Decompose a general two-qubit gate into general controlled-qubit gates












2












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We often seek to decompose multi-qubit unitaries into single-qubit rotations and controlled-rotations, minimising the latter or restricting to gates like CNOTs.



I'm interested in expressing a general 2-qubit unitary in the minimum total number of gates, which can include controlled general unitaries. That is, express $U_{4}$ with as few as possible gates in ${U_2,; |0⟩⟨0|mathbb{1} + |1⟩⟨1|U_2}$. While I could simply take the shortest decomposition to CNOTs and rotations (Vatan et al) and bring some rotations into the CNOTs, I suspect another formulation could add more control-unitaries to achieve fewer total gates.



How can I go about performing this decomposition algorithmically for any 2-qubit unitary?
This decomposition could be useful for easily extending distributed quantum simulators with the ability to effect general 2-qubit unitaries, which otherwise ad-hoc communication code.










share|improve this question











$endgroup$

















    2












    $begingroup$


    We often seek to decompose multi-qubit unitaries into single-qubit rotations and controlled-rotations, minimising the latter or restricting to gates like CNOTs.



    I'm interested in expressing a general 2-qubit unitary in the minimum total number of gates, which can include controlled general unitaries. That is, express $U_{4}$ with as few as possible gates in ${U_2,; |0⟩⟨0|mathbb{1} + |1⟩⟨1|U_2}$. While I could simply take the shortest decomposition to CNOTs and rotations (Vatan et al) and bring some rotations into the CNOTs, I suspect another formulation could add more control-unitaries to achieve fewer total gates.



    How can I go about performing this decomposition algorithmically for any 2-qubit unitary?
    This decomposition could be useful for easily extending distributed quantum simulators with the ability to effect general 2-qubit unitaries, which otherwise ad-hoc communication code.










    share|improve this question











    $endgroup$















      2












      2








      2





      $begingroup$


      We often seek to decompose multi-qubit unitaries into single-qubit rotations and controlled-rotations, minimising the latter or restricting to gates like CNOTs.



      I'm interested in expressing a general 2-qubit unitary in the minimum total number of gates, which can include controlled general unitaries. That is, express $U_{4}$ with as few as possible gates in ${U_2,; |0⟩⟨0|mathbb{1} + |1⟩⟨1|U_2}$. While I could simply take the shortest decomposition to CNOTs and rotations (Vatan et al) and bring some rotations into the CNOTs, I suspect another formulation could add more control-unitaries to achieve fewer total gates.



      How can I go about performing this decomposition algorithmically for any 2-qubit unitary?
      This decomposition could be useful for easily extending distributed quantum simulators with the ability to effect general 2-qubit unitaries, which otherwise ad-hoc communication code.










      share|improve this question











      $endgroup$




      We often seek to decompose multi-qubit unitaries into single-qubit rotations and controlled-rotations, minimising the latter or restricting to gates like CNOTs.



      I'm interested in expressing a general 2-qubit unitary in the minimum total number of gates, which can include controlled general unitaries. That is, express $U_{4}$ with as few as possible gates in ${U_2,; |0⟩⟨0|mathbb{1} + |1⟩⟨1|U_2}$. While I could simply take the shortest decomposition to CNOTs and rotations (Vatan et al) and bring some rotations into the CNOTs, I suspect another formulation could add more control-unitaries to achieve fewer total gates.



      How can I go about performing this decomposition algorithmically for any 2-qubit unitary?
      This decomposition could be useful for easily extending distributed quantum simulators with the ability to effect general 2-qubit unitaries, which otherwise ad-hoc communication code.







      quantum-gate circuit-construction gate-synthesis






      share|improve this question















      share|improve this question













      share|improve this question




      share|improve this question








      edited Feb 13 at 22:48









      Blue

      6,49641555




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      asked Feb 13 at 22:21









      Anti EarthAnti Earth

      2888




      2888






















          1 Answer
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          $begingroup$

          A simple place to start would be to put all the controls on qubit #2, so that you can propagate all of the single-qubit operations on qubit #1 across the two-qubit operations and merge them together. That would give you a circuit with at most 8 gates:



          --------C1-------C2-------C3---S5---
          | | |
          ---S1---*---S2---*---S3---*----S4---


          This is probably not minimal.



