Bose-Einstein Condensates L8-IV 1 / 24 Satyendra Nath Bose Indian - - PowerPoint PPT Presentation

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Bose-Einstein Condensates L8-IV 1 / 24 Satyendra Nath Bose Indian - - PowerPoint PPT Presentation

Bose-Einstein Condensates L8-IV 1 / 24 Satyendra Nath Bose Indian physicist 1 January 18944 February 1974 http: // en.wikipedia.org / wiki / Satyendra_Nath_Bose 2 / 24 What is a Bose-Einstein Condensate? A Bose-Einstein Condensate


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SLIDE 1

Bose-Einstein Condensates

L8-IV

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SLIDE 2

Satyendra Nath Bose

  • Indian physicist
  • 1 January 1894–4 February 1974

http://en.wikipedia.org/wiki/Satyendra_Nath_Bose 2 / 24

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What is a Bose-Einstein Condensate?

A Bose-Einstein Condensate (BEC) is a state in which all (or most) of the atoms are in the same quantum state.

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Review of Quantum Statistics

Bosons Fermions s = 0, 1, 2. . . s = 1/2, 3/2, 5/2 . . . examples: photons, α-particles, most atoms in their ground states examples: electrons, pro- tons, neutrons Any number of particles can be in the same state Only one particle can be in a given state A particle in a state in- creases the probability of finding another particle in that state A particle in a state de- creases to zero the prob- ability of finding another particle in that state fBE = 1 e(E−µ)/kT − 1 fFD = 1 e(E−µ)/kT + 1

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SLIDE 5

What is a Bose-Einstein Condensate?

A Bose-Einstein Condensate (BEC) is a state in which all (or most) of the atoms are in the same quantum state. 1924 – S. N. Bose first explored the statistics of bosons in the context of photons and blackbody radiation. 1924 – aftter seeing Bose’ work, Einstein predicts the existence of a boson-gas condensate. First BEC observed in 1995 by Carl Wieman and Eric Cornell at JILA/University of Colorado. Awarded the 2001 Nobel Prize for their 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, “Observation

  • f 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 BEC

The Critical Temperature

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Superfluid Helium

A sort-of liquid BEC

Click here

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SLIDE 9

Conditions for a BEC

The de Broglie Wavelength

We need

  • 1. The de Broglie wavelength

should be as large as

  • possible. (Cold)
  • 2. The average inter-atomic

spacing should be as small as 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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Metastable States

Example: Supercooled water

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Just How Cold?

To achieve BECs, the temperature must be reduced to just a few millionths of a degree above absolute zero. The first BEC was achieved at T = 200 nK!! How is it possible to achieve such low temperatures?

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SLIDE 14

Laser Cooling and Trapping (“Optical Molasses”)

Magneto Optical Traps, or MOTs

The lowest temperature that can be achieved in a MOT is ∼ 0.0001 K – still way too hot for a BEC. MOT animation

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Evaporative Cooling

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Magnetic Dipole in External Magnetic Field

Fx = ∂Bx ∂x µx U(x) = − µ · B ∝ s · B

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Evaporative Cooling

An RF frequency magnetic field is applied with a certain frequency ν to induce a spin flip from spin “up” to spin “down”, thereby removing higher-energy atoms from the trap. By lowering the applied RF frequency the gas can be gradually cooled by evaporation.

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Evaporative Cooling

Evaporative cooling animation

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Weiman and Cornell’s Apparatus

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Results

Expected Spatial Distribution of Atoms

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Results

Measured Atomic Density as a Function of RF Evaporative Cooling Frequency

Density in the center of the atomic cloud.

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The Velocity Distribution of the Trapped Atoms

Left to right: 400 nK, 200 nK, 50 nK Note that the thermal distribution is round, while the BEC distribution is elliptical.

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The Velocity Distribution of the Trapped Atoms

Left to right: 400 nK, 200 nK, 50 nK Note 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 the transcript of a talk given by Eric Cornell at NIST in 1996 and based 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 of Weiman and Cornell at the University of Colorado. You can find them, and many others, here: http://www.colorado.edu/physics/2000/bec/index.html

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