Tomasz Bigaj - Spacetime Society
... worlds with respect to their similarity to the actual world (see Lewis 1973, Finkelstein 1999, and Bigaj 2004). The next crucial element of the counterfactual reconstruction of the EPR argument is the locality condition. The general semantic locality condition (referred to as SLOC) adopted for the ...
... worlds with respect to their similarity to the actual world (see Lewis 1973, Finkelstein 1999, and Bigaj 2004). The next crucial element of the counterfactual reconstruction of the EPR argument is the locality condition. The general semantic locality condition (referred to as SLOC) adopted for the ...
The pseudodifferential operator square root of the Klein
... Zitterbewegun~ and generally to difficulties for the interpretation of this equation. [Both problems (ii) and (iii) can be overcome by demanding that the KG particles be charged. Also second quantization removes these difficulties.] (iv) There is no good canonical position operator. These are reason ...
... Zitterbewegun~ and generally to difficulties for the interpretation of this equation. [Both problems (ii) and (iii) can be overcome by demanding that the KG particles be charged. Also second quantization removes these difficulties.] (iv) There is no good canonical position operator. These are reason ...
Connecting processing-capable quantum memories over telecommunication links via quantum frequency conversion
... waveguide length, the input signal can be completely converted into an output of a different frequency while its quantum state is preserved. It is this state-preserving feature of SFG and DFG that enables the QFC operation. To build QFC devices compatible with the quantummemory devices described in ...
... waveguide length, the input signal can be completely converted into an output of a different frequency while its quantum state is preserved. It is this state-preserving feature of SFG and DFG that enables the QFC operation. To build QFC devices compatible with the quantummemory devices described in ...
Contradiction of Quantum Mechanics with Local Hidden Variables
... argument for the incompleteness of quantum mechanics. The argument was based on the validity of two premises: no action at a distance (locality) and realism. Bell [2] later showed that the predictions of quantum mechanics are incompatible with the premises of local realism (or local hidden variable ...
... argument for the incompleteness of quantum mechanics. The argument was based on the validity of two premises: no action at a distance (locality) and realism. Bell [2] later showed that the predictions of quantum mechanics are incompatible with the premises of local realism (or local hidden variable ...
Electromagnetic radiation and resonance
... Amongst elementary particles, the most mysterious particle is the particle under number one, namely, the photon. As to other elementary particles, there exist judgments concerning their structure or at least one could estimate their size. In the matter of the photon, not only do any conjectures as t ...
... Amongst elementary particles, the most mysterious particle is the particle under number one, namely, the photon. As to other elementary particles, there exist judgments concerning their structure or at least one could estimate their size. In the matter of the photon, not only do any conjectures as t ...
Slides
... Ideally we want a corresponding equation(s) that describes how the CWF evolves in time. For a weakly interacting Bose-condensed gas at T = 0 this equation is the non-linear Schrodinger equation (Gross-Pitaevskii equation) ...
... Ideally we want a corresponding equation(s) that describes how the CWF evolves in time. For a weakly interacting Bose-condensed gas at T = 0 this equation is the non-linear Schrodinger equation (Gross-Pitaevskii equation) ...
Hydrogen 1
... We now have three differential equations (9, 11 and 12) that provide solutions for the r, and components of the wavefunction. That is, we must solve these differential equations to find the wavefunctions R(r), () and (). Once we have these solutions we can then obtain the total, three-dimens ...
... We now have three differential equations (9, 11 and 12) that provide solutions for the r, and components of the wavefunction. That is, we must solve these differential equations to find the wavefunctions R(r), () and (). Once we have these solutions we can then obtain the total, three-dimens ...