          A general 4x4 unitary has 7+5+3+1=16 real parameters. Every single-qubit gate has three real parameters (Euler angles), and every two-qubit gate has four real parameters (Euler angles + phase kickback). So the above construction has 4*3 + 4*4 = 28 real parameters.



          It is provable that you need at least three different controlled gates for some two-qubit operations. So the absolute best you could hope for is three of those and one single-qubit operation. But some of the degrees of freedom overlap, so I suspect you need more single-qubit gates.






          share|improve this answer











          $endgroup$













          • $begingroup$
            This is a great start (and looks like the quantum shannon decomp), thanks very much! I suspect one can go shorter by controlling on both qubits, as does the smallest (I think?) decomp of SWAP (3 CNOTs)
            $endgroup$
            – Anti Earth
            Feb 14 at 18:07










          • $begingroup$
            As nicely explained here, the cosine-sine decomposition can decompose a 2-qubit U into 3 multiplexors (two of which feature 2 general unitaries, one of which features two Y rotations). Each multiplexor can be two controlled gates (one NOT-controlled, else an additional NOT is needed). So using controlled-unitaries and NOT gates, that's a worst case 9 ops. Allowing NOT-controlled (easy to code up) unitaries, that's 6 ops. Allowing multiplexors (not too difficult to code up), that's 3 ops.
            $endgroup$
            – Anti Earth
            Feb 15 at 0:37










          • $begingroup$
            @AntiEarth My reading of your question was that you would count a "multiplexor" as two separate gates. You may want to clarify exactly what your constraints are.
            $endgroup$
            – Craig Gidney
            Feb 15 at 0:45











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          1 Answer
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          1 Answer
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          $begingroup$

          A simple place to start would be to put all the controls on qubit #2, so that you can propagate all of the single-qubit operations on qubit #1 across the two-qubit operations and merge them together. That would give you a circuit with at most 8 gates:



          --------C1-------C2-------C3---S5---
          | | |
          ---S1---*---S2---*---S3---*----S4---


          This is probably not minimal.



          A general 4x4 unitary has 7+5+3+1=16 real parameters. Every single-qubit gate has three real parameters (Euler angles), and every two-qubit gate has four real parameters (Euler angles + phase kickback). So the above construction has 4*3 + 4*4 = 28 real parameters.



          It is provable that you need at least three different controlled gates for some two-qubit operations. So the absolute best you could hope for is three of those and one single-qubit operation. But some of the degrees of freedom overlap, so I suspect you need more single-qubit gates.






          share|improve this answer











          $endgroup$













          • $begingroup$
            This is a great start (and looks like the quantum shannon decomp), thanks very much! I suspect one can go shorter by controlling on both qubits, as does the smallest (I think?) decomp of SWAP (3 CNOTs)
            $endgroup$
            – Anti Earth
            Feb 14 at 18:07










          • $begingroup$
            As nicely explained here, the cosine-sine decomposition can decompose a 2-qubit U into 3 multiplexors (two of which feature 2 general unitaries, one of which features two Y rotations). Each multiplexor can be two controlled gates (one NOT-controlled, else an additional NOT is needed). So using controlled-unitaries and NOT gates, that's a worst case 9 ops. Allowing NOT-controlled (easy to code up) unitaries, that's 6 ops. Allowing multiplexors (not too difficult to code up), that's 3 ops.
            $endgroup$
            – Anti Earth
            Feb 15 at 0:37










          • $begingroup$
            @AntiEarth My reading of your question was that you would count a "multiplexor" as two separate gates. You may want to clarify exactly what your constraints are.
            $endgroup$
            – Craig Gidney
            Feb 15 at 0:45
















          3












          $begingroup$

          A simple place to start would be to put all the controls on qubit #2, so that you can propagate all of the single-qubit operations on qubit #1 across the two-qubit operations and merge them together. That would give you a circuit with at most 8 gates:



          --------C1-------C2-------C3---S5---
          | | |
          ---S1---*---S2---*---S3---*----S4---


          This is probably not minimal.



