Single superpartner production at Tevatron Run II

We study the single productions of supersymmetric particles at Tevatron Run II which occur in the $2 \to 2-body$ processes involving R-parity violating couplings of type \l'_{ijk} L_i Q_j D_k^c. We focus on the single gaugino productions which receive contributions from the resonant slepton productions. We first calculate the amplitudes of the single gaugino productions. Then we perform analyses of the single gaugino productions based on the three charged leptons and like sign dilepton signatures. These analyses allow to probe supersymmetric particles masses beyond the present experimental limits, and many of the \l'_{ijk} coupling constants down to values smaller than the low-energy bounds. Finally, we show that the studies of the single gaugino productions offer the opportunity to reconstruct the $\tilde \chi^0_1$, $\tilde \chi^{\pm}_1$, $\tilde \nu_L$ and $\tilde l^{\pm}_L$ masses with a good accuracy in a model independent way.Comment: 47 pages, epsfi

First measurement of elastic, inelastic and total cross-section at √=13 TeV by TOTEM and overview of cross-section data at LHC energies

This work is licensed under a Creative Commons Attribution 4.0 International License.The TOTEM collaboration has measured the proton–proton total cross section at √=13 TeV with a luminosity-independent method. Using dedicated ∗=90 m beam optics, the Roman Pots were inserted very close to the beam. The inelastic scattering rate has been measured by the T1 and T2 telescopes during the same LHC fill. After applying the optical theorem the total proton–proton cross section is tot=(110.6 ± 3.4) mb, well in agreement with the extrapolation from lower energies. This method also allows one to derive the luminosity-independent elastic and inelastic cross sections: el=(31.0 ± 1.7) mb and inel=(79.5 ± 1.8) mb

Diffractive χ\chi Production at the Tevatron and the LHC

We present predictions for the diffractive production of $\chi$ mesons in the central rapidity region usually covered by collider detectors. The predicted cross sections are based on the Bialas-Landshoff formalism for both exclusive and inclusive production and makes use of the DPEMC Monte-Carlo simulation adapted with kinematics appropriate for small-mass diffractive production. We compare generator-level results with a CDF measurement for exclusive $\chi$ production, and study background and other scenarios including the contribution of inclusive $\chi$ production. The results agree with the Tevatron data and are extrapolated, highlighting the exclusive \chic production at LHC energies. A possible new measurement at the Tevatron using the D{\O}forward detectors is investigated, taking advantage of the dominance of exclusive production for high enough diffractive mass fraction.Comment: 9 pages, 2 figures, added akcnowledgment

Probing new physics in diphoton production with proton tagging at the Large Hadron Collider

The sensitivities to anomalous quartic photon couplings at the Large Hadron Collider are estimated using diphoton production via photon fusion. The tagging of the protons proves to be a very powerful tool to suppress the background and unprecedented sensitivities down to $6 \cdot 10^{-15}$\gev$^{-4}$ are obtained, providing a new window on extra dimensions and strongly-interacting composite states in the multi-TeV range. Generic contributions to quartic photon couplings from charged and neutral particles with arbitrary spin are also presented.Comment: 4 pages, 3 figure

Resonant sneutrino production at Tevatron Run II

We consider the single chargino production at Tevatron $p \bar p \to \tilde \nu_i \to \tilde \chi^{\pm}_1 l_i^{\mp}$ as induced by the resonant sneutrino production via a dominant \RPV coupling of type \l'_{ijk} L_i Q_j D_k^c. Within a supergravity model, we study the three leptons final state. The comparison with the expected background demonstrate that this signature allows to extend the sensitivity on the \susyq mass spectrum beyond the present LEP limits and to probe the relevant \RPV coupling down to values one order of magnitude smaller than the most stringent low energy indirect bounds. The trilepton signal offers also the opportunity to reconstruct the neutralino mass in a model independent way with good accuracy.Comment: 4 page

A new determination of the Pomeron intercept in hard processes

A method allowing for a direct comparison of data with theoreticalpredictions is proposed for forward jet production at HERA. It avoids thereconstruction of multi-parton contributions by expressing the experimentalcuts directly as correction factors on the QCD forward jet cross-section. Anapplication to the determination of the {\it effective} Pomeron intercept inthe BFKL-LO parametrization from $d\sigma/dx$ data at HERA leads to a good fitwith a significantly higher {\it effective} intercept, $\alpha_P= 1.43 \pm0.025 (stat.) \pm 0.025 (syst.),$ than for proton (total and diffractive)structure functions. It is however less than the value of the pomeron interceptusing dijets with large rapidity intervals obtained at Tevatron. We alsoevaluate the rapidity veto contribution to the higher order BFKL corrections.The method can be extended to other theoretical inputs

First computation of Mueller Tang processes using the full NLL BFKL approach

We present the full next-to-leading order (NLO) prediction for the jet-gap-jet cross section at the LHC within the BFKL approach. We implement, for the first time, the NLO impact factors in the calculation of the cross section. We provide results for differential cross sections as a function of the difference in rapidity and azimuthal angle betwen the two jets and the second leading jet transverse momentum. The NLO corrections of the impact factors induce an overall reduction of the cross section with respect to the corresponding predictions with only LO impact factors. We note that NLO impact factors feature a logarithmic dependence of the cross section on the total center of mass energy which formally violates BFKL factorization. We show that such term is one order of magnitude smaller than the total contribution, and thus can be safely included in the current prediction without a need of further resummation of such logarithmic terms. Fixing the renormalization scale $\mu_R$ according to the principle of minimal sensitivity, suggests $\mu_R$ about 4 times the sum of the transverse jet energies and provides smaller theroretical uncertainties with respect to the leading order case