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Equation 92 · Part 4 · The Entry a Relabeling Cannot Write

Symbol H_S

ΔEΛ(t)=⟨Hf⟩−⟨HS⟩(t)=−ℏω2cos⁡(2gt).\Delta E_\Lambda(t) = \langle H_f\rangle - \langle H_S\rangle(t) = -\frac{\hbar\omega}{2}\cos(2gt).
HSH_S

What this part means

HSH_S is one of the signed contributions combined to compute the quantity on the left.

Its job in the formula

HSH_S is one of the signed contributions combined to compute the quantity on the left.

The passage around this formula

the standard two-level exchange solution, exact for all t under this Hamiltonian. From it, ⟨\langle HSH_S ⟩(t)\rangle(t) = (ℏ\hbarω\omega/2)[cos⁡2(gt)\cos^2(gt) - sin⁡2(gt)\sin^2(gt)] = (ℏ\hbarω\omega/2)cos⁡(2gt)\cos(2gt) , while ⟨\langle HfH_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|HfH_f|e,g⟩\rangle = ℏ\hbarω\omega/2 -…

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Learn the underlying idea

A subscript is a label attached below a symbol. It often selects a time step, component, category, or member of a sequence.

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