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Equation 49 · Part 2 · The Clock That Comes Back Wrong by Exactly Its Mass

Symbol L_rm G

Φ[LG]\Phi[\mathcal L_{\rm G}]
LGL_{\rm G}

What this part means

LrL_rm G is a part of this expression. Its role is fixed by the surrounding article and by the operations shown in the formula.

Its job in the formula

LrL_rm G is a part of this expression. Its role is fixed by the surrounding article and by the operations shown in the formula.

The passage around this formula

Nothing about this phase disturbs conservation of energy or momentum, and it is worth saying explicitly why. Φ\Phi[LG\mathcal L_{\rm G}] does not come from a new term added to any Hamiltonian; it comes from how already-unitary translation and boost operators compose. Each operator in the product T(b\mathbf b)G(v\mathbf v)T(-b\mathbf b)G(-v\mathbf v) conserves probability on its own, and the product of unitaries is unitary regardless of whether the factors commute, so the loop as a whole still conserves probability and leaves every expectation value of energy and momentum exactly where an ordinary, non-extended calculation would put it. What changes is not a conserved quantity but the bookkeeping of…

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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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