• Title/Summary/Keyword: $Ga^+$ 이온

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A Study on Crystallographic and Mossbauer Spectroscopic Properties of Magnetic Oxide (산화물 자성체의 결정학적 및 뫼스바우어 분광학적 특성 연구)

  • Park, Seung-Han
    • Korean Journal of Materials Research
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    • v.9 no.7
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    • pp.701-706
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    • 1999
  • The crystal structure and magnetic properties of magnetic oxide system (F $e_2$ $O_3$)$_{5}$(A $l_2$ $O_3$)$_{4-x}$(G $a_2$ $O_3$)$_{x}$)SiO has been studied using X-ray diffraction and Mossbauer spectroscopy The changes of magnetic structure by the Ga ion substitution and the temperature variation have been investigated using Mossbauer spectroscopy, and the results are compared with those of the SQUIB measurements. Results of X-ray diffraction indicated that the crystal structures of the system change from a cubic spinel type to an orthorhombic via the intermediate region. This magnetic oxide system seems to be new kind of spinel type ferrites containing high concentration of cation vacancies. Various and complicated Mossbauer spectra were observed in the samples (x>0.2) at temperatures lower than room temperature. This result could be explained by freezing of the superparamagnetic dusters. On cooling and substitution, magnetic states of the system show various and multicritical properties. Unexpected dip in magnetization curves below 50K was observed in SQUID measurements. It was interpreted as an effect of spin canting including spin freezing or collective spin behavior.ior.r.

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Slow Positron Beam 기술에 의한 반도체 재료의 격자결함분석 연구현황

  • Lee, Jong-Ram
    • ETRI Journal
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    • v.10 no.1
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    • pp.64-75
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    • 1988
  • GaAs 등 화합물 반도체는 그 표면구조가 아직 확립되어 있지 않고, 표면조건이 소자특성에 큰 영향을 미친다. 소자공정중 이온주입 공정은 self-aligned MESFET(Metal Semiconductor Field Effect Transistor) 제작에 필수적인 기술이나, 이온 주입시 수 $\AA$ 크기의 vacancy 등 격자결함이 발생하며 이들 결함을 제어할 수 있는 기술이 필요하다. 에너지 가변 양전자 소멸기술은 표면에서 $1\mum$정도내에 존재하는 vacancy 형태의 격자결함을 감지해 낼 수 있으며 이들 격자결함의 depth profiling을 할 수 있는 기술이다. 본 고에서는 에너지 가변 양전자 소멸기술의 원리 및 최근 연구결과에 대해서 살펴보기로 한다.

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Analysis of z-axis direction of the ion saturation current to the pressure of the process gas in the ICP system (ICP system에서 공정가스와 압력에 따른 z축 방향의 이온포화 전류밀도 변화 분석)

  • Kim, Dong-Hun;Ju, Jeong-Hun;Kim, Seong-Bong
    • Proceedings of the Korean Institute of Surface Engineering Conference
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    • 2015.11a
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    • pp.280-280
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    • 2015
  • 플라즈마 진단법 중 내부에 삽입하여 측정하는 단일 랭뮤어 탐침법은 플라즈마 특성을 정확하게 측정할 수 있다. 탐침에 (-)극을 걸어서 들어오는 전류를 통해서 이온포화 전류밀도를 측정할 수 있다. 본 연구에서는 유도결합플라즈마에 흐르는 가스와 압력에 따라서 변화를 확인하였다. $H_2$, Ar, $CF_4$ gas로 10 mTorr, 70 mTorr, $CF_4$ 주입위치의 조건으로 플라즈마 밀도를 구하였다.

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Study on the Intrinsic Defects in Undoped GaSb Bulk and MBE-grown GaSb/SI-GaAs Epitaxial Layers for Infrared Photodetectors (적외선검출소자를 위한 GaSb 결정 및 MBE로 성장한 Gasb/SI-GaAs 박막의 진성결함에 관한 연구)

  • Kim, J.O.;Shin, H.W.;Choe, J.W.;Lee, S.J.;Noh, S.K.
    • Journal of the Korean Vacuum Society
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    • v.18 no.2
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    • pp.127-132
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    • 2009
  • We have investigated the intrinsic defects remaining in epitaxial GaSb layers grown on SI-GaAs substrates compared to those in bulk GaSb crystal substrate, which is a basic material of Sb-based strained-layer superlattice infrared photodetectors. From the functional dependence of the band-to-band transition energy of the photomuminescence (PL) spectra observing up to near room-temperature (250 K), the temperature parameters of [$E_o$, $\alpha$, $\beta$] of undoped GaSb crystal are determined by using the Varshni empirical equation describing the temperature variation of the bandgap energy. Additionally to the antisite-Ga ([$Ga_{Sb}$]) with an ionization energy of 29 meV that is well known to a major intrinsic defect in GaSb, epitaxial GaSb layers show a pair of deep states at the emission energy of 732/711 meV that may be related with a complex of two antisite-Ga and antisite-Sb ([$Ga_{Sb}-Sb_{Ga}$]). Based on the analysis of the temperature and the excitation-power dependences of PL, it suggests that excess-Sb substitutes Ga-site by self-diffusion and two anti sites of [$Ga_{Sb}$] and [$Sb_{Ga}$] could form as a complex of [$Ga_{Sb}-Sb_{Ga}$] in GaSb epilayers grown under Sb-rich condition.

