FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2090800669> ?p ?o ?g. }

• W2090800669 endingPage "291" @default.
• W2090800669 startingPage "261" @default.
• W2090800669 abstract "In this paper we present the master integrals necessary for the analytic calculation of the box diagrams with one electron loop (N_{F}=1) entering in the 2-loop (alpha^3) QED virtual corrections to the Bhabha scattering amplitude of the electron. We consider on-shell electrons and positrons of finite mass m, arbitrary squared c.m. energy s, and momentum transfer t; both UV and soft IR divergences are regulated within the continuous D-dimensional regularization scheme. After a brief overview of the method employed in the calculation, we give the results, for s and t in the Euclidean region, in terms of 1- and 2-dimensional harmonic polylogarithms, of maximum weight 3. The corresponding results in the physical region can be recovered by analytical continuation. For completeness, we also provide the analytic expression of the 1-loop scalar box diagram including the first order in (D-4)." @default.
• W2090800669 created "2016-06-24" @default.
• W2090800669 creator A5014656742 @default.
• W2090800669 creator A5024967342 @default.
• W2090800669 creator A5035629756 @default.
• W2090800669 creator A5088563281 @default.
• W2090800669 creator A5088869863 @default.
• W2090800669 date "2004-03-01" @default.
• W2090800669 modified "2023-09-27" @default.
• W2090800669 title "Planar box diagram for the (NF=1) 2-loop QED virtual corrections to Bhabha scattering" @default.
• W2090800669 cites W1972309204 @default.
• W2090800669 cites W1994265177 @default.
• W2090800669 cites W1995182568 @default.
• W2090800669 cites W1996472705 @default.
• W2090800669 cites W2002649361 @default.
• W2090800669 cites W2006569644 @default.
• W2090800669 cites W2009746734 @default.
• W2090800669 cites W2021173673 @default.
• W2090800669 cites W2029030772 @default.
• W2090800669 cites W2032088902 @default.
• W2090800669 cites W2035886875 @default.
• W2090800669 cites W2040511248 @default.
• W2090800669 cites W2045132656 @default.
• W2090800669 cites W2045835733 @default.
• W2090800669 cites W2051878864 @default.
• W2090800669 cites W2068050439 @default.
• W2090800669 cites W2086589970 @default.
• W2090800669 cites W2114391342 @default.
• W2090800669 cites W2125707848 @default.
• W2090800669 cites W2126874184 @default.
• W2090800669 cites W2779956489 @default.
• W2090800669 cites W2961955743 @default.
• W2090800669 cites W3033533480 @default.
• W2090800669 cites W3037555746 @default.
• W2090800669 cites W3100066887 @default.
• W2090800669 cites W3100478408 @default.
• W2090800669 cites W3100979635 @default.
• W2090800669 cites W3101768590 @default.
• W2090800669 cites W3102738991 @default.
• W2090800669 cites W3103192290 @default.
• W2090800669 cites W3103198553 @default.
• W2090800669 cites W3104010051 @default.
• W2090800669 cites W3105232365 @default.
• W2090800669 cites W4236595647 @default.
• W2090800669 cites W4255029341 @default.
• W2090800669 doi "https://doi.org/10.1016/j.nuclphysb.2004.01.026" @default.
• W2090800669 hasPublicationYear "2004" @default.
• W2090800669 type Work @default.
• W2090800669 sameAs 2090800669 @default.
• W2090800669 citedByCount "46" @default.
• W2090800669 countsByYear W20908006692012 @default.
• W2090800669 countsByYear W20908006692013 @default.
• W2090800669 countsByYear W20908006692014 @default.
• W2090800669 countsByYear W20908006692018 @default.
• W2090800669 countsByYear W20908006692019 @default.
• W2090800669 countsByYear W20908006692020 @default.
• W2090800669 countsByYear W20908006692021 @default.
• W2090800669 countsByYear W20908006692022 @default.
• W2090800669 crossrefType "journal-article" @default.
• W2090800669 hasAuthorship W2090800669A5014656742 @default.
• W2090800669 hasAuthorship W2090800669A5024967342 @default.
• W2090800669 hasAuthorship W2090800669A5035629756 @default.
• W2090800669 hasAuthorship W2090800669A5088563281 @default.
• W2090800669 hasAuthorship W2090800669A5088869863 @default.
• W2090800669 hasBestOaLocation W20908006692 @default.
• W2090800669 hasConcept C114614502 @default.
• W2090800669 hasConcept C121332964 @default.
• W2090800669 hasConcept C121684516 @default.
• W2090800669 hasConcept C134786449 @default.
• W2090800669 hasConcept C147120987 @default.
• W2090800669 hasConcept C153013531 @default.
• W2090800669 hasConcept C154945302 @default.
• W2090800669 hasConcept C161794534 @default.
• W2090800669 hasConcept C166124518 @default.
• W2090800669 hasConcept C184670325 @default.
• W2090800669 hasConcept C191486275 @default.
• W2090800669 hasConcept C2524010 @default.
• W2090800669 hasConcept C2776135515 @default.
• W2090800669 hasConcept C2776590265 @default.
• W2090800669 hasConcept C2779000718 @default.
• W2090800669 hasConcept C3079626 @default.
• W2090800669 hasConcept C33923547 @default.
• W2090800669 hasConcept C37914503 @default.
• W2090800669 hasConcept C41008148 @default.
• W2090800669 hasConcept C57691317 @default.
• W2090800669 hasConcept C62520636 @default.
• W2090800669 hasConcept C76494280 @default.
• W2090800669 hasConceptScore W2090800669C114614502 @default.
• W2090800669 hasConceptScore W2090800669C121332964 @default.
• W2090800669 hasConceptScore W2090800669C121684516 @default.
• W2090800669 hasConceptScore W2090800669C134786449 @default.
• W2090800669 hasConceptScore W2090800669C147120987 @default.
• W2090800669 hasConceptScore W2090800669C153013531 @default.
• W2090800669 hasConceptScore W2090800669C154945302 @default.
• W2090800669 hasConceptScore W2090800669C161794534 @default.
• W2090800669 hasConceptScore W2090800669C166124518 @default.
• W2090800669 hasConceptScore W2090800669C184670325 @default.
• W2090800669 hasConceptScore W2090800669C191486275 @default.

• next