Abstract
Starting with QCD, we derive an effective field theory description for forward scattering and factorization violation as part of the soft-collinear effective field theory (SCET) for high energy scattering. These phenomena are mediated by long distance Glauber gluon exchanges, which are static in time, localized in the longitudinal distance, where $|t| \ll s$. In hard scattering, Glauber gluons can induce corrections which invalidate factorization. With SCET, Glauber exchange graphs can be calculated explicitly, and are distinct from graphs with soft, collinear, or ultrasoft gluons. We derive a complete basis of operators which describe the leading power effects of Glauber exchange. Key ingredients include regulating light-cone rapidity singularities and subtractions which prevent double counting. Our results include a novel all orders gauge invariant pure glue soft operator which appears between two collinear rapidity sectors. The 1-gluon Feynman rule for the soft operator coincides with the Lipatov vertex, but it also contributes to emissions with $\ge 2$ soft gluons. Our Glauber operator basis is derived using tree level and one-loop matching calculations from full QCD to SCET. The rapidity RGE yields gluon Reggeization at the amplitude level, and gives the BFKL equation for the soft and collinear functions in the forward scattering cross section. We derive an explicit rule for when eikonalization is valid, and provide a direct connection to the picture of multiple Wilson lines crossing a shockwave. In hard scattering operators Glauber subtractions for soft and collinear loop diagrams ensure that we are not sensitive to the directions for soft and collinear Wilson lines. Conversely, certain Glauber interactions can be absorbed into these soft and collinear Wilson lines by taking them to be in specific directions. We also discuss criteria for factorization violation.
Highlights
Progress in our understanding of interacting four dimensional quantum field theories has come from various directions
For the simplest examples in these categories we show that iterated Glauber exchange yields either phases or contributions that are related to the direction of soft or collinear Wilson lines in the hard scattering operators, and cancel for an inclusive cross section
These components are tied together by propagators that have onshell scaling for their momenta, which are represented by the onshell fields in the effective field theory (EFT), and such contributions are represented by time ordered products of tree level induced Glauber exchange operators in soft-collinear effective field theory (SCET)
Summary
Progress in our understanding of interacting four dimensional quantum field theories has come from various directions. The purpose of this paper is to set up a systematic effective theory with which to study the near forward scattering region of QCD and factorization violation in hard scattering processes in a single framework. The formalism presented here gives a starting point for using a field theoretic method to study the physics of the near forward region, even beyond leading power It provides a direct method of calculating (possible) factorization violating contributions, and potentially could yield field theoretic methods for handling underlying event contributions in hadronic collisions. First we note that in the CSS formalism [21, 31] that Glauber contributions are discussed in detail, but are treated as a momentum region and are not fully separated from soft and collinear gluon dynamics This has advantages for certain steps of a factorization proof, but makes it more difficult to associate unique contributions with Glauber exchange, and to see how factorization arises for processes that retain nontrivial soft functions. We will elaborate on the connection between our EFT and the multi-Wilson line framework in sections 9.2 and 9.3
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.