• Title/Summary/Keyword: ion tracks

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Variation of Conductivity of Fullerite Structures Under Different Types of Pressure

  • Berdinsky, A.S.;Fink, D.;Chun, Hui-Gon;Yoo, Yong-Zoo;Yoo, Ji-Beom;Petrov, A.V.;Alegaonkar, P.S.
    • Journal of Sensor Science and Technology
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    • v.13 no.5
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    • pp.392-398
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    • 2004
  • It is known that the conductivity of fullerite depends on the applied pressure. In this paper we compare the variation of conductivity of three different fullerite structure with pressure. We examined $C_{60}$ powder, filled into thin glass capillaries and also studied fullerite nanotubules produced within etched swift heavy ion tracks in polymer foils. These investigations are compared with the results of planar Si-$C_{60}$-Au structures.

PLASMA SOURCE ION IMPLANTATION OF NITROGEN AND CARBON IONS INTO CO-CEMENTED WC

  • Han, Seung-Hee;Lee, Yeon-Hee;Lee, Jung-Hye;Kim, Hai-Dong;Kim, Gon-Ho;Kim, Yeong-Woo;Cho, Jung-Hee
    • Proceedings of the Korean Vacuum Society Conference
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    • 1999.07a
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    • pp.220-220
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    • 1999
  • In plasma source ion implantation, the target is immersed in the plasma and repetitively biased by negative high voltage pulses to implant the extracted ions from plasma into the surface of the target material. In this way, the problems of line-of-sight implantation in ion-beam ion implantation technique can be effectively solved. In addition, the high dose rate and simplicity of the equipment enable the ion implantation a commercially affordable process. In this work, plasma source ion implantation technique was used to improve the wear resistance of Co-cemented WC. which has been extensively used for high speed tools. Nitrogen and carbon ions were implanted using the pulse bias of -602kV, 25 sec and at various implantation conditions. The implanted samples were examined using scanning Auger electron spectroscopy and XPS to investigate the depth distributions of implanted ions and to reveal the chemical state change due to the ion implantation. The implanted ions were found to have penetrated to the depth of 3000$\AA$. The wear resistance of the implanted samples was measured using pin-on-disc wear tester and the wear tracks were examined with alpha-step profilometer.

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Isotropic Magnetic Bubble Propagation in Ion Implanted Magnetic Bubble Propagation Tracks (이온주입식 자기 버블 전파 회로에서의 자기 버블의 등방성 전파)

  • Choi, Yeon-Bong;Jo, Soon-Chul
    • Journal of the Korean Institute of Telematics and Electronics
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    • v.27 no.11
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    • pp.69-76
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    • 1990
  • To find out whether isotropic magnetic bubble propagation can be achived by changing magnetostriction coefficients, bias margins and bubble collapse fields of $2.5{\mu}m$ period "diamond" bubble propagation tracks were measured which were fabricated on three magnetic garnet thin films with nearly isotropic magnetostriction coefficients (${\lambda}111{\simeq}{\lambda}100$). The results showed substantially isotropic bubble propagation in "super","good" and "bad" tracks for all three garnet films. From the bubble collapse fields, the bubble potential well depths vs. the direction of the in-plane rotating magnetic fields were plotted. The results showed that substantial differances in the potential well shapes exist for the three "good," "bad" and "super" tracks when ${\Delta}(=({\lambda}111-{\lambda}100)/{\lambda}100)$ was 0.5 (film AK92). However, the differences were minimal when ${\Delta}$ were 0.3 (film Aka8) or 0.1 (film AKb1). In other words, the bubble potential wells were nearly isotropic. The above two measurements indicate that nearly isotropic bubble propagation can be achieved when B is between 0.1 and 0.3.

