Options for angular momentum projection II: A finite sum representation of the Hill-Wheeler projector

Abstract An exact and finite sum representation of the Hill-Wheeler projection operator is obtained under the provision that the state on which the operator acts can be expanded as$$\left| {\psi _\alpha } \right\rangle = \sum\limits_{J = J_{\min } }^{J_{\max } } {c_J^\alpha \left| {J,\alpha } \right...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Kelemen, A. [verfasserIn] Dreizler, R. M.

Format:	Artikel
Sprache:	Englisch

Erschienen:	1976

Schlagwörter:	Angular Momentum Elementary Particle High Spin Spin State Integration Method

Anmerkung:	© Springer-Verlag 1976

Übergeordnetes Werk:	Enthalten in: Zeitschrift für Physik. A, Hadrons and nuclei - Springer-Verlag, 1975, 278(1976), 3 vom: Sept., Seite 269-274
Übergeordnetes Werk:	volume:278 ; year:1976 ; number:3 ; month:09 ; pages:269-274

Links:	Volltext

DOI / URN:	10.1007/BF01409178

Katalog-ID:	OLC2029693243

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520			\|a Abstract An exact and finite sum representation of the Hill-Wheeler projection operator is obtained under the provision that the state on which the operator acts can be expanded as$$\left\| {\psi _\alpha } \right\rangle = \sum\limits_{J = J_{\min } }^{J_{\max } } {c_J^\alpha \left\| {J,\alpha } \right\rangle .} $$ The result provides a definite advantage over numerical integration methods, especially if high spin states are considered.
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allfields	10.1007/BF01409178 doi (DE-627)OLC2029693243 (DE-He213)BF01409178-p DE-627 ger DE-627 rakwb eng 530 VZ Kelemen, A. verfasserin aut Options for angular momentum projection II: A finite sum representation of the Hill-Wheeler projector 1976 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1976 Abstract An exact and finite sum representation of the Hill-Wheeler projection operator is obtained under the provision that the state on which the operator acts can be expanded as$$\left\| {\psi _\alpha } \right\rangle = \sum\limits_{J = J_{\min } }^{J_{\max } } {c_J^\alpha \left\| {J,\alpha } \right\rangle .} $$ The result provides a definite advantage over numerical integration methods, especially if high spin states are considered. Angular Momentum Elementary Particle High Spin Spin State Integration Method Dreizler, R. M. aut Enthalten in Zeitschrift für Physik. A, Hadrons and nuclei Springer-Verlag, 1975 278(1976), 3 vom: Sept., Seite 269-274 (DE-627)129415375 (DE-600)189286-1 (DE-576)014793679 0939-7922 nnns volume:278 year:1976 number:3 month:09 pages:269-274 https://doi.org/10.1007/BF01409178 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_24 GBV_ILN_30 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_59 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_70 GBV_ILN_105 GBV_ILN_130 GBV_ILN_150 GBV_ILN_170 GBV_ILN_201 GBV_ILN_2006 GBV_ILN_2010 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2027 GBV_ILN_2185 GBV_ILN_2192 GBV_ILN_2221 GBV_ILN_2279 GBV_ILN_2360 GBV_ILN_4012 GBV_ILN_4028 GBV_ILN_4035 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4277 GBV_ILN_4302 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4319 GBV_ILN_4320 GBV_ILN_4323 GBV_ILN_4336 GBV_ILN_4700 AR 278 1976 3 09 269-274
spelling	10.1007/BF01409178 doi (DE-627)OLC2029693243 (DE-He213)BF01409178-p DE-627 ger DE-627 rakwb eng 530 VZ Kelemen, A. verfasserin aut Options for angular momentum projection II: A finite sum representation of the Hill-Wheeler projector 1976 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1976 Abstract An exact and finite sum representation of the Hill-Wheeler projection operator is obtained under the provision that the state on which the operator acts can be expanded as$$\left\| {\psi _\alpha } \right\rangle = \sum\limits_{J = J_{\min } }^{J_{\max } } {c_J^\alpha \left\| {J,\alpha } \right\rangle .} $$ The result provides a definite advantage over numerical integration methods, especially if high spin states are considered. Angular Momentum Elementary Particle High Spin Spin State Integration Method Dreizler, R. M. aut Enthalten in Zeitschrift für Physik. A, Hadrons and nuclei Springer-Verlag, 1975 278(1976), 3 vom: Sept., Seite 269-274 (DE-627)129415375 (DE-600)189286-1 (DE-576)014793679 0939-7922 nnns volume:278 year:1976 number:3 month:09 pages:269-274 https://doi.org/10.1007/BF01409178 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_24 GBV_ILN_30 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_59 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_70 GBV_ILN_105 GBV_ILN_130 GBV_ILN_150 GBV_ILN_170 GBV_ILN_201 GBV_ILN_2006 GBV_ILN_2010 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2027 GBV_ILN_2185 GBV_ILN_2192 GBV_ILN_2221 GBV_ILN_2279 GBV_ILN_2360 GBV_ILN_4012 GBV_ILN_4028 GBV_ILN_4035 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4277 GBV_ILN_4302 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4319 GBV_ILN_4320 GBV_ILN_4323 GBV_ILN_4336 GBV_ILN_4700 AR 278 1976 3 09 269-274
