• Title/Summary/Keyword: Ar Gas

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Etch characteristics of ZnO thin films using an inductively coupled plasma ($BCl_3/Ar/Cl_2$ 유도결합 플라즈마를 이용한 ZnO 박막의 식각특성 연구)

  • Woo, Jong-Chang;Um, Doo-Seung;Yang, Xuel;Heo, Keyong-Moo;Park, Jung-Soo;Ha, Tae-Kyung;Wi, Jae-Hyung;Joo, Young-Hee;Kim, Dong-Pyo;Kim, Chang-Il
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2009.06a
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    • pp.135-136
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    • 2009
  • The etching characteristics of Zinc Oxide (ZnO) and etch selectivity of ZnO to $SiO_2$ in $BCl_3/Ar/Cl_2$ plasma were investigated. It was found that ZnO etch rate shows a non-monotonic behavior with increasing both Ar fraction in $BCl_3$ plasma, RF power, and gas pressure. The maximum ZnO etch rate of 53 nm/min was obtained for $BCl_3$(16 sccm)/Ar(4 sccm)/$Cl_2$(3 sccm) gas mixture. The chemical state of etched surfaces was investigated with X-ray photoelectron spectroscopy (XPS). From these data, the suggestions on the ZnO etch mechanism were made.

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Damage on the Surface of Zinc Oxide Thin Films Etched in Cl-based Gas Chemistry

  • Woo, Jong-Chang;Ha, Tae-Kyung;Li, Chen;Kim, Seung-Han;Park, Jung-Soo;Heo, Kyung-Mu;Kim, Chang-Il
    • Transactions on Electrical and Electronic Materials
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    • v.12 no.2
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    • pp.51-55
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    • 2011
  • We investigated the etching characteristics of zinc oxide (ZnO) thin films deposited by the atomic layer deposition method. The gases of the inductively coupled plasma chemistry consisted of $Cl_2$, Ar, and $O_2$. The maximum etch rate was 40.3 nm/min at a gas flow ratio of $Cl_2$/Ar=15:5 sccm, radio-frequency power of 600 W, bias power of 200 W, and process pressure of 2 Pa. We also investigated the plasma induced damage in the etched ZnO thin films using X-ray diffraction (XRD), atomic force microscopy and photoluminescence (PL). A highly oriented (100) peak was present in the XRD spectroscopy of the ZnO samples. The full width at half maximum value of the ZnO sample etched using the $O_2/Cl_2$/Ar chemistry was higher than that of the as-deposited sample. The roughness of the ZnO thin films increased from 1.91 nm to 2.45 nm after etching in the $O_2/Cl_2$/Ar plasma chemistry. Also, we obtained a strong band edge emission at 380 nm. The intensities of the peaks in the PL spectra from the samples etched in all of the chemistries were increased. However, there was no deep level emission.

Diagnosis of $BCl_3$ and $BCl_3$/Ar Plasmas with an Optical Emission Spectroscopy during High Density Planar Inductively Coupled Dry Etching (평판형 고밀도 유도결합 건식 식각시 Optical Emission Spectroscopy를 이용한 $BCl_3$$BCl_3$/Ar 플라즈마의 분석)

  • Cho, Guan-Sik;Wantae Lim;Inkyoo Baek;Seungryul Yoo;Park, Hojin;Lee, Jewon;Kuksan Cho;S. J. Pearton
    • Proceedings of the Materials Research Society of Korea Conference
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    • 2003.03a
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    • pp.88-88
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    • 2003
  • Optical Emission Spectroscopy(OES) is a very important technology for real-time monitoring of plasma in a reactor during dry etching process. OES technology is non-invasive to the plasma process. It can be used to collect information on excitation and recombination between electrons and ions in the plasma. It also helps easily diagnose plasma intensity and monitor end-point during plasma etch processing. We studied high density planar inductively coupled BCl$_3$ and BCl$_3$/Ar plasma with an OES as a function of processing pressure, RIE chuck power, ICP source power and gas composition. The scan range of wavelength used was from 400 nm to 1000 nm. It was found that OES peak Intensity was a strong function of ICP source power and processing pressure, while it was almost independent on RIE chuck power in BCl$_3$-based planar ICP processes. It was also worthwhile to note that increase of processing pressure reduced negatively self-induced dc bias. The case was reverse for RIE chuck power. ICP power and gas composition hardly had influence on do bias. We will report OES results of high density planar inductively coupled BCl$_3$ and BCl$_3$/Ar Plasma in detail in this presentation.

