Erratum to: Determination of the strong coupling constant $${{\varvec{\alpha _{\mathrm{s}} (m_{\mathrm{Z}})}}}$$ in next-to-next-to-leading order QCD using H1 jet cross section measurements
The determination of the strong coupling constant $$\alpha _{\mathrm{s}} (m_{\mathrm{Z}})$$ α s ( m Z ) from H1 inclusive and dijet cross section data [1] exploits perturbative QCD predictions in next-to-next-to-leading order (NNLO) [2–4]. An implementation error in the NNLO predictions was found [4...
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| Published in: | The European physical journal. C, Particles and fields Vol. 81; no. 8 |
|---|---|
| Main Authors: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
| Format: | Journal Article |
| Language: | English |
| Published: |
Springer
01.08.2021
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| Subjects: | |
| ISSN: | 1434-6044, 1434-6052 |
| Online Access: | Get full text |
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| Abstract | The determination of the strong coupling constant
$$\alpha _{\mathrm{s}} (m_{\mathrm{Z}})$$
α
s
(
m
Z
)
from H1 inclusive and dijet cross section data [1] exploits perturbative QCD predictions in next-to-next-to-leading order (NNLO) [2–4]. An implementation error in the NNLO predictions was found [4] which changes the numerical values of the predictions and the resulting values of the fits. Using the corrected NNLO predictions together with inclusive jet and dijet data, the strong coupling constant is determined to be
$$\alpha _{\mathrm{s}} (m_{\mathrm{Z}}) =0.1166\,(19)_{\mathrm{exp}}\,(24)_{\mathrm{th}}$$
α
s
(
m
Z
)
=
0.1166
(
19
)
exp
(
24
)
th
. Complementarily,
$$\alpha _{\mathrm{s}} (m_{\mathrm{Z}})$$
α
s
(
m
Z
)
is determined together with parton distribution functions of the proton (PDFs) from jet and inclusive DIS data measured by the H1 experiment. The value
$$\alpha _{\mathrm{s}} (m_{\mathrm{Z}}) =0.1147\,(25)_{\mathrm{tot}}$$
α
s
(
m
Z
)
=
0.1147
(
25
)
tot
obtained is consistent with the determination from jet data alone. Corrected figures and numerical results are provided and the discussion is adapted accordingly. |
|---|---|
| AbstractList | The determination of the strong coupling constant
$$\alpha _{\mathrm{s}} (m_{\mathrm{Z}})$$
α
s
(
m
Z
)
from H1 inclusive and dijet cross section data [1] exploits perturbative QCD predictions in next-to-next-to-leading order (NNLO) [2–4]. An implementation error in the NNLO predictions was found [4] which changes the numerical values of the predictions and the resulting values of the fits. Using the corrected NNLO predictions together with inclusive jet and dijet data, the strong coupling constant is determined to be
$$\alpha _{\mathrm{s}} (m_{\mathrm{Z}}) =0.1166\,(19)_{\mathrm{exp}}\,(24)_{\mathrm{th}}$$
α
s
(
m
Z
)
=
0.1166
(
19
)
exp
(
24
)
th
. Complementarily,
$$\alpha _{\mathrm{s}} (m_{\mathrm{Z}})$$
α
s
(
m
Z
)
is determined together with parton distribution functions of the proton (PDFs) from jet and inclusive DIS data measured by the H1 experiment. The value
$$\alpha _{\mathrm{s}} (m_{\mathrm{Z}}) =0.1147\,(25)_{\mathrm{tot}}$$
α
s
(
m
Z
)
=
0.1147
(
25
)
tot
obtained is consistent with the determination from jet data alone. Corrected figures and numerical results are provided and the discussion is adapted accordingly. The determination of the strong coupling constant [Formula omitted] from H1 inclusive and dijet cross section data [1 (See CR1)] exploits perturbative QCD predictions in next-to-next-to-leading order (NNLO) [2 (See CR2)-4 (See CR4)]. An implementation error in the NNLO predictions was found [4 (See CR4)] which changes the numerical values of the predictions and the resulting values of the fits. Using the corrected NNLO predictions together with inclusive jet and dijet data, the strong coupling constant is determined to be [Formula omitted]. Complementarily, [Formula omitted] is determined together with parton distribution functions of the proton (PDFs) from jet and inclusive DIS data measured by the H1 experiment. The value [Formula omitted] obtained is consistent with the determination from jet data alone. Corrected figures and numerical results are provided and the discussion is adapted accordingly. |