          A general 4x4 unitary has 7+5+3+1=16 real parameters. Every single-qubit gate has three real parameters (Euler angles), and every two-qubit gate has four real parameters (Euler angles + phase kickback). So the above construction has 4*3 + 4*4 = 28 real parameters.



          It is provable that you need at least three different controlled gates for some two-qubit operations. So the absolute best you could hope for is three of those and one single-qubit operation. But some of the degrees of freedom overlap, so I suspect you need more single-qubit gates.






          share|improve this answer











          $endgroup$













          • $begingroup$
            This is a great start (and looks like the quantum shannon decomp), thanks very much! I suspect one can go shorter by controlling on both qubits, as does the smallest (I think?) decomp of SWAP (3 CNOTs)
            $endgroup$
            – Anti Earth
            Feb 14 at 18:07










          • $begingroup$
            As nicely explained here, the cosine-sine decomposition can decompose a 2-qubit U into 3 multiplexors (two of which feature 2 general unitaries, one of which features two Y rotations). Each multiplexor can be two controlled gates (one NOT-controlled, else an additional NOT is needed). So using controlled-unitaries and NOT gates, that's a worst case 9 ops. Allowing NOT-controlled (easy to code up) unitaries, that's 6 ops. Allowing multiplexors (not too difficult to code up), that's 3 ops.
            $endgroup$
            – Anti Earth
            Feb 15 at 0:37










          • $begingroup$
            @AntiEarth My reading of your question was that you would count a "multiplexor" as two separate gates. You may want to clarify exactly what your constraints are.
            $endgroup$
            – Craig Gidney
            Feb 15 at 0:45














          3












          3








          3





          $begingroup$

          A simple place to start would be to put all the controls on qubit #2, so that you can propagate all of the single-qubit operations on qubit #1 across the two-qubit operations and merge them together. That would give you a circuit with at most 8 gates:



          --------C1-------C2-------C3---S5---
          | | |
          ---S1---*---S2---*---S3---*----S4---


          This is probably not minimal.



          A general 4x4 unitary has 7+5+3+1=16 real parameters. Every single-qubit gate has three real parameters (Euler angles), and every two-qubit gate has four real parameters (Euler angles + phase kickback). So the above construction has 4*3 + 4*4 = 28 real parameters.



          It is provable that you need at least three different controlled gates for some two-qubit operations. So the absolute best you could hope for is three of those and one single-qubit operation. But some of the degrees of freedom overlap, so I suspect you need more single-qubit gates.






          share|improve this answer











          $endgroup$



          A simple place to start would be to put all the controls on qubit #2, so that you can propagate all of the single-qubit operations on qubit #1 across the two-qubit operations and merge them together. That would give you a circuit with at most 8 gates:



          --------C1-------C2-------C3---S5---
          | | |
          ---S1---*---S2---*---S3---*----S4---


          This is probably not minimal.



          A general 4x4 unitary has 7+5+3+1=16 real parameters. Every single-qubit gate has three real parameters (Euler angles), and every two-qubit gate has four real parameters (Euler angles + phase kickback). So the above construction has 4*3 + 4*4 = 28 real parameters.



          It is provable that you need at least three different controlled gates for some two-qubit operations. So the absolute best you could hope for is three of those and one single-qubit operation. But some of the degrees of freedom overlap, so I suspect you need more single-qubit gates.







          share|improve this answer














          share|improve this answer



          share|improve this answer








          edited Feb 13 at 23:07

























          answered Feb 13 at 22:33









          Craig GidneyCraig Gidney

          4,576320




          4,576320












          • $begingroup$
            This is a great start (and looks like the quantum shannon decomp), thanks very much! I suspect one can go shorter by controlling on both qubits, as does the smallest (I think?) decomp of SWAP (3 CNOTs)
            $endgroup$
            – Anti Earth
            Feb 14 at 18:07










