Trapped particles and asymmetry-induced transport
... with various m and k z are readily observed15 at frequencies below the plasma E⫻B rotation frequency, i.e., f ⱗm f E . The mode consists of trapped particles on either side of an electrostatic potential barrier which execute E⫻B drift oscillations that are 180° out of phase, while passing partic ...
... with various m and k z are readily observed15 at frequencies below the plasma E⫻B rotation frequency, i.e., f ⱗm f E . The mode consists of trapped particles on either side of an electrostatic potential barrier which execute E⫻B drift oscillations that are 180° out of phase, while passing partic ...
Physics 221 Second Hourly Examination Prepared August 2006
... addition, determine the energy stored in the capacitor C1 before the switch is closed, as well as the energy present in each capacitor in equilibrium. Is energy conserved? Explain why or why not. Answers: 1.5µC; 4.5µC; 6 × 10−3 J; 0.4 × 10−6 J; 1.1 × 10−6 J; resistive losses necessary for equilibri ...
... addition, determine the energy stored in the capacitor C1 before the switch is closed, as well as the energy present in each capacitor in equilibrium. Is energy conserved? Explain why or why not. Answers: 1.5µC; 4.5µC; 6 × 10−3 J; 0.4 × 10−6 J; 1.1 × 10−6 J; resistive losses necessary for equilibri ...
Entanglement, which-way measurements, and a quantum erasure Christian Ferrari Bernd Braunecker
... can be erased, and the interference pattern at the screen can be restored. This result was confirmed experimentally by Dürr et al.9 using a modified Mach–Zehnder interferometer 共see also Refs. 10 and 11兲. II. THE MACH–ZEHNDER INTERFEROMETER We consider the Mach–Zehnder interferometer shown in Fig. 2 ...
... can be erased, and the interference pattern at the screen can be restored. This result was confirmed experimentally by Dürr et al.9 using a modified Mach–Zehnder interferometer 共see also Refs. 10 and 11兲. II. THE MACH–ZEHNDER INTERFEROMETER We consider the Mach–Zehnder interferometer shown in Fig. 2 ...
Bending of electromagnetic waves in all
... separate propagation bands in different spectral regions, due to the different dipole-dipole interaction. For non-spherical shapes, corresponding dipole resonances depend on the orientation and aspect ratio of the particle. It allows to tune spectral range of propagation bands by changing the nanopa ...
... separate propagation bands in different spectral regions, due to the different dipole-dipole interaction. For non-spherical shapes, corresponding dipole resonances depend on the orientation and aspect ratio of the particle. It allows to tune spectral range of propagation bands by changing the nanopa ...
4. Humanities-Computational of the Magnetic
... When T > 0, then some of the si will be +1 and the others –1. The boundary between +1 region and the –1 region is called the partition point. At T = 0, there is no partition point and at low temperatures, the partition points are few. The energy of each partition point is 2J. This model is then tran ...
... When T > 0, then some of the si will be +1 and the others –1. The boundary between +1 region and the –1 region is called the partition point. At T = 0, there is no partition point and at low temperatures, the partition points are few. The energy of each partition point is 2J. This model is then tran ...
Lecture 4, Conservation Laws
... Evidence for conservation of electric charge: Consider reaction e-ve which violates charge conservation but not lepton number or any other quantum number. If the above transition occurs in nature then we should see x-rays from atomic transitions. The absence of such x-rays leads to the limit: te > ...
... Evidence for conservation of electric charge: Consider reaction e-ve which violates charge conservation but not lepton number or any other quantum number. If the above transition occurs in nature then we should see x-rays from atomic transitions. The absence of such x-rays leads to the limit: te > ...
