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The knowledge of the distribution function is significant for the study of transport phenomena. Many quantum states exist in a system, and each quantum state will have a number of distributions of \(n_i\) , as shown in Fig. 5.1, where \(i = 1,2,3,\ldots \) The last quantum state can be represented by \(n_{\Omega }\) . Therefore, the summation of \(n_i\) is equal to the total number of particles (N) distributed across the quantum states.

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Nanoscale Transport Processes

  • 章节

  • 发表日期：

    2025年

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  • Arvind Pattamatta,
  • Sarit K. Das

摘要

The knowledge of the distribution function is significant for the study of transport phenomena. Many quantum states exist in a system, and each quantum state will have a number of distributions of \(n_i\) , as shown in Fig. 5.1, where \(i = 1,2,3,\ldots \) The last quantum state can be represented by \(n_{\Omega }\) . Therefore, the summation of \(n_i\) is equal to the total number of particles (N) distributed across the quantum states.