Description of collective motion in two-dimensional nuclei; Tomonaga's method revisited
Four decades ago, Tomonaga proposed the elementary theory of quantum mechanical collective motion of two-dimensional nuclei of N nucleons. The theory is based essentially on the neglect of 1/sqrtN against unity. Very recently we have given exact canonically conjugate momenta to quadrupole-type colle...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Nishiyama, Seiya [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2015 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Nuclear physics |
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| Übergeordnetes Werk: |
volume:935 ; year:2015 ; pages:1-17 |
| Links: |
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| DOI / URN: |
10.1016/j.nuclphysa.2014.12.005 |
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| 520 | |a Four decades ago, Tomonaga proposed the elementary theory of quantum mechanical collective motion of two-dimensional nuclei of N nucleons. The theory is based essentially on the neglect of 1/sqrtN against unity. Very recently we have given exact canonically conjugate momenta to quadrupole-type collective coordinates under some subsidiary conditions and have derived nuclear quadrupole-type collective Hamiltonian. Even in the case of simple two-dimensional nuclei, we have a subsidiary condition to obtain exact canonical variables. Particularly the structure of the collective subspace satisfying the subsidiary condition is studied in detail. This subsidiary condition is important to investigate what is a structure of the collective subspace. | ||
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10.1016/j.nuclphysa.2014.12.005 doi PQ20160617 (DE-627)OLC1967398771 (DE-599)GBVOLC1967398771 (PRQ)a1451-2f7ad90d4a7959f9ca4c6d19b742ab2188995263f44b94db2d63a1703d2237940 (KEY)0073031920150000935000000001descriptionofcollectivemotionintwodimensionalnucle DE-627 ger DE-627 rakwb eng 530 DNB Nishiyama, Seiya verfasserin aut Description of collective motion in two-dimensional nuclei; Tomonaga's method revisited 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Four decades ago, Tomonaga proposed the elementary theory of quantum mechanical collective motion of two-dimensional nuclei of N nucleons. The theory is based essentially on the neglect of 1/sqrtN against unity. Very recently we have given exact canonically conjugate momenta to quadrupole-type collective coordinates under some subsidiary conditions and have derived nuclear quadrupole-type collective Hamiltonian. Even in the case of simple two-dimensional nuclei, we have a subsidiary condition to obtain exact canonical variables. Particularly the structure of the collective subspace satisfying the subsidiary condition is studied in detail. This subsidiary condition is important to investigate what is a structure of the collective subspace. Nuclear Theory da Providência, João oth Enthalten in Nuclear physics <Amsterdam> / A Amsterdam [u.a.] : Elsevier, 1967 935(2015), Seite 1-17 (DE-627)129504033 (DE-600)208861-7 (DE-576)014907348 0375-9474 nnns volume:935 year:2015 pages:1-17 http://dx.doi.org/10.1016/j.nuclphysa.2014.12.005 Volltext http://arxiv.org/abs/1407.3593 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 GBV_ILN_2014 GBV_ILN_2279 AR 935 2015 1-17 |
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10.1016/j.nuclphysa.2014.12.005 doi PQ20160617 (DE-627)OLC1967398771 (DE-599)GBVOLC1967398771 (PRQ)a1451-2f7ad90d4a7959f9ca4c6d19b742ab2188995263f44b94db2d63a1703d2237940 (KEY)0073031920150000935000000001descriptionofcollectivemotionintwodimensionalnucle DE-627 ger DE-627 rakwb eng 530 DNB Nishiyama, Seiya verfasserin aut Description of collective motion in two-dimensional nuclei; Tomonaga's method revisited 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Four decades ago, Tomonaga proposed the elementary theory of quantum mechanical collective motion of two-dimensional nuclei of N nucleons. The theory is based essentially on the neglect of 1/sqrtN against unity. Very recently we have given exact canonically conjugate momenta to quadrupole-type collective coordinates under some subsidiary conditions and have derived nuclear quadrupole-type collective Hamiltonian. Even in the case of simple two-dimensional nuclei, we have a subsidiary condition to obtain exact canonical variables. Particularly the structure of the collective subspace satisfying the subsidiary condition is studied in detail. This subsidiary condition is important to investigate what is a structure of the collective subspace. Nuclear Theory da Providência, João oth Enthalten in Nuclear physics <Amsterdam> / A Amsterdam [u.a.] : Elsevier, 1967 935(2015), Seite 1-17 (DE-627)129504033 (DE-600)208861-7 (DE-576)014907348 0375-9474 nnns volume:935 year:2015 pages:1-17 http://dx.doi.org/10.1016/j.nuclphysa.2014.12.005 Volltext http://arxiv.org/abs/1407.3593 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 GBV_ILN_2014 GBV_ILN_2279 AR 935 2015 1-17 |
