• Journal of the Korean Institute of Electrical and Electronic Material Engineers
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• v.18 no.1
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• pp.75-80
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• 2005

In this thesis, We Fabricated Cu thin films of 1000 $\AA$, 3000 $\AA$, and 6000 $\AA$ thickness on the single crystal sapphire, polycrystal alumina, and amorphous slide glass substrates deposited by electron beam evaporation(EBE) method. We investigated properties of resistivity and adhesion of these Cu thin films under various conditions, substrate temperature(room temperature, 10$0^{\circ}C$, 20$0^{\circ}C$ under vacuum) and annealing temperatures(400 $^{\circ}C$, 600 $^{\circ}C$ for 30 min after the deposition). We found that these adhesion was increased in order of slide glass, sapphire, and alumina. The adhesion of the Cu thin films on alumina was high value about 4 times, compared with that of the Cu thin films on slide glass. We found that these resistivities were decreased with increasing substrate temperature and thin film thickness. The resistivity(2.05 $\mu$Ω\ulcornercm) of the Cu thin films with 6000 $\AA$ thickness at 200 $^{\circ}C$ on the slide glass was low value, compared with that of aluminum(2.66 $\mu$Ω\ulcornercm).

• Journal of the Korean Vacuum Society
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• v.22 no.2
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• pp.98-104
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• 2013

$VO_2$ is an attractive thermochromic material, in which its electrical and optical properties can be switched by the structural phase-transition about $68^{\circ}C$. Recently, graphene is also a rising material which is researched as a transparent electrode because of its superior electrical and optical characteristics. In this respect, we try to fabricate the hybridized films using $VO_2$ and graphene on transparent sapphire substrate and then we investigate a structure and characterize an optical property for the samples as a function of temperature. According to the result of IR-transmittance analysis of $VO_2$ films as a function of temperature, the graphene-supported sapphire substrates are better about 10% than the bare sapphire substrates. The mean phase transition temperatures are also decreased as the number of graphene-layers increased and the hysteresis of phase transitions are narrowed.

• Journal of the Korean Crystal Growth and Crystal Technology
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• v.26 no.3
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• pp.89-94
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• 2016

In this study, the crystalline property of a-plane GaN epitaxial layer grown on r-plane sapphire by a HVPE method has been investigated according to the V/III ratio and the growth time of multi-step growth. Furthermore, these results were compared with the previous result obtained from the single-step growth of a-plane GaN on r-plane sapphire substrate. In the multi-step growth for a-plane GaN epitaxial layer on r-plane sapphire, the FWHM values of rocking curve in GaN epitaxial layer were decreased as the HCl source flow rate and the growth time were increased. The void formed in epitaxial layer was continuously decreased as the growth time in first step and second step using a higher HCl flow rate was increased. As a result, the GaN layer obtained with the longest growth time on the first step and second step exhibited the lowest FWHM values of 584 arcsec and the smallest dependence of azimuth angle.

• Proceedings of the Korea Association of Crystal Growth Conference
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• 1997.06a
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• pp.247-251
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• 1997

GaN films were grown on three differently oriented sapphire substates; (0001), (11-20), and (1-20). GaN films on the (0001) and (11-20) substates have a haxagonal structure and their growth rate was 0.6 $\mu\textrm{m}$/hr in both case. The film on the (1-102) substrate was too thin to identify its crystalline state. Growth rate was about the half of the others. Substrate orientation is one of the factor determining growth rate. The adhesion between GaN film and alumina substrate seems to be very good judging from the fractography.

• Journal of the Korean Ceramic Society
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• v.46 no.6
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• pp.673-678
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• 2009

The effect of MgO buffer layer on the structural properties of sputter-grown ZnO thin film was investigated. Sapphire (0001) and Si (100) substrate were used for the growth and MgO buffer layer was inserted between ZnO thin film and the substrate. X-ray diffraction pattern indicated that enhanced crystallinity in the ZnO thin film grown was achieved by inserting very thin MgO buffer layer, regardless of the substrate type. The strain in the ZnO thin film could also be controlled by the insertion of the MgO buffer layer, and tendency of the strain was strongly dependent on the substrate type.

