Grover's algorithm with W-state











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In the general form of Grover's algorithm, we start with the uniform superposition of n qubits. Now, suppose instead that we start with a generic state, for example the W state, and the oracle only inverts the phase of one of the basis.



To make it more concrete, let's say we have in input a $W_3$ state $$|Wrangle = frac{1}{sqrt{3}} (|001rangle + |010rangle + |100rangle)$$
and that the oracle inverts only state $$|001rangle$$



At this point, how can we implement the diffusion operator? In other words, how can we amplify only this state in order to obtain the right output with an high probability?










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    In the general form of Grover's algorithm, we start with the uniform superposition of n qubits. Now, suppose instead that we start with a generic state, for example the W state, and the oracle only inverts the phase of one of the basis.



    To make it more concrete, let's say we have in input a $W_3$ state $$|Wrangle = frac{1}{sqrt{3}} (|001rangle + |010rangle + |100rangle)$$
    and that the oracle inverts only state $$|001rangle$$



    At this point, how can we implement the diffusion operator? In other words, how can we amplify only this state in order to obtain the right output with an high probability?










    share|improve this question


























      up vote
      3
      down vote

      favorite









      up vote
      3
      down vote

      favorite











      In the general form of Grover's algorithm, we start with the uniform superposition of n qubits. Now, suppose instead that we start with a generic state, for example the W state, and the oracle only inverts the phase of one of the basis.



      To make it more concrete, let's say we have in input a $W_3$ state $$|Wrangle = frac{1}{sqrt{3}} (|001rangle + |010rangle + |100rangle)$$
      and that the oracle inverts only state $$|001rangle$$



      At this point, how can we implement the diffusion operator? In other words, how can we amplify only this state in order to obtain the right output with an high probability?










      share|improve this question















      In the general form of Grover's algorithm, we start with the uniform superposition of n qubits. Now, suppose instead that we start with a generic state, for example the W state, and the oracle only inverts the phase of one of the basis.



      To make it more concrete, let's say we have in input a $W_3$ state $$|Wrangle = frac{1}{sqrt{3}} (|001rangle + |010rangle + |100rangle)$$
      and that the oracle inverts only state $$|001rangle$$



      At this point, how can we implement the diffusion operator? In other words, how can we amplify only this state in order to obtain the right output with an high probability?







      algorithm entanglement grovers-algorithm






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      edited 23 mins ago









      Blue

      5,63511352




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      asked 7 hours ago









      tigerjack89

      1735




      1735






















          3 Answers
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          up vote
          1
          down vote













          I think that it does not change the original Grover's algorithm idea. Let me explain better, Grover's algorithm does make any distinction about the input or the original state. See figure attached for better representation. I think it will work as a general case.
          enter image description here






          share|improve this answer





















          • Not too sure about it. It seems to me that the one you're representing as diffusion is a reflection about the uniform superposition. Here instead we don't have an uniform superposition in input.
            – tigerjack89
            7 hours ago




















          up vote
          1
          down vote













          Say $ | psi rangle $ represents the uniform suposition.



          Then, the Grover diffusion operator is written :
          $$ 2 | psi rangle langle psi | - I$$



          Now to act on a subset of a superposition, you would need to implement :
          $$ 2 | Wrangle langle W | - I$$



          I am not sure if someone had really looked into how decompose this operation as a circuit. I guess it would be too dependent on the initial state.



          This paper however shows a trick to still get the state you want with a high probability. Check section 3.3.1 .
          The idea is to start with $ | W rangle $ and use a first Grover iteration to inverse amplitudes about average by only marking the target state. Then you would mark the computational basis states that are present initially in $ | psi rangle $ and use inversion about average again. Finally, you would continue with usual Grover iterations. They provide an example to help you visualize the effect of the steps. The target should have a high probability of being measured, even if others states not present in $ | W rangle $ can be measured.






          share|improve this answer




























            up vote
            1
            down vote













            I think, if one starts with the $W$ state which contains only $3$ out of $8$ possible $3$-bit strings then the Grover algorithm will work correctly only of the secret is one of those $3$ strings. If secret has $2$ or $3$ $1$-bits , say 011 there is no matched initial state to amplify.
            There is a reason Grover starts with n Hadamards applied to $n$ qubits - this way all possible $2^n$ $n$-bit strings are present and one of them must match to the secret.






            share|improve this answer










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            • Hi Jan. Welcome to Quantum Computing Stack Exchange! Please use MathJax to format the mathematical expressions in your answer, in the future. I've done it this time.
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            3 Answers
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            active

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            up vote
            1
            down vote













