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量子力学の統計的解釈を,古典的限界から推論する
1Laboratory for Nuclear Studies, Cornell University, Ithaca, New York 14853, USA. kg13@cornell.edu
Nature
|June 13, 2000
まとめ
この研究は,量子力学の統計的解釈が,離散変数を持つシステムに対するシュロディンガー方程式から部分的に導出可能であることを示唆しています. この解釈は,古典的な総運動の記述によって示唆されているが,連続変数についてはそうではないことが示されている.
科学分野:
- 量子力学は,量子力学という
- 統計の解釈 統計の解釈
- 理論物理学の理論物理学です.
背景:
- 量子力学の統計的解釈は,典型的には独立した公理である.
- シュロディンガー方程式は量子システムの進化を統制する.
研究 の 目的:
- 量子力学の統計的解釈がシュロディンガー方程式から推論できるかどうかを調査する.
- 古典的記述と量子的統計的解釈の関係を探求する.
主な方法:
- 連続的および離散的自由度 (例えば座標とスピン) の両方のシステムの分析.
- システムの総運動を古典的に記述できるという要件を適用する.
主要な成果:
- 離散変数の統計的解釈は,特定の古典的条件下でのシュロディンガー方程式によって暗示されています.
- この意味は連続変数には及ばない.
結論:
- 量子力学の統計的解釈は,離散変数のシュレーディンガー方程式から完全に独立しているわけではない.
- すべての変数に対する統計的解釈の完全な導出は,まだ未解決の課題です.
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