Quantum Computation with Topological Phases of Matter
... condensation of a bosonic quasiparticle. To this end, we formulate an extension of the theory of symmetry breaking phase transitions which applies to phases with topological excitations described by quantum groups or modular tensor categories. This enables us to deal with phases whose quasiparticles ...
... condensation of a bosonic quasiparticle. To this end, we formulate an extension of the theory of symmetry breaking phase transitions which applies to phases with topological excitations described by quantum groups or modular tensor categories. This enables us to deal with phases whose quasiparticles ...
Research Statement
... However, the theory has not completely caught up with the experiment. While the photonic platform for quantum information processing has much in its favor, it suffers from imperfect detector efficiency and photon loss which gets worse as the number of optical components is scaled up. It is not under ...
... However, the theory has not completely caught up with the experiment. While the photonic platform for quantum information processing has much in its favor, it suffers from imperfect detector efficiency and photon loss which gets worse as the number of optical components is scaled up. It is not under ...
3D simulation of a silicon quantum dot in
... gate. An undoped silicon dot with height 4 nm and square base L × L is embedded in the oxide layer. We consider three different dot sizes, corresponding to L = 10, 20, and 30 nm. The magnetic field is uniform along the vertical (z) direction. We assume a silicon gyromagnetic factor of 2.6. In Fig. 3 ...
... gate. An undoped silicon dot with height 4 nm and square base L × L is embedded in the oxide layer. We consider three different dot sizes, corresponding to L = 10, 20, and 30 nm. The magnetic field is uniform along the vertical (z) direction. We assume a silicon gyromagnetic factor of 2.6. In Fig. 3 ...
arXiv:quant-ph/0610027v1 4 Oct 2006
... bound arises in a Bayesian setting, we supply the prior probabilities π0 and π1 , which are positive quantities summing up to 1 (the degenerate cases π0 = 0 or π1 = 0 are excluded). Physically discriminating between these hypotheses corresponds to performing a generalised (POVM) measurement on the q ...
... bound arises in a Bayesian setting, we supply the prior probabilities π0 and π1 , which are positive quantities summing up to 1 (the degenerate cases π0 = 0 or π1 = 0 are excluded). Physically discriminating between these hypotheses corresponds to performing a generalised (POVM) measurement on the q ...
Here - Rabia Aslam
... for every boson there is a corresponding fermion and vice versa. Richard Feynman gave another approach for Quantum Mechanics than Schrodinger’s Equation. Although his method was theoretically totally different than Schrodinger’s equation , It gave the same results. Here is the great idea: In classic ...
... for every boson there is a corresponding fermion and vice versa. Richard Feynman gave another approach for Quantum Mechanics than Schrodinger’s Equation. Although his method was theoretically totally different than Schrodinger’s equation , It gave the same results. Here is the great idea: In classic ...
