Local Equilibrium States in Quantum Field Theory in Curved
... to macroscopic systems, with the proviso that these systems do not deviate too far from thermal equilibrium. In contrast to many of the existing approaches, this allows for a conceptually clear description of non-equilibrium phenomena, for example in cosmology. The results are illustrated using the ...
... to macroscopic systems, with the proviso that these systems do not deviate too far from thermal equilibrium. In contrast to many of the existing approaches, this allows for a conceptually clear description of non-equilibrium phenomena, for example in cosmology. The results are illustrated using the ...
BSc programme in Physics-CUCBCSS UG 2014
... another supervisor has to be appointed. However the existing work load should be maintained. Guidelines for doing project The project work provides the opportunity to study a topic in depth that has been chosen or which has been suggested by a staff member. The students first carryout a literature s ...
... another supervisor has to be appointed. However the existing work load should be maintained. Guidelines for doing project The project work provides the opportunity to study a topic in depth that has been chosen or which has been suggested by a staff member. The students first carryout a literature s ...
ZeemanProceduresCautions
... spectrum section. Any departure from the classical pattern in the number of components or the magnitudes of the splitting is an example of an Anomalous Zeeman Effect. We will only observe anomalous cases.2 The results are important because classical physics e ...
... spectrum section. Any departure from the classical pattern in the number of components or the magnitudes of the splitting is an example of an Anomalous Zeeman Effect. We will only observe anomalous cases.2 The results are important because classical physics e ...
Quantum Point Contacts
... can be viewed äs scattering or transmission experiments with modes in an electron waveguide. Quantization—i.e., the discreteness of the mode index— is essential for some phenomena (which necessarily require a description in terms of modes), but not for others (which could have been described semicla ...
... can be viewed äs scattering or transmission experiments with modes in an electron waveguide. Quantization—i.e., the discreteness of the mode index— is essential for some phenomena (which necessarily require a description in terms of modes), but not for others (which could have been described semicla ...
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Electric field of due to a point charge.
... We could have agreed that in the formula for F, the symbols q1 and q2 stand for the magnitudes of the charges. In that case, the absolute value signs would be unnecessary. However, in later equations the sign of the charge will be important, so we really need to keep the magnitude part. On your dia ...
... We could have agreed that in the formula for F, the symbols q1 and q2 stand for the magnitudes of the charges. In that case, the absolute value signs would be unnecessary. However, in later equations the sign of the charge will be important, so we really need to keep the magnitude part. On your dia ...
The unique electronic properties of graphene – a one-atom
... behaviour of electrons. That in itself is nothing new: as ons in high-energy particle physics: neutrinos. But neusummarized in Philip Anderson’s famous dictum trinos have no electric charge and therefore do not “more is different”, we know that when a large number interact strongly with any kind of ...
... behaviour of electrons. That in itself is nothing new: as ons in high-energy particle physics: neutrinos. But neusummarized in Philip Anderson’s famous dictum trinos have no electric charge and therefore do not “more is different”, we know that when a large number interact strongly with any kind of ...
Full-Text PDF
... D-scaled space. Moreover, the large-D electronic geometry and energy correspond to the minimum of an exactly known effective potential and can be determined from classical electrostatics for any atom or molecule. The (D → ∞)-limit is called pseudoclassical, tantamount to h → 0 and/or me → ∞ in the k ...
... D-scaled space. Moreover, the large-D electronic geometry and energy correspond to the minimum of an exactly known effective potential and can be determined from classical electrostatics for any atom or molecule. The (D → ∞)-limit is called pseudoclassical, tantamount to h → 0 and/or me → ∞ in the k ...
Reference - Wayne State Chemistry Department
... Time-dependent Hartree-Fock 共TD-HF兲 and time-dependent configuration interaction 共TD-CI兲 methods with Gaussian basis sets have been compared in modeling the response of hydrogen molecule, butadiene, and hexatriene exposed to very short, intense laser pulses 共760 nm, 3 cycles兲. After the electric fie ...
... Time-dependent Hartree-Fock 共TD-HF兲 and time-dependent configuration interaction 共TD-CI兲 methods with Gaussian basis sets have been compared in modeling the response of hydrogen molecule, butadiene, and hexatriene exposed to very short, intense laser pulses 共760 nm, 3 cycles兲. After the electric fie ...
Manifestations of Berry`s phase in molecules and condensed matter
... Since the first one appeared in 1983, a plethora of publications have dealt with the theory of geometric quantum phases and its applications in various fields. A very useful book [2] containing reprints and some original articles was published in 1989. Other useful publications of various kinds exist: ...
... Since the first one appeared in 1983, a plethora of publications have dealt with the theory of geometric quantum phases and its applications in various fields. A very useful book [2] containing reprints and some original articles was published in 1989. Other useful publications of various kinds exist: ...
Quantum Interference of Unpolarized Single Photons
... “Whether you can observe a thing or not depends on the theory which you use. It is the theory which decides what can be observed.” This objection of Albert Einstein during a lecture given by Heisenberg in 1926 [1] expressed his disbelief in quantum mechanics as it was evolving at that time. The Cope ...
... “Whether you can observe a thing or not depends on the theory which you use. It is the theory which decides what can be observed.” This objection of Albert Einstein during a lecture given by Heisenberg in 1926 [1] expressed his disbelief in quantum mechanics as it was evolving at that time. The Cope ...
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... than single atoms, in which case the complete quantum description of the ensemble–cavity interaction is nontrivial as it in general involves a very large Hilbert space (Baragiola et al., 2010). (Under assumptions of symmetry, exact solutions are possible in a much smaller Hilbert space, see Tavis an ...
... than single atoms, in which case the complete quantum description of the ensemble–cavity interaction is nontrivial as it in general involves a very large Hilbert space (Baragiola et al., 2010). (Under assumptions of symmetry, exact solutions are possible in a much smaller Hilbert space, see Tavis an ...
Quantum relaxation of magnetisation in magnetic particles
... the phonon-mediated relaxation rate, as well as providing a purely nuclearspin mediated relaxation mechanism-this latter purely nuclear relaxation mechanism is most important at short times. The internal bias field e acting on S, generated by the combined hyperfine fields of all the nuclei, can easi ...
... the phonon-mediated relaxation rate, as well as providing a purely nuclearspin mediated relaxation mechanism-this latter purely nuclear relaxation mechanism is most important at short times. The internal bias field e acting on S, generated by the combined hyperfine fields of all the nuclei, can easi ...
Multi-species systems in optical lattices: effects of disorder
... where âi (â†i ) destroys (creates) an atom in the i-th site, in a site-localized state of the ground - the s band [5]. The first term describes nearest neighbors hopping, which occurs with amplitude t, and the second term describes the two-body interactions, which occur with matrix elements propor ...
... where âi (â†i ) destroys (creates) an atom in the i-th site, in a site-localized state of the ground - the s band [5]. The first term describes nearest neighbors hopping, which occurs with amplitude t, and the second term describes the two-body interactions, which occur with matrix elements propor ...
