Nuclear landscape in covariant density functional theory
The neutron and proton drip lines represent the limits of the nuclear landscape. While the proton drip line is measured experimentally up to rather high Z values, the location of the neutron drip line for absolute majority of elements is based on theoretical predictions which involve extreme extrapo...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Afanasjev, A.V. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2013transfer abstract |
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| Schlagwörter: |
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| Umfang: |
5 |
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| Übergeordnetes Werk: |
Enthalten in: Applying the Go/NoGo processing schema to a visual oddball task in older adults - Steiner, Genevieve Z. ELSEVIER, 2016, Amsterdam |
|---|---|
| Übergeordnetes Werk: |
volume:726 ; year:2013 ; number:4 ; day:4 ; month:11 ; pages:680-684 ; extent:5 |
| Links: |
|---|
| DOI / URN: |
10.1016/j.physletb.2013.09.017 |
|---|
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ELV01157612X |
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| 520 | |a The neutron and proton drip lines represent the limits of the nuclear landscape. While the proton drip line is measured experimentally up to rather high Z values, the location of the neutron drip line for absolute majority of elements is based on theoretical predictions which involve extreme extrapolations. The first ever systematic investigation of the location of the proton and neutron drip lines in the covariant density functional theory has been performed by employing a set of the state-of-the-art parametrizations. Calculated theoretical uncertainties in the position of two-neutron drip line are compared with those obtained in non-relativistic DFT calculations. Shell effects drastically affect the shape of two-neutron drip line. In particular, model uncertainties in the definition of two-neutron drip line at Z ∼ 54 , N = 126 and Z ∼ 82 , N = 184 are very small due to the impact of spherical shell closures at N = 126 and 184 . | ||
| 520 | |a The neutron and proton drip lines represent the limits of the nuclear landscape. While the proton drip line is measured experimentally up to rather high Z values, the location of the neutron drip line for absolute majority of elements is based on theoretical predictions which involve extreme extrapolations. The first ever systematic investigation of the location of the proton and neutron drip lines in the covariant density functional theory has been performed by employing a set of the state-of-the-art parametrizations. Calculated theoretical uncertainties in the position of two-neutron drip line are compared with those obtained in non-relativistic DFT calculations. Shell effects drastically affect the shape of two-neutron drip line. In particular, model uncertainties in the definition of two-neutron drip line at Z ∼ 54 , N = 126 and Z ∼ 82 , N = 184 are very small due to the impact of spherical shell closures at N = 126 and 184 . | ||
| 650 | 7 | |a Proton and neutron drip lines |2 Elsevier | |
| 650 | 7 | |a Two-particle separation energies |2 Elsevier | |
| 650 | 7 | |a Covariant density functional theory |2 Elsevier | |
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| 700 | 1 | |a Ray, D. |4 oth | |
| 700 | 1 | |a Ring, P. |4 oth | |
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10.1016/j.physletb.2013.09.017 doi GBVA2013011000027.pica (DE-627)ELV01157612X (ELSEVIER)S0370-2693(13)00734-X DE-627 ger DE-627 rakwb eng 530 DE-600 610 VZ 77.50 bkl Afanasjev, A.V. verfasserin aut Nuclear landscape in covariant density functional theory 2013transfer abstract 5 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The neutron and proton drip lines represent the limits of the nuclear landscape. While the proton drip line is measured experimentally up to rather high Z values, the location of the neutron drip line for absolute majority of elements is based on theoretical predictions which involve extreme extrapolations. The first ever systematic investigation of the location of the proton and neutron drip lines in the covariant density functional theory has been performed by employing a set of the state-of-the-art parametrizations. Calculated theoretical uncertainties in the position of two-neutron drip line are compared with those obtained in non-relativistic DFT calculations. Shell effects drastically affect the shape of two-neutron drip line. In particular, model uncertainties in the definition of two-neutron drip line at Z ∼ 54 , N = 126 and Z ∼ 82 , N = 184 are very small due to the impact of spherical shell closures at N = 126 and 184 . The neutron and proton drip lines represent the limits of the nuclear landscape. While the proton drip line is measured experimentally up to rather high Z values, the location of the neutron drip line for absolute majority of elements is based on theoretical predictions which involve extreme extrapolations. The first ever systematic investigation of the location of the proton and neutron drip lines in the covariant density functional theory has been performed by employing a set of the state-of-the-art parametrizations. Calculated theoretical uncertainties in the position of two-neutron drip line are compared with those obtained in non-relativistic DFT calculations. Shell effects drastically affect the shape of two-neutron drip line. In particular, model uncertainties in the definition of two-neutron drip line at Z ∼ 54 , N = 126 and Z ∼ 82 , N = 184 are very small due to the impact of spherical shell closures at N = 126 and 184 . Proton and neutron drip lines Elsevier Two-particle separation energies Elsevier Covariant density functional theory Elsevier Agbemava, S.E. oth Ray, D. oth Ring, P. oth Enthalten in North-Holland Publ Steiner, Genevieve Z. ELSEVIER Applying the Go/NoGo processing schema to a visual oddball task in older adults 2016 Amsterdam (DE-627)ELV000151122 volume:726 year:2013 number:4 day:4 month:11 pages:680-684 extent:5 https://doi.org/10.1016/j.physletb.2013.09.017 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 726 2013 4 4 1104 680-684 5 |
