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The Matrix Element Method at next-to-leading order QCD for hadronic collisions: single top-quark production at the LHC as an example application

The journal of high energy physics, 2018-05, Vol.2018 (5), p.1-67, Article 141

2018

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Numerical evaluation of virtual corrections to multi-jet production in massless QCD

Computer physics communications, 2013-08, Vol.184 (8), p.1981-1998

2013

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Maximizing the spin correlation of top quark pairs produced at the large hadron collider

Physics letters. B, 2005-03, Vol.609 (3-4), p.271-276

Uwer, Peter

2005

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Nested sums, expansion of transcendental functions, and multiscale multiloop integrals

Journal of mathematical physics, 2002-06, Vol.43 (6), p.3363-3386

2002

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Extending the Matrix Element Method beyond the Born approximation: calculating event weights at next-to-leading order accuracy

The journal of high energy physics, 2015-09, Vol.2015 (9), p.1-35, Article 83

2015

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Determination of the top-quark mass from top-quark pair events with the matrix element method at next-to-leading order: Potential and prospects

Physical review. D, 2023-04, Vol.107 (7), Article 076013

2023

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Matrix element method at NLO for (anti-) kt-jet algorithms

Physical review. D, 2019-10, Vol.100 (7), p.076010-1

2019

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Matrix element method at NLO for (anti-) k t -jet algorithms

Physical review. D, 2019-10, Vol.100 (7), Article 076010

2019

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XSummer- Transcendental functions and symbolic summation in Form

Computer physics communications, 2006-05, Vol.174 (9), p.759-770

2006

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Top-quark physics at colliders

Nuclear and particle physics proceedings, 2015-04, Vol.261-262, p.414-442

2015

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Hadronic top-quark pair-production with one jet and parton showering

The journal of high energy physics, 2012, Vol.2012 (1), Article 137

2012

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Phenomenology of tt¯j + X production at the LHC

The journal of high energy physics, 2022-05, Vol.2022 (5), p.146

2022

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Phenomenology of $$ t\overline{t}j $$ + X production at the LHC

The journal of high energy physics, 2022-05, Vol.2022 (5), Article 146

2022

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Next-to-leading order QCD corrections for single top-quark production in association with two jets

Physical review. D, 2020-01, Vol.101 (1), p.1, Article 016013

2020

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Top quark pair production and decay at hadron colliders

Nuclear physics. B, 2004-07, Vol.690 (1), p.81-137

2004

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Next-to-leading order QCD corrections and massive quarks in e+e− → 3 jets

Nuclear physics. B, 1998-03, Vol.515 (1-2), p.279-320

1998

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Next-to-leading order QCD corrections to five jet production at the LHC

Physical review. D, Particles, fields, gravitation, and cosmology, 2014-02, Vol.89 (3), Article 034019

2014

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The Matrix Element Method at Next-to-leading Order Accuracy

Acta physica Polonica, B, 2015-11, Vol.46 (11), p.2143

2015

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Spin density matrix of top quark pairs produced in electron-positron annihilation including QCD radiative corrections

Physical review. D, Particles and fields, 1999-01, Vol.59 (1), Article 014001

1999

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One-loop splitting amplitudes in gauge theory

Nuclear physics. B, 1999-12, Vol.563 (1), p.477-505

1999

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QCD-corrected spin analysing power of jets in decays of polarized top quarks

Physics letters. B, 2002-07, Vol.539 (3), p.235-241

2002

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Transverse polarization of top quark pairs at the Tevatron and the Large Hadron Collider

Physics letters. B, 1996-01, Vol.368 (1), p.153-162

1996

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Phenomenology of t t ¯ j $$ t\overline{t}j $$ + X production at the LHC

The journal of high energy physics, 2022-05, Vol.2022 (5), p.1-63

2022

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NLO QCD corrections to multi-jet production at the LHC with a centre-of-mass energy of s=8 TeV

Physics letters. B, 2013-01, Vol.718 (3), p.965-978

2013

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NLO QCD corrections to multi-jet production at the LHC with a centre-of-mass energy of

Physics letters. B, 2013-01, Vol.718 (3), p.965-978

2013

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The Matrix Element Method at next-to-leading order QCD for hadronic collisions: single top-quark production at the LHC as an example application

Numerical evaluation of virtual corrections to multi-jet production in massless QCD

Maximizing the spin correlation of top quark pairs produced at the large hadron collider

Nested sums, expansion of transcendental functions, and multiscale multiloop integrals

Extending the Matrix Element Method beyond the Born approximation: calculating event weights at next-to-leading order accuracy

Determination of the top-quark mass from top-quark pair events with the matrix element method at next-to-leading order: Potential and prospects

Matrix element method at NLO for (anti-) kt-jet algorithms

Matrix element method at NLO for (anti-) k t -jet algorithms

XSummer- Transcendental functions and symbolic summation in Form

Top-quark physics at colliders

Hadronic top-quark pair-production with one jet and parton showering

Phenomenology of tt¯j + X production at the LHC

Phenomenology of $$ t\overline{t}j $$ + X production at the LHC

Next-to-leading order QCD corrections for single top-quark production in association with two jets

Top quark pair production and decay at hadron colliders

Next-to-leading order QCD corrections and massive quarks in e+e− → 3 jets

Next-to-leading order QCD corrections to five jet production at the LHC

The Matrix Element Method at Next-to-leading Order Accuracy

Spin density matrix of top quark pairs produced in electron-positron annihilation including QCD radiative corrections

One-loop splitting amplitudes in gauge theory

QCD-corrected spin analysing power of jets in decays of polarized top quarks

Transverse polarization of top quark pairs at the Tevatron and the Large Hadron Collider

Phenomenology of t t ¯ j $$ t\overline{t}j $$ + X production at the LHC

NLO QCD corrections to multi-jet production at the LHC with a centre-of-mass energy of s=8 TeV

NLO QCD corrections to multi-jet production at the LHC with a centre-of-mass energy of

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