{"author_url":"https://blog.hatena.ne.jp/enakai00/","html":"<iframe src=\"https://hatenablog-parts.com/embed?url=https%3A%2F%2Fenakai00.hatenablog.com%2Fentry%2F2022%2F10%2F30%2F090609\" title=\"Quantum Information and Quantum Optics with Superconducting Circuits - Exercise Solutions (Chapter 8)  - \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>","provider_url":"https://hatena.blog","version":"1.0","author_name":"enakai00","blog_title":"\u3081\u3082\u3081\u3082","height":"190","title":"Quantum Information and Quantum Optics with Superconducting Circuits - Exercise Solutions (Chapter 8) ","provider_name":"Hatena Blog","type":"rich","published":"2022-10-30 09:06:09","url":"https://enakai00.hatenablog.com/entry/2022/10/30/090609","categories":[],"blog_url":"https://enakai00.hatenablog.com/","image_url":null,"width":"100%","description":"8.1 By expanding the tensor product, we have the all possible binary numbers.As discussed in 6.1.4, for a single qubit, Hadamard gate can be implemented as: using the coherent drive: that's on resonance and .To apply it to identical flux qubits, we have to have different gaps on neighboring qubits s\u2026"}