          • $begingroup$
            As nicely explained here, the cosine-sine decomposition can decompose a 2-qubit U into 3 multiplexors (two of which feature 2 general unitaries, one of which features two Y rotations). Each multiplexor can be two controlled gates (one NOT-controlled, else an additional NOT is needed). So using controlled-unitaries and NOT gates, that's a worst case 9 ops. Allowing NOT-controlled (easy to code up) unitaries, that's 6 ops. Allowing multiplexors (not too difficult to code up), that's 3 ops.
            $endgroup$
            – Anti Earth
            Feb 15 at 0:37










          • $begingroup$
            @AntiEarth My reading of your question was that you would count a "multiplexor" as two separate gates. You may want to clarify exactly what your constraints are.
            $endgroup$
            – Craig Gidney
            Feb 15 at 0:45


















          • $begingroup$
            This is a great start (and looks like the quantum shannon decomp), thanks very much! I suspect one can go shorter by controlling on both qubits, as does the smallest (I think?) decomp of SWAP (3 CNOTs)
            $endgroup$
            – Anti Earth
            Feb 14 at 18:07










          • $begingroup$
            As nicely explained here, the cosine-sine decomposition can decompose a 2-qubit U into 3 multiplexors (two of which feature 2 general unitaries, one of which features two Y rotations). Each multiplexor can be two controlled gates (one NOT-controlled, else an additional NOT is needed). So using controlled-unitaries and NOT gates, that's a worst case 9 ops. Allowing NOT-controlled (easy to code up) unitaries, that's 6 ops. Allowing multiplexors (not too difficult to code up), that's 3 ops.
            $endgroup$
            – Anti Earth
            Feb 15 at 0:37










          • $begingroup$
            @AntiEarth My reading of your question was that you would count a "multiplexor" as two separate gates. You may want to clarify exactly what your constraints are.
            $endgroup$
            – Craig Gidney
            Feb 15 at 0:45
















          $begingroup$
          This is a great start (and looks like the quantum shannon decomp), thanks very much! I suspect one can go shorter by controlling on both qubits, as does the smallest (I think?) decomp of SWAP (3 CNOTs)
          $endgroup$
          – Anti Earth
          Feb 14 at 18:07




          $begingroup$
          This is a great start (and looks like the quantum shannon decomp), thanks very much! I suspect one can go shorter by controlling on both qubits, as does the smallest (I think?) decomp of SWAP (3 CNOTs)
          $endgroup$
          – Anti Earth
          Feb 14 at 18:07












          $begingroup$
          As nicely explained here, the cosine-sine decomposition can decompose a 2-qubit U into 3 multiplexors (two of which feature 2 general unitaries, one of which features two Y rotations). Each multiplexor can be two controlled gates (one NOT-controlled, else an additional NOT is needed). So using controlled-unitaries and NOT gates, that's a worst case 9 ops. Allowing NOT-controlled (easy to code up) unitaries, that's 6 ops. Allowing multiplexors (not too difficult to code up), that's 3 ops.
          $endgroup$
          – Anti Earth
          Feb 15 at 0:37




          $begingroup$
          As nicely explained here, the cosine-sine decomposition can decompose a 2-qubit U into 3 multiplexors (two of which feature 2 general unitaries, one of which features two Y rotations). Each multiplexor can be two controlled gates (one NOT-controlled, else an additional NOT is needed). So using controlled-unitaries and NOT gates, that's a worst case 9 ops. Allowing NOT-controlled (easy to code up) unitaries, that's 6 ops. Allowing multiplexors (not too difficult to code up), that's 3 ops.
          $endgroup$
          – Anti Earth
          Feb 15 at 0:37












          $begingroup$
          @AntiEarth My reading of your question was that you would count a "multiplexor" as two separate gates. You may want to clarify exactly what your constraints are.
          $endgroup$
          – Craig Gidney
          Feb 15 at 0:45




          $begingroup$
          @AntiEarth My reading of your question was that you would count a "multiplexor" as two separate gates. You may want to clarify exactly what your constraints are.
          $endgroup$
          – Craig Gidney
          Feb 15 at 0:45


















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