{"type":"rich","published":"2022-11-03 16:33:44","image_url":null,"html":"<iframe src=\"https://hatenablog-parts.com/embed?url=https%3A%2F%2Fenakai00.hatenablog.com%2Fentry%2F2022%2F11%2F03%2F163344\" title=\"Quantum Information and Quantum Optics with Superconducting Circuits - Exercise Solutions (Chapter 9)  - \u3081\u3082\u3081\u3082\" class=\"embed-card embed-blogcard\" scrolling=\"no\" frameborder=\"0\" style=\"display: block; width: 100%; height: 190px; max-width: 500px; margin: 10px 0px;\"></iframe>","categories":[],"author_url":"https://blog.hatena.ne.jp/enakai00/","title":"Quantum Information and Quantum Optics with Superconducting Circuits - Exercise Solutions (Chapter 9) ","description":"9.1 (1) So, by setting , we have: where (2) We apply an adiabatic change to . On the other hand, Hence, from the Schroedinger equation , we have: From the definition of , we have: So, --- (2-1)By differentiating the both sides of , So, from (2-1), we have: (3) Since , we have: (4) where The eigenval\u2026","provider_name":"Hatena Blog","version":"1.0","url":"https://enakai00.hatenablog.com/entry/2022/11/03/163344","author_name":"enakai00","width":"100%","blog_url":"https://enakai00.hatenablog.com/","height":"190","blog_title":"\u3081\u3082\u3081\u3082","provider_url":"https://hatena.blog"}