SearcharxivSearch

arXiv subjects

W. James Stirling

Publications and source records attributed to W. James Stirling.

18 recordsLinked to original sources

Single and Double Perturbative Splitting Diagrams in Double Parton Scattering

We discuss the role of two different types of diagram in the proton-proton double parton scattering (DPS) cross section - single and double perturbative splitting graphs. Using explicit calculations of simple graphs from these classes we show that the treatment of these graphs by the 'double PDF' framework for describing the DPS cross section, introduced a number of years ago by Snigirev and collaborators, is unsatisfactory. We suggest that a contribution from single perturbative splitting graphs should be included in the DPS cross section, albeit with a different geometrical prefactor to the contribution from 'zero perturbative splitting' graphs.

hep-ph

Double Parton Scattering Singularity in One-Loop Integrals

We present a detailed study of the double parton scattering (DPS) singularity, which is a specific type of Landau singularity that can occur in certain one-loop graphs in theories with massless particles. A simple formula for the DPS singular part of a four-point diagram with arbitrary internal/external particles is derived in terms of the transverse momentum integral of a product of light cone wavefunctions with tree-level matrix elements. This is used to reproduce and explain some results for DPS singularities in box integrals that have been obtained using traditional loop integration techniques. The formula can be straightforwardly generalised to calculate the DPS singularity in loops with an arbitrary number of external particles. We use the generalised version to explain why the specific MHV and NMHV six-photon amplitudes often studied by the NLO multileg community are not divergent at the DPS singular point, and point out that whilst all NMHV amplitudes are always finite, certain MHV amplitudes do contain a DPS divergence. It is shown that our framework for calculating DPS divergences in loop diagrams is entirely consistent with the `two-parton GPD' framework of Diehl and Schafer for calculating proton-proton DPS cross sections, but is inconsistent with the `double PDF' framework of Snigirev.

hep-ph

Same-sign W pair production as a probe of double parton scattering at the LHC

We study the production of same-sign W boson pairs at the LHC in double parton interactions. Compared with simple factorised double parton distributions (dPDFs), we show that the recently developed dPDFs, GS09, lead to non-trivial kinematic correlations between the W bosons. A numerical study of the prospects for observing this process using same-sign dilepton signatures, including same-sign WWjj, di-boson and heavy flavour backgrounds, at 14 TeV centre-of-mass energy is then performed. It is shown that a small excess of same-sign dilepton events from double parton scattering over a background dominated by single scattering WZ(gamma*) production could be observed at the LHC.

hep-ph

Double Parton Distributions Incorporating Perturbative QCD Evolution and Momentum and Quark Number Sum Rules

It is anticipated that hard double parton scatterings will occur frequently in the collisions of the LHC, producing interesting signals and significant backgrounds to certain single scattering processes. For double scattering processes in which the same hard scale t = ln(Q^2) is involved in both collisions, we require the double parton distributions (dPDFs) D_h^{j_1j_2}(x_1,x_2;t) in order to make theoretical predictions of their rates and properties. We describe the development of a new set of leading order dPDFs that represents an improvement on approaches used previously. First, we derive momentum and number sum rules that the dPDFs must satisfy. The fact that these must be obeyed at any scale is used to construct improved dPDFs at the input scale Q_0, for a particular choice of input scale (Q_0^2 = 1 GeV^2) and corresponding single PDFs (the MSTW2008LO set). We then describe a novel program which uses a direct x-space method to numerically integrate the LO DGLAP equation for the dPDFs, and which may be used to evolve the input dPDFs to any other scale. This program has been used along with the improved input dPDFs to produce a set of publicly available dPDF grids covering the ranges 10^{-6}<x_1<1, 10^{-6}<x_2<1, and 1<Q^2<10^9 GeV^2.

hep-ph

Progress in Parton Distribution Functions

Parton distribution functions (pdfs) are an important ingredient for LHC phenomenology. Recent progress in determining pdfs from global analyses is reviewed, and some of the most important outstanding issues are highlighted. Particular attention is paid to the precision with which predictions for LHC `standard-candle' cross sections can be made, and also to new information that LHC can provide on pdfs.

