bose-einstein condensates - l8-iv
TRANSCRIPT
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Bose-Einstein CondensatesL8-IV
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Satyendra Nath Bose
• Indian physicist• 1 January 1894–4 February 1974
http://en.wikipedia.org/wiki/Satyendra_Nath_Bose
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What is a Bose-Einstein Condensate?
A Bose-Einstein Condensate (BEC) is a state in which all (ormost) of the atoms are in the same quantum state.
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Review of Quantum Statistics
Bosons Fermionss = 0, 1, 2. . . s = 1/2, 3/2, 5/2 . . .examples: photons,α-particles, most atoms intheir ground states
examples: electrons, pro-tons, neutrons
Any number of particlescan be in the same state
Only one particle can be ina given state
A particle in a state in-creases the probability offinding another particle inthat state
A particle in a state de-creases to zero the prob-ability of finding anotherparticle in that state
fBE =1
e(E−µ)/kT − 1fFD =
1e(E−µ)/kT + 1
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What is a Bose-Einstein Condensate?
A Bose-Einstein Condensate (BEC) is a state in which all (ormost) of the atoms are in the same quantum state.
1924 – S. N. Bose first explored the statistics of bosons in thecontext of photons and blackbody radiation.
1924 – aftter seeing Bose’ work, Einstein predicts the existence ofa boson-gas condensate.
First BEC observed in 1995 by Carl Wieman and Eric Cornell atJILA/University of Colorado. Awarded the 2001 Nobel Prize fortheir work.
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Carl Wieman and Eric Cornell
The JILA/University of Colorado team that first observed Bose-Einstein condensation in a gas. From left to right: Carl Wieman,Michael Matthews, Michael Anderson, Jason Ensher, and Eric Cornell. Their discovery was reported in the article, “Observationof Bose-Einstein Condensation in a Dilute Atomic Vapor,” by M. H. Anderson, J. R. Ensher, M. R. Matthews, C. E. Wieman, and E.
A. Cornell, Science 269, 198 (1995).
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Conditions for a BECThe Critical Temperature
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Superfluid HeliumA sort-of liquid BEC
Click here
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Conditions for a BECThe de Broglie Wavelength
We need
1. The de Broglie wavelengthshould be as large aspossible. (Cold)
2. The average inter-atomicspacing should be as smallas possible. (Dense)
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A Problem. . .
A “universal” phase diagram of ordinary matter:
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How Can it be Possible to Achieve a BEC?
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Just How Cold?
To achieve BECs, the temperature must be reduced to just a fewmillionths of a degree above absolute zero. The first BEC wasachieved at T = 200 nK!! How is it possible to achieve such lowtemperatures?
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Laser Cooling and Trapping (“Optical Molasses”)Magneto Optical Traps, or MOTs
The lowest temperature that canbe achieved in a MOT is∼ 0.0001 K – still way too hotfor a BEC.
MOT animation
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Evaporative Cooling
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Magnetic Dipole in External Magnetic Field
Fx =∂Bx
∂xµx U(x) = −~µ · ~B ∝ ~s · ~B
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Evaporative Cooling
An RF frequency magnetic field is applied with a certainfrequency ν to induce a spin flip from spin “up” to spin “down”,
thereby removing higher-energy atoms from the trap. Bylowering the applied RF frequency the gas can be gradually
cooled by evaporation.
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Evaporative Cooling
Evaporative cooling animation18 / 24
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Weiman and Cornell’s Apparatus
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ResultsExpected Spatial Distribution of Atoms
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ResultsMeasured Atomic Density as a Function of RF Evaporative Cooling Frequency
Density in the center of the atomic cloud.21 / 24
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The Velocity Distribution of the Trapped Atoms
Left to right: 400 nK, 200 nK, 50 nKNote that the thermal distribution is round, while the BEC
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The Velocity Distribution of the Trapped Atoms
Left to right: 400 nK, 200 nK, 50 nKNote that the thermal distribution is round, while the BEC
distribution is elliptical.
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Acknowledgments
The content of this lecture was taken primarily from thetranscript of a talk given by Eric Cornell at NIST in 1996 andbased heavily on Dr. Montemayor’s lecture on the same topic.There is a link to Cornell’s paper on the website.
The animations are from a great website discussing the work ofWeiman and Cornell at the University of Colorado. You can findthem, and many others, here:
http://www.colorado.edu/physics/2000/bec/index.html
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