Quantum Capacity #
This focuses on defining and proving theorems about the quantum capacity, the maximum asymptotic rate at which quantum information can be coherently transmitted. The precise definition is not consistent in the literature, see Capacity_doc for a note on what has been used and how that was used to arrive at the following definition:
- A channel A
Emulates
another channel B if there are D and E such that D∘A∘E = B. - A channel A
εApproximates
channel B (of the same dimensions) if the for every state ρ, the fidelity F(A(ρ), B(ρ)) is at least 1-ε. - A channel A
AchievesRate
R:ℝ if for every ε>0, n copies of A emulates some channel B such that log2(dimout(B))/n ≥ R, and that B is εApproximately the identity. - The
quantumCapacity
of the channel A is the supremum of the achievable rates, i.e.sSup { R : ℝ | AchievesRate A R }
.
The most basic facts:
emulates_self
: Every channel emulates itself.emulates_trans
: If A emulates B and B emulates C, then A emulates C. (That is, emulation is an ordering.)εApproximates A B ε
is equivalent to the existence of some δ (depending ε and dims(A)) so that |A-B| has diamond norm at most δ, and δ→0 as ε→0.achievesRate_0
: Every channel achievesRate 0. So, the set of achievable rates is Nonempty.- If a channel achievesRate R₁, it also every achievesRate R₂ every R₂ ≤ R₁, i.e. it is an interval extending left towards -∞. Achievable rates are
¬BddBelow
. bddAbove_achievesRate
: A channel C : dimX → dimY cannot achievesRate R withR > log2(min(dimX, dimY))
. Thus, the interval isBddAbove
.
The nice lemmas we would want:
- Capacity of a replacement channel is zero.
- Capacity of an identity channel is
log2(D)
. - Capacity is superadditive under tensor products. (That is, at least additive. Showing that it isn't exactly additive, unlike classical capacity which is additive, is a much harder task.)
- Capacity of a kth tensor power is exactly k times the capacity of the original channel.
- Capacity does not decrease under tensor sums.
- Capacity does not increase under composition.
Then, we should show that our definition is equivalent to some above. Most, except (3), should be not too hard to prove.
Then the LSD theorem establishes that the single-copy coherent information is a lower bound. This is stated in coherentInfo_le_quantumCapacity
. The corollary, that the n-copy coherent information converges to the capacity, is quantumCapacity_eq_piProd_coherentInfo
.
TODO #
The only notion of "capacity" here currently is "quantum capacity" in the usual sense. But there are several non-equal capacities relevant to quantum channels, see e.g. Watrous's notes for a list:
- Quantum capacity (
quantumCapacity
) - Quantum 1-shot capacity
- Entanglement-assisted classical capacity
- Qss, the quantum side-channel capacity
- Holevo capacity, aka Holevo χ. The Holevo–Schumacher–Westmoreland theorem as a major theorem
- Entanglement-assisted Holevo capacity
- Entanglement-assisted quantum capacity
- One- and two-way distillable entanglement
And other important theorems like superdense coding, nonadditivity, superactivation
A channel Λ₁ Emulates
another channel Λ₂ if there are D and E such that D∘Λ₁∘E = Λ₂.
Instances For
A channel A εApproximates
channel B of the same dimensions if the for every state ρ, the fidelity F(A(ρ), B(ρ)) is at least 1-ε.
Instances For
A channel A AchievesRate
R:ℝ if for every ε>0, some n copies of A emulates a channel B such that log2(dimout(B))/n ≥ R, and that B εApproximates the identity channel.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Equations
- A.quantumCapacity = sSup {R : ℝ | A.AchievesRate R}
Instances For
Every quantum channel emulates itself.
If a quantum channel A emulates B, and B emulates C, then A emulates C.
Every quantum channel perfectly approximates itself, that is, εApproximates
with ε = 0
.
If a quantum channel A approximates B with ε₀, it also approximates B with all larger ε₁.
Every quantum channel achieves a rate of zero.
The identity channel on D dimensional space achieves a rate of log2(D).
A channel cannot achieve a rate greater than log2(D), where D is the input dimension.
A channel cannot achieve a rate greater than log2(D), where D is the output dimension.
The achievable rates are a bounded set.
Quantum channel capacity is nonnegative.
Quantum channel capacity is at most log2(D), where D is the input dimension.
The LSD (Lloyd-Shor-Devetak) theorem: the quantum capacity is at least as large the single-copy coherent
information. The "coherent information" is used in literature to refer to both a function of state and
a channel (coherentInfo
), or a function of just a channel. In the latter case, the state is implicitly
maximized over. Here we use the former definition and state that the lower bound is true for all states.
The quantum capacity is the limit of the coherent information of n-copy uses of the channel.