FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2309199192> ?p ?o ?g. }

• W2309199192 endingPage "273" @default.
• W2309199192 startingPage "246" @default.
• W2309199192 abstract "We present the first lattice-QCD calculation of the isovector polarized parton distribution functions (both helicity and transversity) using the large-momentum effective field theory (LaMET) approach for direct Bjorken-x dependence. We first review the detailed steps of the procedure in the unpolarized case, then generalize to the helicity and transversity cases. We also derive a new mass-correction formulation for all three cases. We then compare the effects of each finite-momentum correction using lattice data calculated at Mπ≈310MeV. Finally, we discuss the implications of these results for the poorly known antiquark structure and predict the sea-flavor asymmetry in the transversely polarized nucleon." @default.
• W2309199192 created "2016-06-24" @default.
• W2309199192 creator A5006121718 @default.
• W2309199192 creator A5008998774 @default.
• W2309199192 creator A5011816116 @default.
• W2309199192 creator A5048139981 @default.
• W2309199192 creator A5085271541 @default.
• W2309199192 date "2016-10-01" @default.
• W2309199192 modified "2023-10-16" @default.
• W2309199192 title "Nucleon helicity and transversity parton distributions from lattice QCD" @default.
• W2309199192 cites W1503983701 @default.
• W2309199192 cites W1667942757 @default.
• W2309199192 cites W1793279480 @default.
• W2309199192 cites W2019959302 @default.
• W2309199192 cites W2020282049 @default.
• W2309199192 cites W2026804913 @default.
• W2309199192 cites W2031517380 @default.
• W2309199192 cites W2042684163 @default.
• W2309199192 cites W2068552757 @default.
• W2309199192 cites W2073018060 @default.
• W2309199192 cites W2093801425 @default.
• W2309199192 cites W2107310939 @default.
• W2309199192 cites W2115016434 @default.
• W2309199192 cites W2133489387 @default.
• W2309199192 cites W2138291582 @default.
• W2309199192 cites W2141450145 @default.
• W2309199192 cites W2151165908 @default.
• W2309199192 cites W2162659200 @default.
• W2309199192 cites W2281983570 @default.
• W2309199192 cites W3101973675 @default.
• W2309199192 cites W3121823746 @default.
• W2309199192 cites W3122427169 @default.
• W2309199192 doi "https://doi.org/10.1016/j.nuclphysb.2016.07.033" @default.
• W2309199192 hasPublicationYear "2016" @default.
• W2309199192 type Work @default.
• W2309199192 sameAs 2309199192 @default.
• W2309199192 citedByCount "167" @default.
• W2309199192 countsByYear W23091991922016 @default.
• W2309199192 countsByYear W23091991922017 @default.
• W2309199192 countsByYear W23091991922018 @default.
• W2309199192 countsByYear W23091991922019 @default.
• W2309199192 countsByYear W23091991922020 @default.
• W2309199192 countsByYear W23091991922021 @default.
• W2309199192 countsByYear W23091991922022 @default.
• W2309199192 countsByYear W23091991922023 @default.
• W2309199192 crossrefType "journal-article" @default.
• W2309199192 hasAuthorship W2309199192A5006121718 @default.
• W2309199192 hasAuthorship W2309199192A5008998774 @default.
• W2309199192 hasAuthorship W2309199192A5011816116 @default.
• W2309199192 hasAuthorship W2309199192A5048139981 @default.
• W2309199192 hasAuthorship W2309199192A5085271541 @default.
• W2309199192 hasBestOaLocation W23091991921 @default.
• W2309199192 hasConcept C109214941 @default.
• W2309199192 hasConcept C117137515 @default.
• W2309199192 hasConcept C121332964 @default.
• W2309199192 hasConcept C172695262 @default.
• W2309199192 hasConcept C180566339 @default.
• W2309199192 hasConcept C185544564 @default.
• W2309199192 hasConcept C2775859700 @default.
• W2309199192 hasConcept C2781235419 @default.
• W2309199192 hasConcept C38976095 @default.
• W2309199192 hasConcept C3909970 @default.
• W2309199192 hasConcept C42238305 @default.
• W2309199192 hasConceptScore W2309199192C109214941 @default.
• W2309199192 hasConceptScore W2309199192C117137515 @default.
• W2309199192 hasConceptScore W2309199192C121332964 @default.
• W2309199192 hasConceptScore W2309199192C172695262 @default.
• W2309199192 hasConceptScore W2309199192C180566339 @default.
• W2309199192 hasConceptScore W2309199192C185544564 @default.
• W2309199192 hasConceptScore W2309199192C2775859700 @default.
• W2309199192 hasConceptScore W2309199192C2781235419 @default.
• W2309199192 hasConceptScore W2309199192C38976095 @default.
• W2309199192 hasConceptScore W2309199192C3909970 @default.
• W2309199192 hasConceptScore W2309199192C42238305 @default.
• W2309199192 hasFunder F4320306076 @default.
• W2309199192 hasFunder F4320306084 @default.
• W2309199192 hasFunder F4320308501 @default.
• W2309199192 hasFunder F4320320879 @default.
• W2309199192 hasFunder F4320321001 @default.
• W2309199192 hasFunder F4320322795 @default.
• W2309199192 hasFunder F4320332359 @default.
• W2309199192 hasLocation W23091991921 @default.
• W2309199192 hasLocation W23091991922 @default.
• W2309199192 hasLocation W23091991923 @default.
• W2309199192 hasLocation W23091991924 @default.
• W2309199192 hasOpenAccess W2309199192 @default.
• W2309199192 hasPrimaryLocation W23091991921 @default.
• W2309199192 hasRelatedWork W2037196217 @default.
• W2309199192 hasRelatedWork W2309199192 @default.
• W2309199192 hasRelatedWork W2735517509 @default.
• W2309199192 hasRelatedWork W2970612932 @default.
• W2309199192 hasRelatedWork W3043960493 @default.
• W2309199192 hasRelatedWork W3097759442 @default.
• W2309199192 hasRelatedWork W3097766099 @default.
• W2309199192 hasRelatedWork W3207590980 @default.
• W2309199192 hasRelatedWork W4200620682 @default.
• W2309199192 hasRelatedWork W4307519707 @default.
• W2309199192 hasVolume "911" @default.

• next