
A conformal field theory approach to the fractional quantum Hall
... the many particles needs to be taken into account, which makes the construction of the wave functions analytically impossible. By making educated guesses, many wave functions describing the FQHE at different fractions have been proposed. The properties of these theoretical states can be compared to ...
... the many particles needs to be taken into account, which makes the construction of the wave functions analytically impossible. By making educated guesses, many wave functions describing the FQHE at different fractions have been proposed. The properties of these theoretical states can be compared to ...
QUANTUM COMPUTING: AN OVERVIEW
... each object separately. In a quantum world, however, only a very tiny fraction of all possible states can be described by such separate specifications. In other words, most quantum states cannot be described by such individual specifications, thereby being called “entangled”. Why and how these two fea ...
... each object separately. In a quantum world, however, only a very tiny fraction of all possible states can be described by such separate specifications. In other words, most quantum states cannot be described by such individual specifications, thereby being called “entangled”. Why and how these two fea ...
Giesecke-Final-ternary-gates
... The number of qudits is free to choose, as well as the number of ancilla qudits. Inputs A to Z are qudits that control the multiplexer at the static qudit, and can also be manipulated by other qudits. The structures shown in Fig. 2.4a and Fig. 2.8 are the most desirable and capable to build quantum ...
... The number of qudits is free to choose, as well as the number of ancilla qudits. Inputs A to Z are qudits that control the multiplexer at the static qudit, and can also be manipulated by other qudits. The structures shown in Fig. 2.4a and Fig. 2.8 are the most desirable and capable to build quantum ...