Matches in SemOpenAlex for { <https://semopenalex.org/work/W4385839470> ?p ?o ?g. }
- W4385839470 abstract "We compute the electromagnetic properties of spin-$frac{1}{2}$ doubly charmed baryons on ($2+1$)-flavor lattices that have a pion mass of $ensuremath{sim}156text{ }text{ }mathrm{MeV}$. The Tsukuba action is employed for the charm quark in addition to the standard isotropic Clover action to quantify the $mathcal{O}({m}_{q}a)$ effects. We calculate the electric and magnetic Sachs form factors and extract the magnetic moments and electric and magnetic-charge radii. We also investigate the individual quark-sector contributions to the charge radii and the magnetic moments. The results provide vital information to understand the size and shape of the doubly charmed baryons. We find that the two heavy-charm quarks drive the charge radii and the magnetic moments to smaller values than that of light baryons. The central values of the observables that are obtained using the relativistic action for the charm quark are 5% to 10% larger than those obtained using the Clover action. Utilizing the available lattice data, we reexamine the quark mass dependence of the observables." @default.
- W4385839470 created "2023-08-16" @default.
- W4385839470 creator A5021018356 @default.
- W4385839470 date "2023-08-15" @default.
- W4385839470 modified "2023-09-27" @default.
- W4385839470 title "Electromagnetic structure of spin- <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:mfrac></mml:mrow></mml:math> doubly charmed baryons in lattice QCD" @default.
- W4385839470 cites W135490822 @default.
- W4385839470 cites W1484856293 @default.
- W4385839470 cites W1515087005 @default.
- W4385839470 cites W1822192376 @default.
- W4385839470 cites W1965628044 @default.
- W4385839470 cites W1967633601 @default.
- W4385839470 cites W1968089298 @default.
- W4385839470 cites W1972432774 @default.
- W4385839470 cites W1979634942 @default.
- W4385839470 cites W1993748689 @default.
- W4385839470 cites W1999794318 @default.
- W4385839470 cites W2002230878 @default.
- W4385839470 cites W2020983834 @default.
- W4385839470 cites W2032506476 @default.
- W4385839470 cites W2035649836 @default.
- W4385839470 cites W2053611167 @default.
- W4385839470 cites W2064941239 @default.
- W4385839470 cites W2068267671 @default.
- W4385839470 cites W2080385215 @default.
- W4385839470 cites W2084790038 @default.
- W4385839470 cites W2091340194 @default.
- W4385839470 cites W2094657751 @default.
- W4385839470 cites W2097474038 @default.
- W4385839470 cites W2098274414 @default.
- W4385839470 cites W2107489310 @default.
- W4385839470 cites W2109288683 @default.
- W4385839470 cites W2111426224 @default.
- W4385839470 cites W2116468736 @default.
- W4385839470 cites W2118672978 @default.
- W4385839470 cites W2125062983 @default.
- W4385839470 cites W2126148378 @default.
- W4385839470 cites W2126271681 @default.
- W4385839470 cites W2130859739 @default.
- W4385839470 cites W2131928089 @default.
- W4385839470 cites W2137539095 @default.
- W4385839470 cites W2139665613 @default.
- W4385839470 cites W2145608054 @default.
- W4385839470 cites W2155967869 @default.
- W4385839470 cites W2226501930 @default.
- W4385839470 cites W2520368248 @default.
- W4385839470 cites W2542291407 @default.
- W4385839470 cites W2730180975 @default.
- W4385839470 cites W2736211965 @default.
- W4385839470 cites W2748571033 @default.
- W4385839470 cites W2786444327 @default.
- W4385839470 cites W2810925807 @default.
- W4385839470 cites W2884056818 @default.
- W4385839470 cites W2952062678 @default.
- W4385839470 cites W3017053733 @default.
- W4385839470 cites W3082694858 @default.
- W4385839470 cites W3099432311 @default.
- W4385839470 cites W3105122601 @default.
- W4385839470 cites W3108284800 @default.
- W4385839470 cites W3118143974 @default.
- W4385839470 cites W3121823746 @default.
- W4385839470 cites W3183882155 @default.
- W4385839470 cites W3197607150 @default.
- W4385839470 cites W3198636602 @default.
- W4385839470 cites W3200015712 @default.
- W4385839470 cites W3208282901 @default.
- W4385839470 cites W4200230231 @default.
- W4385839470 cites W4220749600 @default.
- W4385839470 cites W4230234193 @default.
- W4385839470 cites W4285208388 @default.
- W4385839470 cites W783518698 @default.
- W4385839470 doi "https://doi.org/10.1103/physrevd.108.034504" @default.
- W4385839470 hasPublicationYear "2023" @default.
- W4385839470 type Work @default.
- W4385839470 citedByCount "0" @default.
- W4385839470 crossrefType "journal-article" @default.
- W4385839470 hasAuthorship W4385839470A5021018356 @default.
- W4385839470 hasBestOaLocation W43858394701 @default.
- W4385839470 hasConcept C109214941 @default.
- W4385839470 hasConcept C121332964 @default.
- W4385839470 hasConcept C154153549 @default.
- W4385839470 hasConcept C185544564 @default.
- W4385839470 hasConcept C188082385 @default.
- W4385839470 hasConcept C19694890 @default.
- W4385839470 hasConcept C206094082 @default.
- W4385839470 hasConcept C26873012 @default.
- W4385839470 hasConcept C2775980768 @default.
- W4385839470 hasConcept C2781339351 @default.
- W4385839470 hasConcept C32848918 @default.
- W4385839470 hasConcept C42704618 @default.
- W4385839470 hasConcept C54553102 @default.
- W4385839470 hasConcept C62520636 @default.
- W4385839470 hasConcept C7602139 @default.
- W4385839470 hasConcept C86040059 @default.
- W4385839470 hasConcept C97355855 @default.
- W4385839470 hasConceptScore W4385839470C109214941 @default.
- W4385839470 hasConceptScore W4385839470C121332964 @default.
- W4385839470 hasConceptScore W4385839470C154153549 @default.
- W4385839470 hasConceptScore W4385839470C185544564 @default.
- W4385839470 hasConceptScore W4385839470C188082385 @default.