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The Effects of CF4 Partial Pressure on the Hydrophobic Thin Film Formation on Carbon Steel by Surface Treatment and Coating Method with Linear Microwave Ar/CH4/CF4 Plasma

  • Han, Moon-Ki;Cha, Ju-Hong;Lee, Ho-Jun;Chang, Cheol Jong;Jeon, Chang Yeop
    • Journal of Electrical Engineering and Technology
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    • v.12 no.5
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    • pp.2007-2013
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    • 2017
  • In order to give hydrophobic surface properties on carbon steel, the fluorinated amorphous carbon films were prepared by using linear 2.45GHz microwave PECVD device. Two different process approaches have been tested. One is direct deposition of a-C:H:F films using admixture of $Ar/CH_4/CF_4$ working gases and the other is surface treatment using $CF_4$ plasma after deposition of a-C:H film with $Ar/CH_4$ binary gas system. $Ar/CF_4$ plasma treated surface with high $CF_4$ gas ratio shows best hydrophobicity and durability of hydrophobicity. Nanometer scale surface roughness seems one of the most important factors for hydrophobicity within our experimental conditions. The properties of a-C:H:F films and $CF_4$ plasma treated a-C:H films were investigated in terms of surface roughness, hardness, microstructure, chemical bonding, atomic bonding structure between carbon and fluorine, adhesion and water contact angle by using atomic force microscopy (AFM), nano-indentation, Raman analysis and X-ray photoelectron spectroscopy (XPS).

The Effect of Substrate Pore Size on Gas Permeation Mechanism in Composite Membrane by Plasma Polymerization (플라즈마 중합된 고분자 복합막에서 기질의 기공크기가 기체투과 메카니즘에 미치는 영향)

  • Hyun, Sang-Won;Jung, Il-Hyun
    • Applied Chemistry for Engineering
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    • v.10 no.4
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    • pp.502-508
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    • 1999
  • We prepared non-porous membrane on the $Al_2O_3$ substrate with the different pore by the size by the plasma polymerization of $CHF_3$. We studied the permeability characteristics of membrane by Ar treatment and the effect of substrate pore size on gas permeation mechanism. The selectivity was increased with Ar plasma treatment time and rf-power near the substrate to the cathode while the permeability was decreased. It was observed that the solution-diffusion model would be applied to non-porous layers while it is applied Knudsen diffusion model to the substrate. From the experimental observation, it could be concluded that the pore size of $Al_2O_3$ membrane influenced on the permeability and the selectivity.

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A Study on the Surface of the Dry Etched TaN Thin Film by Adding The CH4 Gas in BCl3/Ar Inductively Coupled Plasma (BCl3/Ar 유도결합 플라즈마 안에 CH4 가스 첨가에 따른 건식 식각된 TaN 박막 표면의 연구)

  • Woo, Jong-Chang;Choi, Chang-Auck;Yang, Woo-Seok;Joo, Young-Hee;Kang, Pil-Seung;Chun, Yoon-Soo;Kim, Chang-Il
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.26 no.5
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    • pp.335-340
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    • 2013
  • In this study, the plasma etching of the TaN thin film with $CH_4/BCl_3/Ar$ gas chemistries was investigated. The etch rate of the TaN thin film and the etch selectivity of TaN to $SiO_2$ was studied as a function of the process parameters, including the amount of $CH_4$. X-ray photoelectron spectroscopy (XPS) and Field-emission scanning electron microscopy (FE-SEM) was used to investigate the chemical states of the surface of the TaN thin film.

Synthesis of SrGa2S4 Phosphor and Its Luminescent Properties (SrGa2S4 형광체의 합성과 발광 특성)

  • Heo, Yeong-Deok;Sim, Jae-Hun;Do, Yeong-Rak
    • Journal of the Korean Chemical Society
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    • v.46 no.2
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    • pp.164-168
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    • 2002
  • SrGa$_2$S$_4$ : Eu is a green emitting phosphor which is applied for field emission display, and cathodoluminescence. Conventionally, SrGa$_2$S$_4$ : Eu is synthesized by solid state reaction, in which a mixture of SrCO$_3$, Ga$_2$O$_3$, and Eu$_2$O$_3$ is fired at high temperatures under flowing H$_2$S and Ar gases. In this study,SrGa$_2$S$_4$ : Eu phosphor is synthesized by using a decomposition method, where SrS, Eu complex, and Ga com-plex are used. The advantage of this method is that toxic H$_2$S gas and Ar gas are not used. The synthetic con-ditions and luminescent properties of SrGa$_2$S$_4$ : Eu phosphor are also investigated.

