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... driven to enable storage in the long-lived D levels; A-to-C cycling transition permits nondestructive determination of when a photon has been absorbed. (b) Ultrabright narrowband source of polarization-entangled photon pairs: each optical parametric amplifier (OPAs 1 and 2) is type-II phase matched; ...
... driven to enable storage in the long-lived D levels; A-to-C cycling transition permits nondestructive determination of when a photon has been absorbed. (b) Ultrabright narrowband source of polarization-entangled photon pairs: each optical parametric amplifier (OPAs 1 and 2) is type-II phase matched; ...
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... In this section we will construct a computational model, based on the lambda calculus, suitable for describing quantum computations. The language used will be an adaptation of the classical lambda calculus, extended with a set of quantum primitives. We will denote it by λi where the subscript stands ...
... In this section we will construct a computational model, based on the lambda calculus, suitable for describing quantum computations. The language used will be an adaptation of the classical lambda calculus, extended with a set of quantum primitives. We will denote it by λi where the subscript stands ...
Towards a Quantum Programming Language
... The recent literature contains several proposals for quantum programming languages. One of the first contributions in this direction is an article by Knill (1996). While not proposing an actual programming language, Knill outlines a set of basic principles for writing pseudo-code for quantum algorit ...
... The recent literature contains several proposals for quantum programming languages. One of the first contributions in this direction is an article by Knill (1996). While not proposing an actual programming language, Knill outlines a set of basic principles for writing pseudo-code for quantum algorit ...
SUPERCONDUCTING QUBITS II: DECOHERENCE F.K. Wilhelm , M.J. Storcz and U. Hartmann
... which conserves entropy. Indeed, also the CPT theorem of relativistic quantum mechanics (Sakurai, 1967) states, that for each quantum system it is possible to find a counterpart (with inversed parity and charge) whose time arrow runs backwards. The apparent contradiction between microreversibility — ...
... which conserves entropy. Indeed, also the CPT theorem of relativistic quantum mechanics (Sakurai, 1967) states, that for each quantum system it is possible to find a counterpart (with inversed parity and charge) whose time arrow runs backwards. The apparent contradiction between microreversibility — ...