Physics 280/Jones Week 02 In-Class Problems Fall 2014 1
... to a stop, and then accelerates back towards the plate, impacting the plate with the same kinetic energy it had at liberation. Surprise! A photon is released. Electrons in an x-ray tube accelerate through a potential difference of 10.0 kV before striking a metal target. If an electron produces one p ...
... to a stop, and then accelerates back towards the plate, impacting the plate with the same kinetic energy it had at liberation. Surprise! A photon is released. Electrons in an x-ray tube accelerate through a potential difference of 10.0 kV before striking a metal target. If an electron produces one p ...
Cooling in Optical Lattices
... • Neutral atoms have weak dipole-dipole interactions but are also very weakly coupled to the environment • Polarization is rotated to bring atoms together • Once together, laser pulses set to specific resonances will only allow specific transitions, and these can be utilized as gates ...
... • Neutral atoms have weak dipole-dipole interactions but are also very weakly coupled to the environment • Polarization is rotated to bring atoms together • Once together, laser pulses set to specific resonances will only allow specific transitions, and these can be utilized as gates ...
Lecture 1: Wave Particle Duality of Light
... and head immediately for the meat of the material. This is a really dumb and lazy idea. Instead, think how much better you would be able to create a context for the material if you would memorize the summary. For example, see if you can describe out loud to yourself the material in the outline below ...
... and head immediately for the meat of the material. This is a really dumb and lazy idea. Instead, think how much better you would be able to create a context for the material if you would memorize the summary. For example, see if you can describe out loud to yourself the material in the outline below ...
... change of trajectory) of light. When light is propagating along a curved trajectory (Fig. 1A), the time-varying momentum along the light path must introduce a geometric polarization rotation to maintain the polarization transverse to its new propagation direction (23), e%̇ ¼ −kð%e ⋅ k̇Þ=k 2 . Here, ...