Quantum Computer Compilers
... evolution of the Hamiltonian of a quantum system • To solve a given problem we initialize the system to the ground state of a simple Hamiltonian • We then evolve the Hamiltonian to one whose ground state encodes the solution to the problem • The evolution needs to be done slowly to always keep the e ...
... evolution of the Hamiltonian of a quantum system • To solve a given problem we initialize the system to the ground state of a simple Hamiltonian • We then evolve the Hamiltonian to one whose ground state encodes the solution to the problem • The evolution needs to be done slowly to always keep the e ...
pdf - Martijn Wubs
... gain, which is information beyond "eff ð!Þ. For loss-loss and gain-gain metamaterials the a and b add up to unity. Only in the case Ta ¼ Tb , as for a passive lossy metamaterial at room temperature, we then find that Neff reduces to the thermal distribution Nth . Thus our QOEM theory explains our ...
... gain, which is information beyond "eff ð!Þ. For loss-loss and gain-gain metamaterials the a and b add up to unity. Only in the case Ta ¼ Tb , as for a passive lossy metamaterial at room temperature, we then find that Neff reduces to the thermal distribution Nth . Thus our QOEM theory explains our ...
