← All parts of this equation

Equation 92 · Part 2 · The Entry a Relabeling Cannot Write

Symbol t

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).
tt

What this part means

t is an argument of the function-like quantity on the left; its role is set by that function’s stated inputs.

Its job in the formula

t is an argument of the function-like quantity on the left; its role is set by that function’s stated inputs.

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…

Read this part in the article →

Learn the underlying idea

A variable is a named place for a value. Its letter is a local label: x can mean position in one formula and a data point in another.

Open the illustrated variables: a letter stands for a value guide →

See this notation across published equations →

Sources cited in the article section

These citations provide research context; check each source for the exact claim it supports.