hep-ph

Soft Gluon Resummation in Transverse Momentum Space for Electroweak Boson Production at Hadron Colliders

The distribution of W and Z bosons produced with small transverse momentum (pt) at hadron colliders receives important contributions from large logarithms arising from soft gluon emission. Although conventionally the all-orders resummation of these `Sudakov' logarithms is performed in impact parameter (Fourier transform) space, pt-space resummation is also possible, and offers certain advantages.We present a detailed phenomenological analysis of W and Z production at small pt at the Tevatron $p \bar p$ collider, using pt-space resummation. A good description of the CDF and D0 data can be obtained provided a significant non-perturbative contribution is included. We also present predictions for the LHC.

hep-ph

BFKL dynamics at hadron colliders

Hadron colliders can provide important tests of BFKL `small-x' dynamics. We discuss two examples of such tests, the inclusive dijet jet cross section at large rapidity separation and the number of associated `mini-jets' in Higgs boson production.

hep-ph

Sudakov Logarithm Resummation for Vector Boson Production at Hadron Colliders

A complete description of W and Z boson production at high-energy colliders requires the resummation of large Sudakov logarithms which dominate the production at small transverse momentum. Currently there are two techniques for performing this resummation: impact parameter space and transverse momentum space. We argue that the latter can be formulated in a way which retains the advantages of the former, while at the same time allowing a smooth transition to finite order dominance at high transverse momentum.

hep-ph

Like-Sign W Boson Production at the LHC as a Probe of Double Parton Scattering

Double parton scattering, i.e. two parton hard scattering processes in the same hadron-hadron collision, may constitute an important background for Higgs and other new particle searches at the LHC. We point out that like-sign W pair production provides a relatively clean way of searching for, and calibrating, double parton scattering at the LHC.

hep-ph

Higgs Boson Production at the Compton Collider

The high precision determination of the partial width $Γ(H \longrightarrow γγ)$ of an intermediate mass Higgs boson is among the most important measurements at a future photon--photon collider. Recently it was shown that large non-Sudakov as well as Sudakov double logarithmic corrections can be summed to all orders in the background process $γγ\longrightarrow q \bar{q}$, $q=\{b,c\}$, from an initially polarized $J_z=0$ state. In addition, running coupling corrections were included exactly to all orders by employing the renormalization group. Thus all necessary theoretical results for calculating the Higgs signal and the non-Higgs continuum background contributions to the process $γγ\longrightarrow q \bar{q}$ are now known. We are therefore able to present for the first time precise predictions for the measurement of the partial width $Γ(H \longrightarrow γγ)$ at the Compton collider ($γγ$) option at a future linear $e^+e^-$ collider. The interplay between signal and background is very sensitive to the experimental cuts and the ability of the detectors to identify $b$-quarks in the final state. We investigate this in some detail using a Monte Carlo analysis, and conclude that a measurement with a 2 % statistical accuracy should be achievable. This could have important consequences for the discovery of physics beyond the Standard Model, in particular for large masses of a pseudoscalar Higgs boson as the decoupling limit is difficult and for a wide range of $\tan β$ impossible to cover at the LHC proton-proton collider.

hep-ph

Anomalous Quartic Couplings in W^+W^-γ, Z^0Z^0γand Z^0γγProduction at Present and Future e^+e^- Colliders

The production of three electroweak gauge bosons in high-energy $e^+e^-$ collisions offers a window on anomalous quartic gauge boson couplings. We investigate the effect of three possible anomalous couplings on the cross sections for $W^+W^-γ$, $Z^0Z^0γ$ and $Z^0γγ$ productions at LEP2 ($\sqrt{s} = 200$ GeV) and at a future linear collider ($\sqrt{s} = 500$ GeV). We find that the combination of energies and processes provides reasonable discrimination between the various anomalous contributions.