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10.1016/j.physletb.2013.09.017 doi GBVA2013011000027.pica (DE-627)ELV01157612X (ELSEVIER)S0370-2693(13)00734-X DE-627 ger DE-627 rakwb eng 530 DE-600 610 VZ 77.50 bkl Afanasjev, A.V. verfasserin aut Nuclear landscape in covariant density functional theory 2013transfer abstract 5 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The neutron and proton drip lines represent the limits of the nuclear landscape. While the proton drip line is measured experimentally up to rather high Z values, the location of the neutron drip line for absolute majority of elements is based on theoretical predictions which involve extreme extrapolations. The first ever systematic investigation of the location of the proton and neutron drip lines in the covariant density functional theory has been performed by employing a set of the state-of-the-art parametrizations. Calculated theoretical uncertainties in the position of two-neutron drip line are compared with those obtained in non-relativistic DFT calculations. Shell effects drastically affect the shape of two-neutron drip line. In particular, model uncertainties in the definition of two-neutron drip line at Z ∼ 54 , N = 126 and Z ∼ 82 , N = 184 are very small due to the impact of spherical shell closures at N = 126 and 184 . The neutron and proton drip lines represent the limits of the nuclear landscape. While the proton drip line is measured experimentally up to rather high Z values, the location of the neutron drip line for absolute majority of elements is based on theoretical predictions which involve extreme extrapolations. The first ever systematic investigation of the location of the proton and neutron drip lines in the covariant density functional theory has been performed by employing a set of the state-of-the-art parametrizations. Calculated theoretical uncertainties in the position of two-neutron drip line are compared with those obtained in non-relativistic DFT calculations. Shell effects drastically affect the shape of two-neutron drip line. In particular, model uncertainties in the definition of two-neutron drip line at Z ∼ 54 , N = 126 and Z ∼ 82 , N = 184 are very small due to the impact of spherical shell closures at N = 126 and 184 . Proton and neutron drip lines Elsevier Two-particle separation energies Elsevier Covariant density functional theory Elsevier Agbemava, S.E. oth Ray, D. oth Ring, P. oth Enthalten in North-Holland Publ Steiner, Genevieve Z. ELSEVIER Applying the Go/NoGo processing schema to a visual oddball task in older adults 2016 Amsterdam (DE-627)ELV000151122 volume:726 year:2013 number:4 day:4 month:11 pages:680-684 extent:5 https://doi.org/10.1016/j.physletb.2013.09.017 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 726 2013 4 4 1104 680-684 5 |
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10.1016/j.physletb.2013.09.017 doi GBVA2013011000027.pica (DE-627)ELV01157612X (ELSEVIER)S0370-2693(13)00734-X DE-627 ger DE-627 rakwb eng 530 DE-600 610 VZ 77.50 bkl Afanasjev, A.V. verfasserin aut Nuclear landscape in covariant density functional theory 2013transfer abstract 5 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The neutron and proton drip lines represent the limits of the nuclear landscape. While the proton drip line is measured experimentally up to rather high Z values, the location of the neutron drip line for absolute majority of elements is based on theoretical predictions which involve extreme extrapolations. The first ever systematic investigation of the location of the proton and neutron drip lines in the covariant density functional theory has been performed by employing a set of the state-of-the-art parametrizations. Calculated theoretical uncertainties in the position of two-neutron drip line are compared with those obtained in non-relativistic DFT calculations. Shell effects drastically affect the shape of two-neutron drip line. In particular, model uncertainties in the definition of two-neutron drip line at Z ∼ 54 , N = 126 and Z ∼ 82 , N = 184 are very small due to the impact of spherical shell closures at N = 126 and 184 . The neutron and proton drip lines represent the limits of the nuclear landscape. While the proton drip line is measured experimentally up to rather high Z values, the location of the neutron drip line for absolute majority of elements is based on theoretical predictions which involve extreme extrapolations. The first ever systematic investigation of the location of the proton and neutron drip lines in the covariant density functional theory has been performed by employing a set of the state-of-the-art