Quantum Theory
... In order to know where an electron is we have to “see” it. To see something it must be hit by a photon. Photons and electrons are roughly the same size, when they collide the electron will no longer be in the same position. ...
... In order to know where an electron is we have to “see” it. To see something it must be hit by a photon. Photons and electrons are roughly the same size, when they collide the electron will no longer be in the same position. ...
The Cutkosky rule of three dimensional noncommutative field
... If the 2+1 dimensional noncommutative field theory gives a 2+1 dimensional quantum gravity theory with massive particles, why isn’t the arbitrary negative energy included? Y.S., Sasakura (2009) One-particle solution in 2+1 dimensional Einstein gravity ...
... If the 2+1 dimensional noncommutative field theory gives a 2+1 dimensional quantum gravity theory with massive particles, why isn’t the arbitrary negative energy included? Y.S., Sasakura (2009) One-particle solution in 2+1 dimensional Einstein gravity ...
Comparison of 3D classical and quantum mechanical He scattering
... mechanical [4]. What does it mean in the picture of quantum mechanics? Since the interaction is generally strong, EhrenfestÕs theorem invalidates the picture of the trajectories. If we adhere the purely stochastic (``Heidelberg approach'') discussion of quantum chaos; the dwell time of atoms near th ...
... mechanical [4]. What does it mean in the picture of quantum mechanics? Since the interaction is generally strong, EhrenfestÕs theorem invalidates the picture of the trajectories. If we adhere the purely stochastic (``Heidelberg approach'') discussion of quantum chaos; the dwell time of atoms near th ...
PRIGOGINE Y LA TEORÍA DEL CAOS: UNA MIRADA FILOSÓFICA.
... as if the system were in a state represented by a diagonal density operator (. It can be proved that decoherence also obtains when the spectrum of the Hamiltonian has a single discrete value non-overlapping with the continuous part; but if the Hamiltonian’s spectrum has more than one non-overlapp ...
... as if the system were in a state represented by a diagonal density operator (. It can be proved that decoherence also obtains when the spectrum of the Hamiltonian has a single discrete value non-overlapping with the continuous part; but if the Hamiltonian’s spectrum has more than one non-overlapp ...
Extrimes of Information Combining
... Quantum Enumerators Fidelity of Quantum ARQ Protocol • Quantum Codes of Finite Lengths • The asymptotical Case (the code length ...
... Quantum Enumerators Fidelity of Quantum ARQ Protocol • Quantum Codes of Finite Lengths • The asymptotical Case (the code length ...
The Ideal Gas on the Canonical Ensemble
... both molecules are in the same state, the second term corresponds to the molecules being in different states. We can now see the problem. When the particles are in different state, we have counted each state twice. The state with one molecule in state 1, the other in state 2, could be written as s = ...
... both molecules are in the same state, the second term corresponds to the molecules being in different states. We can now see the problem. When the particles are in different state, we have counted each state twice. The state with one molecule in state 1, the other in state 2, could be written as s = ...
Open-System Quantum Simulation with Atoms and Ions
... a many-particle system. For the master equation, necessary conditions to achieve such dissipative dynamics which contracts to a pure state is given by the conditions H |ψi = E |ψi, and ∀α cα |ψi = 0. As the last condition illustrates, |ψi is a state decoupled from the environment, which in quantum o ...
... a many-particle system. For the master equation, necessary conditions to achieve such dissipative dynamics which contracts to a pure state is given by the conditions H |ψi = E |ψi, and ∀α cα |ψi = 0. As the last condition illustrates, |ψi is a state decoupled from the environment, which in quantum o ...
“Shut The Front Door!”: Obviating the Challenge of Large
... multiverse [8] where the energy of inflation is internalized locally as a form of gravitational free-fall giving the Euclidean observer his façade of virtual reality (Figs. 2 & 3). If this sounds like a horrendous concatenation violating Occam’s razor, be reminded that if one is inclined to accept t ...
... multiverse [8] where the energy of inflation is internalized locally as a form of gravitational free-fall giving the Euclidean observer his façade of virtual reality (Figs. 2 & 3). If this sounds like a horrendous concatenation violating Occam’s razor, be reminded that if one is inclined to accept t ...
Introduction To Quantum Computing
... Threshold Theorem Our entire discussion so far has been on “perfect” quantum gates, but of course they are not perfect. Various “threshold theorems” have suggested that we need 10^4 to 10^6 gates in less than the decoherence time in order to apply quantum error correction (QEC). QEC is a big enough ...
... Threshold Theorem Our entire discussion so far has been on “perfect” quantum gates, but of course they are not perfect. Various “threshold theorems” have suggested that we need 10^4 to 10^6 gates in less than the decoherence time in order to apply quantum error correction (QEC). QEC is a big enough ...
Symmetry and Asymmetry in the Mendeleïev`s Periodic Table
... Niels Bohr established the relation between the position of each Element in the periodic table and its electronic structure. The chemical properties of each Element are thus COMPLETELY DETERMINED by the distribution of the electrons of this Element. The properties and positioning of these electrons, ...
... Niels Bohr established the relation between the position of each Element in the periodic table and its electronic structure. The chemical properties of each Element are thus COMPLETELY DETERMINED by the distribution of the electrons of this Element. The properties and positioning of these electrons, ...
Quantum Chemistry Postulates Chapter 14 ∫
... For a physical system consisting of a particle(s) there are associated mathematical functions known as wave functions. A wave function carries ‘information’ about everything that can be known (observable/measurable) about the system. Every observable property is associated with an operator. Operatin ...
... For a physical system consisting of a particle(s) there are associated mathematical functions known as wave functions. A wave function carries ‘information’ about everything that can be known (observable/measurable) about the system. Every observable property is associated with an operator. Operatin ...