001     415414
005     20211110152147.0
024 7 _ |a Blondel:2018mad
|2 INSPIRETeX
024 7 _ |a inspire:1692960
|2 inspire
024 7 _ |a arXiv:1809.01830
|2 arXiv
024 7 _ |a 10.3204/PUBDB-2018-04490
|2 datacite_doi
037 _ _ |a PUBDB-2018-04490
041 _ _ |a English
088 1 _ |a arXiv:1809.01830; BU-HEPP-18-04; CERN-TH-2018-145; IFJ-PAN-IV-2018-09; KW 18-003; MITP/18-052; MPP-2018-143; SI-HEP-2018-21
088 _ _ |a arXiv:1809.01830
|2 arXiv
088 _ _ |a BU-HEPP-18-04
|2 Other
088 _ _ |a CERN-TH-2018-145
|2 CERN
088 _ _ |a IFJ-PAN-IV-2018-09
|2 Other
088 _ _ |a KW 18-003
|2 Other
088 _ _ |a MITP/18-052
|2 Other
088 _ _ |a MPP-2018-143
|2 MPG
088 _ _ |a SI-HEP-2018-21
|2 arXiv
100 1 _ |a Blondel, A.
|0 P:(DE-HGF)0
|b 0
111 2 _ |0 C18-01-12
|2 inspire
245 _ _ |a Standard Model Theory for the FCC-ee: The Tera-Z
260 _ _ |c 2018
336 7 _ |a Preprint
|b preprint
|m preprint
|0 PUB:(DE-HGF)25
|s 1542191324_6534
|2 PUB:(DE-HGF)
336 7 _ |a WORKING_PAPER
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336 7 _ |a Electronic Article
|0 28
|2 EndNote
336 7 _ |a preprint
|2 DRIVER
336 7 _ |a Report
|0 PUB:(DE-HGF)29
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336 7 _ |a ARTICLE
|2 BibTeX
336 7 _ |a Output Types/Working Paper
|2 DataCite
500 _ _ |a 243 pages, Report on the 1st Mini workshop: Precision EW and QCD calculations for the FCC studies: methods and tools, 12-13 January 2018, CERN, Geneva, Switzerland
520 _ _ |a The future 100-km circular collider FCC at CERN is planned to operate in one of its modes as an electron-positron FCC-ee machine. We give an overview of the theoretical status compared to the experimental demands of one of four foreseen FCC-ee operating stages, which is Z-boson resonance energy physics, FCC-ee Tera-Z stage for short. The FCC-ee Tera-Z will deliver the highest integrated luminosities as well as very small systematic errors for a study the Standard Model (SM) with unprecedented precision. In fact, the FCC-ee Tera-Z will allow to study at least one more quantum field theoretical perturbative order compared to the LEP/SLC precision. The real problem is that the present precision of theoretical calculations of the various observables within the SM does not match that of the anticipated experimental measurements. The bottle-neck problems are specified. In particular, the issues of precise QED unfolding and of the correct calculation of SM pseudo-observables are critically reviewed. In an Executive Summary we specify which basic theoretical calculations are needed to meet the strong experimental expectations at the FCC-ee Tera-Z. Several methods, techniques and tools needed for higher order multi-loop calculations are presented. By inspection of the Z-boson partial and total decay widths analysis, arguments are given that at the beginning of operation of the FCC-ee Tera-Z, the theory predictions may be tuned to be precise enough not to limit the physics interpretation of the measurements. This statement is based on the anticipated progress in analytical and numerical calculations of multi-loop and multi-scale Feynman integrals and on the completion of two-loop electroweak radiative corrections to the SM pseudo-observables this year. However, the above statement is conditional as the theoretical issues demand a very dedicated and focused investment by the community.
