Quantum blockade and loop currents in graphene with topological defects
... localization, we plot, in Figs. 3共a兲 and 3共b兲, the spatial distribution of LDOS , and local currents i far 共point J in Fig. 2兲 away from and near 共point H in Fig. 2兲 the antiresonance, respectively. The LDOS does not vary much at the two points, but the currents do. In Fig. 3共a兲, where G is not sha ...
... localization, we plot, in Figs. 3共a兲 and 3共b兲, the spatial distribution of LDOS , and local currents i far 共point J in Fig. 2兲 away from and near 共point H in Fig. 2兲 the antiresonance, respectively. The LDOS does not vary much at the two points, but the currents do. In Fig. 3共a兲, where G is not sha ...
physics and narrative - Rutgers Philosophy Department
... other that K cannot be deduced, either by means of the application of a geometrical space-time point-transformation or in any other way, from the complete history of the quantum state of S in K - because transformation in question would need (per impossible!) to map precisely the same history in K i ...
... other that K cannot be deduced, either by means of the application of a geometrical space-time point-transformation or in any other way, from the complete history of the quantum state of S in K - because transformation in question would need (per impossible!) to map precisely the same history in K i ...
the quantum vacuum
... ZPE follows from the uncertainty relation of quantum mechanics. This foundation phase of the quantum vacuum culminated in the inclusion of ZPE into Quantum Electrodynamics (QED) by BORN, HEISENBERG and JORDAN, who predicted fluctuating ZP or vacuum fields even in the absence of any sources (Born, He ...
... ZPE follows from the uncertainty relation of quantum mechanics. This foundation phase of the quantum vacuum culminated in the inclusion of ZPE into Quantum Electrodynamics (QED) by BORN, HEISENBERG and JORDAN, who predicted fluctuating ZP or vacuum fields even in the absence of any sources (Born, He ...
![Dirac multimode ket-bra operators` [equation]](http://s1.studyres.com/store/data/023088225_1-3900fa8a2c451013a9516ce21d0ecd01-300x300.png)
CHAPTERONE(1D2)
... overturned this dogma. It seemed that the speed of light, c was independent of the direction in which it was measured. It seemed that c was an upper limit, a velocity, v could not be added to c. Fitzgerald and Heaviside corresponded about this puzzling result and Heaviside came close to resolving t ...
... overturned this dogma. It seemed that the speed of light, c was independent of the direction in which it was measured. It seemed that c was an upper limit, a velocity, v could not be added to c. Fitzgerald and Heaviside corresponded about this puzzling result and Heaviside came close to resolving t ...
PH504lec0910-9
... How is the charge distributed on the sphere? The electrons must distribute themselves so the field is zero in the solid part. This means there must be -5 microcoulombs of charge on the inner surface, to stop all the field lines from the +5 microcoulomb point charge. There must then be +2 microcoulom ...
... How is the charge distributed on the sphere? The electrons must distribute themselves so the field is zero in the solid part. This means there must be -5 microcoulombs of charge on the inner surface, to stop all the field lines from the +5 microcoulomb point charge. There must then be +2 microcoulom ...
Lecture notes - Oxford Physics
... then be taken up and applied in other areas such as particle physics and condensed matter physics. These concepts include not just quantisation of energy, but also more subtle ideas such as exchange symmetry and many-particle wavefunctions. Before we try to understand the quantum mechanics of a soli ...
... then be taken up and applied in other areas such as particle physics and condensed matter physics. These concepts include not just quantisation of energy, but also more subtle ideas such as exchange symmetry and many-particle wavefunctions. Before we try to understand the quantum mechanics of a soli ...
Renormalization
In quantum field theory, the statistical mechanics of fields, and the theory of self-similar geometric structures, renormalization is any of a collection of techniques used to treat infinities arising in calculated quantities.Renormalization specifies relationships between parameters in the theory when the parameters describing large distance scales differ from the parameters describing small distances. Physically, the pileup of contributions from an infinity of scales involved in a problem may then result in infinities. When describing space and time as a continuum, certain statistical and quantum mechanical constructions are ill defined. To define them, this continuum limit, the removal of the ""construction scaffolding"" of lattices at various scales, has to be taken carefully, as detailed below.Renormalization was first developed in quantum electrodynamics (QED) to make sense of infinite integrals in perturbation theory. Initially viewed as a suspect provisional procedure even by some of its originators, renormalization eventually was embraced as an important and self-consistent actual mechanism of scale physics in several fields of physics and mathematics. Today, the point of view has shifted: on the basis of the breakthrough renormalization group insights of Kenneth Wilson, the focus is on variation of physical quantities across contiguous scales, while distant scales are related to each other through ""effective"" descriptions. All scales are linked in a broadly systematic way, and the actual physics pertinent to each is extracted with the suitable specific computational techniques appropriate for each.