| ArticleNumber | 738 |
| Audience | Academic |
| Author | Contreras, J. G. Gayler, J. Olsson, J. E. Katzy, J. Pitzl, D. Hladkỳ, J. Kiesling, C. Brisson, V. Diaconu, C. Goerlich, L. Chekelian, V. Lipka, K. Pirumov, H. Belousov, A. Meyer, J. Boudry, V. Lange, W. Lebedev, A. Niehues, J. Horisberger, R. Meyer, A. B. Fedotov, A. Bolz, A. Laycock, P. Campbell, A. J. Feltesse, J. Mehta, A. Jung, A. W. Henderson, R. C. W. Favart, L. Kapichine, M. Patel, G. D. Fleischer, M. Dobre, M. Kostka, P. Gehrmann, T. Bylinkin, A. Brandt, G. Buniatyan, A. Bertone, V. Britzger, D. Huss, A. Meyer, H. Jung, H. Avila, K. B. Cantun Fomenko, A. Newman, P. R. Andreev, V. Cvach, J. Eckerlin, G. Cerny, K. Perez, E. Gouzevitch, M. Grindhammer, G. Egli, S. Maxfield, S. J. Kleinwort, C. Greenshaw, T. Currie, J. Nowak, G. Ozerov, D. Huber, F. List, B. List, J. Janssen, X. Baghdasaryan, A. Klein, M. Mikocki, S. Kretzschmar, J. Dainton, J. B. Pascaud, C. Bystritskaya, L. Levonian, S. Hoffmann, D. Gogitidze, N. Haidt, D. Gabathuler, E. Niebuhr, C. Dodonov, V. Martyn, H.-U. Hreus, T. Begzsuren, K. Ghazaryan, S. Grab, C. Petrukhin, A. Krücker, D. Jacquet, M. Greben |
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| CitedBy_id | crossref_primary_10_1103_PhysRevD_111_034023 crossref_primary_10_1103_knrv_2r3t crossref_primary_10_1103_1djw_8zrh |
| Cites_doi | 10.1140/epjc/s10052-017-5314-7 10.1140/epjc/s10052-013-2332-y 10.1088/1674-1137/40/10/100001 10.1103/PhysRevLett.117.042001 10.1103/PhysRevD.86.054009 10.1140/epjc/s10052-017-4717-9 10.1007/JHEP03(2017)156 10.1007/JHEP07(2017)018 10.1088/1126-6708/2008/02/040 10.1140/epjc/s10052-015-3710-4 10.1016/j.physletb.2011.11.053 10.1103/PhysRevD.79.074023 10.1016/j.nuclphysbps.2016.12.028 10.1007/JHEP07(2016)133 10.1140/epjc/s10052-015-3397-6 10.1140/epjc/s10052-015-3318-8 10.1140/epjc/s10052-011-1733-z 10.1140/epjc/s10052-014-3046-5 10.1016/j.nuclphysb.2007.03.035 |
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| Copyright | COPYRIGHT 2021 Springer |
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| DOI | 10.1140/epjc/s10052-021-09394-0 |
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| References | J Blümlein (9394_CR16) 2007; 774 A Gehrmann-De Ridder (9394_CR2) 2016; 1607 9394_CR13 9394_CR10 9394_CR21 9394_CR11 9394_CR17 9394_CR9 9394_CR15 9394_CR7 9394_CR8 9394_CR5 9394_CR6 S Alekhin (9394_CR14) 2012; 86 9394_CR4 A Buckley (9394_CR22) 2015; 75 9394_CR1 RD Ball (9394_CR19) 2012; 707 P Jimenez-Delgado (9394_CR18) 2009; 79 G Dissertori (9394_CR12) 2008; 0802 J Currie (9394_CR3) 2016; 117 LA Harland-Lang (9394_CR20) 2015; 75 |
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| Snippet | The determination of the strong coupling constant
$$\alpha _{\mathrm{s}} (m_{\mathrm{Z}})$$
α
s
(
m
Z
)
from H1 inclusive and dijet cross section data [1]... The determination of the strong coupling constant [Formula omitted] from H1 inclusive and dijet cross section data [1 (See CR1)] exploits perturbative QCD... |
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| SubjectTerms | Distribution (Probability theory) Nuclear energy |
| Title | Erratum to: Determination of the strong coupling constant $${{\varvec{\alpha _{\mathrm{s}} (m_{\mathrm{Z}})}}}$$ in next-to-next-to-leading order QCD using H1 jet cross section measurements |
| Volume | 81 |
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