Plasma characterization of a mesh separated dual plasma source by L-probe and QMS

  • Kim, Dong-Hun;Choe, Ji-Seong;Kim, Seong-Bong;Park, Sang-Jong;Ju, Jeong-Hun
    • Proceedings of the Korean Vacuum Society Conference
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    • 2015.08a
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    • pp.156.2-156.2
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    • 2015
  • 반도체 소자의 크기가 나노사이즈로 줄어들기 때문에, 건식식각의 중요성이 강조되고 있다. dual plasma source를 사용함으로써 plasma 밀도, 이온충돌에너지, 이온플럭스를 조절 가능하다. Low frequency로 이온에너지를 조절하고, high frequency로 이온플럭스를 일반적으로 조절한다. 본 연구는 inductively coupled plasma (ICP)와 capacitively coupled plasma (CCP)를 사용하는 dual plasma source이다. ICP는 AE RPS로 2.4 MHz를 사용하고, CCP는 AE RFX-600으로 13.56 MHz이다. single L-probe는 Hiden ESPion이고, quadrupole mass spectrometer (QMS)는 INFICON CPM-300이다. chuck에 CCP가 인가되고, ICP는 SUS mesh를 거쳐서 영향을 미친다. Gas는 Ar, Ar+CF4 두 조건에서 비료를 하였다. Single L-probe를 이용하여 플라즈마를 측정한 결과 CCP만 인가하였을 때, Te 2.05 eV, Ne 4.07E+10 #/cm3, Ni 5.82E+10 #/cm3의 결과를 얻을 수 있었다. ICP를 방전하고 mesh를 통해서 chuck으로 입사하는 이온을 측정한 결과 mesh에 의해 이온이 중성화되어 거의 입사하지 않음을 확인할 수 있었다. 최종적으로 이온의 영향이 상쇄되고, 라디칼의 영향이 증가하여 높은 etch rate와 선택비를 가지며, 등방성 식각의 영향이 커질 것으로 사료된다.

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Growth of GaAs/AlGaAs structure for photoelectric cathode (광전음극 소자용 GaAs/AlGaAs 구조의 LPE 성장)

  • Bae, Sung Geun;Jeon, Injun;Kim, Kyoung Hwa
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.27 no.6
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    • pp.282-288
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    • 2017
  • In this paper, GaAs/AlGaAs multi-layer structure was grown by liquid phase epitaxy with graphite sliding boat, which can be used as a device structure of a photocathode image sensor. The multi-layer structure was grown on an n-type GaAs substrate in the sequence as follows: GaAs buffer layer, Zn-doped p-type AlGaAs layer as etching stop layer, Zn-doped p-type GaAs layer, and Zn-doped p-type AlGaAs layer. The Characteristics of GaAs/AlGaAs structures were analyzed by using scanning electron microscope (SEM), secondary ion mass spectrometer (SIMS) and hall measurement. The SEM images shows that the p-AlGaAs/p-GaAs/p-AlGaAs multi-layer structure was grown with a mirror-like surface on a whole ($1.25mm{\times}25mm$) substrate. The Al composition in the AlGaAs layer was approximately 80 %. Also, it was confirmed that the free carrier concentration in the p-GaAs layer can be adjusted to the range of $8{\times}10^{18}/cm^2$ by hall measurement. In the result, it is expected that the p-AlGaAs/p-GaAs/p-AlGaAs multi-layer structure grown by the LPE can be used as a device structure of a photoelectric cathode image sensor.

