Deep Inelastic Structure Functions at two Loops

Anomalous dimension of gluonic operator in polarized deep inelastic scattering at $O(1/N_{f})$

Bennett, J F
Gracey, J A

January 1998

We compute the O(1/N_f) correction to the predominantly gluonic flavour singlet twist-2 anomalous di...

Mellin representations for the heavy flavor contributions to deep inelastic structure functions

Bluemlein, J.
Alekhin, S.I.
Deutsches Elektronen-Synchrotron (DESY), Zeuthen (Germany)

January 2003

We derive semi-analytic expressions for the analytic continuation of the mellin transforms of the he...

The 16th moment of the non-singlet structure functions $F_2(x,Q^2)$ and $F_L(x,Q^2)$ to $O$($\alpha^3_S$)

Blumlein, J.
Vermaseren, J. A. M.

January 2005

We present the results of an analytic next-to–next-to leading order QCD calculation of the non-singl...

First results for three-loop deep-inelastic structure functions in QCD

Vermaseren, Jos A M
Moch, S
Vogt, A

November 2002

As a first step towards the complete calculation of deep-inelastic scattering at third order of mass...

Two-loop operator matrix elements calculated up to finite terms

Matiounine, Y
Smith, J
van Neerven, W L

January 1998

We present the two-loop corrected operator matrix elements calculated in N-dimensional regularizatio...

Non-Singlet Structure Functions at Three Loops: Fermionic Contributions

Moch, S
Vermaseren, Jos A M
Vogt, A

September 2002

We compute the fermionic (n_f) contributions to the flavour non-singlet structure functions in unpol...

The 3-loop pure singlet heavy flavor contributions to the structure function F2(x,Q2) and the anomalous dimension

Ablinger, J.
Behring, A.
Blümlein, J.
De Freitas, A.
von Manteuffel, A.
Schneider, C.

January 2015

AbstractThe pure singlet asymptotic heavy flavor corrections to 3-loop order for the deep-inelastic ...

The interplay between perturbative QCD and power corrections: the description of scaling or automodelling limit violation in deep-inelastic scattering

Kataev, A L
Parente, G
Sidorov, A V

January 2000

The summary of the results of our next-to-next-to-leading fits of Tevatron experimental data for $xF...

Impact of the three-loop corrections on the QCD analysis of the deep-inelastic scattering data

Alekhin, S.I

October 2001

AbstractWe perform the analysis of the existing inclusive deep inelastic scattering (DIS) data withi...

Mathematics for structure functions

Vermaseren, Jos A M
Moch, S

January 2000

We show some of the mathematics that is being developed for the computation of deep inelastic struct...

Analytic continuation of the Mellin moments of deep inelastic structure functions

Kotikov, A V
Velizhanin, V N

January 2005

We derive the analytic continuation of the Mellin moments of deep inelastic structure functions at t...

Computing of Charged Current DIS at three loops

Rogal, M
Moch, S

June 2007

We report on our recent results for deep-inelastic neutrino-proton scattering. We have computed the ...

The 3-loop non-singlet heavy flavor contributions and anomalous dimensions for the structure function F2(x,Q2) and transversity

Ablinger, J.(Research Institute for Symbolic Computation (RISC), Johannes Kepler University, Altenbergerstraße 69, Linz, A-4040, Austria)
Behring, A.(Deutsches Elektronen-Synchrotron, DESY, Platanenallee 6, Zeuthen, D-15738, Germany)
Blümlein, J.(Deutsches Elektronen-Synchrotron, DESY, Platanenallee 6, Zeuthen, D-15738, Germany)
De Freitas, A.(Deutsches Elektronen-Synchrotron, DESY, Platanenallee 6, Zeuthen, D-15738, Germany)
Hasselhuhn, A.(Research Institute for Symbolic Computation (RISC), Johannes Kepler University, Altenbergerstraße 69, Linz, A-4040, Austria)
von Manteuffel, A.(PRISMA Cluster of Excellence and Institute of Physics, J. Gutenberg University, Mainz, D-55099, Germany)
Round, M.(Research Institute for Symbolic Computation (RISC), Johannes Kepler University, Altenbergerstraße 69, Linz, A-4040, Austria)
Schneider, C.(Research Institute for Symbolic Computation (RISC), Johannes Kepler University, Altenbergerstraße 69, Linz, A-4040, Austria)
Wißbrock, F.(Research Institute for Symbolic Computation (RISC), Johannes Kepler University, Altenbergerstraße 69, Linz, A-4040, Austria)

October 2014

We calculate the massive flavor non-singlet Wilson coefficient for the heavy flavor contributions to...

The massless three-loop Wilson coefficients for the deep-inelastic structure functions F 2 , F L , xF 3 and g 1

J. Blümlein
P. Marquard
C. Schneider
K. Schönwald

November 2022

Abstract We calculate the massless unpolarized Wilson coefficients for deeply inelastic scattering f...

The massless three-loop Wilson coefficients for the deep-inelastic structure functions $F_2, F_L, xF_3$ and $g_1$

Blümlein, J.
Marquard, P.
Schneider, C.
Schönwald, K.

January 2022

We calculate the massless unpolarized Wilson coefficients for deeply inelastic scattering for the st...

Anomalous dimension of gluonic operator in polarized deep inelastic scattering at $O(1/N_{f})$

Bennett, J F
Gracey, J A

January 1998

We compute the O(1/N_f) correction to the predominantly gluonic flavour singlet twist-2 anomalous di...

Mellin representations for the heavy flavor contributions to deep inelastic structure functions

Bluemlein, J.
Alekhin, S.I.
Deutsches Elektronen-Synchrotron (DESY), Zeuthen (Germany)

January 2003

We derive semi-analytic expressions for the analytic continuation of the mellin transforms of the he...

