An Introduction to
... not actually require one to know or even be able to have these states in hand. Let’s pretend that we know the quantum states that pertain to N molecules in a container of volume V as shown in Fig. 7.2, and let’s label these states by an index J. That is J=1 labels the lowest-energy state of N molecu ...
... not actually require one to know or even be able to have these states in hand. Let’s pretend that we know the quantum states that pertain to N molecules in a container of volume V as shown in Fig. 7.2, and let’s label these states by an index J. That is J=1 labels the lowest-energy state of N molecu ...
Polymer laser fabricated by a simple micromolding process
... from the master. The stamp was subsequently inked by applying a small amount of a solvent using a Q-tip. The spincoated polymer film was placed in contact with the inked stamp. As the stamp material is elastomeric, conformal contact was easily made with the polymer film. The solvent on the stamp dis ...
... from the master. The stamp was subsequently inked by applying a small amount of a solvent using a Q-tip. The spincoated polymer film was placed in contact with the inked stamp. As the stamp material is elastomeric, conformal contact was easily made with the polymer film. The solvent on the stamp dis ...
Excitonic exchange splitting in bulk semiconductors
... static dielectric constant e. Table I ~Refs. 31–41! lists all the quantities used in the calculation for excitonic Bohr radius. Note that, although the LDA results for effective masses and dielectric constants are not very accurate, the LDA wave functions are believed to be very good. This is demons ...
... static dielectric constant e. Table I ~Refs. 31–41! lists all the quantities used in the calculation for excitonic Bohr radius. Note that, although the LDA results for effective masses and dielectric constants are not very accurate, the LDA wave functions are believed to be very good. This is demons ...
On molecular origin of mass-independent fractionation of oxygen
... vibrational motion of O*3 is treated quantum-mechanically using the time-dependent Schrödinger equation and the wave-packet technique. This allows incorporation of all quantum effects associated with molecular vibration (such as ZPE, quantization of states, tunneling, resonances, and symmetry) and c ...
... vibrational motion of O*3 is treated quantum-mechanically using the time-dependent Schrödinger equation and the wave-packet technique. This allows incorporation of all quantum effects associated with molecular vibration (such as ZPE, quantization of states, tunneling, resonances, and symmetry) and c ...
I. Results from Prior NSF Support
... Long term visitors/collaborators who worked on this project during the grant period were Jörg Schmiedmayer (Universität Innsbruk), Bernd Rohwedder (University of Santiago, Chile), Winthrop Smith (University of Connecticut), Herb Bernstein (Hampshire College) and Jana Lehner (University of Ulm). Duri ...
... Long term visitors/collaborators who worked on this project during the grant period were Jörg Schmiedmayer (Universität Innsbruk), Bernd Rohwedder (University of Santiago, Chile), Winthrop Smith (University of Connecticut), Herb Bernstein (Hampshire College) and Jana Lehner (University of Ulm). Duri ...
Review of Cold Rydberg Atoms and Their Applications
... The strong interaction between Rydberg atoms was observed first in Rydberg dipole blockage experiments [52, 53] and later more clearly in long-range Rydberg molecular resonance experiments. In the latter, molecular resonance features were found in the excitation spectra of ultra-cold atoms of rubidiu ...
... The strong interaction between Rydberg atoms was observed first in Rydberg dipole blockage experiments [52, 53] and later more clearly in long-range Rydberg molecular resonance experiments. In the latter, molecular resonance features were found in the excitation spectra of ultra-cold atoms of rubidiu ...
Paper
... from a log-log plot as in the 3D case. Since the transitions became very broad, we characterized them by an error function fit, with the center of the fitted error function taken as the center of the transition (Fig. 4). In the 1D system, at a very shallow lattice depth of 0.25 ER (corresponding to ...
... from a log-log plot as in the 3D case. Since the transitions became very broad, we characterized them by an error function fit, with the center of the fitted error function taken as the center of the transition (Fig. 4). In the 1D system, at a very shallow lattice depth of 0.25 ER (corresponding to ...
Charge Transport in Semiconductors Contents
... that the bandstructure is nothing but the allowed eigenvalues of the quantum mechanical problem for the perfect semiconductor. The k-values are quantized; the quantization is so fine that for all practical purposes, it is assumed continuous. We now direct our attention towards the problem at hand - h ...
... that the bandstructure is nothing but the allowed eigenvalues of the quantum mechanical problem for the perfect semiconductor. The k-values are quantized; the quantization is so fine that for all practical purposes, it is assumed continuous. We now direct our attention towards the problem at hand - h ...
Chapter 7. Statistical Mechanics
... molecules in a container of volume V as shown in Fig. 7.2, and let’s label these states by an index J. That is J=1 labels the first energy state of N molecules in the container of volume V, J=2 labels the second such state, and so on. I understand that it may seem daunting to think of how one actual ...
... molecules in a container of volume V as shown in Fig. 7.2, and let’s label these states by an index J. That is J=1 labels the first energy state of N molecules in the container of volume V, J=2 labels the second such state, and so on. I understand that it may seem daunting to think of how one actual ...
Electronic Transport in Metallic Systems and Generalized Kinetic
... generalized kinetic equations suited for the relevant models of metallic systems. The problem of the electronic transport in solids is an interesting and actual part of the physics of condensed matter.9–26 It includes the transport of charge and heat in crystalline and disordered metallic conductors ...
... generalized kinetic equations suited for the relevant models of metallic systems. The problem of the electronic transport in solids is an interesting and actual part of the physics of condensed matter.9–26 It includes the transport of charge and heat in crystalline and disordered metallic conductors ...
