Quantum Gates and Simon`s Algorithm
... Basic Facts About Boolean Functions Boolean functions Any function f : {0, 1}n → {0, 1}m , where n is the number of input bits and m the number of output bits is said to be a Boolean function. Any Boolean function can be represented by a truth table. If f = (f1 , . . . , fm ), this is a matrix of s ...
... Basic Facts About Boolean Functions Boolean functions Any function f : {0, 1}n → {0, 1}m , where n is the number of input bits and m the number of output bits is said to be a Boolean function. Any Boolean function can be represented by a truth table. If f = (f1 , . . . , fm ), this is a matrix of s ...
- Quantum Optics and Spectroscopy
... difficulty in building a large quantum computer lies mainly in the fact that the quantum mechanical system cannot be shielded well enough from the environment resulting in erroneous calculations. In quantum physics this is known as decoherence which is responsible for the fact that we do not experie ...
... difficulty in building a large quantum computer lies mainly in the fact that the quantum mechanical system cannot be shielded well enough from the environment resulting in erroneous calculations. In quantum physics this is known as decoherence which is responsible for the fact that we do not experie ...
Quantum Chaos, Transport, and Decoherence in Atom
... digital camera I used to take the photographs in this dissertation), Artur Widera, Patrick Bloom, Greg Henry, Arnaud Cursente, Wes Campbell, and Fred the mouse. Thanks also to Adrienne Lipoma and Julie Horn for keeping the lab running smoothly. I have learned much during my graduate studies, due in ...
... digital camera I used to take the photographs in this dissertation), Artur Widera, Patrick Bloom, Greg Henry, Arnaud Cursente, Wes Campbell, and Fred the mouse. Thanks also to Adrienne Lipoma and Julie Horn for keeping the lab running smoothly. I have learned much during my graduate studies, due in ...
Introduction to Quantum Information
... If we encoded each of the k distinct symbols as a distinct binary number, i.e., as a distinct string of 0’s and 1’s, we would need strings composed of log k bits to represent each symbol (2log k = k). Shannon’s analysis shows that messages produced by a stochastic source can be compressed, in the se ...
... If we encoded each of the k distinct symbols as a distinct binary number, i.e., as a distinct string of 0’s and 1’s, we would need strings composed of log k bits to represent each symbol (2log k = k). Shannon’s analysis shows that messages produced by a stochastic source can be compressed, in the se ...
Spin Squeezing, Macrorealism and the Heisenberg uncertainty
... be attributed to a violation of classical principles, such as local-realism or macroscopicrealism in macroscopic systems, e.g., large ensembles of atoms. At first, after reviewing the basic principles and defining what a quantum state is, we will retrace the historical debate started around the foun ...
... be attributed to a violation of classical principles, such as local-realism or macroscopicrealism in macroscopic systems, e.g., large ensembles of atoms. At first, after reviewing the basic principles and defining what a quantum state is, we will retrace the historical debate started around the foun ...
Holonomic Quantum Control with Continuous
... to gain a Berry phase distinct from the other three states. Since Berry phases of different modes add, we analyze the â=b̂-mode contributions individually. For any state that contains the j− δαi component (in either mode), the Berry phase gained for each of the two circles is proportional to their ...
... to gain a Berry phase distinct from the other three states. Since Berry phases of different modes add, we analyze the â=b̂-mode contributions individually. For any state that contains the j− δαi component (in either mode), the Berry phase gained for each of the two circles is proportional to their ...
