Rendiconti della Scuola internazionale di fisica "Enrico Fermi." |
Contents
Introduction | 1 |
Precision measurement of the g factor of | 7 |
Subharmonic excitation of a single electron | 8 |
Observation of timevarying radiation pressure forces | 9 |
Hg optical spectroscopy | 10 |
H WALTHER Singleatom experiments and the test of fundamental quantum physics 1 The oneatom maser 11 Introduction | 11 |
Review of the oneatom maser | 12 |
Dynamics of a single atom | 13 |
Mechanical Hanle effect | 231 |
Arbitrary field limit | 235 |
Onedimensional experiments in optical molasses | 252 |
More on molasses | 258 |
Magnetically assisted Sisyphus effect | 274 |
Calculation of the interferometer phase shift | 275 |
Novel atom sources and devices | 281 |
beams in ASTRID 1 Introduction | 304 |
A new source of nonclassical light | 14 |
Verylowtemperature behaviour of a micromaser | 15 |
A new probe of complementarity in quantum mechanics Summary and conclusion | 17 |
Resonance methods | 18 |
Phase transitions of stored lasercooled ions 21 Introduction | 21 |
Description of the trap | 22 |
23 Outline of the theory 24 Experimental and theoretical results | 24 |
The crystal cloud transition | 25 |
Laser cooling and laser heating | 26 |
The r f heating mechanism | 27 |
S STENHOLM | 29 |
PART III | 30 |
PART II | 39 |
3 | 50 |
F WALLS | 57 |
45 | 64 |
Introduction | 71 |
Localization of atomic position | 78 |
The effect of spontaneous emission on the twoslit atomic interference | 85 |
Laser cooling in a squeezed vacuum | 91 |
Light shifts of the groundstate sublevels | 108 |
31 | 117 |
The limits of lowintensity Sisyphus cooling | 131 |
Equations of motion and their solutions 3 The wave functions | 134 |
Internal state for a moving atom | 141 |
4 | 161 |
two counterpropagating waves | 172 |
Conclusion | 178 |
Two counterpropagating plane waves with orthogonal polarizations | 181 |
9 | 188 |
A ASPECT O EMILE C GERZ R KAISER N VANSTEENKISTE | 224 |
Traps for neutral atoms | 316 |
Magnetooptic trap MOT | 321 |
Emission spectrum of lasercooled atoms | 337 |
85 | 345 |
MILC experiments in an added r f field | 353 |
pag | 361 |
91 | 377 |
E PRITCHARD and W KETTERLE Atom traps and atom optics | 473 |
Why nondissipative cooling mechanisms are not very useful | 482 |
Diffuselight slowing | 488 |
The ion trap | 506 |
ITANO J C BERGQUIST J J BOLLINGER and D J WINELAND | 519 |
Sympathetic laser cooling | 531 |
348 | 536 |
MOORE J M GILLIGAN M G RAIZEN C S WEIMER | 539 |
Future Penning trap experiments | 547 |
Introduction | 553 |
pag | 560 |
589 | 589 |
Introduction and ultimate motivation for the study | 671 |
Comparing r f and optical sources | 677 |
Frequency noise spectral density | 683 |
Allans variance | 693 |
44 | 699 |
Doppler theory of the | 703 |
Conclusion | 715 |
Cold collisions in the absence of light | 733 |
PART II | 746 |
4 | 753 |
Optical manipulation of excitedstate collisions pag | 758 |
Copyright | |