nLab quantum decoherence

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Quantum systems

quantum logic


quantum physics


quantum probability theory – observables and states


quantum information


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Contents

Idea

In quantum physics decoherence refers to the disappearance of quantum entanglement and superposition in the limit where small quantum mechanical systems are coupled to large thermal baths?.

This has been argued to resolve (and has been argued not to resolve) the problem with the interpretation of quantum measurement.

Properties

Environmental representation of quantum channels

The crux of dynamical quantum decoherence is that fundamentally the (time-)evolution of any quantum system ℋ\mathscr{H} may be assumed unitary (say via a Schrödinger equation) when taking the whole evolution of its environment ℬ\mathscr{B} (the “bath”, ultimately the whole observable universe) into account, too, in that the evolution of the total system ℋ⊗ℬ\mathscr{H} \otimes \mathscr{B} is given by a unitary operator

evolve:ℋ⊗ℬ ⟶ ℋ⊗ℬ |ψ,β⟩ ↦ U tot|ψ,β⟩, \array{ \mathllap{ evolve \;\colon\; } \mathscr{H} \otimes \mathscr{B} &\longrightarrow& \mathscr{H} \otimes \mathscr{B} \\ \left\vert \psi, \beta \right\rangle &\mapsto& U_{tot} \left\vert \psi, \beta \right\rangle \mathrlap{\,,} }

after understanding the mixed states ρ:ℋ⊗ℋ *\rho \,\colon\, \mathscr{H} \otimes \mathscr{H}^\ast (density matrices) of the given quantum system as coupled to any given mixed state env:ℬ⊗ℬ *env \,\colon\, \mathscr{B} \otimes \mathscr{B}^\ast of the bath (via tensor product)

couple:ℋ⊗ℋ * ⟶ (ℋ⊗ℬ)⊗(ℋ⊗ℬ) * ρ ↦ ρ⊗env; \array{ \mathllap{ couple \;\colon\; } \mathscr{H} \otimes \mathscr{H}^\ast & \longrightarrow & (\mathscr{H} \otimes \mathscr{B}) \otimes (\mathscr{H} \otimes \mathscr{B})^\ast \\ \rho &\mapsto& \rho \otimes env \mathrlap{\,;} }

…the only catch being that one cannot — and in any case does not (want or need to) — keep track of the precise quantum state of the environment/bath, instead only of its average effect on the given quantum system, which by the rule of quantum probability is the mixed state that remains after the partial trace over the environment:

(1)average:(ℋ⊗ℬ)⊗(ℋ⊗ℬ) * ⟶ ℋ⊗ℋ * ρ^ ↦ Tr ℬ(ρ^). \array{ \mathllap{ average \;\colon\; } (\mathscr{H} \otimes \mathscr{B}) \otimes (\mathscr{H} \otimes \mathscr{B})^\ast &\longrightarrow& \mathscr{H} \otimes \mathscr{H}^\ast \\ \widehat{\rho} &\mapsto& Tr_{\mathscr{B}}\big(\widehat{\rho}\big) \mathrlap{\,.} }

In summary this means for practical purposes that the probabilistic evolution of quantum systems ℋ\mathscr{H} is always of the composite form

ℋ⊗ℋ * →couple to environment (ℋ ⊗ ℬ)⊗(ℋ ⊗ ℬ) * →total unitary evolution (ℋ ⊗ ℬ)⊗(ℋ ⊗ ℬ) * →average over environment ℋ⊗ℋ * ρ ↦ ρ⊗env ↦ U tot⋅(ρ⊗env)⋅U tot † ↦ Tr ℬ(U tot⋅(ρ⊗env)⋅U tot †) \array{ \mathscr{H} \otimes \mathscr{H}^\ast & \xrightarrow{ \array{ \text{couple to} \\ \text{environment} } } & \left( \array{ \mathscr{H} \\ \otimes \\ \mathscr{B} } \right) \otimes \left( \array{ \mathscr{H} \\ \otimes \\ \mathscr{B} } \right)^\ast & \xrightarrow{ \array{ \text{total unitary} \\ \text{evolution} } } & \left( \array{ \mathscr{H} \\ \otimes \\ \mathscr{B} } \right) \otimes \left( \array{ \mathscr{H} \\ \otimes \\ \mathscr{B} } \right)^\ast & \xrightarrow{ \array{ \text{average over} \\ \text{environment} } } & \;\;\;\; \mathscr{H} \otimes \mathscr{H}^\ast \\ \rho &\mapsto& \rho \otimes env &\mapsto& \mathclap{ U_{tot} \cdot (\rho \otimes env) \cdot U_{tot}^\dagger } &\mapsto& \;\;\;\;\;\;\;\;\;\;\;\; \mathclap{ Tr_{\mathscr{B}} \big( U_{tot} \cdot (\rho \otimes env) \cdot U_{tot}^\dagger \big) } }

This composite turns out to be a “quantum channel”

The realization of a quantum channel in the form (2) is also called an environmental representation (eg. Życzkowski & Bengtsson 2004 (3.5)).