parametrizations. Calculated theoretical uncertainties in the position of two-neutron drip line are compared with those obtained in non-relativistic DFT calculations. Shell effects drastically affect the shape of two-neutron drip line. In particular, model uncertainties in the definition of two-neutron drip line at Z ∼ 54 , N = 126 and Z ∼ 82 , N = 184 are very small due to the impact of spherical shell closures at N = 126 and 184 . Proton and neutron drip lines Elsevier Two-particle separation energies Elsevier Covariant density functional theory Elsevier Agbemava, S.E. oth Ray, D. oth Ring, P. oth Enthalten in North-Holland Publ Steiner, Genevieve Z. ELSEVIER Applying the Go/NoGo processing schema to a visual oddball task in older adults 2016 Amsterdam (DE-627)ELV000151122 volume:726 year:2013 number:4 day:4 month:11 pages:680-684 extent:5 https://doi.org/10.1016/j.physletb.2013.09.017 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 726 2013 4 4 1104 680-684 5 |
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10.1016/j.physletb.2013.09.017 doi GBVA2013011000027.pica (DE-627)ELV01157612X (ELSEVIER)S0370-2693(13)00734-X DE-627 ger DE-627 rakwb eng 530 DE-600 610 VZ 77.50 bkl Afanasjev, A.V. verfasserin aut Nuclear landscape in covariant density functional theory 2013transfer abstract 5 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The neutron and proton drip lines represent the limits of the nuclear landscape. While the proton drip line is measured experimentally up to rather high Z values, the location of the neutron drip line for absolute majority of elements is based on theoretical predictions which involve extreme extrapolations. The first ever systematic investigation of the location of the proton and neutron drip lines in the covariant density functional theory has been performed by employing a set of the state-of-the-art parametrizations. Calculated theoretical uncertainties in the position of two-neutron drip line are compared with those obtained in non-relativistic DFT calculations. Shell effects drastically affect the shape of two-neutron drip line. In particular, model uncertainties in the definition of two-neutron drip line at Z ∼ 54 , N = 126 and Z ∼ 82 , N = 184 are very small due to the impact of spherical shell closures at N = 126 and 184 . The neutron and proton drip lines represent the limits of the nuclear landscape. While the proton drip line is measured experimentally up to rather high Z values, the location of the neutron drip line for absolute majority of elements is based on theoretical predictions which involve extreme extrapolations. The first ever systematic investigation of the location of the proton and neutron drip lines in the covariant density functional theory has been performed by employing a set of the state-of-the-art parametrizations. Calculated theoretical uncertainties in the position of two-neutron drip line are compared with those obtained in non-relativistic DFT calculations. Shell effects drastically affect the shape of two-neutron drip line. In particular, model uncertainties in the definition of two-neutron drip line at Z ∼ 54 , N = 126 and Z ∼ 82 , N = 184 are very small due to the impact of spherical shell closures at N = 126 and 184 . Proton and neutron drip lines Elsevier Two-particle separation energies Elsevier Covariant density functional theory Elsevier Agbemava, S.E. oth Ray, D. oth Ring, P. oth Enthalten in North-Holland Publ Steiner, Genevieve Z. ELSEVIER Applying the Go/NoGo processing schema to a visual oddball task in older adults 2016 Amsterdam (DE-627)ELV000151122 volume:726 year:2013 number:4 day:4 month:11 pages:680-684 extent:5 https://doi.org/10.1016/j.physletb.2013.09.017 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 726 2013 4 4 1104 680-684 5 |
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10.1016/j.physletb.2013.09.017 doi GBVA2013011000027.pica (DE-627)ELV01157612X (ELSEVIER)S0370-2693(13)00734-X DE-627 ger DE-627 rakwb eng 530 DE-600 610 VZ 77.50 bkl Afanasjev, A.V. verfasserin aut Nuclear landscape in covariant density functional theory 2013transfer abstract 5 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The neutron and proton drip lines represent the limits of the nuclear landscape. While the proton drip line is measured experimentally up to rather high Z values, the location of the neutron drip line for absolute majority of elements is based on theoretical predictions which involve extreme extrapolations. The first ever systematic investigation of the location of the proton and neutron drip lines in the covariant density functional theory has been performed by employing a set of the state-of-the-art parametrizations. Calculated theoretical uncertainties in the position of two-neutron drip line are compared with those obtained in non-relativistic DFT calculations. Shell effects drastically affect the shape of two-neutron drip line. In particular, model uncertainties in the definition of two-neutron drip line at Z ∼ 54 , N = 126 and Z ∼ 82 , N = 184 are very small due to the impact of spherical shell closures at N = 126 and 184 . The neutron and proton drip lines represent the limits of the nuclear landscape. While the proton drip line is measured experimentally up to rather high Z values, the location of the neutron drip line for absolute majority of elements is based on theoretical predictions which involve extreme extrapolations. The first ever