The Copenhagen interpretation, and pragmatism1 Willem M. de
... mechanical observable is exclusively defined within the context of the measurement serving to measure that observable. Both points are liable to criticism. The first point has its origin in the logical positivist ideal of basing a theory on theory-independent observational data, so as to evade the v ...
... mechanical observable is exclusively defined within the context of the measurement serving to measure that observable. Both points are liable to criticism. The first point has its origin in the logical positivist ideal of basing a theory on theory-independent observational data, so as to evade the v ...
Ei dian otsikkoa - Helsingin yliopisto
... CLIC = Compact Linear Collider ‘only’ 47.9 km A proposed e- – e+ linear collider, with a CM energy of up to 3 TeV in the final design (cf. LEP max. 209 GeV) Linear Can ...
... CLIC = Compact Linear Collider ‘only’ 47.9 km A proposed e- – e+ linear collider, with a CM energy of up to 3 TeV in the final design (cf. LEP max. 209 GeV) Linear Can ...
A logico-conceptual analysis of the Einstein-Podolsky
... these magnitudes are positions and momenta; a much simpler version was later devised by David Bohm, in terms of spin components (Bohm 1951). The measurement of one of these quantities on one of the objects of the pair allows us to infer with certainty the measurement result of the same quantity for ...
... these magnitudes are positions and momenta; a much simpler version was later devised by David Bohm, in terms of spin components (Bohm 1951). The measurement of one of these quantities on one of the objects of the pair allows us to infer with certainty the measurement result of the same quantity for ...
A Post Processing Method for Quantum Prime Factorization
... ACTORIZING large integers has been an important problem from past till now especially in the state of RSA technique [1, 2]. In the RSA data encryption technique it is needed to find a very large integer that equals to multiplication of two large prime numbers. Many types of Prime Factorization metho ...
... ACTORIZING large integers has been an important problem from past till now especially in the state of RSA technique [1, 2]. In the RSA data encryption technique it is needed to find a very large integer that equals to multiplication of two large prime numbers. Many types of Prime Factorization metho ...
Classical field records of a quantum system: Their internal
... benchmarking in 1D shows that the ideal gas results carry over unchanged into the weakly interacting gas. The optimum high-energy cutoff is in general shown to depend strongly on the observable in question (e.g., energy, density fluctuations, phase coherence length, condensate fraction). This explai ...
... benchmarking in 1D shows that the ideal gas results carry over unchanged into the weakly interacting gas. The optimum high-energy cutoff is in general shown to depend strongly on the observable in question (e.g., energy, density fluctuations, phase coherence length, condensate fraction). This explai ...
Physics 207: Lecture 2 Notes
... Forces occur in pairs: FA , B = - FB , A (For every action there is an equal and opposite reaction.) Read: Force of B on A ...
... Forces occur in pairs: FA , B = - FB , A (For every action there is an equal and opposite reaction.) Read: Force of B on A ...
results, conjectures and applications to quasicrystals
... The framework we propose is valid within the one electron approximation. We will ignore explicitly the phonons and the electron–electron interactions as a first step. In this section only non-dissipative transport properties are considered. These are dominated by interference effects due to Bragg re ...
... The framework we propose is valid within the one electron approximation. We will ignore explicitly the phonons and the electron–electron interactions as a first step. In this section only non-dissipative transport properties are considered. These are dominated by interference effects due to Bragg re ...
Luttinger Liquids
... To actually calculate the Fourier transform of this expression to extract the momentum distribution N(p) discussed in the context of Fermi liquids, is a bit complicated. The result is however, as expected, that the discontinuity totally disappears, which shows that there are no stable gapless charge ...
... To actually calculate the Fourier transform of this expression to extract the momentum distribution N(p) discussed in the context of Fermi liquids, is a bit complicated. The result is however, as expected, that the discontinuity totally disappears, which shows that there are no stable gapless charge ...
Multiphoton localization and propagating quantum gap solitons in a
... frequencies is found from the equation h(Ω) = H, which has a root lying in C− only if H < 0. The soliton obtained is quite similar to a vacuum soliton, and we will use the phrase “ordinary soliton” to refer to this solution, despite its inordinate behavior on different polariton branches. Polaritons ...
