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... probe these atomic gases. In the first case, we use an auto-correlation technique to study the interference pattern produced by a gas of atoms, slightly above the Bose-Einstein condensate transition temperature. A moving optical lattice is used to split and recombine the single particle atomic wavef ...
... probe these atomic gases. In the first case, we use an auto-correlation technique to study the interference pattern produced by a gas of atoms, slightly above the Bose-Einstein condensate transition temperature. A moving optical lattice is used to split and recombine the single particle atomic wavef ...
full text - Ghent University Academic Bibliography
... periodiek in een CLC, dat veroorzaakt hoge reflecties voor golflengtes ongeveer even lang als de pitch. Het golflengte gebied waarin hoge reflecties optreden staat bekend als de “bandgap” van het CLC. Zulke “zelf-vormende spiegels” maken het mogelijk om optische componenten met een lage kostprijs te ...
... periodiek in een CLC, dat veroorzaakt hoge reflecties voor golflengtes ongeveer even lang als de pitch. Het golflengte gebied waarin hoge reflecties optreden staat bekend als de “bandgap” van het CLC. Zulke “zelf-vormende spiegels” maken het mogelijk om optische componenten met een lage kostprijs te ...
Outline For Provisional Patent Application
... throughout the entire body. It follows that irradiation from the body also is associated with polarization relaxations and changes within the entire body. It then follows that if the exact field pattern emitted by the body is precisely returned to the body, exactly opposite polarizations are produce ...
... throughout the entire body. It follows that irradiation from the body also is associated with polarization relaxations and changes within the entire body. It then follows that if the exact field pattern emitted by the body is precisely returned to the body, exactly opposite polarizations are produce ...
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... In this case, all light rays that emerge from the slit are approximately parallel to each other. For a diffraction pattern to appear on the screen, a convex lens is placed between the slit and screen to provide convergence of the light rays. 14.5 Single-Slit Diffraction In our consideration of Young ...
... In this case, all light rays that emerge from the slit are approximately parallel to each other. For a diffraction pattern to appear on the screen, a convex lens is placed between the slit and screen to provide convergence of the light rays. 14.5 Single-Slit Diffraction In our consideration of Young ...
Optics and Quantum Electronics
... states with two different time scales (300 µs and 1 s respectively). When it is locked, the in-loop integrated rms phase noise is 0.38π radians measured from 1 Hz to 1 MHz. This is equivalent to 570 as rms phase jitter from 1 Hz to 1 MHz. To our knowledge this is the lowest reported phase jitter bet ...
... states with two different time scales (300 µs and 1 s respectively). When it is locked, the in-loop integrated rms phase noise is 0.38π radians measured from 1 Hz to 1 MHz. This is equivalent to 570 as rms phase jitter from 1 Hz to 1 MHz. To our knowledge this is the lowest reported phase jitter bet ...
ELECTROMAGNETIC WAVE PROPAGATION
... practical difficulties of using EM energy for communication purposes also increase as frequency increases, until finally it can no longer be used. As communication methods improve, the limit to usable frequency has been pushed higher. Today communication satellites use frequencies near 14 GHz. This ...
... practical difficulties of using EM energy for communication purposes also increase as frequency increases, until finally it can no longer be used. As communication methods improve, the limit to usable frequency has been pushed higher. Today communication satellites use frequencies near 14 GHz. This ...
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GRAVITATIONAL WAVE PHYSICS
... two particles in free fall. If we assume two particles moving freely along geodesics of a curved spacetime with coordinates xµ (τ ) and xµ (τ ) + ξ µ (τ ) (for a given value of the proper time τ , ξ µ (τ ) is the displacement vector connecting the two events) it can be shown that, in the ...
... two particles in free fall. If we assume two particles moving freely along geodesics of a curved spacetime with coordinates xµ (τ ) and xµ (τ ) + ξ µ (τ ) (for a given value of the proper time τ , ξ µ (τ ) is the displacement vector connecting the two events) it can be shown that, in the ...
