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Verifying commuting quantum computations via fidelity estimation of - - PowerPoint PPT Presentation

Verifying commuting quantum computations via fidelity estimation of weighted graph states Masahito Hayashi 1,2,3 1:Graduate School of Mathematics, Nagoya University 2: Shenzhen Institute for Quantum Science and Engineering, Southern University


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Verifying commuting quantum computations via fidelity estimation

  • f weighted graph states

Masahito Hayashi1,2,3

1:Graduate School of Mathematics, Nagoya University 2: Shenzhen Institute for Quantum Science and Engineering, Southern University of Science and Technology 3: Centre for Quantum Technologies, National University of Singapore

arXiv:1902.03369

Collaborator: Y. Takeuchi, (T. Morimae, H. Zhu)

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Contents

  • Why verification of weighted graph state?
  • Verification of two-colorable graph state
  • Verification of multiple-colorable graph state
  • Verification of weighted graph state
  • Application to quantum supremacy
  • Conclusion
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How can we demonstrate quantum supremacy?

Quantum supremacy: A task that can be realized by quantum computer but cannot be realized by classical computer. Solving factorization via Shor’s algorithm by using quantum computer However, there is no guarantee that no classical algorithm realizes the same performance as Shor’s algorithm. This type of supremacy depends on the above conjecture.

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Another idea for Quantum supremacy

More convinced conjecture (Conjecture 1): Let be uniformly random degree- three polynomial over . It is #P-hard to approximate up to a multiplicative error of 1/4 + o(1) for a 1/24 fraction of polynomials f.

:{0,1} {0,1}

n

f 

2

F gap( ) : |{ : ( ) 0}| |{ : ( ) 1}| f x f x x f x    

2

gap( ) ( ) 2n f

Bremner, Montanaro, and Shepherd

  • Phys. Rev. Lett. (2016).

More people convince this conjecture.

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SLIDE 5

Another idea for Quantum supremacy

The polynomial-time hierarchy (PH): a hierarychy of complexity classes, 0th PH ⊂1st PH ⊂ 2nd PH ⊂ 3rd PH ⊂… nth PH.. Another more convinced conjecture (Conjecture 2): The PH does not collapse to its third level. 0th PH ⊂1st PH ⊂ 2nd PH ⊂ 3rd PH =nth PH

More people convince this conjecture.

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SLIDE 6

How can we demonstrate quantum supremacy?

Theorem: Assume Conjectures 1 and 2 are true. There exists an IQP circuit whose diagonal gate D is composed of Z, C-Z, and CC-Z gates such that its output probability distribution cannot be classically simulated in polynomial time, within an error 1/192 in l1 norm. Quantum Supremacy: Realization of the output state any IQP circuit whose diagonal gate D is composed of Z, C-Z, and CC-Z gates within an error 1/192 in l1 norm.

Bremner, Montanaro, and Shepherd

  • Phys. Rev. Lett. (2016).
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SLIDE 7

How to verify such output state

The output state of such an IQP circuit is given as a weighted graph state. Weighted graph state: It is sufficient to verify a weighted graph state! Graph state:

: ( 0 1 ) / 2   

, ( , ) n j k j k E

CZ

 

      

, , ( , )

( )

n j k j k j k E

 

       

,

, ,

( ) : 0 0 1 1 ( 0 0 1 1 )

j k

j k j k k j i j k k

I e

      

,

CZ : 0 0 1 1

j k k k j j

I Z    

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How to construct graph state

(1) For each vertex, we set the qubit system to (2) Apply controlled Z to the two-qubit systems connected by edges

: ( 0 1 ) / 2    CZ : 1 1 I Z     : 1 1 Z  

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SLIDE 9

This condition is needed to accept the proper computation

  • utcome.

Acceptance probability is the passing probability with correct state and measurements

Concepts of Verification (same as QKD)

Detectability: State and measurement should be rejected when they are not properly prepared. Acceptability: State and measurement should be accepted when they are properly prepared.

This condition is needed for guaranteeing the precision

  • f computation outcome when the test is passed.

Significance level is the maximum passing probability with incorrect state or measurements (e.g. 5%) Fidelity between the resultant state and target state with significance level

  

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Verification of two-colorable graph state

Since we perfectly trust measurement, it is sufficient to verify only the two-colorable (Black and White) graph state by local measurements. In two-colorable state, the Z values on one color sites decide the X values on the other color sites.

Z measurement on Black Z measurement on White

predicts

X measurement on Black X measurement on White

Our verification: We check whether X outcomes equal the prediction.

G

MH, Morimae 2015

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SLIDE 11

Verification of two-colorable graph state

Z on Black X on White

Computation

2 ' 1 N

G

 

Z on White X on Black N' copies ' copies N 1 copy

Random choice

  • r

incorrect state Stabilizer test

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SLIDE 12

With significance level β, the probability being incorrect computation outcome is less than .

Verification of two-colorable graph state

Once 2N’ tests are passed, the state of the resultant system satisfies with significance level β.

1/ (2 ' 1) N   1 1 (2 ' 1) G G N      

The state passes al least with probability 1.

