Ion Implanted N-Type Resistors on High-Resistivity Substrates

1973 ◽  
Vol 10 (6) ◽  
pp. 944-947 ◽  
Author(s):  
J. W. Hanson ◽  
R. J. Huber ◽  
J. N. Fordemwalt
Keyword(s):  
High Resistivity ◽  
Ion Implanted

Correlation Study of Morphology, Electrical Activation and Contact formation of Ion Implanted 4H-SiC

2009 ◽  
Vol 156-158 ◽  
pp. 493-498
Author(s):  
Ming Hung Weng ◽  
Fabrizio Roccaforte ◽  
Filippo Giannazzo ◽  
Salvatore di Franco ◽  
Corrado Bongiorno ◽  
...  
Keyword(s):  
High Temperature ◽  
Surface Morphology ◽  
Electrical Activation ◽  
Structural Defects ◽  
High Resistivity ◽  
Al Alloy ◽  
High Temperature Annealing ◽  
Capping Layer ◽  
P Type ◽  
Ion Implanted

This paper reports a detailed study of the electrical activation and the surface morphology of 4H-SiC implanted with different doping ions (P for n-type doping and Al for p-type doping) and annealed at high temperature (1650–1700 °C) under different surface conditions (with or without a graphite capping layer). The combined use of atomic force microscopy (AFM), transmission electron microscopy (TEM), and scanning capacitance microscopy (SCM) allowed to clarify the crucial role played by the implant damage both in evolution of 4H-SiC surface roughness and in the electrical activation of dopants after annealing. The high density of broken bonds by the implant makes surface atoms highly mobile and a peculiar step bunching on the surface is formed during high temperature annealing. This roughness can be minimized by using a capping layer. Furthermore, residual lattice defects or precipitates were found in high dose implanted layers even after high temperature annealing. Those defects adversely affect the electrical activation, especially in the case of Al implantation. Finally, the electrical properties of Ni and Ti/Al alloy contacts on n-type and p-type implanted regions of 4H-SiC were studied. Ohmic behavior was observed for contacts on the P implanted area, whilst high resistivity was obtained in the Al implanted layer. Results showed a correlation of the electrical behavior of contacts with surface morphology, electrical activation and structural defects in ion-implanted, particularly, Al doped layer of 4H-SiC.

Ion implanted camel diodes fabricated on high resistivity silicon for microwave and millimetre-wave applications

2002 ◽  
Vol 38 (20) ◽  
pp. 1228 ◽  
Author(s):  
Vo Van Tuyen ◽  
Yunhong Wu ◽  
Zhirun Hu ◽  
A.A. Rezazadeh
Keyword(s):  
High Resistivity ◽  
Millimetre Wave ◽  
High Resistivity Silicon ◽  
Ion Implanted

High Voltage P-N Junction Diodes in Silicon Carbide Using Field Plate Edge Termination

1999 ◽  
Vol 572 ◽  
Author(s):  
R. K. Chilukuri ◽  
P. Ananthanarayanan ◽  
V. Nagapudi ◽  
B. J. Baliga
Keyword(s):  
Breakdown Voltage ◽  
Dielectric Material ◽  
High Resistivity ◽  
Leakage Currents ◽  
Plate Edge ◽  
Field Plate ◽  
P Type ◽  
Post Implantation ◽  
Anneal Temperature ◽  
Ion Implanted

ABSTRACTIn this paper, we report the successful use of field plates as planar edge terminations for P+-N as well as N+-P planar ion implanted junction diodes on 6H- and 4H-SiC. Process splits were done to vary the dielectric material (SiO2 vs. Si3N4), the N-type implant (nitrogen vs. phosphorous), the P-type implant (aluminum vs. boron), and the post-implantation anneal temperature. The nitrogen implanted diodes on 4H-SiC with field plates using SiO2 as the dielectric, exhibited a breakdown voltage of 1100 V, which is the highest ever reported measured breakdown voltage for any planar ion implanted junction diode and is nearly 70% of the ideal breakdown voltage. The reverse leakage current of this diode was less than 1×10−5 A/cm2 even at breakdown. The unterminated nitrogen implanted diodes blocked lower voltages (∼840V). In contrast, the unterminated aluminum implanted diodes exhibited higher breakdown voltages (∼80OV) than the terminated diodes (∼275V). This is attributed to formation of a high resistivity layer at the surface near the edges of the diode by the P-type ion implant, acting as a junction termination extension. Diodes on 4H-SiC showed higher breakdown than those on 6H-SiC. Breakdown voltages were independent of temperature in the range of 25 °C to 150 °C, while the leakage currents increased slowly with temperature, indicating surface dominated components.