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10.1016/j.nuclphysa.2014.12.005 doi PQ20160617 (DE-627)OLC1967398771 (DE-599)GBVOLC1967398771 (PRQ)a1451-2f7ad90d4a7959f9ca4c6d19b742ab2188995263f44b94db2d63a1703d2237940 (KEY)0073031920150000935000000001descriptionofcollectivemotionintwodimensionalnucle DE-627 ger DE-627 rakwb eng 530 DNB Nishiyama, Seiya verfasserin aut Description of collective motion in two-dimensional nuclei; Tomonaga's method revisited 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Four decades ago, Tomonaga proposed the elementary theory of quantum mechanical collective motion of two-dimensional nuclei of N nucleons. The theory is based essentially on the neglect of 1/sqrtN against unity. Very recently we have given exact canonically conjugate momenta to quadrupole-type collective coordinates under some subsidiary conditions and have derived nuclear quadrupole-type collective Hamiltonian. Even in the case of simple two-dimensional nuclei, we have a subsidiary condition to obtain exact canonical variables. Particularly the structure of the collective subspace satisfying the subsidiary condition is studied in detail. This subsidiary condition is important to investigate what is a structure of the collective subspace. Nuclear Theory da Providência, João oth Enthalten in Nuclear physics <Amsterdam> / A Amsterdam [u.a.] : Elsevier, 1967 935(2015), Seite 1-17 (DE-627)129504033 (DE-600)208861-7 (DE-576)014907348 0375-9474 nnns volume:935 year:2015 pages:1-17 http://dx.doi.org/10.1016/j.nuclphysa.2014.12.005 Volltext http://arxiv.org/abs/1407.3593 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 GBV_ILN_2014 GBV_ILN_2279 AR 935 2015 1-17 |
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10.1016/j.nuclphysa.2014.12.005 doi PQ20160617 (DE-627)OLC1967398771 (DE-599)GBVOLC1967398771 (PRQ)a1451-2f7ad90d4a7959f9ca4c6d19b742ab2188995263f44b94db2d63a1703d2237940 (KEY)0073031920150000935000000001descriptionofcollectivemotionintwodimensionalnucle DE-627 ger DE-627 rakwb eng 530 DNB Nishiyama, Seiya verfasserin aut Description of collective motion in two-dimensional nuclei; Tomonaga's method revisited 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Four decades ago, Tomonaga proposed the elementary theory of quantum mechanical collective motion of two-dimensional nuclei of N nucleons. The theory is based essentially on the neglect of 1/sqrtN against unity. Very recently we have given exact canonically conjugate momenta to quadrupole-type collective coordinates under some subsidiary conditions and have derived nuclear quadrupole-type collective Hamiltonian. Even in the case of simple two-dimensional nuclei, we have a subsidiary condition to obtain exact canonical variables. Particularly the structure of the collective subspace satisfying the subsidiary condition is studied in detail. This subsidiary condition is important to investigate what is a structure of the collective subspace. Nuclear Theory da Providência, João oth Enthalten in Nuclear physics <Amsterdam> / A Amsterdam [u.a.] : Elsevier, 1967 935(2015), Seite 1-17 (DE-627)129504033 (DE-600)208861-7 (DE-576)014907348 0375-9474 nnns volume:935 year:2015 pages:1-17 http://dx.doi.org/10.1016/j.nuclphysa.2014.12.005 Volltext http://arxiv.org/abs/1407.3593 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 GBV_ILN_2014 GBV_ILN_2279 AR 935 2015 1-17 |
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Description of collective motion in two-dimensional nuclei; Tomonaga's method revisited |
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Four decades ago, Tomonaga proposed the elementary theory of quantum mechanical collective motion of two-dimensional nuclei of N nucleons. The theory is based essentially on the neglect of 1/sqrtN against unity. Very recently we have given exact canonically conjugate momenta to quadrupole-type collective coordinates under some subsidiary conditions and have derived nuclear quadrupole-type collective Hamiltonian. Even in the case of simple two-dimensional nuclei, we have a subsidiary condition to obtain exact canonical variables. Particularly the structure of the collective subspace satisfying the subsidiary condition is studied in detail. This subsidiary condition is important to investigate what is a structure of the collective subspace. |