In fact all quantum channels on a fixed Hilbert space have such an evironmental representation:

Proposition

(environmental representation of quantum channels)

Every quantum channel

chan:ℋ⊗ℋ *⟶ℋ⊗ℋ * chan \;\;\colon\;\; \mathscr{H} \otimes \mathscr{H}^\ast \longrightarrow \mathscr{H} \otimes \mathscr{H}^\ast

may be written as

  1. a unitary quantum channel, induced by a unitary operator U tot:ℋ⊗ℬ→ℋ⊗ℬU_{tot} \,\colon\, \mathscr{H} \otimes \mathscr{B} \to \mathscr{H} \otimes \mathscr{B}

  2. on a compound system with some ℬ\mathscr{B} (the “bath”), yielding a total system Hilbert space ℋ⊗ℬ\mathscr{H} \otimes \mathscr{B} (tensor product),

  3. and acting on the given mixed state ρ\rho coupled (tensored) with any pure state of the bath system,

  4. followed by partial trace (averaging) over ℬ\mathscr{B} (leading to decoherence in the remaining state)

in that

(2)chan(ρ)=Tr ℬ(U tot⋅(ρ⊗env)⋅U tot †). chan(\rho) \;\;=\;\; Tr_{\mathscr{B}} \big( U_{tot} \cdot (\rho \otimes env) \cdot U_{tot}^\dagger \big) \,.

Conversely, every operation of the form (2) is a quantum channel.

This is originally due to Lindblad 1975 (see top of p. 149 and inside the proof of Lem. 5). For exposition and review see: Nielsen & Chuang 2000 §8.2.2-8.2.3. An account of the infinite-dimensional case is in Attal, Thm. 6.5 & 6.7. These authors focus on the case that the environment is in a pure state, the (parital) generalization to mixed environment states is discussed in Bengtsson & Życzkowski 2006 pp. 258.

Proof

We spell out the proof assuming finite-dimensional Hilbert spaces. (The general case follows the same idea, supplemented by arguments that the following sums converge.)

Now given a completely positive map:

chan:ℋ⊗ℋ *⟶ℋ⊗ℋ *, chan \,\colon\, \mathscr{H} \otimes \mathscr{H}^\ast \longrightarrow \mathscr{H} \otimes \mathscr{H}^\ast \,,

then by operator-sum decomposition there exists a set (finite, under our assumptions) inhabited by at least one element

s ini:S, s_{ini} \,\colon\, S \,,

and an SS-indexed set of linear operators

(3)s:S⊢E s:ℋ⟶ℋ,with∑sE s †⋅E s=Id, s \,\colon\, S \;\;\; \vdash \;\;\; E_s \;\colon\; \mathscr{H} \longrightarrow \mathscr{H} \,,\;\;\;\; \text{with} \;\;\;\; \underset{s}{\sum} E_s^\dagger \cdot E_s \,=\, Id \mathrlap{\,,}

such that

chan(ρ)=∑sE s⋅ρ⋅E s †. chan(\rho) \;=\; \underset{s}{\sum} \, E_s \cdot \rho \cdot E_s^\dagger \,.

Now take

ℬ≡⊕Sℂ \mathscr{B} \,\equiv\, \underset{S}{\oplus} \mathbb{C}

with its canonical Hermitian inner product-structure with orthonormal linear basis (|s⟩) s:S\big(\left\vert s \right\rangle\big)_{s \colon S} and consider the linear map

V:ℋ ⟶ ℋ⊗ℬ |ψ⟩ ↦ ∑sE s|ψ⟩⊗|s⟩. \array{ \mathllap{ V \;\colon\;\; } \mathscr{H} &\longrightarrow& \mathscr{H} \otimes \mathscr{B} \\ \left\vert \psi \right\rangle &\mapsto& \underset{s}{\sum} \, E_s \left\vert \psi \right\rangle \otimes \left\vert s \right\rangle \mathrlap{\,.} }

