Characterization of imaging normal-incidence multilayer mirrors for the 40- to 300-Å range by spectroscopic techniques using a laser-plasma radiation source

1994 ◽  
Author(s):  
Eugene N. Ragozin ◽  
Nikolai N. Kolachevsky ◽  
Mikhail M. Mitropolsky ◽  
Vladimir A. Slemzin ◽  
Nikolai N. Salashchenko
Keyword(s):  
Laser Plasma ◽  
Radiation Source ◽  
Normal Incidence ◽  
Plasma Radiation ◽  
Spectroscopic Techniques ◽  
Multilayer Mirrors

Characterization of multilayer x-ray mirrors for the λ ⋍ 19 nm range using a laser-plasma radiation source

1993 ◽  
Vol 23 (1) ◽  
pp. 76-80 ◽  
Author(s):  
I A Zhitnik ◽  
S V Kuzin ◽  
M M Mitropol'skiĭ ◽  
Evgenii N Ragozin ◽  
V A Slemzin ◽  
...  
Keyword(s):  
Laser Plasma ◽  
Radiation Source ◽  
Plasma Radiation ◽  
X Ray ◽  
Nm Range

Measurements of reflection spectra of soft X-ray multilayer mirrors using a broadband laser-plasma radiation source

2009 ◽  
Vol 39 (5) ◽  
pp. 474-480 ◽  
Author(s):  
E A Vishnyakov ◽  
Konstantin N Mednikov ◽  
A A Pertsov ◽  
Evgenii N Ragozin ◽  
A A Reva ◽  
...  
Keyword(s):  
Laser Plasma ◽  
Radiation Source ◽  
Plasma Radiation ◽  
Reflection Spectra ◽  
Multilayer Mirrors ◽  
X Ray ◽  
Broadband Laser

Spectroscopic characterization of soft x-ray multilayer optics using a broadband laser-plasma radiation source

1997 ◽  
Author(s):  
Eugene N. Ragozin ◽  
Nikolai N. Kolachevsky ◽  
Mikhail M. Mitropolsky ◽  
Yurii Y. Pokrovsky
Keyword(s):  
Laser Plasma ◽  
Radiation Source ◽  
Spectroscopic Characterization ◽  
Plasma Radiation ◽  
X Ray ◽  
Broadband Laser

Micromachining of organic polymers by X-ray photo-etching using a 10Hz laser-plasma radiation source

2005 ◽  
Vol 78-79 ◽  
pp. 452-456 ◽  
Author(s):  
A. Bartnik ◽  
H. Fiedorowicz ◽  
R. Jarocki ◽  
L. Juha ◽  
J. Kostecki ◽  
...  
Keyword(s):  
Laser Plasma ◽  
Radiation Source ◽  
Plasma Radiation ◽  
Organic Polymers ◽  
X Ray

Strong temperature effect on X-ray photo-etching of polytetrafluoroethylene using a 10 Hz laser-plasma radiation source based on a gas puff target

2006 ◽  
Vol 82 (4) ◽  
pp. 529-532 ◽  
Author(s):  
A. Bartnik ◽  
H. Fiedorowicz ◽  
R. Jarocki ◽  
L. Juha ◽  
J. Kostecki ◽  
...  
Keyword(s):  
Temperature Effect ◽  
Laser Plasma ◽  
Radiation Source ◽  
Plasma Radiation ◽  
X Ray

High resolution x-ray absorption spectroscopy using a laser plasma radiation source

2004 ◽  
Vol 75 (11) ◽  
pp. 4606-4609 ◽  
Author(s):  
Ulrich Vogt ◽  
Thomas Wilhein ◽  
Holger Stiel ◽  
Herbert Legall
Keyword(s):  
High Resolution ◽  
Absorption Spectroscopy ◽  
Laser Plasma ◽  
Radiation Source ◽  
Plasma Radiation ◽  
X Ray ◽  
X Ray Absorption

Design, fabrication, and characterization of broadband multilayer mirrors for EUV optics at normal incidence

2000 ◽  
Author(s):  
Zhanshan Wang ◽  
Changjun Kun ◽  
Yueying Ma ◽  
Bin Chen ◽  
Jianlin Cao ◽  
...  
Keyword(s):  
Normal Incidence ◽  
Multilayer Mirrors ◽  
Fabrication And Characterization

Characterization of intergranular cuprous oxide in polycrystalline YBa2Cu3O7-x

1988 ◽  
Vol 46 ◽  
pp. 880-881
Author(s):  
Bradley L. Thiel ◽  
Chan Han R. P. ◽  
Kurosky L. C. Hutter ◽  
I. A. Aksay ◽  
Mehmet Sarikaya
Keyword(s):  
Grain Boundary ◽  
Cuprous Oxide ◽  
Room Temperature ◽  
Boundary Phase ◽  
Spectroscopic Techniques ◽  
Transition Width ◽  
Practical Applications ◽  
Thin Foils ◽  
Superconducting Oxides

The identification of extraneous phases is important in understanding of high Tc superconducting oxides. The spectroscopic techniques commonly used in determining the origin of superconductivity (such as RAMAN, XPS, AES, and EXAFS) are surface-sensitive. Hence a grain boundary phase several nanometers thick could produce irrelevant spectroscopic results and cause erroneous conclusions. The intergranular phases present a major technological consideration for practical applications. In this communication we report the identification of a Cu2O grain boundary phase which forms during the sintering of YBa2Cu3O7-x (1:2:3 compound).Samples are prepared using a mixture of Y2O3. CuO, and BaO2 powders dispersed in ethanol for complete mixing. The pellets pressed at 20,000 psi are heated to 950°C at a rate of 5°C per min, held for 1 hr, and cooled at 1°C per min to room temperature. The samples show a Tc of 91K with a transition width of 2K. In order to prevent damage, a low temperature stage is used in milling to prepare thin foils which are then observed, using a liquid nitrogen holder, in a Philips 430T at 300 kV.

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