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Four decades ago, Tomonaga proposed the elementary theory of quantum mechanical collective motion of two-dimensional nuclei of N nucleons. The theory is based essentially on the neglect of 1/sqrtN against unity. Very recently we have given exact canonically conjugate momenta to quadrupole-type collective coordinates under some subsidiary conditions and have derived nuclear quadrupole-type collective Hamiltonian. Even in the case of simple two-dimensional nuclei, we have a subsidiary condition to obtain exact canonical variables. Particularly the structure of the collective subspace satisfying the subsidiary condition is studied in detail. This subsidiary condition is important to investigate what is a structure of the collective subspace. |
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Four decades ago, Tomonaga proposed the elementary theory of quantum mechanical collective motion of two-dimensional nuclei of N nucleons. The theory is based essentially on the neglect of 1/sqrtN against unity. Very recently we have given exact canonically conjugate momenta to quadrupole-type collective coordinates under some subsidiary conditions and have derived nuclear quadrupole-type collective Hamiltonian. Even in the case of simple two-dimensional nuclei, we have a subsidiary condition to obtain exact canonical variables. Particularly the structure of the collective subspace satisfying the subsidiary condition is studied in detail. This subsidiary condition is important to investigate what is a structure of the collective subspace. |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a2200265 4500</leader><controlfield tag="001">OLC1967398771</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230714170853.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">160206s2015 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1016/j.nuclphysa.2014.12.005</subfield><subfield code="2">doi</subfield></datafield><datafield tag="028" ind1="5" ind2="2"><subfield code="a">PQ20160617</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC1967398771</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)GBVOLC1967398771</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(PRQ)a1451-2f7ad90d4a7959f9ca4c6d19b742ab2188995263f44b94db2d63a1703d2237940</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(KEY)0073031920150000935000000001descriptionofcollectivemotionintwodimensionalnucle</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">DNB</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Nishiyama, Seiya</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Description of collective motion in two-dimensional nuclei; Tomonaga's method revisited</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2015</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Four decades ago, Tomonaga proposed the elementary theory of quantum mechanical collective motion of two-dimensional nuclei of N nucleons. 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This subsidiary condition is important to investigate what is a structure of the collective subspace.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Nuclear Theory</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">da Providência, João</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Nuclear physics <Amsterdam> / A</subfield><subfield code="d">Amsterdam [u.a.] : Elsevier, 1967</subfield><subfield code="g">935(2015), Seite 1-17</subfield><subfield code="w">(DE-627)129504033</subfield><subfield code="w">(DE-600)208861-7</subfield><subfield code="w">(DE-576)014907348</subfield><subfield code="x">0375-9474</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:935</subfield><subfield code="g">year:2015</subfield><subfield code="g">pages:1-17</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">http://dx.doi.org/10.1016/j.nuclphysa.2014.12.005</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="856" ind1="4" ind2="2"><subfield code="u">http://arxiv.org/abs/1407.3593</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2279</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">935</subfield><subfield code="j">2015</subfield><subfield code="h">1-17</subfield></datafield></record></collection>
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