allfields_unstemmed	10.1007/BF01409178 doi (DE-627)OLC2029693243 (DE-He213)BF01409178-p DE-627 ger DE-627 rakwb eng 530 VZ Kelemen, A. verfasserin aut Options for angular momentum projection II: A finite sum representation of the Hill-Wheeler projector 1976 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1976 Abstract An exact and finite sum representation of the Hill-Wheeler projection operator is obtained under the provision that the state on which the operator acts can be expanded as$$\left\| {\psi _\alpha } \right\rangle = \sum\limits_{J = J_{\min } }^{J_{\max } } {c_J^\alpha \left\| {J,\alpha } \right\rangle .} $$ The result provides a definite advantage over numerical integration methods, especially if high spin states are considered. Angular Momentum Elementary Particle High Spin Spin State Integration Method Dreizler, R. M. aut Enthalten in Zeitschrift für Physik. A, Hadrons and nuclei Springer-Verlag, 1975 278(1976), 3 vom: Sept., Seite 269-274 (DE-627)129415375 (DE-600)189286-1 (DE-576)014793679 0939-7922 nnns volume:278 year:1976 number:3 month:09 pages:269-274 https://doi.org/10.1007/BF01409178 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_24 GBV_ILN_30 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_59 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_70 GBV_ILN_105 GBV_ILN_130 GBV_ILN_150 GBV_ILN_170 GBV_ILN_201 GBV_ILN_2006 GBV_ILN_2010 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2027 GBV_ILN_2185 GBV_ILN_2192 GBV_ILN_2221 GBV_ILN_2279 GBV_ILN_2360 GBV_ILN_4012 GBV_ILN_4028 GBV_ILN_4035 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4277 GBV_ILN_4302 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4319 GBV_ILN_4320 GBV_ILN_4323 GBV_ILN_4336 GBV_ILN_4700 AR 278 1976 3 09 269-274
allfieldsGer	10.1007/BF01409178 doi (DE-627)OLC2029693243 (DE-He213)BF01409178-p DE-627 ger DE-627 rakwb eng 530 VZ Kelemen, A. verfasserin aut Options for angular momentum projection II: A finite sum representation of the Hill-Wheeler projector 1976 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1976 Abstract An exact and finite sum representation of the Hill-Wheeler projection operator is obtained under the provision that the state on which the operator acts can be expanded as$$\left\| {\psi _\alpha } \right\rangle = \sum\limits_{J = J_{\min } }^{J_{\max } } {c_J^\alpha \left\| {J,\alpha } \right\rangle .} $$ The result provides a definite advantage over numerical integration methods, especially if high spin states are considered. Angular Momentum Elementary Particle High Spin Spin State Integration Method Dreizler, R. M. aut Enthalten in Zeitschrift für Physik. A, Hadrons and nuclei Springer-Verlag, 1975 278(1976), 3 vom: Sept., Seite 269-274 (DE-627)129415375 (DE-600)189286-1 (DE-576)014793679 0939-7922 nnns volume:278 year:1976 number:3 month:09 pages:269-274 https://doi.org/10.1007/BF01409178 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_24 GBV_ILN_30 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_59 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_70 GBV_ILN_105 GBV_ILN_130 GBV_ILN_150 GBV_ILN_170 GBV_ILN_201 GBV_ILN_2006 GBV_ILN_2010 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2027 GBV_ILN_2185 GBV_ILN_2192 GBV_ILN_2221 GBV_ILN_2279 GBV_ILN_2360 GBV_ILN_4012 GBV_ILN_4028 GBV_ILN_4035 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4277 GBV_ILN_4302 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4319 GBV_ILN_4320 GBV_ILN_4323 GBV_ILN_4336 GBV_ILN_4700 AR 278 1976 3 09 269-274