2 ' 1 N

G

 

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SLIDE 13

Verification of m-colorable graph state

It is natural to apply the cover protocol to N systems. To evaluate the performance of the above protocol, we need to prepare a general theory. (1) We randomly choose one color with equal prob 1/m. (2) We measure node whose color is not the chosen color with Z basis. (3) We measure node whose color is the chosen color with X basis.

Cover protocol:

Zhu MH arXiv:1806.05565

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General theory for verification

is a POVM element. Assume that we apply the measurement to N systems. Theorem: Once N tests are passed, the state of the resultant system satisfies with significance level

 G G   { , } I     1 1 ( ) G G N        1 ( ) ( ) 1 N      ( ) : 1 G G      

Zhu MH arXiv:1806.05565

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SLIDE 15

Verification of m-colorable graph state

Once N tests are passed, the state of the resultant system satisfies with significance level β.

(1 ) 1 m G G N       

The state passes al least with probability 1.

1 N

G

 

Zhu MH arXiv:1806.05565

1 ( ) m   

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(1) We randomly choose one color with equal prob 1/m. (2) We measure node whose color is not the chosen color with Z basis. (3) We measure node l whose color is the chosen color with basis .

Adaptive verification of m- colorable weighted graph state with perfect match

{ ( ) , ( ) }

k l k l

Z Z     1 : ( 0 1 ) 2

i

e     :Outcome

l

Z

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SLIDE 17

Adaptive verification of m- colorable weighted graph state with perfect match

Once N tests are passed, the state of the resultant system satisfies with significance level β.

(1 ) 1 m G G N       

The state passes al least with probability 1.

1 N

G

 

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SLIDE 18

(1) We randomly choose one color with equal prob 1/m. (2) We measure node whose color is not the chosen color with Z basis. (3) We measure node l whose color is the chosen color with basis .

Adaptive verification of m- colorable weighted graph state with imperfect match

{ ( ) , ( ) }

h h k l k l

Z Z     ( ) : One of

h k l

Z  2 2 , , , h h h h     | ( ) ( ) |

h k l k l

Z Z h      : No. of meshes h :Outcome

l

Z

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Adaptive verification of m- colorable weighted graph state with imperfect match

Once N tests are passed, the state of the resultant system satisfies with significance level β.

(1 ) 1 sin 4 m G G n N h         

The state passes al least with probability

1 N

G

  max | | 2

(1 sin ) 4

l l

N A

h  

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SLIDE 20

(1) We choose one color with equal prob 1/m. (2) We measure node whose color is not the chosen color with Z basis. (3) We measure node l whose color is the chosen color with basis Here, j is chosen with equal prob 1/h. (4) We reject only when outcome is

Non-adaptive verification of m- colorable weighted graph state with perfect match

{ , } j j h h     ( ) is always onne of

h l

z  2 2 , , , h h h h     :Outcome

l

Z :Outcome J ( )

k l

Z   

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SLIDE 21

Non-adaptive verification of m- colorable weighted graph state with perfect match

Once N tests are passed, the state of the resultant system satisfies with significance level β.

(1 ) 1 m h G G N       

The state passes al least with probability 1.

1 N

G

 

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SLIDE 22

(1) We randomly choose one color with equal prob 1/m. (2) We measure node whose color is not the chosen color with Z basis. (3) We measure node l whose color is the chosen color with basis Here, j is chosen with equal prob 1/h. (4) We reject only when

Non-adaptive verification of m- colorable weighted graph state with imperfect match

{ , } j j h h     | ( ) |

k l

J Z h h        :Outcome

l

Z :Outcome J

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SLIDE 23

Non-adaptive verification of m- colorable weighted graph state with imperfect match

Once N tests are passed, the state of the resultant system satisfies with significance level β.

(1 ) 1 sin 4 m h G G n N h         

The state passes al least with probability

1 N

G

  max | | 2

(1 sin ) 4

l l

N A

h  

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SLIDE 24

Application to Quantum Supremacy via IQP circuit

There exists an output sate

  • f IQP circuit

whose diagonal gate D is composed of Z, C-Z, and CC-Z gates satisfying the following. No distribution on the n-bit system satisfies the following;

  • can be classically simulated in polynomial time

for n.

  • Q

Q

1

1/ 192

G

Q Q  

IQP

2

( ) : | |

G

Q z z G 

IQP

G

Assume Conjectures 1 and 2 are true.

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SLIDE 25

Application to Quantum Supremacy via IQP circuit

We set

2

8 192 (1 ) n N      

Once N tests are passed, we apply the measurement on Z to the resultant system. Then, the output distribution satisfies with significance level β.

2 h 

1

' 1/ 192

G

Q Q   ' Q

IQP

2

( ) : | |

G

Q z z G  : n

Size of IQP circuit

m n 

,

2

j k

  

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Conclusion

  • We have proposed a method to verify weighted

graph state.

  • We applied the result to quantum supremacy via

IQP circuit.

  • The required number of sampling is only linear for

the size of circuit.

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SLIDE 27

References

  • MH Morimae, Phys. Rev. Lett 115, 220502 (2015).
  • Zhu, MH, arXiv:1806.05565
  • MH Takeuchi, arXiv:1902.03369
  • Bremner, Montanaro, and Shepherd Phys. Rev. Lett. (2016).