CO2 laser drives extreme ultraviolet nano-lithography — second life of mature laser technology

2013 ◽  
Vol 21 (4) ◽  
Author(s):  
K. Nowak ◽  
T. Ohta ◽  
T. Suganuma ◽  
J. Fujimoto ◽  
H. Mizoguchi ◽  
...  

AbstractIt was shown both theoretically and experimentally that nanosecond order laser pulses at 10.6 micron wavelength were superior for driving the Sn plasma extreme ultraviolet (EUV) source for nano-lithography for the reasons of higher conversion efficiency, lower production of debris and higher average power levels obtainable in CO2 media without serious problems of beam distortions and nonlinear effects occurring in competing solid-state lasers at high intensities. The renewed interest in such pulse format, wavelength, repetition rates in excess of 50 kHz and average power levels in excess of 18 kiloWatt has sparked new opportunities for a matured multi-kiloWatt CO2 laser technology. The power demand of EUV source could be only satisfied by a Master-Oscillator-Power-Amplifier system configuration, leading to a development of a new type of hybrid pulsed CO2 laser employing a whole spectrum of CO2 technology, such as fast flow systems and diffusion-cooled planar waveguide lasers, and relatively recent quantum cascade lasers. In this paper we review briefly the history of relevant pulsed CO2 laser technology and the requirements for multi-kiloWatt CO2 laser, intended for the laser-produced plasma EUV source, and present our recent advances, such as novel solid-state seeded master oscillator and efficient multi-pass amplifiers built on planar waveguide CO2 lasers.

Author(s):  
Z. Mucha ◽  
S. Müller ◽  
J. H. Schäfer ◽  
J. Uhlenbusch ◽  
W. Viöl

1992 ◽  
Vol 20 (5) ◽  
pp. 322-336 ◽  
Author(s):  
Hidekazu HATANAKA ◽  
Nobuo KAWAHARA ◽  
Katsumi MIDORIKAWA ◽  
Minoru OBARA ◽  
Hideo TASHIRO

Author(s):  
A. Kareem Dahash Ali ◽  
Nihad Ali Shafeek

This study included the fabrication of    compound (Tl2-xHgxBa2-ySryCa2Cu3O10+δ) in a manner solid state and under hydrostatic pressure ( 8 ton/cm2) and temperature annealing(850°C), and determine the effect of the laser on the structural and electrical properties elements in the compound, and various concentrations of x where (x= 0.1,0.2,0.3 ). Observed by testing the XRD The best ratio of compensation for x is 0.2 as the value of a = b = 5.3899 (A °), c = 36.21 (A °) show that the installation of four-wheel-based type and that the best temperature shift is TC= 142 K  .When you shine a CO2 laser on the models in order to recognize the effect of the laser on these models showed the study of X-ray diffraction of these samples when preparing models with different concentrations of the values ​​of x, the best ratio of compensation is 0.2 which showed an increase in the values ​​of the dimensions of the unit cell a=b = 5.3929 (A °), c = 36.238 (A°). And the best transition temperature after shedding laser is TC=144 K. 


1988 ◽  
Vol 17 (4) ◽  
pp. 91-93
Author(s):  
D. P. Juyal ◽  
N. K. Barthwal ◽  
A. L. Singh ◽  
S. P. Gupta ◽  
M. T. Rudrappa ◽  
...  

2007 ◽  
Vol 90 (19) ◽  
pp. 191503 ◽  
Author(s):  
Yoshifumi Ueno ◽  
Tatsuya Ariga ◽  
George Soumagne ◽  
Takeshi Higashiguchi ◽  
Shoichi Kubodera ◽  
...  

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