collisions at sqrt(s) = 7 TeV

The inclusive production cross sections for forward jets, as well for jets in dijet events with at least one jet emitted at central and the other at forward pseudorapidities, are measured in the range of transverse momenta pt = 35-150 GeV/c in proton-proton collisions at sqrt(s) = 7 TeV by the CMS experiment at the LHC. Forward jets are measured within pseudorapidities 3.2<|eta|<4.7, and central jets within the |eta|<2.8 range. The double differential cross sections with respect to pt and eta are compared to predictions from three approaches in perturbative quantum chromodynamics: (i) next-to-leading-order calculations obtained with and without matching to parton-shower Monte Carlo simulations, (ii) PYTHIA and HERWIG parton-shower event generators with different tunes of parameters, and (iii) CASCADE and HEJ models, including different non-collinear corrections to standard single-parton radiation. The single-jet inclusive forward jet spectrum is well described by all models, but not all predictions are consistent with the spectra observed for the forward-central dijet events.Comment: Submitted to the Journal of High Energy Physic

Ratios of dijet production cross sections as a function of the absolute difference in rapidity between jets in proton-proton collisions at √s = 7TeV

A study of dijet production in proton-proton collisions was performed at root s = 7 TeV for jets with p(T) > 35 GeV and vertical bar y vertical bar < 4.7 using data collected with the CMS detector at the LHC in 2010. Events with at least one pair of jets are denoted as "inclusive". Events with exactly one pair of jets are called "exclusive". The ratio of the cross section of all pairwise combinations of jets to the exclusive dijet cross section as a function of the rapidity difference between jets vertical bar Delta y vertical bar is measured for the first time up to vertical bar Delta y vertical bar = 9.2. The ratio of the cross section for the pair consisting of the most forward and the most backward jet from the inclusive sample to the exclusive dijet cross section is also presented. The predictions of the Monte Carlo event generators PYTHIA6 and PYTHIA8 agree with the measurements. In both ratios the HERWIG++ generator exhibits a more pronounced rise versus vertical bar Delta y vertical bar than observed in the data. The BFKL-motivated generators CASCADE and HEJ+ARIADNE predict for these ratios a significantly stronger rise than observed

Hormonal control of spermatogenesis: expression of FSJH receptor and androgen receptor genes

FSH and testosterone are the main hormonal regulators of spermatogenesis. The actions of androgens and FSH are mediated by their respective receptors. Receptor gene expression (mRNA and protein). is an important determinant of hormone action. Biochemical aspects of the regulation of androgen and FSH receptor gene expression in the testis were chosen as the subject of the studies described in this thesis. Regulation of the expression of the receptor genes was studied at the level of gene transcription, and at the level of mRNA and protein expression. In Chapters 2-4, a detailed characterization is given of the effects of FSH on androgen and FSH receptor mRNA and protein expression in cultured immature Sertoli cells. For the androgen receptor, these findings were extended by measurements of androgen receptor gene transcription initiation rate in cultured immature Sertoli cells and LNCaP Oymph node carcinoma of the prostate) cells (Chapter 5). Preliminary results concerning a putative paracrine factor, produced by Sertoli cells and affecting androgen receptor mRNA expression in peritubular myoid cells, are presented in Chapter 6. The effects of testosterone deprivation iD. vivo on androgen receptor mRNA and protein expression in the adult rat testis were examined as described in Chapter 7.ffi vitro effects of testosterone on androgen receptor gene expression in cultured testicular cells and LNCaP cells are described in the Chapters 2, 3 and 5. In the General Discussion (Chapter 8) we have considered some aspects of regulation of spermatogenesis by FSH and testosterone and have discussed them in relation to our experimental data as well as in a broader perspective. This way, we hope that the results which we have presented, and discussions which we have tried to initiate, may contribute to research concerning hormonal control of spermatogenesis, now and in the futur

Study of exclusive two-photon production of W+W- in pp collisions at √s=7 TeV and constraints on anomalous quartic gauge couplings

A search for exclusive or quasi-exclusive W+W- production by photon-photon interactions, pp -> p(*)W(+)W(-)p(*), at \/s = 7 TeV is reported using data collected by the CMS detector with an integrated luminosity of 5.05 fb(-1). Events are selected by requiring a mu(+/-)mu(-/+) vertex with no additional associated charged tracks and dilepton transverse momentum p(T)(mu(+/-)mu(-/+)) > 30 GeV. Two events passing all selection requirements are observed in the data, compared to a standard model expectation of 2.2 +/- 0.4 signal events with 0.84 +/- 0.15 background. The tail of the dilepton p(T) distribution is studied for deviations from the standard model. No events are observed with p(T) > 100 GeV. Model-independent upper limits are computed and compared to predictions involving anomalous quartic gauge couplings. The limits on the parameters a(0,c)(W)/A(2) with a dipole form factor and an energy cutoff A(cutoff) = 500 GeV are of the order of 10(-4)

Measurement of the inelastic proton-proton cross section at root √s√s=7TeV=7 TeV

A measurement is presented of the inelastic proton–proton cross section at a centre-of-mass energy of $√s$$=7 TeV$. Using the CMS detector at the LHC, the inelastic cross section is measured through two independent methods based on information from (i) forward calorimetry (for pseudorapidity 3 200MeV/c . The measurements cover a large fraction of the inelastic cross section for particle production over about nine units of pseudorapidity and down to small transverse momenta. The results are compared with those of other experiments, and with models used to describe high-energy hadronic interactions