536 _ _ |0 G:(DE-HGF)POF3-611
|c POF3-611
|f POF III
|x 0
|a 611 - Fundamental Particles and Forces (POF3-611)
588 _ _ |a Dataset connected to INSPIRE
650 _ 7 |a quantum electrodynamics
|2 INSPIRE
650 _ 7 |a electroweak interaction: radiative correction
|2 INSPIRE
650 _ 7 |a electroweak interaction: precision measurement
|2 INSPIRE
650 _ 7 |a form factor
|2 INSPIRE
650 _ 7 |a Yang-Mills
|2 INSPIRE
650 _ 7 |a electron positron: colliding beams
|2 INSPIRE
650 _ 7 |a CERN Lab
|2 INSPIRE
650 _ 7 |a FCC-ee
|2 INSPIRE
650 _ 7 |a SLAC SLC Linac
|2 INSPIRE
650 _ 7 |a CERN LEP Stor
|2 INSPIRE
650 _ 7 |a programming
|2 INSPIRE
650 _ 7 |a numerical calculations
|2 INSPIRE
650 _ 7 |a new physics
|2 INSPIRE
693 _ _ |0 EXP:(DE-MLZ)NOSPEC-20140101
|5 EXP:(DE-MLZ)NOSPEC-20140101
|e No specific instrument
|x 0
700 1 _ |a Gluza, J.
|0 P:(DE-HGF)0
|b 1
|e Corresponding author
700 1 _ |a Jadach, S.
|b 2
700 1 _ |a Janot, P.
|b 3
700 1 _ |a Riemann, T.
|b 4
700 1 _ |a Akhundov, A.
|b 5
700 1 _ |a Arbuzov, A.
|b 6
700 1 _ |a Boels, R.
|b 7
700 1 _ |a Bondarenko, S.
|b 8
700 1 _ |a Borowka, S.
|b 9
700 1 _ |a Carloni Calame, C. M.
|b 10
700 1 _ |a Dubovyk, I.
|0 P:(DE-H253)PIP1019266
|b 11
700 1 _ |a Dydyshka, Ya.
|b 12
700 1 _ |a Flieger, W.
|b 13
700 1 _ |a Freitas, A.
|b 14
700 1 _ |a Grzanka, K.
|b 15
700 1 _ |a Hahn, T.
|b 16
700 1 _ |a Huber, T.
|b 17
700 1 _ |a Kalinovskaya, L.
|b 18
700 1 _ |a Lee, R.
|b 19
700 1 _ |a Marquard, P.
|0 P:(DE-H253)PIP1019895
|b 20
|u desy
700 1 _ |a Montagna, G.
|b 21
700 1 _ |a Nicrosini, O.
|b 22
700 1 _ |a Papadopoulos, C. G.
|b 23
700 1 _ |a Piccinini, F.
|b 24
700 1 _ |a Pittau, R.
|b 25
700 1 _ |a Pł aczek, W.
|b 26
700 1 _ |a Prausa, M.
|b 27
700 1 _ |a Riemann, S.
|0 P:(DE-H253)PIP1003733
|b 28
|u desy
700 1 _ |a Rodrigo, G.
|b 29
700 1 _ |a Sadykov, R.
|b 30
700 1 _ |a Skrzypek, M.
|b 31
700 1 _ |a Stöckinger, D.
|b 32
700 1 _ |a Usovitsch, J.
|b 33
700 1 _ |a Ward, B. F. L.
|b 34
700 1 _ |a Weinzierl, S.
|b 35
700 1 _ |a Yang, G.
|b 36
700 1 _ |a Yost, S. A.
|b 37
856 4 _ |y OpenAccess
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910 1 _ |a External Institute
|0 I:(DE-HGF)0
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910 1 _ |a Deutsches Elektronen-Synchrotron
|0 I:(DE-588b)2008985-5
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910 1 _ |a Deutsches Elektronen-Synchrotron
|0 I:(DE-588b)2008985-5
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|6 P:(DE-H253)PIP1003733
913 1 _ |a DE-HGF
|b Forschungsbereich Materie
|l Materie und Universum
|1 G:(DE-HGF)POF3-610
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914 1 _ |y 2018
915 _ _ |a OpenAccess
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915 _ _ |a Creative Commons Attribution CC BY 4.0
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915 _ _ |a Published
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920 1 _ |0 I:(DE-H253)ZEU-THEO-20120731
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980 _ _ |a preprint
980 _ _ |a VDB
980 _ _ |a UNRESTRICTED
980 _ _ |a report
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