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ION HEATING PROCESS DURING PLASMA IMMERSION ION IMPLANTATION

X.B. Tian , X.F. Wang , A.G. Liu , L.P. Wang , S. Y. Wang , B. Y. Tang and P. K. Chu 1)Advanced Welding Production & Technology National Key Laboratory , Harbin Institute of Technology , Harbin 150001 , China 2)Department of Physics & Materials Science , City University of Hong Kong , China

金属学报(英文版)

The research on plasma immersion ion implantation has been conducted for a little over ten years. Much is needed to investigate including processing technlogy, plasma sheath dynamics, interaction of plasma and surface, etc. Of the processing methods elavated temperature technique is usually used in PIII to produce a thick modified layer by means of the thermal diffusion. Meanwhile plasma ion heating is more recently developed by Ronghua Wei et al[1]. Therefore the temeperature is a critical parameter in plasma ion processing. In this paper we present the theoretical model and analysize the effect of imlantation voltage, plasma density, ion mass,etc on the temperature rise.

关键词: plasma immersion ion implantation , null , null

Capacitance of High-Voltage Coaxial Cable in Plasma Immersion Ion Implantation

X.B. Tian , L.P. Wang , D. T.K.Kwok , B. Y Tang , P.K.Chu

材料科学技术(英文)

Plasma immersion ion implantation (PIII) is an excellent technique for the surf see modification of complex-shaped components. Owing to pulsed operation mode of the high voltage and large slew rate, the capacitance on the high-voltage coaxial cable can be detrimental to the process and cannot be ignored. In fact, a significant portion of the rise-time/fall-time of the implantation voltage pulse and big initial current can be attributed to the coaxial cable.

关键词:

Mechanical Alloying of Fe_(100-x) B_x

Lizhi CHENG , Wei FENG , Xinquan DONG , Kuichang BAI and Kaiyuan HE (Dept. of Materials Science and Engineering , Northeastern University Shenyang 110006 , China)

材料科学技术(英文)

The formation of nonequilibrium phase by mechanical alloying (MA) of Fe and B powders in a high energy vibration ball mill has been made for Fe100-xBx system with x=15. 30, 35, 45,55 and 70. By using the X-ray diffraction, magnetic measurement and M6ssbauer spectrummethods, it was revealed that the structure of the MA product varies with milling time and B contents.

关键词:

Dependence of Ni, Al and B boundary concentrations on the B bulk concentration for the Ni3Al-x at.% B grain boundary

Nuclear Instruments & Methods in Physics Research Section B-Beam Interactions with Materials and Atoms

We have applied the embedded atom method (EAM). to calculate boundary concentration distributions of Ni, Al and B, and B probabilities in the "interstitial" and, the "substitutional" sites, at the Ni3Al-x at.% B (100% Ni\100% Ni) [001]/Sigma5(210)/36.87 degrees. grain boundary at the equilibrium. We propose that the bulk effects of B on the grain boundary include the positive effect on the Ni enrichment at the grain boundary, i.e. the B atoms induce Ni atoms to substitute into Al sites, the negative effect on it, i.e. the B atoms substitute into Ni sites, and the neutral effect on it, i.e. the B atoms insert into interstices in the grain boundary. Our calculations show that owing to combination of the positive effect and the negative effect, corresponding to B-enrichment increasing, the Ni-enrichment and the Al-depletion become more and more obvious, when x increases from 0.1 to 0.5. Then, corresponding to B-enrichment decreasing, the Ni-enrichment and the Al-depletion also become more and more obvious, when x decreases from 0.9 to 0.5. Thus, between low (x = 0.1) and high (x = 0.9) B bulk concentrations, there is a B bulk concentration (x = 0.5), at which the Ni-enrichment and the Al-depletion become the most obvious, even if Ni is approximately saturated. (C) 2001 Elsevier Science B.V. All rights reserved.

关键词: computer-simulation;boron;segregation;fracture;metals;alloys

Study of properties of mixed ferro-ferrimagnetic ising compounds with (A(x)B(1-x))(y)C

Communications in Theoretical Physics

The magnetic properties of the mixed ferro-ferrimagnetic compounds with (A(x)B(1-x))(y)C-z where A(z) B-z and C are three different magnetic ions and form three different sublattices, are studied by using the standard mean-field theory. The phase diagram which is related to experimental work of molecule-based ferro-ferrimagnet ((NixMn1-xII)-Mn-II)(1.5)[Cr-III(CN)(6)].zH(2)O is obtained. The magnetization curves(z) internal energy(z) and specific heat of the same mixed (A(x)B(1-x))(y)C system are also investigated.