Observe that this is a linear isometry

⟨ψ|V †V|ψ⟩ =∑s,s′⟨ψ|E s′ †E s|ψ⟩⟨s′|s⟩⏟δ s s′ =⟨ψ|∑sE s †E s⏟Id|ψ⟩ =⟨ψ|ψ⟩. \begin{array}{ll} \left\langle \psi \right\vert V^\dagger V \left\vert \psi \right\rangle \\ \;=\; \underset{s,s'}{\sum} \left\langle \psi \right\vert E_{s'}^\dagger E_s \left\vert \psi \right\rangle \underset{ \delta_s^{s'} }{ \underbrace{ \left\langle s' \vert s \right\rangle } } \\ \;=\; \left\langle \psi \right\vert \underset{ Id }{ \underbrace{ \underset{s}{\sum} E_{s}^\dagger E_s } } \left\vert \psi \right\rangle \\ \;=\; \left\langle \psi \vert \psi \right\rangle \mathrlap{\,.} \end{array}

This implies that VV is injective so that we have a direct sum-decomposition of its codomain into its image and its cokernel orthogonal complement, which is unitarily isomorphic to dim(ℬ)−1dim(\mathscr{B})-1 summands of ℋ\mathscr{H} that we may identify as follows:

ℋ⊗ℬ≃V(ℋ)⊕(ℋ⊗(ℬ⊖ℂ|s 0⟩)). \mathscr{H} \otimes \mathscr{B} \;\simeq\; V\big( \mathscr{H} \big) \oplus \Big( \mathscr{H} \otimes \big( \mathscr{B} \ominus \mathbb{C}\left\vert s_0 \right\rangle \big) \Big) \,.

In total this yields a unitary operator

U:ℋ⊗ℬ≃ℋ⊕(ℋ⊗(ℬ⊖ℂ|s ini⟩))⟶V(ℋ)⊕(ℋ⊗(ℬ⊖ℂ|s ini⟩))≃ℋ⊗ℬ U \;\colon\; \mathscr{H} \otimes \mathscr{B} \,\simeq\, \mathscr{H} \oplus \Big( \mathscr{H} \otimes \big( \mathscr{B} \ominus \mathbb{C}\left\vert s_{ini} \right\rangle \big) \Big) \underoverset{}{}{\longrightarrow} V\big( \mathscr{H} \big) \oplus \Big( \mathscr{H} \otimes \big( \mathscr{B} \ominus \mathbb{C}\left\vert s_{ini} \right\rangle \big) \Big) \;\simeq\; \mathscr{H} \otimes \mathscr{B}

and we claim that this has the desired action on couplings of the ℋ\mathscr{H}-system to the pure bath state |s ini⟩\left\vert s_{ini} \right\rangle:

trace ℬ(U(|s ini⟩ρ⟨s ini|)U †) =∑s,s′trace ℬ(|s⟩E s⋅ρ⋅E s′ †⟨s′|) =∑s,s′⟨s′|s⟩⏟δ s s′E s⋅ρ⋅E s′ † =∑sE s⋅ρ⋅E s † =chan(ρ). \begin{array}{l} trace^{\mathscr{B}} \Big( U \big( \left\vert s_{ini} \right\rangle \rho \left\langle s_{ini} \right\vert \big) U^\dagger \Big) \\ \;=\; \underset{s,s'}{\sum} trace^{\mathscr{B}} \big( \left\vert s \right\rangle E_s \cdot \rho \cdot E_{s'}^\dagger \left\langle s' \right\vert \big) \\ \;=\; \underset{s,s'}{\sum} \underset{ \delta_{s}^{s'} }{ \underbrace{ \left\langle s' \vert s \right\rangle } } E_s \cdot \rho \cdot E_{s'}^\dagger \\ \;=\; \underset{s}{\sum} E_s \cdot \rho \cdot E_{s}^\dagger \\ \;=\; chan(\rho) \,. \end{array}

This concludes the construction of an environmental representation where the environment is in a pure state.

Remark

The above theorem is often phrased as “… and the environment can be assumed to be in a pure state”. But in fact the proof crucially uses the assumption that the environment is in a pure state. It is not clear that there is a proof that works more generally.

In fact, if the environment is taken to be in the maximally mixed state, then the resulting quantum channels are called noisy operations or unistochastic quantum channels and are not expected to exhaust all quantum channels.

References

Precursor discussion:

Original discusssion identifying quantum decoherence as interaction with an averaged environment (“bath”):

With regards to the measurement problem and interpretations of quantum mechanics:

Textbook accounts:

Further review:

See also:

A proposal for mathematical quantification of coherence:

which was rediscovered and then became famous with:

See also:

Last revised on February 12, 2024 at 11:23:39. See the history of this page for a list of all contributions to it.

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