Low-Pressure Crystallization of Sol–Gel-Derived PbZr0.52Ti0.48O3Thin Films at Low Temperature for Low-Voltage Operation

2003 ◽  
Vol 42 (Part 1, No. 5A) ◽  
pp. 2756-2758 ◽  
Author(s):  
Ding-Yeong Wang ◽  
Chao-Hsin Chien ◽  
Chun-Yen Chang ◽  
Ching-Chich Leu ◽  
Jung-Yen Yang ◽  
...  
2010 ◽  
Vol 96 (19) ◽  
pp. 192115 ◽  
Author(s):  
Hyojin Bong ◽  
Wi Hyoung Lee ◽  
Dong Yun Lee ◽  
Beom Joon Kim ◽  
Jeong Ho Cho ◽  
...  

1999 ◽  
Author(s):  
Yoshikazu Fujimori ◽  
Toshiyuki Takeda ◽  
Takashi Nakamura ◽  
Hidemi Takasu

1994 ◽  
Vol 04 (C6) ◽  
pp. C6-153-C6-158 ◽  
Author(s):  
A. Sylvestre ◽  
P. Crozat ◽  
R. Adde ◽  
A. De Lustrac ◽  
Y. Jin

Author(s):  
Yasuyuki Ito ◽  
Maho Ushikubo ◽  
Seiichi Yokoyama ◽  
Hironori Matsunaga ◽  
Tsutomu Atsuki ◽  
...  

1997 ◽  
Vol 117 (3) ◽  
pp. 227-232
Author(s):  
Maho Ushikubo ◽  
Seiich Yokoyama ◽  
Yasuyuki Ito ◽  
Hironori Matsunaga ◽  
Tsutomu Atuki ◽  
...  

2001 ◽  
Vol 39 (1-4) ◽  
pp. 223-230
Author(s):  
Kazunari Maki ◽  
Nobuyuki Soyama ◽  
Kaoru Nagamine ◽  
Satoru Mori ◽  
Katsumi Ogi

Author(s):  
Gert Ehrlich

The field ion microscope, devised by Erwin Muller in the 1950's, was the first instrument to depict the structure of surfaces in atomic detail. An FIM image of a (111) plane of tungsten (Fig.l) is typical of what can be done by this microscope: for this small plane, every atom, at a separation of 4.48Å from its neighbors in the plane, is revealed. The image of the plane is highly enlarged, as it is projected on a phosphor screen with a radius of curvature more than a million times that of the sample. Müller achieved the resolution necessary to reveal individual atoms by imaging with ions, accommodated to the object at a low temperature. The ions are created at the sample surface by ionization of an inert image gas (usually helium), present at a low pressure (< 1 mTorr). at fields on the order of 4V/Å.


Author(s):  
Klaus-Ruediger Peters

A new generation of high performance field emission scanning electron microscopes (FSEM) is now commercially available (JEOL 890, Hitachi S 900, ISI OS 130-F) characterized by an "in lens" position of the specimen where probe diameters are reduced and signal collection improved. Additionally, low voltage operation is extended to 1 kV. Compared to the first generation of FSEM (JE0L JSM 30, Hitachi S 800), which utilized a specimen position below the final lens, specimen size had to be reduced but useful magnification could be impressively increased in both low (1-4 kV) and high (5-40 kV) voltage operation, i.e. from 50,000 to 200,000 and 250,000 to 1,000,000 x respectively.At high accelerating voltage and magnification, contrasts on biological specimens are well characterized1 and are produced by the entering probe electrons in the outmost surface layer within -vl nm depth. Backscattered electrons produce only a background signal. Under these conditions (FIG. 1) image quality is similar to conventional TEM (FIG. 2) and only limited at magnifications >1,000,000 x by probe size (0.5 nm) or non-localization effects (%0.5 nm).


Author(s):  
Arthur V. Jones

With the introduction of field-emission sources and “immersion-type” objective lenses, the resolution obtainable with modern scanning electron microscopes is approaching that obtainable in STEM and TEM-but only with specific types of specimens. Bulk specimens still suffer from the restrictions imposed by internal scattering and the need to be conducting. Advances in coating techniques have largely overcome these problems but for a sizeable body of specimens, the restrictions imposed by coating are unacceptable.For such specimens, low voltage operation, with its low beam penetration and freedom from charging artifacts, is the method of choice.Unfortunately the technical dificulties in producing an electron beam sufficiently small and of sufficient intensity are considerably greater at low beam energies — so much so that a radical reevaluation of convential design concepts is needed.The probe diameter is usually given by


1987 ◽  
Vol 48 (C6) ◽  
pp. C6-487-C6-492
Author(s):  
W. Liu ◽  
D. M. Ren ◽  
C. L. Bao ◽  
T. T. Tsong

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