Home > Publications database > High precision QED Initial State Corrections for $e^+ e^- \rightarrow \gamma^*/Z^*$ Annihilation > print |
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024 | 7 | _ | |a 10.1142/S021773232230004X |2 doi |
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088 | _ | _ | |a TTP-22-011 |2 Other |
088 | _ | _ | |a SAGEX-22-19 |2 Other |
100 | 1 | _ | |a Blümlein, Johannes |0 P:(DE-H253)PIP1003764 |b 0 |e Corresponding author |
245 | _ | _ | |a High precision QED Initial State Corrections for $e^+ e^- \rightarrow \gamma^*/Z^*$ Annihilation |
260 | _ | _ | |a Singapur |c 2022 |b World Scientific Publ. |
336 | 7 | _ | |a article |2 DRIVER |
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500 | _ | _ | |a 24 pages LATEX, 5 FiguresFulltext corresponds to the Post referee version Waiting for fulltext |
520 | _ | _ | |a The precise knowledge of the QED initial state corrections is of instrumental importance in studyinghigh luminosity measurements in $e^+e^-$ annihilation at facilities like LEP, the International Linear ColliderILC, CLIC, a Giga-$Z$ facility, and the planned FCC\_ee. Logarithmic corrections of up to $O(\alpha^6 L^5)$ arenecessary with various subleading terms taken into account. This applies to both the inclusive measurementof processes like $e^+ e^- \rightarrow \gamma^*/Z^*$ and also the forward--backward asymmetry. As has been shownrecently, techniques from massive QCD, such as the computation of massive on--shell operator matrix elements canbe used for these calculations. We give an introduction to this topic and present both the calculationmethods and the numerical corrections having been reached so far. |
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650 | _ | 7 | |a angular distribution, asymmetry |2 INSPIRE |
650 | _ | 7 | |a luminosity, high |2 INSPIRE |
650 | _ | 7 | |a annihilation |2 INSPIRE |
650 | _ | 7 | |a quantum electrodynamics |2 INSPIRE |
650 | _ | 7 | |a ILC Coll |2 INSPIRE |
650 | _ | 7 | |a initial state |2 INSPIRE |
650 | _ | 7 | |a quantum chromodynamics |2 INSPIRE |
650 | _ | 7 | |a CERN LEP Stor |2 INSPIRE |
650 | _ | 7 | |a CERN CLIC |2 INSPIRE |
650 | _ | 7 | |a electron, annihilation |2 INSPIRE |
650 | _ | 7 | |a quantum electrodynamics, higher-order |2 INSPIRE |
650 | _ | 7 | |a radiation, initial-state interaction |2 INSPIRE |
650 | _ | 7 | |a Initial state radiation |2 autogen |
650 | _ | 7 | |a precision QED |2 autogen |
650 | _ | 7 | |a higher order calculations |2 autogen |
650 | _ | 7 | |a e+e− experiments |2 autogen |
650 | _ | 7 | |a Z-boson observables |2 autogen |
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700 | 1 | _ | |a Schönwald, Kay |0 P:(DE-H253)PIP1026518 |b 1 |
773 | _ | _ | |a 10.1142/S021773232230004X |g Vol. 37, no. 07, p. 2230004 |0 PERI:(DE-600)2008260-5 |n 07 |p 2230004 |t Modern physics letters / A |v 37 |y 2022 |x 0217-7323 |
787 | 0 | _ | |a Blümlein, Johannes et.al. |d 2022 |i IsParent |0 PUBDB-2022-01054 |r DESY-22-024 ; arXiv:2202.08476 ; DO-TH 22/04 ; TTP-22-011 ; SAGEX-22-19 |t High precision QED Initial State Corrections for $e^+ e^- \rightarrow \gamma^*/Z^*$ Annihilation |
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