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On a classical limit for electronic degrees of freedom that satisfies the Pauli exclusion principle

机译:满足Pauli排除原则的电子自由度的经典限制

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Fermions need to satisfy the Pauli exclusion principle: no two can be in the same state. This restriction is most compactly expressed in a second quantization formalism by the requirement that the creation and annihilation operators of the electrons satisfy anti- commutation relations. The usual dassical limit of quantum me- chanics corresponds to creation and annihilation operators that satisfy commutation relations. as for a harmonic oscillator. we discuss a simple classical limit for Fermions. This limit is shown to correspond to an anharmonic oscillator. with just one bound excited state. The vibrational quantum number of this anharmonic oscillator, which is therefore limited to the range 0 to 1, is the classical analog of the quantum mechanical occupancy. This inter- pretation is also true for Bosons, except that they correspond to a harmonic oscillator so that the occupancy is from 0 up. The formalism is intended to be useful for simulating the behavior of highly correlated Fermionic systems, so the extension to many electron states is also discussed.
机译:费米子必须满足保利排除原则:任何两个都不能处于同一状态。在第二个量化形式主义中,通过电子的生成和an灭算符满足反换向关系的要求,可以最紧凑地表达这一限制。量子力学通常常见的极限是满足换向关系的创造和an灭算符。至于谐波振荡器。我们讨论了费米子的一个简单的经典极限。示出该极限对应于非谐振荡器。只具有一种束缚的兴奋状态因此,该非谐振荡器的振动量子数被限制在0到1的范围内,是量子力学占有率的经典模拟。这种解释对于玻色子也适用,只是它们对应于谐波振荡器,因此占用率为0到0。形式主义旨在用于模拟高度相关的费米电子系统的行为,因此也讨论了扩展到许多电子态的问题。

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