Aziz MOUZALI - Academia.edu (original) (raw)
Teacher researcher in physics.
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To simulate the evolution and behavior of an n-qubits system, a quantum simulator within the fram... more To simulate the evolution and behavior of an n-qubits system, a quantum simulator within the framework of the computer algebra system Maple called Feynman program has been built by S.Fritzsche and T.Radtke (5). In this work we use this program to implement the nine qubit Shor quantum error correcting code on a classical computer (8). We will present the encoding and decoding circuits and describe the error correction procedure using the Shor code gen- erators. We will verify that if any X, Y or Z error occur on any single qubit this correction procedure always allow to recover the usuful information. More- over, it permit at the end to put all the ancillas in the j0> state and then to use them again. The simulation permit also the decoding without correction to measure all the output errors and know something about the canal transmitting the information.. This option is necessary if any error superposition E=coI+cxX +cyY+czZ occur on one qubit because the correction procedure doe...
Communications in Theoretical Physics, 2012
To simulate the evolution and behavior of an n-qubits system, a quantum simulator within the fram... more To simulate the evolution and behavior of an n-qubits system, a quantum simulator within the framework of the computer algebra system Maple called Feynman program has been built by S.Fritzsche and T.Radtke [5]. In this work we use this program to implement the nine qubit Shor quantum error correcting code on a classical computer [8]. We will present the encoding and decoding circuits and describe the error correction procedure using the Shor code gen-erators. We will verify that if any X, Y or Z error occur on any single qubit this correction procedure always allow to recover the usuful information. More-over, it permit at the end to put all the ancillas in the j0> state and then to use them again. The simulation permit also the decoding without correction to measure all the output errors and know something about the canal transmitting the information.. This option is necessary if any error superposition E=co I+cxX +cyY+czZ occur on one qubit because the correction procedure does...
To simulate the evolution and behavior of an n-qubits system, a quantum simulator within the fram... more To simulate the evolution and behavior of an n-qubits system, a quantum simulator within the framework of the computer algebra system Maple called Feynman program has been built by S.Fritzsche and T.Radtke (5). In this work we use this program to implement the nine qubit Shor quantum error correcting code on a classical computer (8). We will present the encoding and decoding circuits and describe the error correction procedure using the Shor code gen- erators. We will verify that if any X, Y or Z error occur on any single qubit this correction procedure always allow to recover the usuful information. More- over, it permit at the end to put all the ancillas in the j0> state and then to use them again. The simulation permit also the decoding without correction to measure all the output errors and know something about the canal transmitting the information.. This option is necessary if any error superposition E=coI+cxX +cyY+czZ occur on one qubit because the correction procedure doe...
Communications in Theoretical Physics, 2012
To simulate the evolution and behavior of an n-qubits system, a quantum simulator within the fram... more To simulate the evolution and behavior of an n-qubits system, a quantum simulator within the framework of the computer algebra system Maple called Feynman program has been built by S.Fritzsche and T.Radtke [5]. In this work we use this program to implement the nine qubit Shor quantum error correcting code on a classical computer [8]. We will present the encoding and decoding circuits and describe the error correction procedure using the Shor code gen-erators. We will verify that if any X, Y or Z error occur on any single qubit this correction procedure always allow to recover the usuful information. More-over, it permit at the end to put all the ancillas in the j0> state and then to use them again. The simulation permit also the decoding without correction to measure all the output errors and know something about the canal transmitting the information.. This option is necessary if any error superposition E=co I+cxX +cyY+czZ occur on one qubit because the correction procedure does...