far from the Fermi liquid regime
... This review is organized as follows. In section 2, we briefly summarize the main ideas of Fermi liquid theory as applied to both clean and disordered systems. Section 3 is devoted to a general discussion of the phenomenology of the main NFL systems. Section 3.1 focuses on NFL behaviour of clean syst ...
... This review is organized as follows. In section 2, we briefly summarize the main ideas of Fermi liquid theory as applied to both clean and disordered systems. Section 3 is devoted to a general discussion of the phenomenology of the main NFL systems. Section 3.1 focuses on NFL behaviour of clean syst ...
Study Guide to accompany Physics Including Human Applications
... PART II Prerequisite Chart (1) Prerequisite Chart (2) There are two other aspects of learning physics we would like to mention. While it is obvious that we learn by doing, it is not so apparent that we learn by interacting with other persons studying the same material. Nevertheless, our experiences ...
... PART II Prerequisite Chart (1) Prerequisite Chart (2) There are two other aspects of learning physics we would like to mention. While it is obvious that we learn by doing, it is not so apparent that we learn by interacting with other persons studying the same material. Nevertheless, our experiences ...
K c
... experimental conditions may disturb the balance and shift the equilibrium position so that more or less of the desired product is formed. • In this section we will study 5 factor which can effect chemical equilibrium namely : concentration, pressure, volume, temperature, and catalyst. • Le Châtelier ...
... experimental conditions may disturb the balance and shift the equilibrium position so that more or less of the desired product is formed. • In this section we will study 5 factor which can effect chemical equilibrium namely : concentration, pressure, volume, temperature, and catalyst. • Le Châtelier ...
Interaction between Atomic Ensembles and Optical
... dipole to be driven by the unperturbed incident field, but have to selfconsistently include the field emitted by the atom, and circulating in the cavity, into the total driving field. Thus for η > 1, the backaction of the cavity field generated by the oscillating atomic dipole on that same dipole is ...
... dipole to be driven by the unperturbed incident field, but have to selfconsistently include the field emitted by the atom, and circulating in the cavity, into the total driving field. Thus for η > 1, the backaction of the cavity field generated by the oscillating atomic dipole on that same dipole is ...
Molecules in intense laser fields: Studies of ionization, high
... Charged particles in laser fields The first thing we must do is to set up the theoretical framework that describes the interaction between particles and electromagnetic fields. Although we often imagine that the particle under consideration is the electron, this chapter treats an arbitrary particle ...
... Charged particles in laser fields The first thing we must do is to set up the theoretical framework that describes the interaction between particles and electromagnetic fields. Although we often imagine that the particle under consideration is the electron, this chapter treats an arbitrary particle ...
60 Annual Meeting Austrian Physical Society 6–10 September 2010
... sessions AKE and GEP which will take place at Haus der Natur (Museumsplatz 5; reachable by bus no. 1 from the main station or bus no. 8 from the Faculty of Natural Sciences). All lecture rooms are equipped with computer and beamer for which you only need to bring your USB-stick. Operating system is ...
... sessions AKE and GEP which will take place at Haus der Natur (Museumsplatz 5; reachable by bus no. 1 from the main station or bus no. 8 from the Faculty of Natural Sciences). All lecture rooms are equipped with computer and beamer for which you only need to bring your USB-stick. Operating system is ...
Beyond the Standard Model
... The first version of these notes was written up for lectures at the 1995 AIO-school (a school for PhD students) on theoretical particle physics. Later they were adapted for lectures at the Radboud University in Nijmegen, aimed at undergraduate students in their fourth year. This means that no detail ...
... The first version of these notes was written up for lectures at the 1995 AIO-school (a school for PhD students) on theoretical particle physics. Later they were adapted for lectures at the Radboud University in Nijmegen, aimed at undergraduate students in their fourth year. This means that no detail ...
An Unshunted Comparator as a Device for Quantum Measurements
... tion of the superconductor across the comparator equal to 2π. (In fact we will see that the phase may change by 4π or any other multiple, with implications for the comparator behavior.) One of the comparator junctions is inductively coupled (weakly) to a superconducting flux qubit, as seen in Fig. 1 ...
... tion of the superconductor across the comparator equal to 2π. (In fact we will see that the phase may change by 4π or any other multiple, with implications for the comparator behavior.) One of the comparator junctions is inductively coupled (weakly) to a superconducting flux qubit, as seen in Fig. 1 ...
Düren (ppt 10,1MB)
... A state of classical identical particle system can be described by a phase-space distribution f(x,p). The time evolution of f(x,p) obeys the Boltzmann equation. In quantum mechanics, because of the uncertainty principle, the phase-space distributions seem useless, but… Wigner introduced the fi ...
... A state of classical identical particle system can be described by a phase-space distribution f(x,p). The time evolution of f(x,p) obeys the Boltzmann equation. In quantum mechanics, because of the uncertainty principle, the phase-space distributions seem useless, but… Wigner introduced the fi ...
Q ua nt um
... the collective dipole coupling strength by N , where N is the number of resonant atoms, as predicted by the Tavis-Cummings model. To our knowledge this is the first observation of this nonlinearity in a system in which the atom number can be changed one by one in a discrete fashion. In addition, the ...
... the collective dipole coupling strength by N , where N is the number of resonant atoms, as predicted by the Tavis-Cummings model. To our knowledge this is the first observation of this nonlinearity in a system in which the atom number can be changed one by one in a discrete fashion. In addition, the ...
sl(3) link homology 1 Introduction
... Let us briefly discuss whether the invariants defined in [6] and the present paper should be called homology or cohomology. We are building functors from the category of link cobordisms to the category of abelian groups. Homology is a covariant functor, cohomology a contravariant one. A link cobordi ...
... Let us briefly discuss whether the invariants defined in [6] and the present paper should be called homology or cohomology. We are building functors from the category of link cobordisms to the category of abelian groups. Homology is a covariant functor, cohomology a contravariant one. A link cobordi ...
