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... The purpose of physics is to study entities of the natural world, existing independently from any particular observer's perception, and obeying universal and intelligible rules. Many physicists (inc. me) look at certain and reproducible events as real, so we like : If, without in any way disturbing ...
... The purpose of physics is to study entities of the natural world, existing independently from any particular observer's perception, and obeying universal and intelligible rules. Many physicists (inc. me) look at certain and reproducible events as real, so we like : If, without in any way disturbing ...
elements of quantum mechanics
... the photon description is natural when we deal with highly energetic photon of very short wavelength. Light and other electromagnetic radiation sometimes act like waves and sometimes like particles. Interference and diffraction demonstrate wave behaviour while emission and absorption of photons demo ...
... the photon description is natural when we deal with highly energetic photon of very short wavelength. Light and other electromagnetic radiation sometimes act like waves and sometimes like particles. Interference and diffraction demonstrate wave behaviour while emission and absorption of photons demo ...
What quantum computers may tell us about quantum mechanics
... Information theory began in the mid twentieth century, with Claude Shannon’s seminal discovery of how to quantify classical information (Shannon 1948). Shannon’s bit, or binary digit, became the fundamental unit, providing a metric for comparing forms of information and optimizing the amount of reso ...
... Information theory began in the mid twentieth century, with Claude Shannon’s seminal discovery of how to quantify classical information (Shannon 1948). Shannon’s bit, or binary digit, became the fundamental unit, providing a metric for comparing forms of information and optimizing the amount of reso ...
Bose-Einstein Condensation and Free DKP field
... the last term is an infinity quantity β–dependent, and, as in the spin 0 sector, it will be cancelled by the N (β) contribution, thus with all security we set it to be XZ d3 p ...
... the last term is an infinity quantity β–dependent, and, as in the spin 0 sector, it will be cancelled by the N (β) contribution, thus with all security we set it to be XZ d3 p ...
Why is there an invariant speed c?
... The reason is that a particle undergoing such motion can move a distance larger than LP during TP in a discontinuous way. Moreover, since the direction of each discontinuous movement may be forward and backward, the average velocity of the particle can still be smaller than c. ...
... The reason is that a particle undergoing such motion can move a distance larger than LP during TP in a discontinuous way. Moreover, since the direction of each discontinuous movement may be forward and backward, the average velocity of the particle can still be smaller than c. ...
A classical path to unification - Max-Planck
... neous collapse of the state vectors for both particles a and b. Entanglement appears in this representation as a causality-violating space-like phenomenon directly connecting the two measurement processes. The right panel C represents the interpretation of entanglement for a classical model exhibit ...
... neous collapse of the state vectors for both particles a and b. Entanglement appears in this representation as a causality-violating space-like phenomenon directly connecting the two measurement processes. The right panel C represents the interpretation of entanglement for a classical model exhibit ...
Topological Phases of Matter classification and application
... Hall liquids, engineered quantum systems,... ...
... Hall liquids, engineered quantum systems,... ...
PROBABILITIES FOR SINGLE EVENTS
... where p↑ = | <↑ |ψ > |2 and p↓ = 1 − p↑ . As N becomes large this approaches a continuum normal distribution that is sharply peaked about f = p↑ . The width becomes arbitrarily small with large N as N −1/2 . Thus, the probability for finding f in some range about p↑ can be made close to one by choos ...
... where p↑ = | <↑ |ψ > |2 and p↓ = 1 − p↑ . As N becomes large this approaches a continuum normal distribution that is sharply peaked about f = p↑ . The width becomes arbitrarily small with large N as N −1/2 . Thus, the probability for finding f in some range about p↑ can be made close to one by choos ...
Optical Faraday Rotation Abstract
... Since the external …elds are weak, a perturbative approach can be used.10 In a perturbation theory limit, one can work with state amplitudes rather than density matrix elements. The state vector for the oscillator can be written as j (t)i = a0 (t) jL = 0i + ...
... Since the external …elds are weak, a perturbative approach can be used.10 In a perturbation theory limit, one can work with state amplitudes rather than density matrix elements. The state vector for the oscillator can be written as j (t)i = a0 (t) jL = 0i + ...
Quantum Connections
... modules made of such entangled ion crystals. One is to physically move a few of the ion qubits through space, from one module to another, by passing them through a complex maze of electrodes (a method proposed in 2000 by Monroe, along with Wineland and David Kielpinski, then at nist). The ions can b ...
... modules made of such entangled ion crystals. One is to physically move a few of the ion qubits through space, from one module to another, by passing them through a complex maze of electrodes (a method proposed in 2000 by Monroe, along with Wineland and David Kielpinski, then at nist). The ions can b ...