12 Quantum Electrodynamics
... and Bleuler in Subsection 7.5.3. In their quantization scheme, the propagator took a pleasant covariant form. But this happened at the expense of another disadvantage, that this Lagrangian describes the propagation of four particles of which only two correspond to physical states. Accordingly, the H ...
... and Bleuler in Subsection 7.5.3. In their quantization scheme, the propagator took a pleasant covariant form. But this happened at the expense of another disadvantage, that this Lagrangian describes the propagation of four particles of which only two correspond to physical states. Accordingly, the H ...
`Electronium`: a quantum atomic teaching model
... quantity. Within the atom, the electron is seen as an extended object, consisting of the substance Electronium, which is distributed around the nucleus. Electronium is not particulate in nature but is a continuum with varying density. The absolute square of the -function is interpreted as being pro ...
... quantity. Within the atom, the electron is seen as an extended object, consisting of the substance Electronium, which is distributed around the nucleus. Electronium is not particulate in nature but is a continuum with varying density. The absolute square of the -function is interpreted as being pro ...
Propagation of double Rydberg wave packets F Robicheaux and R C Forrey doi:10.1088/0953-4075/38/2/027
... works perfectly well for time-independent calculations of resonance parameters, it works very poorly for this time-dependent problem. The reason is that unless |β| is larger than ∼1.7 there are always some eigenvalues of the time-independent problem that have positive imaginary parts which causes an ...
... works perfectly well for time-independent calculations of resonance parameters, it works very poorly for this time-dependent problem. The reason is that unless |β| is larger than ∼1.7 there are always some eigenvalues of the time-independent problem that have positive imaginary parts which causes an ...
Majorana Fermions - Physics | Oregon State University
... deconfinement physics expected for QSLs. Comparing these with recent dynamical calculations involving gauge flux excitations and Majorana fermions of the pure Kitaev model, we propose the excitation spectrum of α-RuCl3 as a prime candidate for fractionalized Kitaev physics. ...
... deconfinement physics expected for QSLs. Comparing these with recent dynamical calculations involving gauge flux excitations and Majorana fermions of the pure Kitaev model, we propose the excitation spectrum of α-RuCl3 as a prime candidate for fractionalized Kitaev physics. ...
Dephasing and the Orthogonality Catastrophe in Tunneling through a Quantum... The “Which Path?” Interferometer
... QD. These virtual processes result in power-law suppression of the Aharonov-Bohm oscillations. This is an example of the orthogonality catastrophe [10,11], and is an inevitable consequence of “measurement” by local interaction with a many-body system. (We neglect the additional orthogonality catastr ...
... QD. These virtual processes result in power-law suppression of the Aharonov-Bohm oscillations. This is an example of the orthogonality catastrophe [10,11], and is an inevitable consequence of “measurement” by local interaction with a many-body system. (We neglect the additional orthogonality catastr ...
Steven French and Décio Krause, Identity in Physics: A Historical
... problem first appears in non-relativistic QM, with bosonic and fermionic quantum statistics. It becomes only more acute in relativistic QM and QFT, where one encounters states of indeterminate particle number, and where particle number becomes a frame-dependent quantity. So the quantum theory appear ...
... problem first appears in non-relativistic QM, with bosonic and fermionic quantum statistics. It becomes only more acute in relativistic QM and QFT, where one encounters states of indeterminate particle number, and where particle number becomes a frame-dependent quantity. So the quantum theory appear ...
The Semiotic Flora of Elementary Particles
... Kn = - dE/dL and the sum of all these forces will contain the same infinite factor, such that the pressure (measurable) becomes infinite, which it clearly isn' t in reality. Casimir' s calculations, as well as Spaarnay' s experiment even show that the pressure is negative, i.e., the force on the pis ...
... Kn = - dE/dL and the sum of all these forces will contain the same infinite factor, such that the pressure (measurable) becomes infinite, which it clearly isn' t in reality. Casimir' s calculations, as well as Spaarnay' s experiment even show that the pressure is negative, i.e., the force on the pis ...
IMFUFA- Roskilde Universitetscenter- postbox 260
... Kn = - dE/dL and the sum of all these forces will contain the same infinite factor, such that the pressure (measurable) becomes infinite, which it clearly isn't in reality. ...
... Kn = - dE/dL and the sum of all these forces will contain the same infinite factor, such that the pressure (measurable) becomes infinite, which it clearly isn't in reality. ...
Quantum Entanglement: Where Dark Energy and Negative Gravity
... Note that division by 2 in the above equation is due to arithmetic averaging and not due to using Newton’s kinetic energy because in this particular interpretation velocity tends to be the velocity of light without multiplying it with as in unit interval physics using Sigalotti’s critical value [2 ...
... Note that division by 2 in the above equation is due to arithmetic averaging and not due to using Newton’s kinetic energy because in this particular interpretation velocity tends to be the velocity of light without multiplying it with as in unit interval physics using Sigalotti’s critical value [2 ...
Notes on Elementary Particle Physics
... Every particle (massive or massless2 ) is subject to gravitational interaction. Particles that are electrically charged experience electromagnetic interaction. There are two more interactions responsible for happenings in the domain of elementary particles, namely the strong interaction responsible ...
... Every particle (massive or massless2 ) is subject to gravitational interaction. Particles that are electrically charged experience electromagnetic interaction. There are two more interactions responsible for happenings in the domain of elementary particles, namely the strong interaction responsible ...
The next stage: quantum game theory
... methods. In most of the cases quantum description of the system provides advantages over the classical situation. Game theory, the study of (rational) decision making in conflict situations, seems to ask for a quantum version. For example, games against nature [1] include those for which nature is qu ...
... methods. In most of the cases quantum description of the system provides advantages over the classical situation. Game theory, the study of (rational) decision making in conflict situations, seems to ask for a quantum version. For example, games against nature [1] include those for which nature is qu ...