8.07 Class Notes Fall 2010
... The Easy Electromagnetism ............................................................................. 42 6.2.1 The Solution to Maxwell’s Equations........................................................... 42 6.2.2 The free space-time dependent Green’s function .................................... ...
... The Easy Electromagnetism ............................................................................. 42 6.2.1 The Solution to Maxwell’s Equations........................................................... 42 6.2.2 The free space-time dependent Green’s function .................................... ...
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... The collision-induced dissociation 共CID兲 of the N2 molecule by an energetic nitrogen atom is a process of importance in the upper atmosphere of Titan, a moon of Saturn, which has a nitrogen atmosphere.1 The energized nitrogen atoms produced by dissociation populate Titan’s atmospheric corona and can ...
... The collision-induced dissociation 共CID兲 of the N2 molecule by an energetic nitrogen atom is a process of importance in the upper atmosphere of Titan, a moon of Saturn, which has a nitrogen atmosphere.1 The energized nitrogen atoms produced by dissociation populate Titan’s atmospheric corona and can ...
Chapter 4 Two Fluid Equations and Waves
... Note that the different variables may actuall have a different phase in the plane wave solution. However, we can absorb the pahse into the amplitude etc by allowing these ampplitude to be complex. ...
... Note that the different variables may actuall have a different phase in the plane wave solution. However, we can absorb the pahse into the amplitude etc by allowing these ampplitude to be complex. ...
Visualizing the Coupling between Red and Blue Stark States
... the semiclassical predictions. These images were recorded in the vicinity of avoided crossings between red and blue Stark states, and reveal the nodal structure along the ξ coordinate of the red Stark states involved. To illustrate this, Figs. 3(a)–3(f) show raw images and extracted radial distribut ...
... the semiclassical predictions. These images were recorded in the vicinity of avoided crossings between red and blue Stark states, and reveal the nodal structure along the ξ coordinate of the red Stark states involved. To illustrate this, Figs. 3(a)–3(f) show raw images and extracted radial distribut ...
Plasma Density Features Associated with Strong Convection in the
... calculations, 44 trajectories were used to cover the ionosphere poleward of 42° magnetic latitude. Figure 1 also illustrates our adopted auroral oval, which corresponds to the K p = 5 auroral oval described by Comfort [1972]. When field tubes of plasma enter this region they are subjected to an ion ...
... calculations, 44 trajectories were used to cover the ionosphere poleward of 42° magnetic latitude. Figure 1 also illustrates our adopted auroral oval, which corresponds to the K p = 5 auroral oval described by Comfort [1972]. When field tubes of plasma enter this region they are subjected to an ion ...
Nanoscale Domain Stability in Organic Monolayers on Metals Z. Suo Y. F. Gao
... Under certain conditions, a SAM spontaneously forms domains. For example, for an incomplete monolayer, patches of the monolayer coexist with patches of the bare metal, 关8 –10兴. 共The ‘‘bare metal’’ can actually be covered by the lying-down phase, 关1兴.兲 Also, when a monolayer of dissimilar alkanethiol ...
... Under certain conditions, a SAM spontaneously forms domains. For example, for an incomplete monolayer, patches of the monolayer coexist with patches of the bare metal, 关8 –10兴. 共The ‘‘bare metal’’ can actually be covered by the lying-down phase, 关1兴.兲 Also, when a monolayer of dissimilar alkanethiol ...
Ice, spin ice and spin liquids lecture April 16, 2013
... This makes it possible to fine tune the model to an exactly soluble Rokhsar-Kivelson (RK) point g = µ, where the ground-state wave is an equally-weighted sum of all possible ice (dimer) configurations.49 The authors then argued, by continuity, that a quantum liquid phase would occur for a finite ran ...
... This makes it possible to fine tune the model to an exactly soluble Rokhsar-Kivelson (RK) point g = µ, where the ground-state wave is an equally-weighted sum of all possible ice (dimer) configurations.49 The authors then argued, by continuity, that a quantum liquid phase would occur for a finite ran ...
Document
... From the experiments: When the bar magnet is stationary, the galvanometer not show any deflection (no current flows in the coil). When the bar magnet is moved relatively towards the coil, the galvanometer shows a momentary deflection to the right (Figure 7.1b). When the bar magnet is moved relat ...
... From the experiments: When the bar magnet is stationary, the galvanometer not show any deflection (no current flows in the coil). When the bar magnet is moved relatively towards the coil, the galvanometer shows a momentary deflection to the right (Figure 7.1b). When the bar magnet is moved relat ...
107, 195303 (2011)
... uniform s-wave superfluid in the presence of both Zeeman field and Rashba type of SOC. Under the mean-field approximation, we derive the superfluid gap and atom density equations and solve them self-consistently in the BCSBEC crossover region. Our main results are the following: (I) It is well known ...
... uniform s-wave superfluid in the presence of both Zeeman field and Rashba type of SOC. Under the mean-field approximation, we derive the superfluid gap and atom density equations and solve them self-consistently in the BCSBEC crossover region. Our main results are the following: (I) It is well known ...
Optical Properties of Semiconductor Nanostructures in Magnetic Field DISSERTATION
... properties are determined mainly by a quasi-particle consisting of one electron and one hole called exciton. First, the exciton theory is developed starting with the one-electron Hamiltonian in a crystal, continuing with the Luttinger and Bir-Pikus Hamiltonian, and ending with the exciton Hamiltonia ...
... properties are determined mainly by a quasi-particle consisting of one electron and one hole called exciton. First, the exciton theory is developed starting with the one-electron Hamiltonian in a crystal, continuing with the Luttinger and Bir-Pikus Hamiltonian, and ending with the exciton Hamiltonia ...
Difficulties in the Implementation of Quantum Computers Abhilash
... superposition to create a paradigm that is more powerful than that of classical computing. The field has grown from the exotic arena confined to a few theoretical physicists into a full scale theoretical and experimental research area with millions of dollars being spent to build prototypes of quant ...
... superposition to create a paradigm that is more powerful than that of classical computing. The field has grown from the exotic arena confined to a few theoretical physicists into a full scale theoretical and experimental research area with millions of dollars being spent to build prototypes of quant ...
