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Quantization of Massless Fields with Continuous Spin
https://ir.soken.ac.jp/records/4717
https://ir.soken.ac.jp/records/4717e6887153-3175-40d8-a9b5-ebee1cc2dc7c
Item type | 学術雑誌論文 / Journal Article(1) | |||||
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公開日 | 2014-07-02 | |||||
タイトル | ||||||
タイトル | Quantization of Massless Fields with Continuous Spin | |||||
タイトル | ||||||
タイトル | Quantization of Massless Fields with Continuous Spin | |||||
言語 | en | |||||
言語 | ||||||
言語 | eng | |||||
資源タイプ | ||||||
資源タイプ識別子 | http://purl.org/coar/resource_type/c_6501 | |||||
資源タイプ | journal article | |||||
アクセス権 | ||||||
アクセス権 | metadata only access | |||||
アクセス権URI | http://purl.org/coar/access_right/c_14cb | |||||
著者 |
HIRATA, Kohji
× HIRATA, Kohji |
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著者別名 |
平田, 光司
× 平田, 光司 |
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抄録 | ||||||
内容記述タイプ | Abstract | |||||
内容記述 | Quantization is carried out of massless fields with continuous spin that correspond to particular cases of irreducible unitary representations of the Poincaré group. On the basis of the covariant field equations, obtained by Wigner, Lorentz- and gauge-covariant commutation relations and Hamiltonian densities are explicitly obtained. Our main conclusions are as follows. For the case of a single- (double-) valued representation the covariant local Hamiltonian density result only from Fermi- (Bose-) quantization, whereas the causal commutation relations result only from Bose- (Fermi-) quantization. A consistent quantum field theory is therefore impossible for any of these cases. | |||||
書誌情報 |
Progress of Theoretical Physics en : Progress of Theoretical Physics 巻 58, 号 2, p. 652-666, 発行日 1977 |
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出版者 | ||||||
出版者 | Publication Office of Progress of Theoretical Physics | |||||
ISSN | ||||||
収録物識別子タイプ | ISSN | |||||
収録物識別子 | 0033-068X | |||||
DOI | ||||||
識別子タイプ | DOI | |||||
関連識別子 | https://doi.org/10.1143/PTP.58.652 | |||||
関連名称 | 10.1143/PTP.58.652 | |||||
権利 | ||||||
権利情報 | © 1977 Progress of Theoretical Physics |