allfieldsSound	10.1007/BF01409178 doi (DE-627)OLC2029693243 (DE-He213)BF01409178-p DE-627 ger DE-627 rakwb eng 530 VZ Kelemen, A. verfasserin aut Options for angular momentum projection II: A finite sum representation of the Hill-Wheeler projector 1976 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1976 Abstract An exact and finite sum representation of the Hill-Wheeler projection operator is obtained under the provision that the state on which the operator acts can be expanded as$$\left\| {\psi _\alpha } \right\rangle = \sum\limits_{J = J_{\min } }^{J_{\max } } {c_J^\alpha \left\| {J,\alpha } \right\rangle .} $$ The result provides a definite advantage over numerical integration methods, especially if high spin states are considered. Angular Momentum Elementary Particle High Spin Spin State Integration Method Dreizler, R. M. aut Enthalten in Zeitschrift für Physik. A, Hadrons and nuclei Springer-Verlag, 1975 278(1976), 3 vom: Sept., Seite 269-274 (DE-627)129415375 (DE-600)189286-1 (DE-576)014793679 0939-7922 nnns volume:278 year:1976 number:3 month:09 pages:269-274 https://doi.org/10.1007/BF01409178 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_24 GBV_ILN_30 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_59 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_70 GBV_ILN_105 GBV_ILN_130 GBV_ILN_150 GBV_ILN_170 GBV_ILN_201 GBV_ILN_2006 GBV_ILN_2010 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2027 GBV_ILN_2185 GBV_ILN_2192 GBV_ILN_2221 GBV_ILN_2279 GBV_ILN_2360 GBV_ILN_4012 GBV_ILN_4028 GBV_ILN_4035 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4277 GBV_ILN_4302 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4319 GBV_ILN_4320 GBV_ILN_4323 GBV_ILN_4336 GBV_ILN_4700 AR 278 1976 3 09 269-274
language	English
source	Enthalten in Zeitschrift für Physik. A, Hadrons and nuclei 278(1976), 3 vom: Sept., Seite 269-274 volume:278 year:1976 number:3 month:09 pages:269-274
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topic_facet	Angular Momentum Elementary Particle High Spin Spin State Integration Method
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author	Kelemen, A.
spellingShingle	Kelemen, A. ddc 530 misc Angular Momentum misc Elementary Particle misc High Spin misc Spin State misc Integration Method Options for angular momentum projection II: A finite sum representation of the Hill-Wheeler projector
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topic_title	530 VZ Options for angular momentum projection II: A finite sum representation of the Hill-Wheeler projector Angular Momentum Elementary Particle High Spin Spin State Integration Method
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title	Options for angular momentum projection II: A finite sum representation of the Hill-Wheeler projector
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title_full	Options for angular momentum projection II: A finite sum representation of the Hill-Wheeler projector
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title_sort	options for angular momentum projection ii: a finite sum representation of the hill-wheeler projector
title_auth	Options for angular momentum projection II: A finite sum representation of the Hill-Wheeler projector
abstract	Abstract An exact and finite sum representation of the Hill-Wheeler projection operator is obtained under the provision that the state on which the operator acts can be expanded as$$\left\| {\psi _\alpha } \right\rangle = \sum\limits_{J = J_{\min } }^{J_{\max } } {c_J^\alpha \left\| {J,\alpha } \right\rangle .} $$ The result provides a definite advantage over numerical integration methods, especially if high spin states are considered. © Springer-Verlag 1976
abstractGer	Abstract An exact and finite sum representation of the Hill-Wheeler projection operator is obtained under the provision that the state on which the operator acts can be expanded as$$\left\| {\psi _\alpha } \right\rangle = \sum\limits_{J = J_{\min } }^{J_{\max } } {c_J^\alpha \left\| {J,\alpha } \right\rangle .} $$ The result provides a definite advantage over numerical integration methods, especially if high spin states are considered. © Springer-Verlag 1976
abstract_unstemmed	Abstract An exact and finite sum representation of the Hill-Wheeler projection operator is obtained under the provision that the state on which the operator acts can be expanded as$$\left\| {\psi _\alpha } \right\rangle = \sum\limits_{J = J_{\min } }^{J_{\max } } {c_J^\alpha \left\| {J,\alpha } \right\rangle .} $$ The result provides a definite advantage over numerical integration methods, especially if high spin states are considered. © Springer-Verlag 1976
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title_short	Options for angular momentum projection II: A finite sum representation of the Hill-Wheeler projector
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