Javascript must be enabled to continue!
Impact of jet-production data on the next-to-next-to-leading-order determination of HERAPDF2.0 parton distributions
View through CrossRef
AbstractThe HERAPDF2.0 ensemble of parton distribution functions (PDFs) was introduced in 2015. The final stage is presented, a next-to-next-to-leading-order (NNLO) analysis of the HERA data on inclusive deep inelastic ep scattering together with jet data as published by the H1 and ZEUS collaborations. A perturbative QCD fit, simultaneously of $$\alpha _s(M_Z^2)$$
α
s
(
M
Z
2
)
and the PDFs, was performed with the result $$\alpha _s(M_Z^2)= 0.1156 \pm 0.0011~\mathrm{(exp)}~ ^{+0.0001}_{-0.0002}~ \mathrm{(model}$$
α
s
(
M
Z
2
)
=
0.1156
±
0.0011
(
exp
)
-
0.0002
+
0.0001
(
model
$$\mathrm{+ parameterisation)}~ \pm 0.0029~\mathrm{(scale)}$$
+
parameterisation
)
±
0.0029
(
scale
)
. The PDF sets of HERAPDF2.0Jets NNLO were determined with separate fits using two fixed values of $$\alpha _s(M_Z^2)$$
α
s
(
M
Z
2
)
, $$\alpha _s(M_Z^2)=0.1155$$
α
s
(
M
Z
2
)
=
0.1155
and 0.118, since the latter value was already chosen for the published HERAPDF2.0 NNLO analysis based on HERA inclusive DIS data only. The different sets of PDFs are presented, evaluated and compared. The consistency of the PDFs determined with and without the jet data demonstrates the consistency of HERA inclusive and jet-production cross-section data. The inclusion of the jet data reduced the uncertainty on the gluon PDF. Predictions based on the PDFs of HERAPDF2.0Jets NNLO give an excellent description of the jet-production data used as input.
Springer Science and Business Media LLC
I. Abt
R. Aggarwal
V. Andreev
M. Arratia
V. Aushev
A. Baghdasaryan
A. Baty
K. Begzsuren
O. Behnke
A. Belousov
A. Bertolin
I. Bloch
V. Boudry
G. Brandt
I. Brock
N. H. Brook
R. Brugnera
A. Bruni
A. Buniatyan
P. J. Bussey
L. Bystritskaya
A. Caldwell
A. J. Campbell
K. B. Cantun Avila
C. D. Catterall
K. Cerny
V. Chekelian
Z. Chen
J. Chwastowski
J. Ciborowski
R. Ciesielski
J. G. Contreras
A. M. Cooper-Sarkar
M. Corradi
L. Cunqueiro Mendez
J. Currie
J. Cvach
J. B. Dainton
K. Daum
R. K. Dementiev
A. Deshpande
C. Diaconu
S. Dusini
G. Eckerlin
S. Egli
E. Elsen
L. Favart
A. Fedotov
J. Feltesse
J. Ferrando
M. Fleischer
A. Fomenko
B. Foster
C. Gal
E. Gallo
D. Gangadharan
A. Garfagnini
J. Gayler
A. Gehrmann-De Ridder
T. Gehrmann
A. Geiser
L. K. Gladilin
E. W. N. Glover
L. Goerlich
N. Gogitidze
Yu. A. Golubkov
M. Gouzevitch
C. Grab
T. Greenshaw
G. Grindhammer
G. Grzelak
C. Gwenlan
D. Haidt
R. C. W. Henderson
J. Hladký
D. Hochman
D. Hoffmann
R. Horisberger
T. Hreus
F. Huber
A. Huss
P. M. Jacobs
M. Jacquet
T. Janssen
N. Z. Jomhari
A. W. Jung
H. Jung
I. Kadenko
M. Kapichine
U. Karshon
J. Katzy
P. Kaur
C. Kiesling
R. Klanner
M. Klein
U. Klein
C. Kleinwort
H. T. Klest
R. Kogler
I. A. Korzhavina
P. Kostka
N. Kovalchuk
J. Kretzschmar
D. Krücker
K. Krüger
M. Kuze
M. P. J. Landon
W. Lange
P. Laycock
S. H. Lee
B. B. Levchenko
S. Levonian
A. Levy
W. Li
J. Lin
K. Lipka
B. List
J. List
B. Lobodzinski
B. Löhr
E. Lohrmann
O. R. Long
A. Longhin
F. Lorkowski
O. Yu. Lukina
I. Makarenko
E. Malinovski
J. Malka
H.-U. Martyn
S. Masciocchi
S. J. Maxfield
A. Mehta
A. B. Meyer
J. Meyer
S. Mikocki
V. M. Mikuni
M. M. Mondal
T. Morgan
A. Morozov
K. Müller
B. Nachman
K. Nagano
J. D. Nam
Th. Naumann
P. R. Newman
C. Niebuhr
J. Niehues
G. Nowak
J. E. Olsson
Yu. Onishchuk
D. Ozerov
S. Park
C. Pascaud
G. D. Patel
E. Paul
E. Perez
A. Petrukhin
I. Picuric
I. Pidhurskyi
J. Pires
D. Pitzl
R. Polifka
A. Polini
S. Preins
M. Przybycień
A. Quintero
K. Rabbertz
V. Radescu
N. Raicevic
T. Ravdandorj
P. Reimer
E. Rizvi
P. Robmann
R. Roosen
A. Rostovtsev
M. Rotaru
M. Ruspa
D. P. C. Sankey
M. Sauter
E. Sauvan
S. Schmitt
B. A. Schmookler
U. Schneekloth
L. Schoeffel
A. Schöning
T. Schörner-Sadenius
F. Sefkow
I. Selyuzhenkov
M. Shchedrolosiev
L. M. Shcheglova
S. Shushkevich
I. O. Skillicorn
W. Słomiński
A. Solano
Y. Soloviev
P. Sopicki
D. South
V. Spaskov
A. Specka
L. Stanco
M. Steder
N. Stefaniuk
B. Stella
U. Straumann
C. Sun
B. Surrow
M. R. Sutton
T. Sykora
P. D. Thompson
K. Tokushuku
D. Traynor
B. Tseepeldorj
Z. Tu
O. Turkot
T. Tymieniecka
A. Valkárová
C. Vallée
P. Van Mechelen
A. Verbytskyi
W. A. T. Wan Abdullah
D. Wegener
K. Wichmann
M. Wing
E. Wünsch
S. Yamada
Y. Yamazaki
J. Žáček
A. F. Żarnecki
O. Zenaiev
J. Zhang
Z. Zhang
R. Žlebčík
H. Zohrabyan
F. Zomer
Title: Impact of jet-production data on the next-to-next-to-leading-order determination of HERAPDF2.0 parton distributions
Description:
AbstractThe HERAPDF2.
