scholarly journals Spatially resolved photoionization of ultracold atoms on an atom chip

2007 ◽  
Vol 75 (6) ◽  
Author(s):  
S. Kraft ◽  
A. Günther ◽  
J. Fortágh ◽  
C. Zimmermann
2010 ◽  
Vol 19 (8) ◽  
pp. 083205
Author(s):  
Cheng Feng ◽  
Yan Bo ◽  
Ke Min ◽  
Wang Yu-Zhu

2008 ◽  
Vol 41 (6) ◽  
pp. 065301 ◽  
Author(s):  
M Singh ◽  
M Volk ◽  
A Akulshin ◽  
A Sidorov ◽  
R McLean ◽  
...  

2010 ◽  
Vol 81 (6) ◽  
Author(s):  
Atreju Tauschinsky ◽  
Rutger M. T. Thijssen ◽  
S. Whitlock ◽  
H. B. van Linden van den Heuvell ◽  
R. J. C. Spreeuw

Author(s):  
C. T. Fancher ◽  
A. R. Ziltz ◽  
A. J. Pyle ◽  
M. K. Ivory ◽  
S. Aubin
Keyword(s):  

2007 ◽  
Author(s):  
Mandip Singh ◽  
Michael Volk ◽  
Alexander Akulshin ◽  
Russell McLean ◽  
Andrei Sidorov ◽  
...  
Keyword(s):  

2009 ◽  
Vol 87 (6) ◽  
pp. 633-638 ◽  
Author(s):  
O. Cherry ◽  
J. D. Carter ◽  
J. D.D. Martin

We have fabricated an atom chip that magnetically traps laser cooled 87Rb by generating high magnetic-field gradients using micrometre scale current-carrying wires. The wires are fabricated on a Si wafer (with a 40 nm SiO2 layer) using 1.2 μm thick Au and a 20 nm thick adhesion layer, and are patterned with lift-off photolithography. We characterize the number and temperature of the cold atoms trapped by the chip.


2015 ◽  
Vol 48 (11) ◽  
pp. 115002 ◽  
Author(s):  
I Herrera ◽  
Y Wang ◽  
P Michaux ◽  
D Nissen ◽  
P Surendran ◽  
...  

Author(s):  
David C. Joy

Electron channeling patterns (ECP) were first found by Coates (1967) while observing a large bulk, single crystal of silicon in a scanning electron microscope. The geometric pattern visible was shown to be produced as a result of the changes in the angle of incidence, between the beam and the specimen surface normal, which occur when the sample is examined at low magnification (Booker, Shaw, Whelan and Hirsch 1967).A conventional electron diffraction pattern consists of an angularly resolved intensity distribution in space which may be directly viewed on a fluorescent screen or recorded on a photographic plate. An ECP, on the other hand, is produced as the result of changes in the signal collected by a suitable electron detector as the incidence angle is varied. If an integrating detector is used, or if the beam traverses the surface at a fixed angle, then no channeling contrast will be observed. The ECP is thus a time resolved electron diffraction effect. It can therefore be related to spatially resolved diffraction phenomena by an application of the concepts of reciprocity (Cowley 1969).


Author(s):  
Steven M. Le Vine ◽  
David L. Wetzel

In situ FT-IR microspectroscopy has allowed spatially resolved interrogation of different parts of brain tissue. In previous work the spectrrscopic features of normal barin tissue were characterized. The white matter, gray matter and basal ganglia were mapped from appropriate peak area measurements from spectra obtained in a grid pattern. Bands prevalent in white matter were mostly associated with the lipid. These included 2927 and 1469 cm-1 due to CH2 as well as carbonyl at 1740 cm-1. Also 1235 and 1085 cm-1 due to phospholipid and galactocerebroside, respectively (Figs 1and2). Localized chemical changes in the white matter as a result of white matter diseases have been studied. This involved the documentation of localized chemical evidence of demyelination in shiverer mice in which the spectra of white matter lacked the marked contrast between it and gray matter exhibited in the white matter of normal mice (Fig. 3).The twitcher mouse, a model of Krabbe’s desease, was also studied. The purpose in this case was to look for a localized build-up of psychosine in the white matter caused by deficiencies in the enzyme responsible for its breakdown under normal conditions.


Author(s):  
David L. Wetzel ◽  
John A. Reffner ◽  
Gwyn P. Williams

Synchrotron radiation is 100 to 1000 times brighter than a thermal source such as a globar. It is not accompanied with thermal noise and it is highly directional and nondivergent. For these reasons, it is well suited for ultra-spatially resolved FT-IR microspectroscopy. In efforts to attain good spatial resolution in FT-IR microspectroscopy with a thermal source, a considerable fraction of the infrared beam focused onto the specimen is lost when projected remote apertures are used to achieve a small spot size. This is the case because of divergence in the beam from that source. Also the brightness is limited and it is necessary to compromise on the signal-to-noise or to expect a long acquisition time from coadding many scans. A synchrotron powered FT-IR Microspectrometer does not suffer from this effect. Since most of the unaperatured beam’s energy makes it through even a 12 × 12 μm aperture, that is a starting place for aperture dimension reduction.


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