Examples of using The wavefunction in English and their translations into Portuguese
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According to the Copenhagen interpretation, the wavefunction collapses when a measurement is performed.
For his fundamental research in quantum mechanics,especially for his statistical interpretation of the wavefunction"49.
That is, components of the wavefunction are decoupled from a coherent system, and acquire phases from their immediate surroundings.
Therefore, discarding higher modes never leads to drastic changes in the wavefunction spacetime structure.
The wavefunctions on the transmission eigenchannels reveal that the central complex couples more strongly with the left electrode.
We have used the projector augumented wave(paw)method to describe the wavefunctions and charge densities.
The wavefunction of the Schrödinger wave equation reduces to the three equations that when solved lead to the first three quantum numbers.
Since you can't tell the difference between the two until you taste it,“the wavefunction collapses in your mouth, not in your eyes.”.
Probality densities corresponding to the wavefunctions of an electron in a hydrogen atom processing definite energy and angular momentum Schrödinger wave equation.
Bosons are particles whose wavefunction is symmetric under such an exchange or permutation,so if we swap the particles the wavefunction does not change.
In de Broglie-Bohm theory, the wavefunction is defined at both slits, but each particle has a well-defined trajectory that passes through exactly one of the slits.
In his exposition Everett presented his derivation of probability andalso stated explicitly that observers in all branches of the wavefunction were equally"real.
Secondly, observation or measurement has no special laws ormechanics, unlike in the Copenhagen interpretation which considers the wavefunction collapse as a special kind of event which occurs as a result of observation.
It makes two assumptions: first, the wavefunction is not simply a description of the object's state, but that it actually is entirely equivalent to the object, a claim it has in common with some other interpretations.
Causality of the solution is provided by minimal axiomatics invoked only at the initial stage, the problem posing,via the time-asymmetric homogeneous initial conditions imposed upon the wavefunction and the source.
In Bohm's 1952 papers he used the wavefunction to construct a quantum potential that, when included in Newton's equations, gave the trajectories of the particles streaming through the two slits.
Using a pair of entangled photons and performing only a pair of measurements, one for each photon, it is possible, through several repetitions of this process,to distinguish the scenario where the wavefunction presents an instantaneous collapse from another where it takes a finite time to occur.
When the energy of the system is measured, the wavefunction collapses into one of its eigenstates and so the particle wavefunction is described by the pure eigenstate corresponding to the measured energy.
The wavefunction obtained by fixing the parameters to such values is then an approximation to the ground state wavefunction, and the expectation value of the energy in that state is an upper bound to the ground state energy.
It is typically used for a semiclassical calculation in quantum mechanics in which the wavefunction is recast as an exponential function, semiclassically expanded, and then either the amplitude or the phase is taken to be changing slowly.
In effect the wavefunction interferes with itself and guides the particles by the quantum potential in such a way that the particles avoid the regions in which the interference is destructive and are attracted to the regions in which the interference is constructive, resulting in the interference pattern on the detector screen.
Fermions are particleswhose wavefunction is antisymmetric, so under such a swap the wavefunction gets a minus sign, meaning that the amplitude for two identical fermions to occupy the same state must be zero.
In this work, we investigated the influence of a screw dislocation on the energy levels and the wavefunctions of an electron confined in a two-dimensional pseudoharmonic quantum dot under the influence of an external magnetic field inside a dot and aharonov-bohm field inside a pseudodot.
Utilizing research1 into the nature of quantum decoherence andthe possibility of establishing passive control over the wavefunction affecting a specified number of pointer states in observed reality, Project TRAILHEAD ultimately established a limited degree of control around O5-9's place in this established plane of existence.
Effectively, in the many-worlds interpretation the multiverse evolves as a universal wavefunction.
He also agreed with an observation from the floor that the number of branches of the universal wavefunction was an uncountable infinity.
A wavefunction different from the exact one is obtained by use of the method described above.
In the theory of electroweak interaction,the left-handed component of electron's wavefunction forms a weak isospin doublet with the electron neutrino.