... frequencies is found from the equation h(Ω) = H, which has a root lying in C− only if H < 0. The soliton obtained is quite similar to a vacuum soliton, and we will use the phrase “ordinary soliton” to refer to this solution, despite its inordinate behavior on different polariton branches. Polaritons ...
Spintronics and Quantum Dots for Quantum Computing and
... quantum dots have been measured [29], with at most one spin per dot. The relatively small T2∗ decoherence times (a few ns at vanishing magnetic field), which have been seen in these experiments, probably originate from a large inhomogeneous broadening due to a strong variation of g-factors [29]. Nev ...
... quantum dots have been measured [29], with at most one spin per dot. The relatively small T2∗ decoherence times (a few ns at vanishing magnetic field), which have been seen in these experiments, probably originate from a large inhomogeneous broadening due to a strong variation of g-factors [29]. Nev ...
Experimental Creation and Measurement of Motional Quantum
... number states jnx ny nz i. We will consider coupling to only the x^ dimension harmonic oscillator with number states jnxi = jni [n = 1; 2;...,1; see Fig. 1(a)]. To couple the motional and internal degrees of freedom of ...
... number states jnx ny nz i. We will consider coupling to only the x^ dimension harmonic oscillator with number states jnxi = jni [n = 1; 2;...,1; see Fig. 1(a)]. To couple the motional and internal degrees of freedom of ...
Get PDF - OSA Publishing
... Finally, the eigenstate of the ad hoc Hamiltonian turns out to be the same as the true scattering eigenstate—other than the reservoir degree of freedom, which it is missing. This fact allows a correct real-space interacting eigenstate solution [6,7,27,28] for the nonreservoir dynamics that account f ...
... Finally, the eigenstate of the ad hoc Hamiltonian turns out to be the same as the true scattering eigenstate—other than the reservoir degree of freedom, which it is missing. This fact allows a correct real-space interacting eigenstate solution [6,7,27,28] for the nonreservoir dynamics that account f ...
Quantum gases in optical lattices
... Meanwhile, William Phillips and coremarkable aspect about this phase potentials are then used to “split” each atom such workers at NIST in Gaithersburg, US, transition is that it can occur even at a that it simultaneously moves to the right and to have studied the initial effects on 1D the left, and ...
... Meanwhile, William Phillips and coremarkable aspect about this phase potentials are then used to “split” each atom such workers at NIST in Gaithersburg, US, transition is that it can occur even at a that it simultaneously moves to the right and to have studied the initial effects on 1D the left, and ...
Renormalization group
In theoretical physics, the renormalization group (RG) refers to a mathematical apparatus that allows systematic investigation of the changes of a physical system as viewed at different distance scales. In particle physics, it reflects the changes in the underlying force laws (codified in a quantum field theory) as the energy scale at which physical processes occur varies, energy/momentum and resolution distance scales being effectively conjugate under the uncertainty principle (cf. Compton wavelength).A change in scale is called a ""scale transformation"". The renormalization group is intimately related to ""scale invariance"" and ""conformal invariance"", symmetries in which a system appears the same at all scales (so-called self-similarity). (However, note that scale transformations are included in conformal transformations, in general: the latter including additional symmetry generators associated with special conformal transformations.)As the scale varies, it is as if one is changing the magnifying power of a notional microscope viewing the system. In so-called renormalizable theories, the system at one scale will generally be seen to consist of self-similar copies of itself when viewed at a smaller scale, with different parameters describing the components of the system. The components, or fundamental variables, may relate to atoms, elementary particles, atomic spins, etc. The parameters of the theory typically describe the interactions of the components. These may be variable ""couplings"" which measure the strength of various forces, or mass parameters themselves. The components themselves may appear to be composed of more of the self-same components as one goes to shorter distances.For example, in quantum electrodynamics (QED), an electron appears to be composed of electrons, positrons (anti-electrons) and photons, as one views it at higher resolution, at very short distances. The electron at such short distances has a slightly different electric charge than does the ""dressed electron"" seen at large distances, and this change, or ""running,"" in the value of the electric charge is determined by the renormalization group equation.