1995
DOI: 10.1103/physrevlett.74.1311
|View full text |Cite
|
Sign up to set email alerts
|

Long Atomic Coherence Times in an Optical Dipole Trap

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

3
114
0

Year Published

1998
1998
2016
2016

Publication Types

Select...
7
2

Relationship

0
9

Authors

Journals

citations
Cited by 170 publications
(117 citation statements)
references
References 15 publications
3
114
0
Order By: Relevance
“…In practice, the intensity minimum in bottle beams is not exactly equal to zero because of different experimental imperfections. Various methods and techniques have been proposed to produce 3D optical dark potentials in a controllable way, such as creating an intensity minimum by surrounding a region in 3D space with several beams [96,97], crossing at least two cylindrical-vector and vortex beams with a phase dislocation along the beam axis that leads to a zero-intensity point [98], by destructive interference of several Laguerre-Gauss light beams [95,99] or using uniaxial c-cut crystals [100]. However, these methods have several drawbacks such as the fact that in some of them the intensity minimum is not exactly equal to zero, the extreme precise control on the optical elements being used, the field fluctuations introduced at and close to the zero-amplitude point, or the non trivial generation of Laguerre-Gauss and cylindrical-vector and vortex beams [101].…”
Section: Generating a 3d Dark Focus With Conical Refractionmentioning
confidence: 99%
“…In practice, the intensity minimum in bottle beams is not exactly equal to zero because of different experimental imperfections. Various methods and techniques have been proposed to produce 3D optical dark potentials in a controllable way, such as creating an intensity minimum by surrounding a region in 3D space with several beams [96,97], crossing at least two cylindrical-vector and vortex beams with a phase dislocation along the beam axis that leads to a zero-intensity point [98], by destructive interference of several Laguerre-Gauss light beams [95,99] or using uniaxial c-cut crystals [100]. However, these methods have several drawbacks such as the fact that in some of them the intensity minimum is not exactly equal to zero, the extreme precise control on the optical elements being used, the field fluctuations introduced at and close to the zero-amplitude point, or the non trivial generation of Laguerre-Gauss and cylindrical-vector and vortex beams [101].…”
Section: Generating a 3d Dark Focus With Conical Refractionmentioning
confidence: 99%
“…Long coherence times are therefore a crucial parameter for the applicability of a physical system for quantum information processing. We follow the previously discussed methods to study decoherence of quantum states of neutral atoms in optical dipole traps [8,9,10]. A theoretical description of these effects can be based on the Bloch equations [11]…”
Section: Dephasing and Coherencementioning
confidence: 99%
“…Meanwhile, the motional decoherence effect is significantly weakened due to elimination of the ac Stark shift in the optical dipole trap. The coherent time of atoms in a dark trap can thus be maintained to several seconds [48]. Another important application of the blue detuned trap may lay on equaling the polarizability for the ground and Rydberg state atoms [49].…”
Section: Trapping Single Atoms In a Blue Detuned Optical Trapmentioning
confidence: 99%