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CHARACTERISTICS OF DIAMONDLIKE CARBON COATED ALUMINA SEALS AT TEMPERATURES UP TO $400^{\circ}C$ (플라즈마 증착방식에 의해 DLC코팅된 알루미나 세라믹의 코팅박막 특성에 관한 연구)

  • Ok, Chul-Ho;Kim, Byoung-Yong;Kang, Dong-Hun
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2007.11a
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    • pp.397-397
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    • 2007
  • Diamondlike carbon (DLC) coatings were deposited on alumina ceramic seals using a plasma immersion ion deposition technique (PIID). Then they were subjected to tribological tests using a pin-on-disc tribometer under a high load (1.3 GPa) and under elevated temperatures up to 400C. Coefficients of friction (COFs) were recorded and compared with that of the untreated alumina while the wear tracks were analyzed using SEM with EDS to characterize the DLC films. To enhance the DLC adhesion to the substrate, various interlayers including Si and Cr were deposited using the PIID process or an ion beam assisted deposition (IBAD) method. It was observed that the DLC coating, if adhering well to the substrate, reduced the COFs significantly, from 0.4-0.8 for the uncoated alumina to about 0.05-0.1, within the tested temperature range. The adhesion was determined by the interlayer type and possibly by the application method. Cr interlayer did not perform as well as the Si interlayer. This could also be due to the fact that the Cr interlayer and the subsequent DLC coating had to be done in two different processing systems, while both the Si interlayer and the subsequent DLC film were deposited in one system without breaking the chamber. The coating failure mode was found to be delamination between the Cr and the alumina substrate. In contrast, the Si interlayer with proper DLC deposition procedures resulted in very good adhesion and hence excellent tribological performance. Further study may lead to future DLC applications of ceramic seals.

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Tracking Control of Maximum Power Point using Step-up Chopper (체승 Chopper를 이용한 최대 출력점 추적 제어)

  • Chung, Y.T.;Han, K.H.;Jang, K.H.;Kwon, H.;Kang, S.W.;Lee, S.H.;Kim, Y.J.
    • Proceedings of the KIEE Conference
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    • 1990.11a
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    • pp.323-325
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    • 1990
  • In this paper, a new method to track the maximum power point is presented. The proposed scheme achieves the maximum power the step-up chopper, which tracks the maximum power point by sensing only the actual current from the photovoltaic array. Also it adopts the protect ion circuit to protect the battery system against the overvoltage and overvoltage by utilizing hysterisis characteristic.

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A SOLUTION TO THE PROBLEM WITH ABSORBED DOSE

  • Braby, Leslie A.
    • Nuclear Engineering and Technology
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    • v.40 no.7
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    • pp.533-538
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    • 2008
  • In some situations, for example at very low doses, in microbeam irradiation experiments, or around high energy heavy ion tracks, use of the absorbed dose to describe the energy transferred to the irradiated target can be misleading. Since absorbed dose is the expected value of energy per mass it takes into account all of the targets which do not have any energy deposition. In many situations that results in numerical values, in Joules per kg, which are much less than the energy deposited in targets that have been crossed by a charged particle track. This can lead to confusion about the biochemical processes that lead to the consequences of irradiation. There are a few alternative approaches to describing radiation that avoid this potential confusion. Examples of specific situations that can lead to confusion are given. It is concluded that using the particle radiance spectrum and the exposure time, instead of absorbed dose, to describe these irradiations minimizes the potential for confusion about the actual nature of the energy deposition.

Numerical Analysis on Plasma Particles inside Electro-magnetic Field Using Particle-in-cell Method (Particle-in-cell 기법을 이용한 전자기장내 플라즈마 입자의 거동 해석)

  • Han, Doo-Hee;Joe, Min-Kyung;Shin, Junsu;Sung, Hong-Gye;Kim, Su-Kyum
    • Journal of the Korean Society for Aeronautical & Space Sciences
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    • v.45 no.11
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    • pp.932-938
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    • 2017
  • Particle-in-cell method which blends Eulerian grids and Lagrangian particle is utilized to solve simplified hall-effect thruster. Since this study individually tracks not only neutrons and ions but also electrons, message passing interface(mpi) scheme is adopted for parallel computer cluster. Helical movement of an electron cloud in constant magnetic field is validated comparing with an exact solution. A plasma in radial magnetic field and axial electric field in a reaction cylinder is established. Electrons do double helix movement and are well anchored in a cylinder. Ionization of neutrons by impact with high-speed electrons generates ion particles. They are accelerated by axial electric field, which forms a plume of a plasma-effect thruster.