Hydrophobic and Mechanical Characteristics of Hydrogenated Amorphous Carbon Films Synthesized by Linear Ar/CH4 Microwave Plasma

  • Han, Moon-Ki;Kim, Taehwan;Cha, Ju-Hong;Kim, Dong-Hyun;Lee, Hae June;Lee, Ho-Jun
    • Applied Science and Convergence Technology
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    • v.26 no.2
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    • pp.34-41
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    • 2017
  • A 2.45 GHz microwave plasma with linear antenna has been prepared for hydrophobic and wear-resistible surface coating of carbon steel. Wear-resistible properties are required for the surface protection of cutting tools and achieved by depositing a hydrogenated amorphous carbon film on steel surface through linear microwave plasma source that has $TE_{10}-TEM$ waveguide. Compared to the existing RF plasma source driven by 13.56 MHz, linear microwave plasma source can easily generate high density plasma and provide faster deposition rate and wider process windows. In this study, $Ar/CH_4$ gas mixtures are used for hydrogenated amorphous carbon film deposition. When microwave power of 1000 W is applied, 40 cm long uniform $Ar/CH_4$ plasma could be obtained in gas pressure of 200~400 mTorr. The Vickers hardness measurement of hydrogenated amorphous carbon film on steel surface was evaluated. It was found the optimized deposition condition at $Ar:CH_4=25:25$ sccm, 300 mTorr with microwave power of 1000W and RF bias power of 100W. By deposition of hydrogenated amorphous carbon film, contact angle on steel surfaces increases from $43.9^{\circ}$ to $93.2^{\circ}$.

Reduce of Etching Damage of PZT Thin Firms with Addition of Ar and O2 in Cl2/CF4 Plasma (Cl2/CF4 플라즈마에 Ar, O2 첨가에 따른 PZT 박막의 식각 손상 개선 효과)

  • 강명구;김경태;김창일
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.15 no.4
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    • pp.319-324
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    • 2002
  • In this study, the reduce of plasma etching damage in PZT thin film with addictive gas and re-annealing after etching have been investigated. The PZT thin films were etched as a function of $Cl_2/CF_4$ with addition of Ar and $O_2$ with inductively coupled plasma. The etch rates of PZT thin films were 1450 ${\AA}/min$ at 30% additive Ar and 1100 ${\AA}/min$ at 10% auditive $O_2$ into $Cl_2/CF_4$ gas mixing ratio of 8/2. In order to reduce plasma damage of PZT thin films after etching, the etched PZT thin films were re-annealed at various temperatures at $O_2$ atmosphere. From the hysteresis curries, the ferroelectric properties are improved by $O_2$ re-annealing process. The improvement of ferroelectric behavior at annealed PZT films is consistent wish the increase of the (100) and (200) PZT peaks revealed by x-ray diffraction (XRD). From x ray photoelectron spectroscopy (XPS) analysis, the intensity of Pb-O, Zr-O and Ti-O peak are increased and the chemical residue peak is reduced by $O_2$ re-annealing. The ferroelectric behavior consistent with the dielectric nature of $Ti_xO_y$ is recovered by $O_2$ recombination during rapid thermal annealing process.

Deposition of ZnO Thin Films by RF Magnetron Sputtering and Charcaterization of the ZnO thin film SAW filter (RF 마그네트론 스터터링에 의한 ZnO박막증착 및 SAW 필터 특성 분석)

  • Lee, Yong-Ui;Yang, Hyeong-Guk;Kim, Yeong-Jin;Han, Jeong-In;Kim, Hyeong-Jun
    • Korean Journal of Materials Research
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    • v.4 no.7
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    • pp.783-791
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    • 1994
  • Piezoelectric ZnO thin films were deposited on 7059 glass substrate by rf magnetron sputtering. The effects of deposition parameter, such as rf power, gas pressure and $O_{2}$/Ar gas ratio, on the crystallinity and electrical properties of the deposited ZnO thin films were studied. It was found that the deposition rate was higher than the previously reported values. ZnO films were suitable for SAW filter since a standard deviation of XRD (002) peak rocking curve was less than $6^{\circ}$. ZnO thin films, which were deposited at $O_{2}$/Ar ratio larger than 25%, showed high resistance. SAW filter was fabricated using ZnO film, of which thickness was 0.25 of the wavelength of the propatating surface acoustic wave. The measured frequency response was consistent with the calculated one. The SAW filter had center frequency 39.08 MHz, phase velocity 2501 m/sec and insertion loss 29 dB.

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