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Equation 24 · The Entry a Relabeling Cannot Write

What does this equation mean?

ΔEΛ(ρ):=Tr[ρDΛ],\Delta E_\Lambda(\rho) := \mathrm{Tr}[\rho D_\Lambda],

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Inputs and operationsTr[ρ D_Lambda]
Result or conditionΔ E_Lambda(ρ) :
How to read the two sides of this formula. Follow the article passage for the meaning of each quantity.

This equation states an equality: the expressions on both sides have the same value under the article’s assumptions. Read the equation part by part below; each part has a contextual explanation and a link to its mathematical background.

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ΔEΛ\Delta E_\Lambda

Symbol Δ E_Lambda

Δ ELE_Lambda is part of the quantity the equation computes from the expression on the right.

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ρ\rho

Symbol ρ

ρ is an argument of the function-like quantity on the left; its role is set by that function’s stated inputs.

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DΛD_\Lambda

Symbol D_Lambda

DLD_Lambda is an input to the expression that computes the quantity on the left.

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=

=

The expressions on both sides represent the same quantity under the stated assumptions.

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change

change

Capital delta attached to a quantity marks a difference between two values of that quantity; the article’s sign convention determines the order.

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How to interpret it

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What the article says around this equation

DΛD_\Lambda is Hermitian on Hf\mathcal H_f — a positive, unital map applied to a self-adjoint input stays self-adjoint — and it carries units of energy, since both terms do. Its state-dependent reading, ΔEΛ(ρ):=Tr[ρDΛ]\Delta E_\Lambda(\rho) := \mathrm{Tr}[\rho D_\Lambda]. is a real number in units of energy for every fine state ρ\rho : how much the coarse description, evaluated through HcH_c pulled back along Λ\Lambda , disagrees with the fine description’s own HfH_f , for that specific state. Because expectation values determine a Hermitian operator uniquely — two Hermitian operators with the same trace against every density matrix are the same operator — the strongest statement follows at once: Δ\Delta EΛ(ρ)E_\Lambda(\rho) = 0 for every fine state ρ\rho…
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DΛD_\Lambda is Hermitian on Hf\mathcal H_f — a positive, unital map applied to a self-adjoint input stays self-adjoint — and it carries units of energy, since both terms do. Its state-dependent reading, ΔEΛ(ρ):=Tr[ρDΛ]\Delta E_\Lambda(\rho) := \mathrm{Tr}[\rho D_\Lambda]. is a real number in units of energy for every fine state ρ\rho : how much the coarse description, evaluated through HcH_c pulled back along Λ\Lambda , disagrees with the fine description’s own HfH_f , for that specific state. Because expectation values determine a Hermitian operator uniquely — two Hermitian operators with the same trace against every density matrix are the same operator — the strongest statement follows at once: Δ\Delta EΛ(ρ)E_\Lambda(\rho) = 0 for every fine state ρ\rho if and only if DΛD_\Lambda = 0 as an operator identity, that is, if and only if Λ†(Hc)\Lambda^\dagger(H_c) = HfH_f exactly. Energy is preserved for every possible input under that one algebraic condition, never as a statistical tendency and never approximately.

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