Electrical spectroscopy of high resistivity ion-implanted layers by current-voltage measurements

2008 ◽  
Vol 93 (10) ◽  
pp. 102114 ◽  
Author(s):  
Tiziana Cesca ◽  
Andrea Gasparotto ◽  
Beatrice Fraboni
Keyword(s):  
High Resistivity ◽  
Current Voltage ◽  
Ion Implanted

scholarly journals Ultrafast Carrier Trapping and High Resistivity of MeV Energy Ion Implanted GaAs

1996 ◽  
Vol 90 (4) ◽  
pp. 851-854 ◽  
Author(s):  
K.P. Korona ◽  
J. Jasiński ◽  
A. Kurpiewski ◽  
M. Kamińska ◽  
C. Jagadish ◽  
...  
Keyword(s):  
High Resistivity ◽  
Carrier Trapping ◽  
Ultrafast Carrier ◽  
Ion Implanted

Electron Diffraction Analysis of Microtwin Structures in Regrown (III) Silicon

1982 ◽  
Vol 40 ◽  
pp. 460-461
Author(s):  
P. Ling ◽  
R. Gronsky ◽  
J. Washburn
Keyword(s):  
Electron Diffraction ◽  
Ion Implantation ◽  
Diffraction Analysis ◽  
Diffraction Pattern ◽  
Direct Consequence ◽  
The Other ◽  
Electron Diffraction Analysis ◽  
Defect Microstructures ◽  
Ion Implanted

The defect microstructures of Si arising from ion implantation and subsequent regrowth for a (111) substrate have been found to be dominated by microtwins. Figure 1(a) is a typical diffraction pattern of annealed ion-implanted (111) Si showing two groups of extra diffraction spots; one at positions (m, n integers), the other at adjacent positions between <000> and <220>. The object of the present paper is to show that these extra reflections are a direct consequence of the microtwins in the material.

Defects in ion implanted silicon

1978 ◽  
Vol 36 (1) ◽  
pp. 386-387
Author(s):  
J.A. Lambert ◽  
P.S. Dobson
Keyword(s):  
Defect Structure ◽  
Dislocation Loops ◽  
Frank Loop ◽  
Burgers Vector ◽  
Temperature Range ◽  
Perfect Dislocation ◽  
Contrast Analysis ◽  
Image Position ◽  
Ion Implanted

The defect structure of ion-implanted silicon, which has been annealed in the temperature range 800°C-1100°C, consists of extrinsic Frank faulted loops and perfect dislocation loops, together with‘rod like’ defects elongated along <110> directions. Various structures have been suggested for the elongated defects and it was argued that an extrinsically faulted Frank loop could undergo partial shear to yield an intrinsically faulted defect having a Burgers vector of 1/6 <411>.This defect has been observed in boron implanted silicon (1015 B+ cm-2 40KeV) and a detailed contrast analysis has confirmed the proposed structure.

A technique to prepare cross-sectional TEM specimens of semiconducting devices

1986 ◽  
Vol 44 ◽  
pp. 742-743
Author(s):  
A. K. Rai ◽  
P. P. Pronko
Keyword(s):  
Thin Films ◽  
Surface Region ◽  
Sample Surface ◽  
Specific Region ◽  
Cross Sectional ◽  
Thin Sections ◽  
The Past ◽  
Device Structures ◽  
Ion Implanted

Several techniques have been reported in the past to prepare cross(x)-sectional TEM specimen. These methods are applicable when the sample surface is uniform. Examples of samples having uniform surfaces are ion implanted samples, thin films deposited on substrates and epilayers grown on substrates. Once device structures are fabricated on the surfaces of appropriate materials these surfaces will no longer remain uniform. For samples with uniform surfaces it does not matter which part of the surface region remains in the thin sections of the x-sectional TEM specimen since it is similar everywhere. However, in order to study a specific region of a device employing x-sectional TEM, one has to make sure that the desired region is thinned. In the present work a simple way to obtain thin sections of desired device region is described.

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