120 watt continuous wave solar-pumped laser with a liquid light-guide lens and an Nd:YAG rod

2012 ◽  
Vol 37 (13) ◽  
pp. 2670 ◽  
Author(s):  
T. H. Dinh ◽  
T. Ohkubo ◽  
T. Yabe ◽  
H. Kuboyama
Keyword(s):  
Author(s):  
Gyung-Dong Kim ◽  
Hyuk Jin Kang ◽  
Sung-Hoon Ahn ◽  
Chul Ki Song ◽  
Chang Back ◽  
...  

A light guide panel is an element of the liquid-crystal display backlight unit, which is extensively used for display devices. In this study, a laser-marking process is applied to the fabrication of light guide panels, and the new fabrication process may replace existing manufacturing methods such as silk screen printing, stamping, or V-cutting methods. The objective of this research is to evaluate the feasibility of the laser patterning system. A series of light guide patterns were made with a 50 W CO2 laser (continuous wave) to understand the effects of laser power and scanning speed on the geometry of groove patterns. The width and depth of the fabricated grooves increased with increasing laser power and decreasing scanning speed. In order to analyse surface geometry, scanning electron microscopy (SEM) photography was used and, for luminance measurement, a Topcon-BM7 was used. As a result, the marking conditions of the laser patterning, 5W and 0.4m/s, were suggested.


2014 ◽  
Vol 3 (2) ◽  
Author(s):  
Wernholt von Tempelhoff ◽  
Frank Ulrich ◽  
Hans-Joachim Schwarzmaier

AbstractBackground:The most common type of primary brain tumors are gliomas. For patients unsuitable for open microsurgery having been treated by radiochemotherapy, laser irradiation has proven to be an alternative palliative option. From summer 1997 until winter 2006 we performed about 60 laser-interstitial thermotherapy (LITT) treatments, starting with patients with large recurrent tumors who had no other therapeutic option. In the present article we report about the neurobiological background, the technique and our experience with LITT of cerebral gliomas.Materials and method:For laser irradiation we used a specially designed light guide (LITT standard applicator; Trumpf Medizintechnik, Umkirch, Germany). The tip of this light guide is a special optical diffuser which is characterized by a homogeneous spherical or ellipsoid emission profile. The light guide was introduced into an appropriate protective sheath (Somatex, Teltow, Germany). For the laser light source, we used a continuous wave 1064-nm Nd:YAG laser (mediLas fibertom 4060 N; Dornier MedTech, Weßling, Germany). Laser irradiation was performed under general anesthesia in a 0.5 T open configuration magnetic resonance (MR) system (Signa SP; General Electric, Milwaukee, WI, USA). Usually, the tip of the light guide was positioned in the center of the tumor using the built-in localization system (Flashpoint 3000; IGT, Boulder, CO, USA) in combination, where appropriate, with a specially designed navigation system (Localite™, Bonn, Germany). The position of the light guide was then controlled using multiplanar reconstructions of T1-weighted sequences. For near real-time control, temperature monitoring was performed using an experimental software package based on the temperature-dependent shift of the MR signal. Laser irradiation was ceased when the temperature monitoring revealed a steady state temperature profile within the heated tissue. Since 2008 we have used traditional stereotactic targeting and methionine positron emission tomography/computed tomography (MET-PET/CT) instead of the ‘open’ MR system for planning and follow-up in LITT of brain tumors.Results:We started the LITT treatment of gliomas in the early 1990s (benign gliomas in eloquent regions/not suitable for surgery). In 1997 we started to treat patients with recurrent gliobastomas/anaplastic gliomas. All of these patients had an increased survival in comparison to the natural course of recurrent glioblastomas. There were no procedure-related deaths or permanent neurological deficits. Two factors seem to be important for the overall success of the LITT procedure: 1) an early enrollment in the LITT therapy after diagnosis of a tumor recurrence, and 2) a corresponding smaller tumor mass at the beginning of the therapy.Conclusion:Cytoreduction by laser irradiation seems to be a promising option for patients suffering from gliomas.


