Book contents
- Frontmatter
- Contents
- Preface
- Preface to paperback edition
- 1 Introduction: Unifying Themes of Bose–Einstein Condensation
- Part one Review Papers
- 2 Some Comments on Bose–Einstein Condensation
- 3 Bose–Einstein Condensation and Superfluidity
- 4 Bose-Einstein Condensation in Liquid Helium
- 5 Sum Rules and Bose–Einstein Condensation
- 6 Dilute-Degenerate Gases
- 7 Prospects for Bose–Einstein Condensation in Magnetically Trapped Atomic Hydrogen
- 8 Spin-Polarized Hydrogen: Prospects for Bose–Einstein Condensation and Two-Dimensional Superfluidity
- 9 Laser Cooling and Trapping of Neutral Atoms
- 10 Kinetics of Bose–Einstein Condensate Formation in an Interacting Bose Gas
- 11 Condensate Formation in a Bose Gas
- 12 Macroscopic Coherent States of Excitons in Semiconductors
- 13 Bose–Einstein Condensation of a Nearly Ideal Gas: Excitons in Cu2O
- 14 Bose–Einstein Condensation of Excitonic Particles in Semiconductors
- 15 Crossover from BCS Theory to Bose–Einstein Condensation
- 16 Bose–Einstein Condensation of Bipolarons in High-Tc Superconductors
- 17 The Bosonization Method in Nuclear Physics
- 18 Kaon Condensation in Dense Matter
- 19 Broken Gauge Symmetry in a Bose Condensate
- Part two Brief Reports
- Appendix. BEC 93 Participant List
- Index
9 - Laser Cooling and Trapping of Neutral Atoms
Published online by Cambridge University Press: 15 December 2009
- Frontmatter
- Contents
- Preface
- Preface to paperback edition
- 1 Introduction: Unifying Themes of Bose–Einstein Condensation
- Part one Review Papers
- 2 Some Comments on Bose–Einstein Condensation
- 3 Bose–Einstein Condensation and Superfluidity
- 4 Bose-Einstein Condensation in Liquid Helium
- 5 Sum Rules and Bose–Einstein Condensation
- 6 Dilute-Degenerate Gases
- 7 Prospects for Bose–Einstein Condensation in Magnetically Trapped Atomic Hydrogen
- 8 Spin-Polarized Hydrogen: Prospects for Bose–Einstein Condensation and Two-Dimensional Superfluidity
- 9 Laser Cooling and Trapping of Neutral Atoms
- 10 Kinetics of Bose–Einstein Condensate Formation in an Interacting Bose Gas
- 11 Condensate Formation in a Bose Gas
- 12 Macroscopic Coherent States of Excitons in Semiconductors
- 13 Bose–Einstein Condensation of a Nearly Ideal Gas: Excitons in Cu2O
- 14 Bose–Einstein Condensation of Excitonic Particles in Semiconductors
- 15 Crossover from BCS Theory to Bose–Einstein Condensation
- 16 Bose–Einstein Condensation of Bipolarons in High-Tc Superconductors
- 17 The Bosonization Method in Nuclear Physics
- 18 Kaon Condensation in Dense Matter
- 19 Broken Gauge Symmetry in a Bose Condensate
- Part two Brief Reports
- Appendix. BEC 93 Participant List
- Index
Summary
Abstract
We present a simple review of the basic physical processes allowing one to control, with laser beams, the velocity and the position of neutral atoms. The control of the velocity corresponds to a cooling of atoms, that is, a reduction of the atomic velocity spread around a given value. The control of the position means a trapping of atoms in real space. The best present performances will be given, in terms of the lowest temperatures and the highest densities. The corresponding highest quantum degeneracy will also be estimated. It is imposed by fundamental limits, which will be described briefly. We also give the general trends in this field of research and outline the new directions which look promising for observing quantum statistical effects in laser cooled atomic samples, but which are for the moment restricted by unsolved problems.
Introducing the Simple Schemes
The radiative forces acting on atoms in a light field can be split into two parts, a reactive one and a dissipative one. The dissipative force (radiation pressure), which basically involves scattering processes, is velocity dependent. We will see that this dependence leads to the Doppler cooling scheme and to the concept of optical molasses, and we will give the corresponding minimal achievable temperature. The dissipative force can be made position dependent, through a gradient of the magnetic field, so that the atoms are also trapped in the so-called magneto-optical trap.
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- Bose-Einstein Condensation , pp. 173 - 201Publisher: Cambridge University PressPrint publication year: 1995
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