The 16th moment of the non-singlet structure functions $F_2(x,Q^2)$ and $F_L(x,Q^2)$ to $O$($\alpha^3_S$)

Blumlein, J.
Vermaseren, J. A. M.

January 2005

We present the results of an analytic next-to–next-to leading order QCD calculation of the non-singl...

First results for three-loop deep-inelastic structure functions in QCD

Vermaseren, Jos A M
Moch, S
Vogt, A

November 2002

As a first step towards the complete calculation of deep-inelastic scattering at third order of mass...

Two-loop operator matrix elements calculated up to finite terms

Matiounine, Y
Smith, J
van Neerven, W L

January 1998

We present the two-loop corrected operator matrix elements calculated in N-dimensional regularizatio...

Non-Singlet Structure Functions at Three Loops: Fermionic Contributions

Moch, S
Vermaseren, Jos A M
Vogt, A

September 2002

We compute the fermionic (n_f) contributions to the flavour non-singlet structure functions in unpol...

The 3-loop pure singlet heavy flavor contributions to the structure function F2(x,Q2) and the anomalous dimension

Ablinger, J.
Behring, A.
Blümlein, J.
De Freitas, A.
von Manteuffel, A.
Schneider, C.

January 2015

AbstractThe pure singlet asymptotic heavy flavor corrections to 3-loop order for the deep-inelastic ...

The interplay between perturbative QCD and power corrections: the description of scaling or automodelling limit violation in deep-inelastic scattering

Kataev, A L
Parente, G
Sidorov, A V

January 2000

The summary of the results of our next-to-next-to-leading fits of Tevatron experimental data for $xF...

Impact of the three-loop corrections on the QCD analysis of the deep-inelastic scattering data

Alekhin, S.I

October 2001

AbstractWe perform the analysis of the existing inclusive deep inelastic scattering (DIS) data withi...

Mathematics for structure functions

Vermaseren, Jos A M
Moch, S

January 2000

We show some of the mathematics that is being developed for the computation of deep inelastic struct...

Analytic continuation of the Mellin moments of deep inelastic structure functions

Kotikov, A V
Velizhanin, V N

January 2005

We derive the analytic continuation of the Mellin moments of deep inelastic structure functions at t...

Computing of Charged Current DIS at three loops

Rogal, M
Moch, S

June 2007

We report on our recent results for deep-inelastic neutrino-proton scattering. We have computed the ...

The 3-loop non-singlet heavy flavor contributions and anomalous dimensions for the structure function F2(x,Q2) and transversity

Ablinger, J.(Research Institute for Symbolic Computation (RISC), Johannes Kepler University, Altenbergerstraße 69, Linz, A-4040, Austria)
Behring, A.(Deutsches Elektronen-Synchrotron, DESY, Platanenallee 6, Zeuthen, D-15738, Germany)
Blümlein, J.(Deutsches Elektronen-Synchrotron, DESY, Platanenallee 6, Zeuthen, D-15738, Germany)
De Freitas, A.(Deutsches Elektronen-Synchrotron, DESY, Platanenallee 6, Zeuthen, D-15738, Germany)
Hasselhuhn, A.(Research Institute for Symbolic Computation (RISC), Johannes Kepler University, Altenbergerstraße 69, Linz, A-4040, Austria)
von Manteuffel, A.(PRISMA Cluster of Excellence and Institute of Physics, J. Gutenberg University, Mainz, D-55099, Germany)
Round, M.(Research Institute for Symbolic Computation (RISC), Johannes Kepler University, Altenbergerstraße 69, Linz, A-4040, Austria)
Schneider, C.(Research Institute for Symbolic Computation (RISC), Johannes Kepler University, Altenbergerstraße 69, Linz, A-4040, Austria)
Wißbrock, F.(Research Institute for Symbolic Computation (RISC), Johannes Kepler University, Altenbergerstraße 69, Linz, A-4040, Austria)

October 2014

We calculate the massive flavor non-singlet Wilson coefficient for the heavy flavor contributions to...

The massless three-loop Wilson coefficients for the deep-inelastic structure functions F 2 , F L , xF 3 and g 1

J. Blümlein
P. Marquard
C. Schneider
K. Schönwald

November 2022

Abstract We calculate the massless unpolarized Wilson coefficients for deeply inelastic scattering f...

The massless three-loop Wilson coefficients for the deep-inelastic structure functions $F_2, F_L, xF_3$ and $g_1$

Blümlein, J.
Marquard, P.
Schneider, C.
Schönwald, K.

January 2022

We calculate the massless unpolarized Wilson coefficients for deeply inelastic scattering for the st...

Anomalous dimension of gluonic operator in polarized deep inelastic scattering at $O(1/N_{f})$

Bennett, J F
Gracey, J A

January 1998

We compute the O(1/N_f) correction to the predominantly gluonic flavour singlet twist-2 anomalous di...

Mellin representations for the heavy flavor contributions to deep inelastic structure functions

Bluemlein, J.
Alekhin, S.I.
Deutsches Elektronen-Synchrotron (DESY), Zeuthen (Germany)

January 2003

We derive semi-analytic expressions for the analytic continuation of the mellin transforms of the he...

The 16th moment of the non-singlet structure functions $F_2(x,Q^2)$ and $F_L(x,Q^2)$ to $O$($\alpha^3_S$)

Blumlein, J.
Vermaseren, J. A. M.

January 2005

We present the results of an analytic next-to–next-to leading order QCD calculation of the non-singl...

Deep Inelastic Structure Functions at two Loops

Abstract

Extracted data

Deep Inelastic Structure Functions at two Loops

Abstract

Extracted data

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