Why doesn't the contextual QRAC contradict Nayak's bound?
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A QRAC encodes $n$ bits in $m$ qubits so that one of the bits can be retrieved. Let $p>0.5$ be the success probability of the receiver correctly obtaining any one of the $n$ bits of their choice by performing the appropriate measurement. Nayak's bound states that such an $(n, m, p)$ -QRAC must satisfy $m \geq (1−H(p))n$ , where H(·) is the entropy function. So for any constant $p$ , the "compression ratio" ( $m/n$ ) that can be obtained is at least $(1-H(p))$ . That is we can only get a constant
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Why doesn't the contextual QRAC contradict Nayak's bound?
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A QRAC encodes
n
𝑛
bits in
m
𝑚
qubits so that one of the bits can be retrieved. Let
p>0.5
𝑝
>
0.5
be the success probability of the receiver correctly obtaining any one of the
n
𝑛
bits of their choice by performing the appropriate measurement.
Nayak's bound states that such an
(n,m,p)
(
𝑛
,
𝑚
,
𝑝
)
-QRAC must satisfy
m≥(1−H(p))n
𝑚
≥
(
1
−
𝐻
(
𝑝
)
)
𝑛
, where H(·) is the entropy function. So for any constant
p
𝑝
, the "compression ratio" (
m/n
𝑚
/
𝑛
) that can be obtained is at least
(1−H(p))
(
1
−
𝐻
(
𝑝
)
)
. That is we can only get a constant (in
n
𝑛
) factor space savings.
This paper introduces a Quantum Random Access code that claims (in section 7) to be able to store
≈0.5⋅
3
u
≈
0.5
⋅
3
𝑢
bits in
C
u
2
1.5
u
𝐶
𝑢
2
1.5
𝑢
qubits where
C
𝐶
is a constant
≈243
≈
243
, where the success probability is 0.999.
I'm confused how this doesn't violate Nayak's bound since the space savings is not a constant factor, yet the success probability is constant.
contextuality
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edited Mar 30, 2024 at 11:48
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asked Mar 6, 2024 at 11:09
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I just came across the question, and I don't quite understand, but I had a follow up to Nayak's bound and QRAC preparation. I am assuming that Nayak's bounds apply to pure states as in quantum states that are preparable.
So in the paper linked in the original post the idea is to used mixed states, which would mean 4-qubit pure states and then sample them in a way that is able to produce a biased measurement according to a specific basis. From my limited understanding of mixed states, it means we can purify the pure state into a pure state of higher dimensions, which is kind of hacking Hayak's bound right? In the sense that the left hand side is actually greater than the 4-qubit pure states being used. So Nayak's bounds still hold? The purified state is of the higher degree as stated by the bound.
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answered Feb 19 at 15:21
timmy1691
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