            I think that it does not change the original Grover's algorithm idea. Let me explain better, Grover's algorithm does make any distinction about the input or the original state. See figure attached for better representation. I think it will work as a general case.
            enter image description here






            share|improve this answer





















            • Not too sure about it. It seems to me that the one you're representing as diffusion is a reflection about the uniform superposition. Here instead we don't have an uniform superposition in input.
              – tigerjack89
              7 hours ago

















            up vote
            1
            down vote













            I think that it does not change the original Grover's algorithm idea. Let me explain better, Grover's algorithm does make any distinction about the input or the original state. See figure attached for better representation. I think it will work as a general case.
            enter image description here






            share|improve this answer





















            • Not too sure about it. It seems to me that the one you're representing as diffusion is a reflection about the uniform superposition. Here instead we don't have an uniform superposition in input.
              – tigerjack89
              7 hours ago















            up vote
            1
            down vote










            up vote
            1
            down vote









            I think that it does not change the original Grover's algorithm idea. Let me explain better, Grover's algorithm does make any distinction about the input or the original state. See figure attached for better representation. I think it will work as a general case.
            enter image description here






            share|improve this answer












            I think that it does not change the original Grover's algorithm idea. Let me explain better, Grover's algorithm does make any distinction about the input or the original state. See figure attached for better representation. I think it will work as a general case.
            enter image description here







            share|improve this answer












            share|improve this answer



            share|improve this answer










            answered 7 hours ago









            Gustavo Banegas

            11115




            11115












            • Not too sure about it. It seems to me that the one you're representing as diffusion is a reflection about the uniform superposition. Here instead we don't have an uniform superposition in input.
              – tigerjack89
              7 hours ago




















            • Not too sure about it. It seems to me that the one you're representing as diffusion is a reflection about the uniform superposition. Here instead we don't have an uniform superposition in input.
              – tigerjack89
              7 hours ago


















            Not too sure about it. It seems to me that the one you're representing as diffusion is a reflection about the uniform superposition. Here instead we don't have an uniform superposition in input.
            – tigerjack89
            7 hours ago






            Not too sure about it. It seems to me that the one you're representing as diffusion is a reflection about the uniform superposition. Here instead we don't have an uniform superposition in input.
            – tigerjack89
            7 hours ago














            up vote
            1
            down vote













            Say $ | psi rangle $ represents the uniform suposition.



            Then, the Grover diffusion operator is written :
            $$ 2 | psi rangle langle psi | - I$$



            Now to act on a subset of a superposition, you would need to implement :
            $$ 2 | Wrangle langle W | - I$$



            I am not sure if someone had really looked into how decompose this operation as a circuit. I guess it would be too dependent on the initial state.



            This paper however shows a trick to still get the state you want with a high probability. Check section 3.3.1 .
            The idea is to start with $ | W rangle $ and use a first Grover iteration to inverse amplitudes about average by only marking the target state. Then you would mark the computational basis states that are present initially in $ | psi rangle $ and use inversion about average again. Finally, you would continue with usual Grover iterations. They provide an example to help you visualize the effect of the steps. The target should have a high probability of being measured, even if others states not present in $ | W rangle $ can be measured.






            share|improve this answer

























              up vote
              1
              down vote













              Say $ | psi rangle $ represents the uniform suposition.



              Then, the Grover diffusion operator is written :
              $$ 2 | psi rangle langle psi | - I$$



              Now to act on a subset of a superposition, you would need to implement :
              $$ 2 | Wrangle langle W | - I$$



              I am not sure if someone had really looked into how decompose this operation as a circuit. I guess it would be too dependent on the initial state.



              This paper however shows a trick to still get the state you want with a high probability. Check section 3.3.1 .
              The idea is to start with $ | W rangle $ and use a first Grover iteration to inverse amplitudes about average by only marking the target state. Then you would mark the computational basis states that are present initially in $ | psi rangle $ and use inversion about average again. Finally, you would continue with usual Grover iterations. They provide an example to help you visualize the effect of the steps. The target should have a high probability of being measured, even if others states not present in $ | W rangle $ can be measured.






              share|improve this answer























                up vote
                1
                down vote










                up vote
                1
                down vote









                Say $ | psi rangle $ represents the uniform suposition.



                Then, the Grover diffusion operator is written :
                $$ 2 | psi rangle langle psi | - I$$



                Now to act on a subset of a superposition, you would need to implement :
                $$ 2 | Wrangle langle W | - I$$



                I am not sure if someone had really looked into how decompose this operation as a circuit. I guess it would be too dependent on the initial state.



                This paper however shows a trick to still get the state you want with a high probability. Check section 3.3.1 .
                The idea is to start with $ | W rangle $ and use a first Grover iteration to inverse amplitudes about average by only marking the target state. Then you would mark the computational basis states that are present initially in $ | psi rangle $ and use inversion about average again. Finally, you would continue with usual Grover iterations. They provide an example to help you visualize the effect of the steps. The target should have a high probability of being measured, even if others states not present in $ | W rangle $ can be measured.






                share|improve this answer












                Say $ | psi rangle $ represents the uniform suposition.



