Effect of gas composition and purity on excimer laser operation

1994 ◽  
Author(s):  
J. Gabzdyl ◽  
I. J. Stares ◽  
D. Yates ◽  
Michael R. Osborne ◽  
Michael A. O'Key
1993 ◽  
Author(s):  
Robert E. Turner ◽  
John L. Remo ◽  
Vinod Kumar

1993 ◽  
Vol 21 (5) ◽  
pp. 566-576 ◽  
Author(s):  
Shigeyuki TAKAGI ◽  
Koji KAKIZAKI ◽  
Noboru OKAMOTO ◽  
Saburo SATO ◽  
Tatsumi GOTO

2018 ◽  
Vol 6 ◽  
Author(s):  
Xin Guo ◽  
Jinbin Ding ◽  
Yi Zhou ◽  
Yu Wang

The corrosion behaviors of the ArF excimer laser copper alloy electrodes were studied. The morphology, composition and impurities were characterized by optical microscope, scanning electron microscopy, electron microprobe and glow discharge mass spectrometer methods. The anode produces the reef, the corrosion pits, the hole layer and the $1{-}10~\unicode[STIX]{x03BC}\text{m}$ level flake impurity. The cathode produces the particles, the sputtering pits, the element reduce layer and the $1~\unicode[STIX]{x03BC}\text{m}$ level particle impurity. Besides the Cu element, other elements in the alloy participate in the corrosion: Al element in the reef is over 1.5 times of the anode, Zn element in the particles is 1.3 times of the cathode, many trace elements congregate on the copper surface several and even hundreds of times. These elements are responsible to a great degree for the impurities and the rapid energy decline of the long-time idled laser.


1996 ◽  
Vol 35 (3) ◽  
pp. 482 ◽  
Author(s):  
Michael Decker ◽  
Volker Sick

1981 ◽  
Vol 39 (1-2) ◽  
pp. 75-78 ◽  
Author(s):  
R. Salimbeni ◽  
M. Matera ◽  
M. Vannini ◽  
P. Burlamacchi

Author(s):  
G.D. Danilatos

Over recent years a new type of electron microscope - the environmental scanning electron microscope (ESEM) - has been developed for the examination of specimen surfaces in the presence of gases. A detailed series of reports on the system has appeared elsewhere. A review summary of the current state and potential of the system is presented here.The gas composition, temperature and pressure can be varied in the specimen chamber of the ESEM. With air, the pressure can be up to one atmosphere (about 1000 mbar). Environments with fully saturated water vapor only at room temperature (20-30 mbar) can be easily maintained whilst liquid water or other solutions, together with uncoated specimens, can be imaged routinely during various applications.


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