hep-ph

Radiation Zeros in W^+W^-γProduction at High-Energy Colliders

The vanishing of the cross section for particular points in phase space - radiation zeros - is examined for the process $ q \bar q \to W^+W^- γ$ at high energy. Unlike the process $q \bar q' \to W^\pm γ$, actual zeros only occur in the soft-photon limit. However, for photon energies that are not too large, the cross section does exhibit deep dips in regions of phase space corresponding to the position of the actual zeros. We show that in these regions the sensitivity to possible anomalous quartic couplings is very large.

hep-ph

Renormalization Group Improved Heavy Quark Production in Polarized γγCollisions

The experimental determination of the partial width $Γ(H \longrightarrow γγ)$ of an intermediate mass Higgs is among the most important measurements at a future photon photon collider. Recently it was shown that large non-Sudakov as well as Sudakov double logarithmic (DL) corrections can be summed to all orders in the background process $γγ(J_z=0) \longrightarrow q \bar{q}$. It was found that positivity and stability of the cross section was only restored at the four-loop level. One remaining large source of uncertainty stems from the fact that the scale of the strong coupling is unspecified within the double logarithmic approximation. In this paper we include the leading and next-to-leading order running coupling to all orders. We thus remove the inherent scale uncertainty of both the exact one-loop and all-orders DL result without encountering any Landau-pole singularities. The effect is significant and, for the non-Sudakov form factor, is found to correspond to an effective scale of roughly $α_s(9m_q^2)$.

hep-ph

Sudakov Logarithm Resummation in Transverse Momentum Space for Electroweak Boson Production at Hadron Colliders

A complete description of W and Z boson production at high-energy hadron colliders requires the resummation of large Sudakov double logarithms which dominate the transverse momentum (q_T) distribution at small q_T. We compare different prescriptions for performing this resummation, in particular implicit impact parameter space resummation versus explicit transverse momentum space resummation. We argue that the latter method can be formulated so as to retain the advantages of the former, while at the same time allowing a smooth transition to finite order dominance at high q_T.

hep-ph

Heavy Quark Production at a $γγ$ Collider: the Effect of Large Logarithmic Perturbative Corrections

We present quantitative results on the cross section for $γ+ γ(J_z=0) \to b \bar{b}\to two b$-jets based on the recently achieved all orders resummation of large soft (Sudakov) and hard (non-Sudakov) double logarithms. The next-to-leading order QCD perturbative corrections are included exactly. We find that one needs to include at least four loops for the novel hard leading logarithms, on the cross section level, in order to be safe from large opposite sign cancellations that plagued earlier phenomenological studies. We find that the background to intermediate mass Higgs boson production at a future photon linear collider (PLC) is thus reasonably well under control and should allow the direct determination of the partial Higgs width $Γ(H \to γ+ γ)$. Assuming high efficiency $b$-tagging, the total Higgs width measurement at a PLC is thus a realistic goal.

hep-ph

All-Orders Resummation of Leading Logarithmic Contributions to Heavy Quark Production in Polarized γγCollisions

The measurements of the $γγ$ and $b \bar b$ partial decay widths of an intermediate-mass Standard Model Higgs boson are among the most important goals of a future photon linear collider. While in an initially polarized $J_z=0$ state the background process $γγ\to b \bar b$ is suppressed by $\frac{m^2_b}{s}$, radiative corrections remove this suppression and are known to be very sizable at theone-loop level. In particular a new type of purely hard double logarithmic (DL) correction can even make the cross section negative at this order in perturbation theory. The second order term of the series is also known and enters with a positive sign at the two loop level. From a theoretical as well as a practical point of view it is clearlydesirable to resum this series and to know its high energy behavior. In this paper, we derive the series of these novel ``non-Sudakov'' logarithms to all orders and calculate the high energy limit analytically. We also give explicit three loop corrections in the DL-approximation as a check of our results and show that the three loop structure also reveals the higher order behavior of mixed hard and soft double logarithms. We are thus able to resum the virtual DL-corrections to $γγ(J_z=0) \to b \bar b$ to all orders.

hep-ph