                Then, the Grover diffusion operator is written :
                $$ 2 | psi rangle langle psi | - I$$



                Now to act on a subset of a superposition, you would need to implement :
                $$ 2 | Wrangle langle W | - I$$



                I am not sure if someone had really looked into how decompose this operation as a circuit. I guess it would be too dependent on the initial state.



                This paper however shows a trick to still get the state you want with a high probability. Check section 3.3.1 .
                The idea is to start with $ | W rangle $ and use a first Grover iteration to inverse amplitudes about average by only marking the target state. Then you would mark the computational basis states that are present initially in $ | psi rangle $ and use inversion about average again. Finally, you would continue with usual Grover iterations. They provide an example to help you visualize the effect of the steps. The target should have a high probability of being measured, even if others states not present in $ | W rangle $ can be measured.







                share|improve this answer












                share|improve this answer



                share|improve this answer










                answered 2 hours ago









                cnada

                1,691211




                1,691211






















                    up vote
                    1
                    down vote













                    I think, if one starts with the $W$ state which contains only $3$ out of $8$ possible $3$-bit strings then the Grover algorithm will work correctly only of the secret is one of those $3$ strings. If secret has $2$ or $3$ $1$-bits , say 011 there is no matched initial state to amplify.
                    There is a reason Grover starts with n Hadamards applied to $n$ qubits - this way all possible $2^n$ $n$-bit strings are present and one of them must match to the secret.






                    share|improve this answer










                    New contributor




                    Jan Balewski is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
                    Check out our Code of Conduct.


















                    • Hi Jan. Welcome to Quantum Computing Stack Exchange! Please use MathJax to format the mathematical expressions in your answer, in the future. I've done it this time.
                      – Blue
                      22 mins ago

















                    up vote
                    1
                    down vote













                    I think, if one starts with the $W$ state which contains only $3$ out of $8$ possible $3$-bit strings then the Grover algorithm will work correctly only of the secret is one of those $3$ strings. If secret has $2$ or $3$ $1$-bits , say 011 there is no matched initial state to amplify.
                    There is a reason Grover starts with n Hadamards applied to $n$ qubits - this way all possible $2^n$ $n$-bit strings are present and one of them must match to the secret.






                    share|improve this answer










                    New contributor




                    Jan Balewski is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
                    Check out our Code of Conduct.


















                    • Hi Jan. Welcome to Quantum Computing Stack Exchange! Please use MathJax to format the mathematical expressions in your answer, in the future. I've done it this time.
                      – Blue
                      22 mins ago















                    up vote
                    1
                    down vote










                    up vote
                    1
                    down vote









                    I think, if one starts with the $W$ state which contains only $3$ out of $8$ possible $3$-bit strings then the Grover algorithm will work correctly only of the secret is one of those $3$ strings. If secret has $2$ or $3$ $1$-bits , say 011 there is no matched initial state to amplify.
                    There is a reason Grover starts with n Hadamards applied to $n$ qubits - this way all possible $2^n$ $n$-bit strings are present and one of them must match to the secret.






                    share|improve this answer










                    New contributor




                    Jan Balewski is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
                    Check out our Code of Conduct.









                    I think, if one starts with the $W$ state which contains only $3$ out of $8$ possible $3$-bit strings then the Grover algorithm will work correctly only of the secret is one of those $3$ strings. If secret has $2$ or $3$ $1$-bits , say 011 there is no matched initial state to amplify.
                    There is a reason Grover starts with n Hadamards applied to $n$ qubits - this way all possible $2^n$ $n$-bit strings are present and one of them must match to the secret.







                    share|improve this answer










                    New contributor




                    Jan Balewski is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
                    Check out our Code of Conduct.









                    share|improve this answer



                    share|improve this answer








                    edited 20 mins ago









                    Blue

                    5,63511352




                    5,63511352






                    New contributor




                    Jan Balewski is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
                    Check out our Code of Conduct.









                    answered 51 mins ago









                    Jan Balewski

                    162




                    162




                    New contributor




                    Jan Balewski is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
                    Check out our Code of Conduct.





                    New contributor





                    Jan Balewski is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
                    Check out our Code of Conduct.






                    Jan Balewski is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
                    Check out our Code of Conduct.












                    • Hi Jan. Welcome to Quantum Computing Stack Exchange! Please use MathJax to format the mathematical expressions in your answer, in the future. I've done it this time.
                      – Blue
                      22 mins ago




















                    • Hi Jan. Welcome to Quantum Computing Stack Exchange! Please use MathJax to format the mathematical expressions in your answer, in the future. I've done it this time.
                      – Blue
                      22 mins ago


















                    Hi Jan. Welcome to Quantum Computing Stack Exchange! Please use MathJax to format the mathematical expressions in your answer, in the future. I've done it this time.
                    – Blue
                    22 mins ago






                    Hi Jan. Welcome to Quantum Computing Stack Exchange! Please use MathJax to format the mathematical expressions in your answer, in the future. I've done it this time.
                    – Blue
                    22 mins ago




















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