Narrowing of the generation band in the case of combined switching ofQ of a ruby laser by an acousto-optical shutter and a bleaching filter

1994 ◽  
Vol 61 (5-6) ◽  
pp. 736-738
Author(s):  
B. N. Tyushkevich ◽  
V. I. Dashkevich ◽  
Yu. M. Shcherbak
Keyword(s):  
Ruby Laser ◽  
Generation Band ◽  
Optical Shutter ◽  
Bleaching Filter

Passive Optical Shutter for Reducing the Fluorescent Output of a Pulsed Ruby Laser

1968 ◽  
Vol 39 (3) ◽  
pp. 419-419
Author(s):  
Burton G. Schuster ◽  
Robert D. Watson
Keyword(s):  
Ruby Laser ◽  
Optical Shutter

The effects of bleaching filter density on the spectrum of a Q-switched ruby laser

1973 ◽  
Vol 19 (1) ◽  
pp. 847-851
Author(s):  
Yu. F. Morgun ◽  
M. A. Muravitskii ◽  
L. A. Lavrovskii
Keyword(s):  
Ruby Laser ◽  
Bleaching Filter

Q-switched ruby laser treatment of congenital nevi

1995 ◽  
Vol 131 (5) ◽  
pp. 621-623 ◽  
Author(s):  
D. J. Goldberg
Keyword(s):  
Laser Treatment ◽  
Ruby Laser

Lentigo Maligna Partially Treated with Ruby Laser

2007 ◽  
Vol 69 (5) ◽  
pp. 511-514 ◽  
Author(s):  
Takako KURIHARA ◽  
Yoshihide HONDA
Keyword(s):  
Ruby Laser ◽  
Lentigo Maligna

Pulsed ruby laser accelerated degradation of amorphous hydrogenated silicon

1993 ◽  
Vol 164-166 ◽  
pp. 235-238 ◽  
Author(s):  
O. Klíma ◽  
O. Štika ◽  
Ho Tha Ha ◽  
S. Fouad Abdel Hamied ◽  
J. Stuchlík ◽  
...  
Keyword(s):  
Ruby Laser ◽  
Hydrogenated Silicon ◽  
Accelerated Degradation ◽  
Amorphous Hydrogenated Silicon

Raman-Spektren von SnJ4, GeJ4, TiBr4 und TiJ4 in flüssiger und kristalliner Phase / Raman Spectra of SnJ4, GeJ4, TiBr4, and TiJ4 in the Liquid and Crystalline Phase

1970 ◽  
Vol 25 (12) ◽  
pp. 1374-1381 ◽  
Author(s):  
W. Kiefer ◽  
H. W. Schrötter
Keyword(s):  
Raman Spectra ◽  
Ruby Laser ◽  
Detection System ◽  
Point Group ◽  
Visible Region ◽  
Group Symmetry ◽  
Pure Liquid ◽  
Electronic Detection ◽  
Polarization Studies ◽  
First Time

The Raman spectra of four molecules absorbing in the visible region (SnJ4, GeJ4, TiBr4, and TiJ4) are presented. They were excited with a quasi-continuous ruby laser and recorded with a special electronic detection system. Except for TiJ4, complete Raman spectra of crystal powder pellets could be obtained for the first time. The assignment reported by previous authors was confirmed by accurate polarization studies of solutions or pure liquid. The assignment is also in the solid state possible on the basis of Td point group symmetry. The fundamental vibrations of TiJ4 in solutions are: ν1 (A1) =162, ν2 (E) =51, ν3 (F2) =319 and ν4 (F2) Y = 67 cm-1

scholarly journals Microfluidic Optical Shutter Flexibly x-y Actuated via Electrowetting-on-Dielectrics with <20 ms Response Time

2017 ◽  
Vol 2017 ◽  
pp. 1-5
Author(s):  
Henning Fouckhardt ◽  
Johannes Strassner ◽  
Carina Heisel ◽  
Dominic Palm ◽  
Christoph Doering
Keyword(s):  
Optical Properties ◽  
Response Time ◽  
Visible Spectral Range ◽  
Contact Structures ◽  
Light Path ◽  
Cell Type ◽  
Electrically Conductive ◽  
Droplet Movement ◽  
In Series ◽  
Optical Shutter

Tunable microoptics deals with devices of which the optical properties can be changed during operation without mechanically moving solid parts. Often a droplet is actuated instead, and thus tunable microoptics is closely related to microfluidics. One such device/module/cell type is an optical shutter, which is moved in or out of the path of the light. In our case the transmitting part comprises a moving transparent and electrically conductive water droplet, embedded in a nonconductive blackened oil, that is, an opaque emulsion with attenuation of 30 dB at 570 nm wavelength over the 250 μm long light path inside the fluid (15 dB averaged over the visible spectral range). The insertion loss of the cell is 1.5 dB in the “open shutter” state. The actuation is achieved via electrowetting-on-dielectrics (EWOD) with rectangular AC voltage pulses of 2·90 V peak-to-peak at 1 kHz. To flexibly allow for horizontal, vertical, and diagonal droplet movement in the upright x-y plane, the contact structures are prepared such that four possible stationary droplet positions exist. The cell is configured as two capacitors in series (along the z axis), such that EWOD forces act symmetrically in the front and back of the 60 nl droplet with a response time of <20 ms.

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