systematic investigation of the location of the proton and neutron drip lines in the covariant density functional theory has been performed by employing a set of the state-of-the-art parametrizations. Calculated theoretical uncertainties in the position of two-neutron drip line are compared with those obtained in non-relativistic DFT calculations. Shell effects drastically affect the shape of two-neutron drip line. In particular, model uncertainties in the definition of two-neutron drip line at Z ∼ 54 , N = 126 and Z ∼ 82 , N = 184 are very small due to the impact of spherical shell closures at N = 126 and 184 . Proton and neutron drip lines Elsevier Two-particle separation energies Elsevier Covariant density functional theory Elsevier Agbemava, S.E. oth Ray, D. oth Ring, P. oth Enthalten in North-Holland Publ Steiner, Genevieve Z. ELSEVIER Applying the Go/NoGo processing schema to a visual oddball task in older adults 2016 Amsterdam (DE-627)ELV000151122 volume:726 year:2013 number:4 day:4 month:11 pages:680-684 extent:5 https://doi.org/10.1016/j.physletb.2013.09.017 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 726 2013 4 4 1104 680-684 5 |
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530 DE-600 610 VZ 77.50 bkl Nuclear landscape in covariant density functional theory Proton and neutron drip lines Elsevier Two-particle separation energies Elsevier Covariant density functional theory Elsevier |
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Applying the Go/NoGo processing schema to a visual oddball task in older adults |
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Applying the Go/NoGo processing schema to a visual oddball task in older adults |
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Nuclear landscape in covariant density functional theory |
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Nuclear landscape in covariant density functional theory |
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Afanasjev, A.V. |
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Applying the Go/NoGo processing schema to a visual oddball task in older adults |
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nuclear landscape in covariant density functional theory |
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Nuclear landscape in covariant density functional theory |
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The neutron and proton drip lines represent the limits of the nuclear landscape. While the proton drip line is measured experimentally up to rather high Z values, the location of the neutron drip line for absolute majority of elements is based on theoretical predictions which involve extreme extrapolations. The first ever systematic investigation of the location of the proton and neutron drip lines in the covariant density functional theory has been performed by employing a set of the state-of-the-art parametrizations. Calculated theoretical uncertainties in the position of two-neutron drip line are compared with those obtained in non-relativistic DFT calculations. Shell effects drastically affect the shape of two-neutron drip line. In particular, model uncertainties in the definition of two-neutron drip line at Z ∼ 54 , N = 126 and Z ∼ 82 , N = 184 are very small due to the impact of spherical shell closures at N = 126 and 184 . |
| abstractGer |
The neutron and proton drip lines represent the limits of the nuclear landscape. While the proton drip line is measured experimentally up to rather high Z values, the location of the neutron drip line for absolute majority of elements is based on theoretical predictions which involve extreme extrapolations. The first ever systematic investigation of the location of the proton and neutron drip lines in the covariant density functional theory has been performed by employing a set of the state-of-the-art parametrizations. Calculated theoretical uncertainties in the position of two-neutron drip line are compared with those obtained in non-relativistic DFT calculations. Shell effects drastically affect the shape of two-neutron drip line. In particular, model uncertainties in the definition of two-neutron drip line at Z ∼ 54 , N = 126 and Z ∼ 82 , N = 184 are very small due to the impact of spherical shell closures at N = 126 and 184 . |
| abstract_unstemmed |
The neutron and proton drip lines represent the limits of the nuclear landscape. While the proton drip line is measured experimentally up to rather high Z values, the location of the neutron drip line for absolute majority of elements is based on theoretical predictions which involve extreme extrapolations. The first ever systematic investigation of the location of the proton and neutron drip lines in the covariant density functional theory has been performed by employing a set of the state-of-the-art parametrizations. Calculated theoretical uncertainties in the position of two-neutron drip line are compared with those obtained in non-relativistic DFT calculations. Shell effects drastically affect the shape of two-neutron drip line. In particular, model uncertainties in the definition of two-neutron drip line at Z ∼ 54 , N = 126 and Z ∼ 82 , N = 184 are very small due to the impact of spherical shell closures at N = 126 and 184 . |
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Nuclear landscape in covariant density functional theory |
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