Quantum Complementarity for the Superconducting Condensate and the Resulting Electrodynamic Duality. Abstract
... which one intends to measure ’the position of the electron’ [ read ’the phase of the superconductor’], otherwise these words have no meaning [3].” Today we might say that when we interpret experiments with quantum mechanics, we use a semi-classical approach and this approach requires that the quanti ...
... which one intends to measure ’the position of the electron’ [ read ’the phase of the superconductor’], otherwise these words have no meaning [3].” Today we might say that when we interpret experiments with quantum mechanics, we use a semi-classical approach and this approach requires that the quanti ...
Motion of charged particles in magnetic fields created by symmetric
... recent results on the existence of first integrals and chaos can be consulted in [2, 3, 17]. In this work we shall not study the magnetic lines (a static situation), but the motion of a charged particle in the presence of a magnetic field (a dynamical situation). Contrary to what happens in some pla ...
... recent results on the existence of first integrals and chaos can be consulted in [2, 3, 17]. In this work we shall not study the magnetic lines (a static situation), but the motion of a charged particle in the presence of a magnetic field (a dynamical situation). Contrary to what happens in some pla ...
Edge theory of ferromagnetic quantum Hall states
... the one which edge physics we would like to understand, it is expected that the charge dynamics is reduced to the edge of the system. This is maybe an oversimplification with respect to a general experimental situation where sharp edges ~i.e., edges with steep confining potential! are not always pre ...
... the one which edge physics we would like to understand, it is expected that the charge dynamics is reduced to the edge of the system. This is maybe an oversimplification with respect to a general experimental situation where sharp edges ~i.e., edges with steep confining potential! are not always pre ...
Entropy, Strings, and Partitions of Integers
... where n is a non-negative integer and ~ = 1.05 × 10−34 J·s is Planck’s constant. Terminology: An oscillator with energy En “is in state n” or “has n excitations at frequency ω.” ...
... where n is a non-negative integer and ~ = 1.05 × 10−34 J·s is Planck’s constant. Terminology: An oscillator with energy En “is in state n” or “has n excitations at frequency ω.” ...
Quantum Computer Compilers - Computer Science, Columbia
... • “I’d say almost any prediction about what a quantum computer will look like will, with high probability, be wrong. Ion trappers are encouraged because we can at least see a straightforward path to making a large processor, but the technical problems are extremely challenging. It might be fair to s ...
... • “I’d say almost any prediction about what a quantum computer will look like will, with high probability, be wrong. Ion trappers are encouraged because we can at least see a straightforward path to making a large processor, but the technical problems are extremely challenging. It might be fair to s ...
Simulating physics with computers
... describe the possibility of simulating physics in the classical approximation, a thing which is usuaUy described by local differential equations. But the physical world is quantum mechanical, and therefore the proper problem is the simulation of quantum physics--which is what I really want to talk a ...
... describe the possibility of simulating physics in the classical approximation, a thing which is usuaUy described by local differential equations. But the physical world is quantum mechanical, and therefore the proper problem is the simulation of quantum physics--which is what I really want to talk a ...
Randomness and Multi-level Interactions in Biology1
... their gravitational fields. As a consequence, the Solar system, for example, turns out to be non-additive, and the non-linearity of the equations expresses this fact. Mathematically, non-additivity (nonlinearity) is enhanced as soon as more than two “bodies” (entities) interact and modify by this ea ...
... their gravitational fields. As a consequence, the Solar system, for example, turns out to be non-additive, and the non-linearity of the equations expresses this fact. Mathematically, non-additivity (nonlinearity) is enhanced as soon as more than two “bodies” (entities) interact and modify by this ea ...
The Status of our Ordinary Three Dimensions in a Quantum Universe 1
... time t 1 , the collapse postulate gives only chances that the wavefunction of the system will be at any other state at a later time, t 2 . Because these laws give different predictions regarding the future states of quantum systems, the question immediately arises: in which circumstances does each l ...
... time t 1 , the collapse postulate gives only chances that the wavefunction of the system will be at any other state at a later time, t 2 . Because these laws give different predictions regarding the future states of quantum systems, the question immediately arises: in which circumstances does each l ...
The stuff the world is made of: physics and reality
... perspective following from this human interaction. We can only observe the universe from the earth, and this gave us the perspective that the earth plays a central role. In an analogous way we can only observe the micro-world from our position in the macro-world; this forces us to extend the concept ...
... perspective following from this human interaction. We can only observe the universe from the earth, and this gave us the perspective that the earth plays a central role. In an analogous way we can only observe the micro-world from our position in the macro-world; this forces us to extend the concept ...
Highly doubly excited S states of the helium atom
... with real b, B. A typical choice for b is b = l / N or smaller ( N is the principal quantum number of the HeC ion to which the Rydberg series converges). By solving (8) we get a large number of converged complex eigenvalues that represent the doubly excited resonances. 2.2. Numerical computation of ...
... with real b, B. A typical choice for b is b = l / N or smaller ( N is the principal quantum number of the HeC ion to which the Rydberg series converges). By solving (8) we get a large number of converged complex eigenvalues that represent the doubly excited resonances. 2.2. Numerical computation of ...
Classical Cryptographic Protocols in a Quantum World
... “simple hybrid arguments”. They use rewinding neither in the simulation nor in any of the steps that show the correctness of simulation.1 Our observation allows us to port a general result of Canetti, Lindell, Ostrovsky and Sahai [13] to the quantum setting. We obtain the following: in the G ZK -hy ...
... “simple hybrid arguments”. They use rewinding neither in the simulation nor in any of the steps that show the correctness of simulation.1 Our observation allows us to port a general result of Canetti, Lindell, Ostrovsky and Sahai [13] to the quantum setting. We obtain the following: in the G ZK -hy ...