이온 빔 스퍼터링 방법으로 제작한 Mo 박막의 특성조사

  • Jo, Sang-Hyeon;Kim, Hyo-Jin;Yun, Yeong-Mok;Lee, Seong-Ho
    • Proceedings of the Korean Vacuum Society Conference
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    • 2012.02a
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    • pp.304-304
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    • 2012
  • CIGS(CuInGaSe2) 태양전지의 후면전극(Back contact)으로 널리 사용되는 Mo 박막은 낮은 면저항, 높은 반사율, 광흡수층 Na-path 제공 등의 조건이 요구된다. 일반적으로 Mo 박막 제작은 DC 마그네트론 스퍼터링 방법이 가장 널리 사용되며, 제작조건에 따라 태양전지 효율에 강한 영향을 미치는 것으로 보고되고 있다. 본 연구에서는 DC 마그네트론 스퍼터링 시 기판에 이온빔(Ion-beam)을 동시 조사하는 이온 빔 스퍼터링 증착(Ion-beam sputter deposition)법으로 Mo 박막을 제작하였다. 제작된 박막의 전기적 및 광학적 특성은 4-point probe, UV-Vis-NIR spectrometer로 각각 조사하였으며 Na-path 제어를 위한 구조적 특성은 XRD, FE-SEM으로 분석하였다. 분석결과에 따르면 기존 DC 마그네트론 스퍼터링 방법보다 상대적으로 더 치밀한 구조와 높은 반사율을 가지는 박막이 제작됨을 알 수 있었다. Mo 박막의 최적조건은 DC power 300 W, Ion-gun power 50 W, Ar flow rate 20 sccm 였다.

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Optical Properties of Er-implanted GaN (Er 이온 주입된 GaN의 광학적 특성)

  • Son, Chang-Sik
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.18 no.12
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    • pp.1101-1105
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    • 2005
  • We have investigated the optical properties of Erbium (Er)-implanted GaN by photoluminescence (PL). Various doses of Er ion were implanted on GaN epilayers by ion implantation. Visible green emission lines due to inner 4f shell transitions for $Er^{3+}$ were observed from the PL spectrum of Er-implanted GaN. The emission spectrum consists of two narrow green lines at 537 and 558 nm. The green emission lines are identified as $Er^{3+}$ transitions from the $^{5}H_{11/2}$ and $^{4}S_{3/2}$ levels to the $^{4}I_{15/2}$ ground state. The stronger peaks in the case with the dose of $5{\times}10^{14}cm^{-2}$, together with the relatively higher intensity of the $Er^{3+}$ luminescence in the lower doped sample. It implies that some damage remains in the case with the dose of $1{\times}10^{16}cm^{-2}$. The peak positions of emission lines due to inner 4f shell transitions for $Er^{3+}$ do not change with increasing temperature. It indicates that $Er^{3+}$ related emission depends very little on the ambient temperature.

Reactive Ion Etching of InP, InGaAs and InAIAs by SiCl$_4$ and Cl$_2$ Gases: Effects of Gas Flow Rate, rf Power, Process Pressure and Ar Addition (SiCl$_4$와 Cl$_2$가스에 의한 InP, InGaAs 및 InAIAs의 반응성 이온 식각: 가스유량, rf 전력, 공정압력, Ar 첨가의 영향)

  • 유재수;송진동;배성주;정지훈;이용탁
    • Proceedings of the IEEK Conference
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    • 2001.06b
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    • pp.25-28
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    • 2001
  • In this paper, we have investigated the effects of gas flow rate, rf power, process pressure and Ar addition on reactive ion etching of InP, InGaAs and InAlAs using Sic14 and Cl$_2$ gases. The etch rates were measured by using a surface profiler. The etched profiles, sidewall roughness, and surface morphology were observed by scanning electron microscopy and by atomic force microscopy. The selective etching of InGaAs to InP and InAlAs was studied by varying the etching parameters. It was found that Cl$_2$ gas is more efficient for the selective etching of InGaAs to InAlAs than SiCl$_4$ gas. The etch selectivity of InGaAs to InAlAs is strongly dependent on the rf power and the process pressure.

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Impact ionization rate of the highly-doped AlGaAs/GaAs quantum well (고준위 도핑된 AlGaAs/GaAs 양자 우물의 충돌 이온화율)

  • 윤기정;황성범;송정근;홍창희
    • Journal of the Korean Institute of Telematics and Electronics A
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    • v.33A no.4
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    • pp.121-128
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    • 1996
  • The impact ionization rate of thethighly-doped AlGaAs/GaAs quantum well structure is calculated, which is an important parameter ot design theinfrared detector APD and the novel neural device. In conjunction with ensemble monte carlo method and quantum mechanical treatment, we analyze the effects of the parameters of quantum well structure on the impact ionization rate. Since the number of the occupied subbands increases while the energy of the subbands decreases as the width of quantum well increases, the impact ionization rate increases in the range of th esmall well width but gradually the increament slows down and is finally saturated. Due to the effect of the energy of the injected electrons into the quantum well and the tunneling through the barrier, the impact ionization rate increases for the range of the small barrier width and decreases for the range of the large barrier width. Thus, there exists a barrier width to maximize the impact ionzation rate for a mole fraction x, and the barrier width moves to the larger vaue as the mole fraction x increases. The impact ionization rate is much more sensitive to the variation of the doping density than that of the other quantum well parameters. We found that there is a limit of the doping density to confine the electronics in the quantum well effectively.

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