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Structure and Photoluminescence of ZnS - ZnSe Superlattices Grown by Hot Wall Epitaxy
최용대(Y. D. Choi),S. Sakakibara(S. Sakakibara),K. Ishino(K. Ishino),A. Ishida(A. Ishida),H. Fujiyasu(H. Fujiyasu) 한국진공학회(ASCT) 1994 Applied Science and Convergence Technology Vol.3 No.2
Hot wall epitaxy법에 의하여 GaAs(100)면 위에 ZnS-ZnSe 초격자를 성장하였다. ZnS-ZnSe 초격자의 주기는 x-선 회절 패턴에 의하여 확인되었고, 이것은 변형을 고려하여 계산된 이론적인 패턴과 비교되었다. 경계면에 평행한 ZnS와 ZnSe의 변형의 비는 ZnSe에 대하여 ZnS의 두께가 증가할수록 감소되었다. ZnS-ZnSe 초격자의 photoluminescence(PL)는 고에너지 영역의 예리한 스펙트럼과 저에너지 영역의 폭이 넓은 스펙트럼으로 구성되어 있다. PL의 광자 에너지는 Kronig-Penney 모델을 사용하여 계산된 이론적인 에너지 값과 비교한 결과 type I의 초격자임을 알았다. ZnS-ZnSe superlattices(SLs) were grown on the GaAs(100) by hot wall epitaxy. The period of ZnS-ZnSe SLs grown was confirmed by X-ray diffraction patterns, and compared with the theoretical pattern calculated considering the strain. It was calculated that the strain ratios of ZnS and ZnSe parallel to interfaces are decreased with increasing the ZnS thickness for ZnSe one. The photoluminescence(PL) of ZnS-ZnSe SLs consists of a sharp. line in the high energy region and of broad spectra in the lower energy region. The peak photon energy of ZnS-ZnSe PL was compared with the energy of the theoretical calculations using Kronig-Penney model, and ZnS-ZnSe SLs were considered to be type I.
Extension of the operational regime of the LHD towards a deuterium experiment
Takeiri, Y.,Morisaki, T.,Osakabe, M.,Yokoyama, M.,Sakakibara, S.,Takahashi, H.,Nakamura, Y.,Oishi, T.,Motojima, G.,Murakami, S.,Ito, K.,Ejiri, A.,Imagawa, S.,Inagaki, S.,Isobe, M.,Kubo, S.,Masamune, S IOP 2017 Nuclear fusion. Fusion nucléaire. &n.Illiga Vol.57 No.10
<P>As the finalization of a hydrogen experiment towards the deuterium phase, the exploration of the best performance of hydrogen plasma was intensively performed in the large helical device. High ion and electron temperatures, <I>T</I> <SUB>i</SUB> and <I>T</I> <SUB>e</SUB>, of more than 6 keV were simultaneously achieved by superimposing high-power electron cyclotron resonance heating onneutral beam injection (NBI) heated plasma. Although flattening of the ion temperature profile in the core region was observed during the discharges, one could avoid degradation by increasing the electron density. Another key parameter to present plasma performance is an averaged beta value <img ALIGN='MIDDLE' ALT='$\left\langle \beta \right\rangle $ ' SRC='http://ej.iop.org/images/0029-5515/57/10/102023/nfaa7fc2ieqn001.gif'/>. The high <img ALIGN='MIDDLE' ALT='$\left\langle \beta \right\rangle $ ' SRC='http://ej.iop.org/images/0029-5515/57/10/102023/nfaa7fc2ieqn002.gif'/> regime around 4% was extended to an order of magnitude lower than the earlier collisional regime. Impurity behaviour in hydrogen discharges with NBI heating was also classified with a wide range of edge plasma parameters. The existence of a no impurity accumulation regime, where the high performance plasma is maintained with high power heating >10 MW, was identified. Wide parameter scan experiments suggest that the toroidal rotation and the turbulence are the candidates for expelling impurities from the core region.</P>