用波动参考系测量爱因斯坦固体定容时的平均能量和摩尔比热

Y. Shin
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引用次数: 3

摘要

我们报告了爱因斯坦固体中的观察者效应,这是一个量子力学系统,由观察者参照系的波动引起;迄今为止的研究都是在假设观察者的参照系在整个测量过程中保持不变的情况下进行的,因此,在整个测量过程中实际测量到的是一个未解决的问题,在这个问题中,观察者的参照系被假设是波动的。我们研究了一个具有波动参考系的观察者在恒定体积下测量爱因斯坦固体的平均能量和摩尔比热。爱因斯坦固体由每摩尔N个相同的非相互作用的简谐振子组成,其中N是温度为T时的阿伏伽德罗数。爱因斯坦固体的平均能量和摩尔比热在恒定体积下为观察者参照系的两种类型的波动而制定,以便考虑教学和实验演示。爱因斯坦固体的平均能量由正则系综平均的定义表述,其恒容摩尔比热由平均能量与t求导得到。爱因斯坦固体的恒容摩尔比热在低温下根据观察者参照系的起伏分布表现出新的特征:T = 0 K时,方波和锯齿波波动分别为0和3R,其中R为气体常数。
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The Average Energy and Molar Specific Heat at Constant Volume of an Einstein Solid Measured by an Observer with Fluctuating Frame of Reference
We report an observer effect in an Einstein solid, a quantum-mechanical system, induced by fluctuations of an observer’s frame of reference; which has been studied so far under the assumption that the observer’s frame of reference remains constant throughout the performance of a measurement, thus, what is actually measured throughout the performance of a measurement is an unresolved problem during which the observer’s frame of reference is assumed to fluctuate. We investigate the average energy and molar specific heat at constant volume of an Einstein solid measured by an observer with fluctuating frame of reference. The Einstein solid consists of N identical non-interacting simple harmonic oscillators per mole, where N is the Avogadro’s number at temperature T . The average energy and molar specific heat at constant volume of the Einstein solid are formulated for two types of fluctuations of the observer’s frame of reference in order to consider pedagogical and experimental demonstrations. The average energy of the Einstein solid is formulated from the definition of canonical ensemble average and the molar specific heat at constant volume of it is calculated by differentiating the average energy with T. The molar specific heat at constant volume of the Einstein solid exhibits novel features at low temperatures according to the distribution of fluctuations of the observer’s frame of reference: 0 and 3R at T = 0 K for square-wave and sawtooth-wave fluctuations, respectively, where R is the gas constant.
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