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| 001 | 858800 | ||
| 005 | 20240610120828.0 | ||
| 024 | 7 | _ | |a 10.1103/PhysRevC.97.024325 |2 doi |
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| 024 | 7 | _ | |a 1538-4497 |2 ISSN |
| 024 | 7 | _ | |a 2469-9985 |2 ISSN |
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| 100 | 1 | _ | |a Burrows, M. |0 P:(DE-HGF)0 |b 0 |
| 245 | _ | _ | |a Ab initio translationally invariant nonlocal one-body densities from no-core shell-model theory |
| 260 | _ | _ | |a Woodbury, NY |c 2018 |b Inst. |
| 264 | _ | 1 | |3 online |2 Crossref |b American Physical Society (APS) |c 2018-02-21 |
| 264 | _ | 1 | |3 print |2 Crossref |b American Physical Society (APS) |c 2018-02-01 |
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| 336 | 7 | _ | |a Journal Article |0 0 |2 EndNote |
| 520 | _ | _ | |a Background: It is well known that effective nuclear interactions are in general nonlocal. Thus if nuclear densities obtained from ab initio no-core shell-model (NCSM) calculations are to be used in reaction calculations, translationally invariant nonlocal densities must be available.Purpose: Though it is standard to extract translationally invariant one-body local densities from NCSM calculations to calculate local nuclear observables like radii and transition amplitudes, the corresponding nonlocal one-body densities have not been considered so far. A major reason for this is that the procedure for removing the center-of-mass component from NCSM wave functions up to now has only been developed for local densities.Results: A formulation for removing center-of-mass contributions from nonlocal one-body densities obtained from NCSM and symmetry-adapted NCSM (SA-NCSM) calculations is derived, and applied to the ground state densities of 4He, 6Li, 12C, and 16O. The nonlocality is studied as a function of angular momentum components in momentum as well as coordinate space.Conclusions: We find that the nonlocality for the ground state densities of the nuclei under consideration increases as a function of the angular momentum. The relative magnitude of those contributions decreases with increasing angular momentum. In general, the nonlocal structure of the one-body density matrices we studied is given by the shell structure of the nucleus, and cannot be described with simple functional forms. |
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| 536 | _ | _ | |a DFG project 196253076 - TRR 110: Symmetrien und Strukturbildung in der Quantenchromodynamik (196253076) |0 G:(GEPRIS)196253076 |c 196253076 |x 1 |
| 536 | _ | _ | |a Chiral dynamics in Few-Baryon Systems (jikp03_20090701) |0 G:(DE-Juel1)jikp03_20090701 |c jikp03_20090701 |x 2 |f Chiral dynamics in Few-Baryon Systems |
| 542 | _ | _ | |i 2018-02-21 |2 Crossref |u https://link.aps.org/licenses/aps-default-license |
| 542 | _ | _ | |i 2019-02-21 |2 Crossref |u https://link.aps.org/licenses/aps-default-accepted-manuscript-license |
| 588 | _ | _ | |a Dataset connected to CrossRef |
| 700 | 1 | _ | |a Elster, Ch. |0 P:(DE-HGF)0 |b 1 |e Corresponding author |
| 700 | 1 | _ | |a Popa, G. |0 P:(DE-HGF)0 |b 2 |
| 700 | 1 | _ | |a Launey, K. D. |0 P:(DE-HGF)0 |b 3 |
| 700 | 1 | _ | |a Nogga, A. |0 P:(DE-Juel1)131273 |b 4 |u fzj |
| 700 | 1 | _ | |a Maris, P. |0 P:(DE-HGF)0 |b 5 |
| 773 | 1 | 8 | |a 10.1103/physrevc.97.024325 |b American Physical Society (APS) |d 2018-02-21 |n 2 |p 024325 |3 journal-article |2 Crossref |t Physical Review C |v 97 |y 2018 |x 2469-9985 |
| 773 | _ | _ | |a 10.1103/PhysRevC.97.024325 |g Vol. 97, no. 2, p. 024325 |0 PERI:(DE-600)2844098-5 |n 2 |p 024325 |t Physical review / C |v 97 |y 2018 |x 2469-9985 |
| 856 | 4 | _ | |u https://juser.fz-juelich.de/record/858800/files/PhysRevC.97.024325.pdf |y OpenAccess |
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