• 한국초전도학회:학술대회논문집
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• v.10
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• pp.155-159
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• 2000

YBCO step-edge dc SQUID magnetometers on sapphire substrates have been fabricated. CeO2 buffer layer and YBCO films were deposited in situ on the low angle (${\sim}$35$^{\circ}$) steps formed on the sapphire substrates. Typical 5-${\mu}$m-wide junction has R$_n$ of 5 ${\omega}$ and I$_c$ of 50 ${\mu}$A with large I$_c$R$_n$ product of 250 ${\mu}$V at 77K. According to applied bias current, depth of voltage modulation was changed and maximum voltage was measured 16 ${\mu}$V. Field noise of do SQUID was measured 100${\sim}$300 fT/${\surd}^{Hz}$ in the 1 $^{kHz}$, and about 1.5 pT/${\surd}^{Hz}$ in the 1/f region. For ac bias reversal method, field noise was decreased in the 1/f region. The QRS peak of magnetocardiogram was measured 50 pT in the magnetically shielded room.

• Progress in Superconductivity
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• v.1 no.2
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• pp.146-150
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• 2000

Step edge Josephson junctions in c-axis oriented $YBa_2Cu_3O_7$ films were fabricated on $CeO_2$ buffered sapphire substrates. The step angle was controlled in the wide range of $20^{\circ}\sim75^{\circ}$ by the Ar ion milling technique. I-V curves of junction fabricated on the thickness ratio of $\sim$0.8 and the step angle of $35^{\circ}$ were exhibited RSJ-like behavior with $I_CR_N$ product of $\sim250{\mu}A$ and critical current density of $\sim2\times10^4A/cm^2$ at 77 K. Critical current of step edge junction was increased linearly with decreasing temperature but the normal resistance was almost constant. Total samples of step edge Josephson junction was satisfied a scaling behavior of $I_CR_N{\propto}(J_C)^{0.5}$.

• Proceedings of the Korean Vacuum Society Conference
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• 2011.02a
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• pp.51-51
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• 2011

We have grown nanocrystalline graphite on sapphire substrate by using solid carbon source molecular beam epitaxy. Changes of structure from amorphous carbon to nanocrystalline graphite controlled by the growth temperature have been investigated by Raman spectroscopy. Raman spectra show D, G, and 2D peaks, whose intensities vary on the growth temperature. Atomic force microscopy reveals that the surface is very flat. Sapphire substrates of different cutting direction produce similar results. Simulations suggest that the interaction between carbon and oxygen causes disorders. Electrical transport measurements exhibit a Dirac-like peak, including a carrier type change by an external gate voltage bias.

• Korean Journal of Materials Research
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• v.7 no.6
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• pp.492-497
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• 1997

HVPE를 이용하여 sapphire기판 위에서 후막 GaN의 성장특성을 조사하였다. 성장온도가 100$0^{\circ}C$에서 110$0^{\circ}C$로 증가하여도 성장속도는 영향을 받지않고 50-60$\mu\textrm{m}$/hr의 성장속도를 나타내었으나 표면특성과 결정성은 향상되었다. 110$0^{\circ}C$에서 성장된 후막 GaN는 DCXRD측정결과 451arcsec의 반티폭을 나타내었으며, PL측정결과 10K에서 19meV의 반치폭을 나타내었다. Ga 공급원의 온도가 93$0^{\circ}C$에서 77$0^{\circ}C$로 감소하여도 성장속도는 영향을 받지 않았으나, 77$0^{\circ}C$의 온도에서 GaN의 결정성이 향상되었다. HCI의 양이 5sccm에서 20sccm으로 증가함에 따라 성장속도가 15$\mu\textrm{m}$/hr에서 60$\mu\textrm{m}$/hr으로 증가하였으며, 표면특성도 향상되었다.

• Korean Journal of Materials Research
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• v.29 no.1
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• pp.59-64
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• 2019

This study investigates the optical characteristics of InGaN multiple quantum wells(MQWs) light emitting diodes(LEDs) on planar sapphire substrates(PSSs), nano-sized PSS(NPSS) and micro-sized PSS(MPSS). We obtain the results as the patterning size of the sapphire substrates approach the nanometer scale: The light from the back side of the device increases and the total light extraction becomes larger than the MPSS- and planar-LEDs. The experiment is conducted by Monte Carlo ray-tracing, which is regarded as one of the most suitable ways to simulate light propagation in LEDs. The results show fine consistency between simulation and measurement of the samples with different sized patterned substrates. Notably, light from the back side becomes larger in the NPSS LEDs. We strongly propose that the increase in the light intensity of NPSS LEDs is due to an abnormal optical distribution, which indicates an increase of extraction probability through NPSS.