2015 ◽  
Vol 121 (4) ◽  
pp. 473-482 ◽  
Author(s):  
J. Almeida ◽  
D. Liang ◽  
C. R. Vistas ◽  
R. Bouadjemine ◽  
E. Guillot

Author(s):  
P. A. Molian ◽  
K. H. Khan ◽  
W. E. Wood

In recent years, the effects of chromium on the transformation characteristics of pure iron and the structures produced thereby have been extensively studied as a function of cooling rate. In this paper, we present TEM observations made on specimens of Fe-10% Cr and Fe-20% Cr alloys produced through laser surface alloying process with an estimated cooling rate of 8.8 x 104°C/sec. These two chromium levels were selected in order to study their phase transformation characteristics which are dissimilar in the two cases as predicted by the constitution diagram. Pure iron (C<0.01%, Si<0.01%, Mn<0.01%, S=0.003%, P=0.008%) was electrodeposited with chromium to the thicknesses of 40 and 70μm and then vacuum degassed at 400°F to remove the hydrogen formed during electroplating. Laser surface alloying of chromium into the iron substrate was then performed employing a continuous wave CO2 laser operated at an incident power of 1200 watts. The laser beam, defocussed to a spot diameter of 0.25mm, scanned the material surface at a rate of 30mm/sec, (70 ipm).


Author(s):  
M. Hibino ◽  
K. Irie ◽  
R. Autrata ◽  
P. schauer

Although powdered phosphor screens are usually used for scintillators of STEM, it has been found that the phosphor screen of appropriate thickness should be used depending on the accelerating voltage, in order to keep high detective quantum efficiency. 1 It has been also found that the variation in sensitivity, due to granularity of phosphor screens, makes the measurement of fine electron probe difficult and that the sensitivity reduces with electron irradiation specially at high voltages.In order to find out a preferable scintillator for STEM, single crystals of YAG (yttrium aluminum garnet), which are used for detecting secondary and backscattered electrons in SEM were investigated and compared with powdered phosphor screens, at the accelerating voltages of 100kV and 1 MV. A conventional electron detection system, consisting of scintillator, light guide and PMT (Hamamatsu Photonics R268) was used for measurements. Scintillators used are YAG single crystals of 1.0 to 3.2mm thicknesses (with surfaces matted for good interface to the light guide) and of 0.8mm thickness (with polished surface), and powdered P-46 phosphor screens of 0.07mm and 1.0mm thicknesses for 100kV and 1MV, respectively. Surfaces on electron-incidence side of all scintillators are coated with reflecting layers.


2007 ◽  
Vol 177 (4S) ◽  
pp. 614-614
Author(s):  
Thorsten Bach ◽  
Thomas R.W. Herrmann ◽  
Roman Ganzer ◽  
Andreas J. Gross

Phlebologie ◽  
2000 ◽  
Vol 29 (05) ◽  
pp. 142-145
Author(s):  
T. Hertel ◽  
B. Kahle ◽  
H. G. Kluess ◽  
M. Marshall ◽  
E. Rabe ◽  
...  
Keyword(s):  

2020 ◽  
pp. 131-138

The nonlinear optical properties of pepper oil are studied by diffraction ring patterns and Z-scan techniques with continuous wave beam from solid state laser at 473 nm wavelength. The nonlinear refractive index of the sample is calculated by both techniques. The sample show high nonlinear refractive index. Based on Fresnel-Kirchhoff diffraction integral, the far-field intensity distributions of ring patterns have been calculated. It is found that the experimental results are in good agreement with the theoretical results. Also the optical limiting property of pepper oil is reported. The results obtained in this study prove that the pepper oil has applications in nonlinear optical devices.


2018 ◽  
pp. 156-161
Author(s):  
Alexei K. Solovyov

Underground spaces in town centres present a big attraction for investors. However, they put special requirements to the internal environment. Those requirements can be fulfilled by means of daylighting. Examples of lighting of underground spaces are discussed. It is shown that the common systems of natural lighting are not always possible to use and cause big heat losses. Hollow light guide pipes allow avoid the shortcomings of common daylight systems. Method of calculation of daylight factors from hollow light guide pipes is shown. The results of calculation of daylight factors under the light guide pipes of different diameters in the different depths are presented.


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