Chapter 5 Experimental Apparatus II
... of photons that have already been spontaneously scattered by MOT atoms, or “radiation trapping,” leads to temperature and density limitations in free-space MOTs [Sesko91; Ellinger94]. These rescattering events are particularly problematic in that they may be much more likely to be absorbed than regu ...
... of photons that have already been spontaneously scattered by MOT atoms, or “radiation trapping,” leads to temperature and density limitations in free-space MOTs [Sesko91; Ellinger94]. These rescattering events are particularly problematic in that they may be much more likely to be absorbed than regu ...
Interacting Cold Rydberg Atoms: a Toy Many-Body
... Techniques for laser cooling and trapping of neutral atoms by laser light were developed in the 80’s and 90’s. It was in particular demonstrated that atomic samples could be cooled down to temperatures below 100 µK starting from vapors at room temperature. The basic mechanism that makes laser coolin ...
... Techniques for laser cooling and trapping of neutral atoms by laser light were developed in the 80’s and 90’s. It was in particular demonstrated that atomic samples could be cooled down to temperatures below 100 µK starting from vapors at room temperature. The basic mechanism that makes laser coolin ...
Addressing of individual atoms in an optical dipole trap
... Josephson junctions [Mak01] and cavity quantum electrodynamics. Each of these approaches has its own advantages and disadvantages. Our approach is to use neutral atoms as carriers of quantum information, which is encoded in their long-living hyperfine ground states. The main advantage of neutral ato ...
... Josephson junctions [Mak01] and cavity quantum electrodynamics. Each of these approaches has its own advantages and disadvantages. Our approach is to use neutral atoms as carriers of quantum information, which is encoded in their long-living hyperfine ground states. The main advantage of neutral ato ...
Ionization of Rydberg atoms by standing
... experiment. There are no other free parameters in the simulations. For a lattice with perfect contrast and for atoms frozen in place at either intensity maxima or minima, the ratio of tPI for initial condition CMIN to that for CMAX would be infinity. On the basis of the actual contrast between intens ...
... experiment. There are no other free parameters in the simulations. For a lattice with perfect contrast and for atoms frozen in place at either intensity maxima or minima, the ratio of tPI for initial condition CMIN to that for CMAX would be infinity. On the basis of the actual contrast between intens ...
Laser Safety Powerpoint 2015
... Monochromatic - all light produced by the laser is of one wavelength or color. Exceptions included multiline gas lasers and new white-light lasers. ex. Nd:YAG (532,1064nm) ...
... Monochromatic - all light produced by the laser is of one wavelength or color. Exceptions included multiline gas lasers and new white-light lasers. ex. Nd:YAG (532,1064nm) ...
Optical pumping of a lithium atomic beam for atom interferometry
... I0 = P/(πw02 ) and, in the calculations, we use the same power P = 5 mW for the two laser beams. Initially, the atomic population is equally distributed among the 8 ground state sublevels. Figure 2 plot the populations of the sublevels of the ground state as a function of time t. In this ideal case, ...
... I0 = P/(πw02 ) and, in the calculations, we use the same power P = 5 mW for the two laser beams. Initially, the atomic population is equally distributed among the 8 ground state sublevels. Figure 2 plot the populations of the sublevels of the ground state as a function of time t. In this ideal case, ...
Atomic Line Spectra: the Bohr model Line Spectra of Excited Atoms
... Bohr received the Nobel Prize in 1922 for his theory. However, there are problems — • theory is successful only for H. • quantum idea artificially introduced. • So, we go on to QUANTUM or WAVE MECHANICS to understand the atom ...
... Bohr received the Nobel Prize in 1922 for his theory. However, there are problems — • theory is successful only for H. • quantum idea artificially introduced. • So, we go on to QUANTUM or WAVE MECHANICS to understand the atom ...
Atomic Line Spectra: the Bohr model Line Spectra of Excited Atoms
... Atomic Spectra Spectra and and Bohr Bohr If e-’s are in quantized energy states, then ∆E between states can have only certain values. This explains sharp line spectra. ...
... Atomic Spectra Spectra and and Bohr Bohr If e-’s are in quantized energy states, then ∆E between states can have only certain values. This explains sharp line spectra. ...
RCLED - Crosslight Software
... True 3D simulation of band structure physics including MQW strain effects. Current flow and self-heating may be included self-consistently in 3D. ...
... True 3D simulation of band structure physics including MQW strain effects. Current flow and self-heating may be included self-consistently in 3D. ...
Slide 1
... Niels Bohr was the first to offer an explanation for line spectra Bohr Model of the Hydrogen Atom • Only orbits of defined energy and radii are permitted in the hydrogen atom • An electron in a permitted orbit has a specific energy and will not radiate energy and will not spiral into the nucleus • E ...
... Niels Bohr was the first to offer an explanation for line spectra Bohr Model of the Hydrogen Atom • Only orbits of defined energy and radii are permitted in the hydrogen atom • An electron in a permitted orbit has a specific energy and will not radiate energy and will not spiral into the nucleus • E ...
