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Canonical quantization of the Dirac oscillator field in (1+1) and (3+1) dimensions

机译:(1 + 1)和(3 + 1)维中Dirac振荡器场的规范化量化

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he main goal of this work is to study the Dirac oscillator as a quantum field usingthe canonical formalism of quantum field theory and to develop the canonical quantizationprocedure for this system in (1 + 1) and (3 + 1) dimensions. This is possible because the Diracoscillator is characterized by the absence of the Klein paradox and by the completeness of itseigenfunctions. We show that the Dirac oscillator field can be seen as constituted by infinitedegrees of freedom which are identified as decoupled quantum linear harmonic oscillators. Weobserve that while for the free Dirac field the energy quanta of the infinite harmonic oscillatorsare the relativistic energies of free particles, for the Dirac oscillator field the quanta are theenergies of relativistic linear harmonic oscillators.
机译:这项工作的主要目的是使用量子场论的规范形式来研究狄拉克振荡器作为量子场,并开发该系统在(1 + 1)和(3 +1)维度上的规范量化程序。这是可能的,因为Diracoscillator的特点是不存在Klein悖论,并且其本征函数完整。我们证明狄拉克振荡器场可以看作是由无限自由度构成的,这些自由度被确定为解耦量子线性谐波振荡器。我们观察到,对于自由狄拉克场,无限谐波振荡器的能量量子是自由粒子的相对论能量,对于狄拉克振荡器场,量子是相对论线性谐波振荡器的能量。

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