Module: Mikrowelt: Bose-Einstein-Kondensat/Photonenstatistik
Sequence: lev0_start
Branching Point: Particles and Light under Control

Sequence: lev1_traps
Branching Point: Particle Traps

Sequence: lev2_trapspaul
Slide: Functional Principle of the Paul Trap

Slide: Scheme of the Paul Trap

Slide: Original of a Paul Trap; Detail

Slide: Large-scale Model of a Paul Trap

Slide: Nobel Prize for Physics, 1989
Sequence: lev2_trapsring
Slide: Scheme of a Ring Trap

Slide: Ion Crystal in a Ring Trap

Slide: Adding by Means of an Ion Crystal

Slide: A 50-Ion Crystal ...
Slide: More Complex Ion Crystals ...
Sequence: lev2_trapsioffe
Slide: Ioffe-Pritchard Trap

Sequence: lev1_bec
Branching Point: Bose-Einstein Condensation
Sequence: lev1_qchaos
Branching Point:

Quantum Chaos

Sequence: lev2_qchaoshist
Slide:

In the old quantum theory ...

Slide: Using Bohr's atomic model ...
Slide:

On the applicability of Bohr's atomic model ...

Slide:

An extension of the Bohr-Sommerfeld quantum condition ...

Slide:

In a note added in proof of his 1917 article ...

Sequence: lev2_qchaosclass
Slide:

Chaotic dynamics

Slide:

Sensible Dependence on Initial Conditions

Slide:

Fixpoint Attractor

Slide:

Limit Cycle

Slide:

Torus Attractor

Slide:

Strange Attractor

Slide:

Classical Chaos

Sequence: lev2_qchaosqm
Slide:
Slide:
Slide:

Rydberg Atoms ...

Slide:

The Quantum Mechanical Picture ...

Sequence: lev1_hbtstat
Branching Point: Photon Statistics According to Hanbury Brown and Twiss

Sequence: lev2_hbtclass
Slide: Classical Light

Sequence: lev2_hbtlaser
Slide: Laser Light

Sequence: lev2_hbtnoncl
Slide: Non-classical Light

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Ion Crystal in a Ring Trap

The linear arrangement is the most simple structure of an ion crystal. It is preferrably used today in order to conduct elementary arithmetic operations with a view on the quantum computer.
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