Error mitigation + error correction
March 15nd, 2022 - Unitary Fund Group Meeting
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Andrea Mari
Special focus on: �Error mitigation for universal gates on encoded qubits,
Christophe Piveteau, David Sutter, Sergey Bravyi, Jay M. Gambetta, Kristan Temme
�https://arxiv.org/abs/2103.04915
Outline
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< H, S, CNOT > / U(1)
S
S
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Magic States
{ H, S, CNOT} augmented with the T gate is a universal gateset
Hard to implement in a fault-tolerant way
Outline
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Phys.�gate
Quantum error correction
Clifford gates can be
applied transversally
Clifford gates can be applied transversally apart from the S gate
Transversal gate
Logical qubits
=
Phys.�gate
Phys.�gate
Physical qubits
T gates cannot be applied transversally ⇒ T gates are very hard to error correct!
Outline
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Magic States
Magic states are states |A> such that:
Adaptive Clifford operations applied to |0>...|0> |A> ….|A> is universal.
Example of a magic state:
Different notations for the same state, both used in this talk.
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T-gate gadget: first example
T-gate gadget: second example
Outline
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Instead of the ideal magic state we can only prepare a noisy state
Twirling with respect to:
Error rate
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What channel do we get if we replace �the ideal magic state
with the noisy magic state ?
Result = a T gate with dephasing noise in the logical space
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Ideal T gate = linear combination of noisy operations
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First method:�
Sampling overhead:
Physical error rate
A constant
Logical error rate
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Second method (not considered in this talk).�
T logical gate = T physical gate on a single qubit
Disadvantage = larger PEC overhead. ~50 times more.
Advantage = T-gate gadgets are not necessary (no auxiliary qubits)
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Results
Number of T gates
Physical error rate
Assume k=2/5
2000 T gates
200 T gates
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Conclusions
�Error mitigation for universal gates on encoded qubits,
Christophe Piveteau, David Sutter, Sergey Bravyi, Jay M. Gambetta, Kristan Temme
https://arxiv.org/abs/2103.04915