By Hans J. Krappe, Reinhard Lipperheide, Institut für Kernphysik
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Additional resources for Advanced Methods in the Evaluation of Nuclear Scattering Data
In particular, we analyze the effect of the detectors on the qubit state during manipulations, when in real devices the qubit-detector coupling cannot be switched off completely. 2 Linear amplifiers and the master equation Three time scales characterize a quantum measurement process. 1 During a quantum measurement a detector is coupled to a qubit in such a way that the value of a macroscopic observable of the detector is influenced by the qubit's state (the charge or flux influences the output current or voltage).
R) a n d ffmt are the Hamiltonians of the qubit, the left(right) reservoir of PC and qubit-PC interaction, respectively. ej(r) are the energy levels in the left(right) reservoir, and il is the tunneling matrix element of the PC. When the upper dot is occupied (az = — 1), the tunneling current does not flow through the PC. Since our interest is in the dephasing of the qubit, we neglect the tunneling between upper and lower dots. ec pn(t)Jdt'pn(t')E(t-t'), Jo where £ is a 'self-energy' which describes the qubit-detector interactions 8 ' 9 .
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Advanced Methods in the Evaluation of Nuclear Scattering Data by Hans J. Krappe, Reinhard Lipperheide, Institut für Kernphysik