关键词: mixed ferro-ferrimagnet;Ising model;phase diagram;internal energy;specific heat;mean-field analysis;magnetic-properties;prussian blue;alloy

Magnetic and magnetostrictive properties of the Laves-phase compounds Tb(1-x)Pr(x)(Fe(0.4)Co(0.6))(1.9)B(0.1) (0 <= x <= 1)

Journal of Physics D-Applied Physics

Single-phase Tb(1-x)Pr(x)(Fe(0.4)Co(0.6))(1.9)B(0.1)(0 <= x <= 1) compounds have been synthesized by arc melting and subsequent annealing at ambient pressure. The lattice parameter increases while the Curie temperature decreases linearly with increasing Pr content. The saturation magnetization at 5 and 295 K of the Tb(1-x) Pr(x)(Fe(0.4)Co(0.6))(1.9)B(0.1) compounds decreases when x <= 0.5, then increases with further increasing x. The smallest magnetostriction at room temperature (RT) for Tb(0.5)Pr(0.5)(Fe(0.4)Co(0.6))(1.9)B(0.1) is attributed to its total rare-earth moment which is close to zero, due to the antiparallel alignment of the Pr and Tb moments. The normalized RT magnetization and magnetostriction show that Tb(0.2)Pr(0.8)(Fe(0.4)Co(0.6))(1.9)B(0.1) has the smallest anisotropy, which agrees with the easy magnetization direction along < 1 1 1 > for the compounds with x <= 0.8, but along < 1 1 0 > for the compounds with x = 0.9 and 1.0.

关键词: alloys;prfe2

Structure, magnetic properties and magnetostriction of laves compounds Nd(1-x)Pr(x)(Fe(0.35)Co(0.55)B(0.1))(2)

Journal of Magnetism and Magnetic Materials

The C15 Laves phases with composition Nd(1-x)Pr(x)(Fe(0.35)Co(0.55)B(0.1))(2) (0 <= x <= 1) have been synthesized by arc melting and subsequent annealing. The Curie temperature T(c) and the saturation magnetizations M(s) at 5 and 295 K decrease with increasing Pr content. The linear anisotropic magnetostriction lambda(a) = lambda(parallel to)-lambda(perpendicular to) at room temperature for Nd(1-x)Pr(x)(Fe(0.35)Co(0.55)B(0.1))(2) alloys with 0 <= x <= 0.4 initially reaches a negative minimum, then increases and changes its sign with increasing magnetic field H, and the lambda(a) for the alloys with x >= 0.6 is positive and increases as magnetic field H increases. (C) 2008 Elsevier B.V. All rights reserved.

关键词: structure;magnetic property;magnetostriction;phase;alloys;boron

Monte Carlo simulation study of the bulk effects of boron on the Ni3Al-x at.% B grain boundary

Materials Letters

The embedded atom method (EAM) has been used to calculate boundary concentration distributions of Ni, Al, and B, and B probabilities in the "interstitial" and the "substitutional" sites, at the Ni3Al-x at.% B (100% Ni/100% Ni) [001]/Sigma5(210)/36.87degrees grain boundary at the equilibrium. It has been proposed by us that the bulk effects of B on the grain boundary include the main effect, that is, the B atoms induce Ni atoms to substitute into Al sites, and the sub-effect, that is, the B atoms substitute into Ni sites. In this work, it is found that at as x increases from 0.1 to 1.0, the B probability in the "interstitial" sites decreases from 97.3% to 38.8%, while that in the "substitutional" sites increases from 2.7% to 61.2%. It is also found that owing to combination of the main effect and the sub-effect, corresponding to B enrichment increasing, the Ni enrichment and the Al depletion become more and more obvious when x increases from 0.1 to 0.5. Then, corresponding to B enrichment decreasing, the Ni enrichment and the Al depletion also become more and more obvious when x decreases from 0.9 to 0.5. Thus, between low (x = 0.1) and high (x = 0.9) B bulk concentrations, there is a B bulk concentration (x = 0.5), at which the Ni enrichment and the Al depletion become the most obvious, and Ni is approximately saturated. (C) 2002 Elsevier Science B.V All rights reserved.

关键词: grain boundary concentrations;inducing and segregating species;bulk;effects;metals;alloys;ni

INTRINSIC MAGNETISM AND MAGNETIC ANISOTROPY OF AMORPHOUS Fe_(1-x)(Si,B)_x ALLOYS

GUAN Kehong WANG Jun Northeast University of Technology , Shenyang , China GUAN Kehong , Associate Professor , Dept.of Material Science and Engineering , Northeast Univeristy of Technology , Shenyang 110006 , China

金属学报(英文版)

The magnetic moment and the magnetostriction decrease slightly with the increase of total Si+B content.A maximum of the Curie temperature appears at about 25 at.-% of Si+B.The magnetic anisotropy is uninfluential by the content of Si+B,but much influnce by the demagnetization effect of streak.A qualitative explanation of the experimental phenomenon seems to be noted by the aid of the electron transition and structure model of amorphous al- loys.

关键词: Fe-Si-B alloy , null , null , null , null , null

MAGNETIC PROPERTIES AND CRYSTALLIZATION OF RAPIDLY QUENCHED(Fe_(1-x)Ga_x)_(77.5)Nd_4B_(18.5) ALLOYS

YANG Hongying SHEN Baogen YANG Linyuan GUO Huiqun Laboratory of Magnetics , Institute of Physics , Academia Sinica , Beijing , China

金属学报(英文版)

The Curie temperature increases but crystallization temperature decreases with the in- crease of Ga content,x,of amorphous(Fe_(1-x)Ga_x)_(77.5)Nd_4B_(18.5) alloys.The average magnetic moment of Fe atoms is almost a constant.By X-ray diffraction and ther- momagnetic measurements,the crystalline phases of the alloys,an unknown phase and α-(Fe,Ga)besides Fe_3 B as major one,were identified.The relationship between room temperature coercive field and Ga.content was also studied.

关键词: magnetic properties , null , null , null

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