Atomic dipole trap formed by a Gaussian standing wave

1998 ◽  
Author(s):  
Pavel Zemanek ◽  
Christopher J. Foot
Keyword(s):  
Standing Wave ◽  
Dipole Trap ◽  
Atomic Dipole

scholarly journals Single atoms in a standing-wave dipole trap

2003 ◽  
Vol 67 (3) ◽  
Author(s):  
Wolfgang Alt ◽  
Dominik Schrader ◽  
Stefan Kuhr ◽  
Martin Müller ◽  
Victor Gomer ◽  
...  
Keyword(s):  
Standing Wave ◽  
Dipole Trap ◽  
Single Atoms

Erratum: Single atoms in a standing-wave dipole trap [Phys. Rev. A 67, 033403 (2003)]

2005 ◽  
Vol 71 (1) ◽  
Author(s):  
Wolfgang Alt ◽  
Dominik Schrader ◽  
Stefan Kuhr ◽  
Martin Müller ◽  
Victor Gomer ◽  
...  
Keyword(s):  
Standing Wave ◽  
Dipole Trap ◽  
Single Atoms

scholarly journals Number-triggered loading and collisional redistribution of neutral atoms in a standing wave dipole trap

2006 ◽  
Vol 8 (10) ◽  
pp. 259-259 ◽  
Author(s):  
L Förster ◽  
W Alt ◽  
I Dotsenko ◽  
M Khudaverdyan ◽  
D Meschede ◽  
...  
Keyword(s):  
Standing Wave ◽  
Neutral Atoms ◽  
Dipole Trap

scholarly journals Analysis of dephasing mechanisms in a standing-wave dipole trap

2005 ◽  
Vol 72 (2) ◽  
Author(s):  
S. Kuhr ◽  
W. Alt ◽  
D. Schrader ◽  
I. Dotsenko ◽  
Y. Miroshnychenko ◽  
...  
Keyword(s):  
Standing Wave ◽  
Dipole Trap

Eels Under Standing Wave Conditions

1982 ◽  
Vol 40 ◽  
pp. 492-495
Author(s):  
O.L. Krivanek ◽  
J. TaftØ
Keyword(s):  
Standing Wave ◽  
Wave Conditions ◽  
Set Up ◽  
A Site ◽  
Complex Crystal

It is well known that a standing electron wavefield can be set up in a crystal such that its intensity peaks at the atomic sites or between the sites or in the case of more complex crystal, at one or another type of a site. The effect is usually referred to as channelling but this term is not entirely appropriate; by analogy with the more established particle channelling, electrons would have to be described as channelling either through the channels or through the channel walls, depending on the diffraction conditions.

Voltage and Orientation Dependence of Characteristic X-Ray Production in Thin Crystals

1985 ◽  
Vol 43 ◽  
pp. 414-415
Author(s):  
G. Thomas ◽  
K. M. Krishnan ◽  
Y. Yokota ◽  
H. Hashimoto
Keyword(s):  
Standing Wave ◽  
Incident Beam ◽  
Orientation Dependence ◽  
Incident Plane Wave ◽  
Crystalline Materials ◽  
X Ray ◽  
Incident Plane ◽  
Crystal Unit Cell ◽  
Beam Orientation ◽  
Acceleration Voltage

For crystalline materials, an incident plane wave of electrons under conditions of strong dynamical scattering sets up a standing wave within the crystal. The intensity modulations of this standing wave within the crystal unit cell are a function of the incident beam orientation and the acceleration voltage. As the scattering events (such as inner shell excitations) that lead to characteristic x-ray production are highly localized, the x-ray intensities in turn, are strongly determined by the orientation and the acceleration voltage. For a given acceleration voltage or wavelength of the incident wave, it has been shown that this orientation dependence of the characteristic x-ray emission, termed the “Borrmann effect”, can also be used as a probe for determining specific site occupations of elemental additions in single crystals.

3-D optical transfer in excitation field synthesis microscopes

1995 ◽  
Vol 53 ◽  
pp. 64-65
Author(s):  
Vijay Krishnamurthi ◽  
Brent Bailey ◽  
Frederick Lanni
Keyword(s):  
Standing Wave ◽  
Spatial Information ◽  
3D Structure ◽  
Complete Recovery ◽  
Weighting Factor ◽  
Optical Transfer Function ◽  
Excitation Field ◽  
Optical Transfer ◽  
Set Up ◽  
Focus Plane

Excitation field synthesis (EFS) refers to the use of an interference optical system in a direct-imaging microscope to improve 3D resolution by axially-selective excitation of fluorescence within a specimen. The excitation field can be thought of as a weighting factor for the point-spread function (PSF) of the microscope, so that the optical transfer function (OTF) gets expanded by convolution with the Fourier transform of the field intensity. The simplest EFS system is the standing-wave fluorescence microscope, in which an axially-periodic excitation field is set up through the specimen by interference of a pair of collimated, coherent, s-polarized beams that enter the specimen from opposite sides at matching angles. In this case, spatial information about the object is recovered in the central OTF passband, plus two symmetric, axially-shifted sidebands. Gaps between these bands represent "lost" information about the 3D structure of the object. Because the sideband shift is equal to the spatial frequency of the standing-wave (SW) field, more complete recovery of information is possible by superposition of fields having different periods. When all of the fields have an antinode at a common plane (set to be coincident with the in-focus plane), the "synthesized" field is peaked in a narrow infocus zone.

Standing wave diffraction with a beam of slow atoms

1997 ◽  
Vol 44 (10) ◽  
pp. 1863-1882 ◽  
Author(s):  
S. KUNZE , S. DURR, K. DIECKMANN , M.
Keyword(s):  
Standing Wave ◽  
Wave Diffraction
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