0 ensemble of parton distribution functions (PDFs) was introduced in 2015.
The final stage is presented, a next-to-next-to-leading-order (NNLO) analysis of the HERA data on inclusive deep inelastic ep scattering together with jet data as published by the H1 and ZEUS collaborations.
A perturbative QCD fit, simultaneously of $$\alpha _s(M_Z^2)$$
α
s
(
M
Z
2
)
and the PDFs, was performed with the result $$\alpha _s(M_Z^2)= 0.
1156 \pm 0.
0011~\mathrm{(exp)}~ ^{+0.
0001}_{-0.
0002}~ \mathrm{(model}$$
α
s
(
M
Z
2
)
=
0.
1156
±
0.
0011
(
exp
)
-
0.
0002
+
0.
0001
(
model
$$\mathrm{+ parameterisation)}~ \pm 0.
0029~\mathrm{(scale)}$$
+
parameterisation
)
±
0.
0029
(
scale
)
.
The PDF sets of HERAPDF2.
0Jets NNLO were determined with separate fits using two fixed values of $$\alpha _s(M_Z^2)$$
α
s
(
M
Z
2
)
, $$\alpha _s(M_Z^2)=0.
1155$$
α
s
(
M
Z
2
)
=
0.
1155
and 0.
118, since the latter value was already chosen for the published HERAPDF2.
0 NNLO analysis based on HERA inclusive DIS data only.
The different sets of PDFs are presented, evaluated and compared.
The consistency of the PDFs determined with and without the jet data demonstrates the consistency of HERA inclusive and jet-production cross-section data.
The inclusion of the jet data reduced the uncertainty on the gluon PDF.
Predictions based on the PDFs of HERAPDF2.
0Jets NNLO give an excellent description of the jet-production data used as input.
Related Results
The azimuthal correlation between the leading jet and the scattered lepton in deep inelastic scattering at HERA
The azimuthal correlation between the leading jet and the scattered lepton in deep inelastic scattering at HERA
Abstract
The azimuthal correlation angle,
$$\Delta \phi $$
Δ
ϕ...
Cavitation in Submerged Water Jet at High Jet Pressure
Cavitation in Submerged Water Jet at High Jet Pressure
Recent industrial applications have unfolded a promising prospect for submerged water jet. Apart from widely acknowledged water jet properties, submerged water jet is characterized...
Measurement of inclusive and leading subjet fragmentation in pp and Pb–Pb collisions at $$ \sqrt{s_{\textrm{NN}}} $$ = 5.02 TeV
Measurement of inclusive and leading subjet fragmentation in pp and Pb–Pb collisions at $$ \sqrt{s_{\textrm{NN}}} $$ = 5.02 TeV
AbstractThis article presents new measurements of the fragmentation properties of jets in both proton–proton (pp) and heavy-ion collisions with the ALICE experiment at the Large Ha...
Study on the image recognition of ammonia ignition process induced by methanol micro-jet
Study on the image recognition of ammonia ignition process induced by methanol micro-jet
<div class="section abstract"><div class="htmlview paragraph">Ammonia is regarded as a possible carbon-free energy source for engines, drawing more and more attention. ...
Passive control of coaxial jet with supersonic primary jet and sonic secondary jet
Passive control of coaxial jet with supersonic primary jet and sonic secondary jet
The mixing enhancement of a coaxial jet with a Mach 1.4 primary jet and sonic secondary jet, at different convective Mach numbers, is presented in this study. Rectangular tabs of a...
“Lavender Haze” in the Airways
“Lavender Haze” in the Airways
Introduction
Taylor Swift has dominated global press in recent years through the success of her Eras Tour, her use of authenticity in branding (Khanal 234), and her choreographed e...
Study of energy flow fluctuations within jets at heavy-ion collisions with ALICE
Study of energy flow fluctuations within jets at heavy-ion collisions with ALICE
This dissertation advances the understanding of the strong nuclear force under extreme conditions akin to those in the early universe by analyzing data from the ALICE detector at C...
Characteristics on drag reduction of bionic jet surface based on earthworm's back orifice jet
Characteristics on drag reduction of bionic jet surface based on earthworm's back orifice jet
In order to reduce the drag reduction of the fluid on the solid wall, based on the biology characteristics of earthworm, the earthworm's back orifice jet characteristic is analyzed...

