Equation 91 · The Entry a Relabeling Cannot Write

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H_{SB}

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H_{SB}

Symbol H_SB

$H_S$ B is a part of this expression. Its role is fixed by the surrounding article and by the operations shown in the formula.

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subscript

The lower label selects a particular version, component, or indexed member of the quantity. For example, x₀ and xₜ can be values at different positions.

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How to interpret it

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What the article says around this equation

the standard two-level exchange solution, exact for all t under this Hamiltonian. From it, $\langle$ $H_S$ $\rangle(t)$ = ( $\hbar$ $\omega$ /2)[ $\cos^2(gt)$ - $\sin^2(gt)$ ] = ( $\hbar$ $\omega$ /2) $\cos(2gt)$ , while $\langle$ $H_f$ $\rangle$ is exactly time-independent — a general fact for any state evolving under its own generator, not special to this one — and equal here to $\langle$ e,g| $H_f$ |e,g $\rangle$ = $\hbar$ $\omega$ /2 - $\hbar$ $\omega$ /2 + 0 = 0 , since $H_{SB}$ is purely off-diagonal in this basis. The ledger reading follows immediately:

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Sources cited in the article section

[12] Circuit Quantum Electrodynamics ↗

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