Simulation of Dispersionless Injections and Drift Echoes
... between the “double peaks” in (a1) of Fig. 3 are mostly filled. In order to determine the initial radial location of the electrons that contribute to the injected flux, we can divide the initial distribution and show only the electrons which had certain initial radial distances. In (b1) and (b2) of ...
... between the “double peaks” in (a1) of Fig. 3 are mostly filled. In order to determine the initial radial location of the electrons that contribute to the injected flux, we can divide the initial distribution and show only the electrons which had certain initial radial distances. In (b1) and (b2) of ...
Electric Fields and Potentials
... magnetic pole. Coulomb’s Law describes the force between two electric charges, just as Newton’s Law of Gravity describes the gravitational force between two masses. Both equations are vector equations and both have the same form. Thus, your experiences of the force and energy changes when walking up ...
... magnetic pole. Coulomb’s Law describes the force between two electric charges, just as Newton’s Law of Gravity describes the gravitational force between two masses. Both equations are vector equations and both have the same form. Thus, your experiences of the force and energy changes when walking up ...
12 Quantum Electrodynamics
... In this chapter we want to couple electrons and photons with each other by an appropriate interaction and study the resulting interacting field theory, the famous quantum electrodynamics (QED). Since the coupling should not change the two physical degrees of freedom described by the four-component p ...
... In this chapter we want to couple electrons and photons with each other by an appropriate interaction and study the resulting interacting field theory, the famous quantum electrodynamics (QED). Since the coupling should not change the two physical degrees of freedom described by the four-component p ...
Geometric phases and cyclic isotropic cosmologies
... a 2-valued function, as in the Konig-Penney approximation for electrons on a Bloch lattice. In the standard case of a scalar field in a potential with many local minima, as shown in [25, 26] the field can move through tunnelings from one local minimum to another. In our case instead, the interpretat ...
... a 2-valued function, as in the Konig-Penney approximation for electrons on a Bloch lattice. In the standard case of a scalar field in a potential with many local minima, as shown in [25, 26] the field can move through tunnelings from one local minimum to another. In our case instead, the interpretat ...
V08: Mößbauer Effect
... • An atom undergoing α-decay emits an α-particle, which is the nucleus of a 42 He atom. Due to Heisenberg’s uncertainty principle the kinetic energy of the α-particle in the nucleus can be high enough that it tunnels through the potential barrier of the quantum well, which holds the nucleus together ...
... • An atom undergoing α-decay emits an α-particle, which is the nucleus of a 42 He atom. Due to Heisenberg’s uncertainty principle the kinetic energy of the α-particle in the nucleus can be high enough that it tunnels through the potential barrier of the quantum well, which holds the nucleus together ...
CHAPTER 28 Sources Of Magnetic Field
... Polarization is a characteristic of all transverse waves. This chapter is about light, but to introduce some basic polarization concepts, let's go back to transverse waves on a string. For a string that in equilibrium lies along the x-axis, the displacement may be along the y-direction. In this case ...
... Polarization is a characteristic of all transverse waves. This chapter is about light, but to introduce some basic polarization concepts, let's go back to transverse waves on a string. For a string that in equilibrium lies along the x-axis, the displacement may be along the y-direction. In this case ...
