q-Deformed and c-Deformed Harmonic Oscillators(Particles and Fields)
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概要
- 論文の詳細を見る
Hamilton functions of classical deformed oscillators (c-deformed oscillators) are derived from Hamiltonians of q-deformed oscillators of the Macfarlane and Dubna types. A new scale parameter, l_q, with the dimension of length, is introduced to relate a dimensionless parameter characterizing the deformation with the natural length of the harmonic oscillator. Contraction from q-deformed oscillators to c-deformed oscillators is accomplished by keeping l_q finite while taking the limit h → 0. The c-deformed Hamilton functions for both types of oscillators are found to be invariant under discrete translations: the step of the translation for the Dubna oscillator is half of that for the Macfarlane oscillator. The c-deformed oscillator of the Macfarlane type has propagating solutions in addition to localized ones. Reinvestigation of the q-deformed oscillator carried out in the light of these findings for the c-deformed systems proves that the q-deformed systems are invariant under the same translation symmetries as the c-deformed systems and have propagating waves of the Bloch type.
- 理論物理学刊行会の論文
- 2003-10-25
著者
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Sogami Ikuo
Department Of Physics Kyoto Sangyo University
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SOGAI Ikuo
Department of Physics, Kyoto sangyo University
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KOIZUMI Kouzou
Department of Physics, Kyoto Sangyo University
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Koizumi K
Department Of Physics Kyoto Sangyo University
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Koizumi Kouzou
Department Of Physics Kyoto Sangyo University
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MIR-KASIMOV Rufat
Bogoliubov Laboratory of Theoretical Physics, Joint Institute for Nuclear Research
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Mir-kasimov Rufat
Bogoliubov Laboratory Of Theoretical Physics Joint Institute For Nuclear Research:department Of Math
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SOGAMI Ikuo
Departmevet of Physics, Kyoto Sangyo University
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Mir-Kasimov Rufat
Bogoliubov Laboratory of Theoretical Physics, Joint Institute for Nuclear Research:Department of Mathematics, Izmir Institute of High Technology
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