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Sickle particulars of microparticles

Blood, 2020-07, Vol.136 (2), p.154-155

Kato, Gregory J.

2020

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P01-06: Applying a systematic approach to the development of evidence-based adverse outcome pathways (AOPs) for regulatory use

Toxicology letters, 2023-09, Vol.384, p.S75-S75

2023

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Host genetics and geography influence microbiome composition in the sponge Ircinia campana

The Journal of animal ecology, 2019-11, Vol.88 (11), p.1684-1695

2019

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Metoprolol and propranolol in migraine prophylaxis: a double-blind multicentre study

Acta neurologica Scandinavica, 1984-09, Vol.70 (3), p.160-168

1984

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Subarachnoidal hemorrhage in a perspective of 20 years

Läkartidningen, 1995-09, Vol.92 (38), p.3433

1995

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THYMIC CYST OF THE NECK. REPORT OF A CASE

Acta pathologica et microbiologica Scandinavica, 1963, Vol.59, p.45-50

1963

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The three-loop splitting functions Pqg(2) and Pgg(2,NF)

Nuclear physics. B, 2017-09, Vol.922 (C), p.1-40

2017

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Glutathionylation of the Active Site Cysteines of Peroxiredoxin 2 and Recycling by Glutaredoxin

The Journal of biological chemistry, 2016-02, Vol.291 (6), p.3053-3062

2016

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

Nuclear physics. B, 2015-01, Vol.890, p.48-151

2015

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The non-first-order-factorizable contributions to the three-loop single-mass operator matrix elements AQg(3) and ΔAQg(3)

Physics letters. B, 2024-07, Vol.854, p.138713, Article 138713

2024

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The polarized three-loop anomalous dimensions from on-shell massive operator matrix elements

Nuclear physics. B, 2019-11, Vol.948, p.114753, Article 114753

2019

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The three-loop single mass polarized pure singlet operator matrix element

Nuclear physics. B, 2020-04, Vol.953, p.114945, Article 114945

2020

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Heavy quark form factors at two loops

Physical review. D, 2018-05, Vol.97 (9), Article 094022

2018

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The polarized transition matrix element Agq(N) of the variable flavor number scheme at O(αs3)

Nuclear physics. B, 2021-03, Vol.964, p.115331, Article 115331

2021

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

Nuclear physics. B, 2014-09, Vol.886 (C), p.733-823

2014

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Calculating three loop ladder and V-topologies for massive operator matrix elements by computer algebra

Computer physics communications, 2016-05, Vol.202, p.33-112

2016

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Clinical Implications of Rabphillin-3A-Like Gene Alterations in Breast Cancer

PloS one, 2015-06, Vol.10 (6), p.e0129216-e0129216

2015

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The unpolarized and polarized single-mass three-loop heavy flavor operator matrix elements Agg,Q and ∆Agg,Q

The journal of high energy physics, 2022-12, Vol.2022 (12), p.134, Article 134

2022

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The first–order factorizable contributions to the three–loop massive operator matrix elements AQg(3) and ΔAQg(3)

Nuclear physics. B, 2024-02, Vol.999, p.116427, Article 116427

2024

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The 3-loop non-singlet heavy flavor contributions to the structure function g1(x,Q2) at large momentum transfer

Nuclear physics. B, 2015-08, Vol.897 (C), p.612-644

2015

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Asymptotic 3-loop heavy flavor corrections to the charged current structure functions FLW+−W−(x,Q2) and F2W+−W−(x,Q2)

Physical review. D, 2016-12, Vol.94 (11)

2016

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Proteomic identification of 3-nitrotyrosine-containing rat cardiac proteins: effects of biological aging

American journal of physiology. Heart and circulatory physiology, 2005-01, Vol.288 (1), p.H371-H381

2005

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The non-first-order-factorizable contributions to the three-loop single-mass operator matrix elements A Q g ( 3 ) and Δ A Q g ( 3 )

Physics letters. B, 2024-07, Vol.854, p.138713, Article 138713

2024

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The first–order factorizable contributions to the three–loop massive operator matrix elements A Q g ( 3 ) and Δ A Q g ( 3 )

Nuclear physics. B, 2024-02, Vol.999, p.116427, Article 116427

2024

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The 3-loop pure singlet heavy flavor contributions to the structure function F 2 ( x , Q 2 ) and the anomalous dimension

Nuclear physics. B, 2015-01, Vol.890, p.48-151

2015

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Sickle particulars of microparticles

P01-06: Applying a systematic approach to the development of evidence-based adverse outcome pathways (AOPs) for regulatory use

Host genetics and geography influence microbiome composition in the sponge Ircinia campana

Metoprolol and propranolol in migraine prophylaxis: a double-blind multicentre study

Subarachnoidal hemorrhage in a perspective of 20 years

THYMIC CYST OF THE NECK. REPORT OF A CASE

The three-loop splitting functions Pqg(2) and Pgg(2,NF)

Glutathionylation of the Active Site Cysteines of Peroxiredoxin 2 and Recycling by Glutaredoxin

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

The non-first-order-factorizable contributions to the three-loop single-mass operator matrix elements AQg(3) and ΔAQg(3)

The polarized three-loop anomalous dimensions from on-shell massive operator matrix elements

The three-loop single mass polarized pure singlet operator matrix element

Heavy quark form factors at two loops

The polarized transition matrix element Agq(N) of the variable flavor number scheme at O(αs3)

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

Calculating three loop ladder and V-topologies for massive operator matrix elements by computer algebra

Clinical Implications of Rabphillin-3A-Like Gene Alterations in Breast Cancer

The unpolarized and polarized single-mass three-loop heavy flavor operator matrix elements Agg,Q and ∆Agg,Q

The first–order factorizable contributions to the three–loop massive operator matrix elements AQg(3) and ΔAQg(3)

The 3-loop non-singlet heavy flavor contributions to the structure function g1(x,Q2) at large momentum transfer

Asymptotic 3-loop heavy flavor corrections to the charged current structure functions FLW+−W−(x,Q2) and F2W+−W−(x,Q2)

Proteomic identification of 3-nitrotyrosine-containing rat cardiac proteins: effects of biological aging

The non-first-order-factorizable contributions to the three-loop single-mass operator matrix elements A Q g ( 3 ) and Δ A Q g ( 3 )

The first–order factorizable contributions to the three–loop massive operator matrix elements A Q g ( 3 ) and Δ A Q g ( 3 )

The 3-loop pure singlet heavy flavor contributions to the structure function F 2 ( x , Q 2 ) and the anomalous dimension

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