Maskless Patterning of Cr Films Using Focused Ion Beams

1983 ◽  
Vol 27 ◽  
Author(s):  
K. Gamo ◽  
K. Moriizumi ◽  
T. Matsui ◽  
S. Namba

ABSTRACTCharacteristics of maskless patterning of Cr films using focused Sb+ ion implantation have been investigated. Dose and depth dependence of the etching rate of Sb-implanted layers during plasma etching using CCl4 were measured. Sb profiles were also measured by Rutherford backscattering techniques. It was found that a sharp threshold dose exists to form an etch-resistant layer by Sb implantation. It was also found that a latent image of an Sb implanted pattern at a dose ≥3.8×1015/cm2 was developed by the plasma etching, and that Cr patterns with a thickness of a few hundred nanometers were formed by the present maskless patterning technique.

1985 ◽  
Vol 45 ◽  
Author(s):  
Kenji Gamo ◽  
Susumu Namba

Recent advances of focused ion beam systems and their applications are presented. The applications include maskless ion implantation and various maskless patterning techniques which make use of ion induced chemical effects. These are ion beam assisted etching, deposition and ion beam modification techniques and are promising to improve patterning speed and extend applications of focused ion beams.


1986 ◽  
Vol 76 ◽  
Author(s):  
Kenji Gamo ◽  
Katsuyuki Yonehara ◽  
Shohei Nagatomo ◽  
Susumu Namba

ABSTRACTMaskless patterning of Mo and Si was done by implanting 50 keV focused Ga+ ion beam and by plasma etching using CF4 gas. The implantation is done to modify the chemical properties of the sample surface. It was found that Mo films became etch-resistant for the plasma etching after implantation at a dose higher than 4×1015 /cm2. Si crystals showed a positive tone pattern due to a radiation enhanced etching at a dose lower than 5x1016/cm2. At higher doses, the etching rate decreased and above 8 x 1016/cm2, no etching was observed in the implanted region. Patterns with a thickness of a several hundred nanometers were formed by the present maskless patterning technique.


1987 ◽  
Vol 101 ◽  
Author(s):  
Zheng Xu ◽  
Kenji Gamo ◽  
Susumu Namba

ABSTRACTCharacteristics of ion beam assisted etching (IBAE) for SiO2 have been investigated to reveal'a possibility for maskless etching using focused ion beams. The ion beam assisted etching was done by bombarding 50 keV unfocused ion beams in XeF2 atmosphere and effect of various etching parameter on etching characteristics have been investigated. These are the effects of XeF2 gas pressure, bombarding ion species, bombarding angle and H2 addition, etc. Significant enhancements up to 100 times larger than physical sputtering were achieved. The selectivity of SiO2 to Si could be tailored to specific requirements from 0.1 to 6 by changing the gas mixing ratio. The etching rate was approximately proportional to the energy deposition rate bombarded by ion beam on surface. Carbon contamination on surface after etching were improved by the introduction of XeF2 gas.


1990 ◽  
Vol 56 (7) ◽  
pp. 1181-1184
Author(s):  
Haruo KASAHARA ◽  
Hiroshi SAWARAGI ◽  
Ryuso AIHARA

1995 ◽  
Vol 7 (8) ◽  
pp. 845-847 ◽  
Author(s):  
A. Orth ◽  
J.P. Reithmaier ◽  
F. Faller ◽  
A. Forchel

Author(s):  
Kenji Gamo ◽  
Ge Huang ◽  
Kouichi Moriizumi ◽  
Norihiko Samoto ◽  
Ryuichi Shimizu ◽  
...  

Author(s):  
John F. Walker ◽  
J C Reiner ◽  
C Solenthaler

The high spatial resolution available from TEM can be used with great advantage in the field of microelectronics to identify problems associated with the continually shrinking geometries of integrated circuit technology. In many cases the location of the problem can be the most problematic element of sample preparation. Focused ion beams (FIB) have previously been used to prepare TEM specimens, but not including using the ion beam imaging capabilities to locate a buried feature of interest. Here we describe how a defect has been located using the ability of a FIB to both mill a section and to search for a defect whose precise location is unknown. The defect is known from electrical leakage measurements to be a break in the gate oxide of a field effect transistor. The gate is a square of polycrystalline silicon, approximately 1μm×1μm, on a silicon dioxide barrier which is about 17nm thick. The break in the oxide can occur anywhere within that square and is expected to be less than 100nm in diameter.


2007 ◽  
Vol 91 (12) ◽  
pp. 122105 ◽  
Author(s):  
S. J. Robinson ◽  
C. L. Perkins ◽  
T.-C. Shen ◽  
J. R. Tucker ◽  
T. Schenkel ◽  
...  

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