Can MS ¯ $$ \overline\mathrm{MS}} $$ parton distributions be negative?

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Can MS ¯ $$ \overline\mathrm{MS}} $$ parton distributions be negative? ; volume:2020 ; number:11 ; day:24 ; month:11 ; year:2020 ; pages:1-30 ; date:11.2020
Journal of high energy physics ; 2020, Heft 11 (24.11.2020), 1-30, 11.2020

Creator: Candido, Alessandro
Forte, Stefano
Hekhorn, Felix

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP11(2020)129

URN: urn:nbn:de:101:1-2021010421343049925041

Rights: Open Access; Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 15.08.2025, 7:23 AM CEST

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Candido, Alessandro
Forte, Stefano
Hekhorn, Felix
SpringerLink (Online service)

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Charmonium-like resonances with JPC = 0++, 2++ in coupled D D ¯ $$ \mathrmD}\overline{\mathrm{D}} $$ , D s D ¯ s $$ \mathrm{D}}_{\mathrm{s}}{\overline{\mathrm{D}}}_{\mathrm{s}} $$ scattering on the lattice

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$T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ and LST$

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$Quark mass anomalous dimension and Λ MS ¯ $$ \varLambda}_{\overline{\mathrm{MS}}} $$ from the twisted mass Dirac operator spectrum$

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$T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed nonlinear Schrödinger$

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$Heavy-flavor hadro-production with heavy-quark masses renormalized in the MS ¯ $$ \overline\mathrm{MS}} $$ , MSR and on-shell schemes$

Heavy-flavor hadro-production with heavy-quark masses renormalized in the MS ¯ $$ \overline\mathrm{MS}} $$ , MSR and on-shell schemes

Charmonium-like resonances with JPC = 0++, 2++ in coupled D D ¯ $$ \mathrmD}\overline{\mathrm{D}} $$ , D s D ¯ s $$ \mathrm{D}}_{\mathrm{s}}{\overline{\mathrm{D}}}_{\mathrm{s}} $$ scattering on the lattice

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Can MS ¯ $$ \overline\mathrm{MS}} $$ parton distributions be negative?

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Other Objects (12)

On the positivity of $$\overline\textrm{MS}}$$ MS ¯ parton distributions

P-wave quarkonium wavefunctions at the origin in the MS ¯ $$ \overline\mathrm{MS}} $$ scheme

Gauge-independent M S ¯ $$ \overline\mathrm{MS}} $$ renormalization in the 2HDM

Top-quark pair hadroproduction at NNLO: differential predictions with the MS ¯ $$ \overline\mathrm{MS}} $$ mass

Entanglement entropy for T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ , J T ¯ $$ \mathrmJ}\overline{\mathrm{T}} $$ , T J ¯ $$ \mathrmT}\overline{\mathrm{J}} $$ deformed holographic CFT

Thermodynamics of T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ , J T ¯ $$ \mathrmJ}\overline{\mathrm{T}} $$ , T J ¯ $$ \mathrmT}\overline{\mathrm{J}} $$ deformed conformal field theories

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ and LST

Quark mass anomalous dimension and Λ MS ¯ $$ \varLambda}_{\overline{\mathrm{MS}}} $$ from the twisted mass Dirac operator spectrum

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed nonlinear Schrödinger

Generalized parton distributions

Heavy-flavor hadro-production with heavy-quark masses renormalized in the MS ¯ $$ \overline\mathrm{MS}} $$ , MSR and on-shell schemes

Charmonium-like resonances with JPC = 0++, 2++ in coupled D D ¯ $$ \mathrmD}\overline{\mathrm{D}} $$ , D s D ¯ s $$ \mathrm{D}}_{\mathrm{s}}{\overline{\mathrm{D}}}_{\mathrm{s}} $$ scattering on the lattice

On the positivity of $$\overline\textrm{MS}}$$ MS ¯ parton distributions

P-wave quarkonium wavefunctions at the origin in the MS ¯ $$ \overline\mathrm{MS}} $$ scheme

Gauge-independent M S ¯ $$ \overline\mathrm{MS}} $$ renormalization in the 2HDM

Top-quark pair hadroproduction at NNLO: differential predictions with the MS ¯ $$ \overline\mathrm{MS}} $$ mass

Entanglement entropy for T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ , J T ¯ $$ \mathrmJ}\overline{\mathrm{T}} $$ , T J ¯ $$ \mathrmT}\overline{\mathrm{J}} $$ deformed holographic CFT

Thermodynamics of T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ , J T ¯ $$ \mathrmJ}\overline{\mathrm{T}} $$ , T J ¯ $$ \mathrmT}\overline{\mathrm{J}} $$ deformed conformal field theories

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ and LST

Quark mass anomalous dimension and Λ MS ¯ $$ \varLambda}_{\overline{\mathrm{MS}}} $$ from the twisted mass Dirac operator spectrum

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed nonlinear Schrödinger

Generalized parton distributions

Heavy-flavor hadro-production with heavy-quark masses renormalized in the MS ¯ $$ \overline\mathrm{MS}} $$ , MSR and on-shell schemes

Charmonium-like resonances with JPC = 0++, 2++ in coupled D D ¯ $$ \mathrmD}\overline{\mathrm{D}} $$ , D s D ¯ s $$ \mathrm{D}}_{\mathrm{s}}{\overline{\mathrm{D}}}_{\mathrm{s}} $$ scattering on the lattice

On the positivity of $$\overline\textrm{MS}}$$ MS ¯ parton distributions

P-wave quarkonium wavefunctions at the origin in the MS ¯ $$ \overline\mathrm{MS}} $$ scheme

Gauge-independent M S ¯ $$ \overline\mathrm{MS}} $$ renormalization in the 2HDM

Top-quark pair hadroproduction at NNLO: differential predictions with the MS ¯ $$ \overline\mathrm{MS}} $$ mass

Entanglement entropy for T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ , J T ¯ $$ \mathrmJ}\overline{\mathrm{T}} $$ , T J ¯ $$ \mathrmT}\overline{\mathrm{J}} $$ deformed holographic CFT

Thermodynamics of T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ , J T ¯ $$ \mathrmJ}\overline{\mathrm{T}} $$ , T J ¯ $$ \mathrmT}\overline{\mathrm{J}} $$ deformed conformal field theories

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ and LST

Quark mass anomalous dimension and Λ MS ¯ $$ \varLambda}_{\overline{\mathrm{MS}}} $$ from the twisted mass Dirac operator spectrum

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed nonlinear Schrödinger

Generalized parton distributions

Heavy-flavor hadro-production with heavy-quark masses renormalized in the MS ¯ $$ \overline\mathrm{MS}} $$ , MSR and on-shell schemes

Charmonium-like resonances with JPC = 0++, 2++ in coupled D D ¯ $$ \mathrmD}\overline{\mathrm{D}} $$ , D s D ¯ s $$ \mathrm{D}}_{\mathrm{s}}{\overline{\mathrm{D}}}_{\mathrm{s}} $$ scattering on the lattice

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