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        "quote": "where $\\hbar = h / 2 \\pi$ is Planck’s constant divided by 2$\\pi$. Such a pair of observables are said to be <u class=\"concept-term\" data-concept-identity=\"urn:uuid:58ad6734-94de-4363-a2b2-559a9a10aebb\" data-concept-route=\"/concept-identities#concept-58ad6734-94de-4363-a2b2-559a9a10aebb\" id=\"first-5d7e3e3238db3e40f868-en\">complementary</u>. With some restriction on admissible domains they hold for the position operator $Q = A _ { x }$ and the momentum operator $P = - i \\hbar { \\bf d } / { \\bf d } x$ discussed in <a href=\"../chapter-13/06-unbounded-operators#example-13-19\" class=\"cross-reference\" id=\"xref-01-basic-concepts-7\" data-reference=\"example-13-19\">Examples 13.19</a> and 13.20. For, let $f$ be a function in the intersection of their domains, then",
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