Ψ|Ψ is conserved, establishing the nature of the operations as unitary to emulate the quantum condition. Measurement of the wavefunction at a node is simulated on a classical computer while on a quantum computer the wavefunction is measured, the information developed in the simulation is exchanged with nearby modes, and the process is repeated until complete."/>
Generation of displays of solutions to physics problems represented by complex mathematical equations using quantum computations or simulation of quantum computations on classic computers
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Generation of displays of solutions to physics problems represented by complex mathematical equations using quantum computations or simulation of quantum computations on classic computers
Generation of displays of solutions to physics problems represented by complex mathematical equations using quantum computations or simulation of quantum computations on classic computers
Graphic displays or audio sound representations of numerical solutions of physics problems modeled by complicated, computationally complex mathematics are generated by Type I and Type II quantum computers, which employs a plurality of classically interconnected nodes each consisting of relatively few qubits, or classical computers emulating Type I and Type II quantum computers. This is done by setting the boundary conditions so that conservation is maintained within a high precision and performing multi-demensional computations as a series of single dimensional computations employing pseudo-random number generators on a classical computer to simulate the stochastic nature of the quantum process. On a quantum computer randomness is supplied the quantum process direction. An operator U on a quantum wavefunction Ψ ensures that, to the limit of experimental accuracy on a real quantum computer, the Hermitian inner product Ψ|Ψ is conserved, establishing the nature of the operations as unitary to emulate the quantum condition. Measurement of the wavefunction at a node is simulated on a classical computer while on a quantum computer the wavefunction is measured, the information developed in the simulation is exchanged with nearby modes, and the process is repeated until complete.
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