• 한국진공학회지
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• 제7권s1호
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• pp.160-166
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• 1998

The field emission characteristics of defective diamond films grown by microwave plasma enhanced chemical vapor deposition (MPECVD) have been studied. X-ray diffraction, the poor crystal quality and/or small grain sizes of the diamond phase and the inclusion of the non-diamond carbon phases in these films have been condirmed by raman spectroscopy, scanning electron microscopy, atomic force microscopy, and the reflectance measurements. The degrees of the film defectiveness and the emission characteristics were dependent on the methane concentration. Current-versus-voltage measurements have demonstrated that the defective diamond films have good electron emission characteristics. characteristics strongly suggests the defect-related electron-emission mechanism. The defective diamond films deposited on Si substrates show the field emission current density of 1$\mu\textrm{A}/\textrm{cm}^2$ and 1mA/$\textrm{cm}^2$ have been measured at electric fields as low as 4.5V/$\mu\textrm{m}$ and 7.6V/$\mu\textrm{m}$, respectively. We also observed the similar emission characteristics from the defective diamond film deposited on Cr/Si substrate and could decrease the deposition temperature to $600^{\circ}C$.

• 한국진공학회지
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• 제7권s1호
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• pp.134-139
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• 1998

Amorphous fluorocarbon (a-C:F) is of interest for low dielectric interlayer material, but in this work we applied this material to FED field emitter. N-doped a-C:F films were deposited by inductively coupled plasma chemical vapor deposition (ICPCVD). The Raman spectra were measured to study the film structure and inter-band optical absorption coefficients were measured using Perkin-Elmer UV-VIS-IR spectrophotometer and optical band gap was obtained using Tauc's plot. XPS spectrum and AFM image were investigated to study bond structure and surface morphology. Current-electric field(I-E) characteristic of the film was measured for the characterization of electron emission properties. The optimum doping concentration was found to be [N2]/[CF4]=9% in the gas phase. The turn-on field and the emission current density at $[N_2]/[CF_4]$=9% were found to be 7.34V/$\mu\textrm{m}$ and 16 $\mu\textrm{A}/\textrm{cm}^2$ at 12.8V/$\mu\textrm{m}$, respectively.

• 한국정보디스플레이학회:학술대회논문집
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• 한국정보디스플레이학회 2007년도 7th International Meeting on Information Display 제7권1호
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• pp.486-489
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• 2007

Carbon nanotube (CNT) cathodes having a trench structure similar to the structure of the gated triodetype cathode were successfully fabricated by a screenprinting method with multi-walled carbon nanotubes. We observed that a liquid method not only readily removes the organic residues on the CNT films, but also satisfactorily protrudes the CNTs out of the electrode surface. The CNT cathodes prepared by the liquid method showed a turned-on field of $1.4\;V/{\mu}m$. The emission current density of them was about $3.1\;mA/cm^2$ at the electric field of $3\; V/{\mu}m$. The liquid method appears to be a promising surface treatment of CNT cathode for gated triode-type FEDs applications.

• 한국세라믹학회지
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• 제39권1호
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• pp.92-98
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• 2002

Pb(Zr$_{0.8}$Ti$_{0.2}$)O$_3$강유전체 음극의 상부 전극 크기를 변화시키며(500$mu extrm{m}$~900$\mu\textrm{m}$)비대칭 전극 구조에서의 전자 방출에 대하여 연구하였다. 펄스 전기장을 가했을 때 나타나는 분극 반전에 의한 전류 밀도는 상부 전극 크기를 감소시킴에 따라 증가하였다. 이것은 비대팅 전극 구조에 의해 강유전체 표면에서 stray-field가 발생하고, stray field가 전극의 모서리 부근의 강유전체 표면 하부에도 분극 반전을 발생시켰기 때문이다. 전기장 전산모사를 통하여 이러한 stay-field의 존재 가능성을 예측할 수 있었고, 분극 반전에 의한 전류 밀도 측정 결과 stray-field가 미치는 거리는 약 11-l4$\mu\textrm{m}$이었다. 전자방출의 문턱전계는 항전계 의 약 3배인 61-68kV/cm이었으며, 문턱전계가 단순히 강유전체의 항전계에 의해 결정되는 것이 아니라, 강유전 음극의 구조에 의해 결정되는 stray-field의 세기와 stray-field가 미치는 거리에 영향을 받음을 전산모사를 통해 예측할 수 있었다.

• 한국전기전자재료학회논문지
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• 제16권1호
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• pp.53-59
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• 2003

Using Platinum-silicide (PtSi) formed between silicon substrate and carbon film, we have improved the field emission of electrons from carbon films. Pt films were deposited on n-Si(100) substrates at room temperature by DC sputter technique. After deposition, these PtSi thin films were annealed at 400 ~ $600^{\circ}C$ in a vacuum chamber, and the carbon films were deposited on those Pt/Si substrates by laser ablation at room temperature. The field emission property of C/Pt/Si system is found to be better than that of C/Si system and it is showed that property was improved with increasing annealing temperature. The reasons why the field emission from carbon film was improved can be considered as follows, (1)the resistance of carbon films was decreased due to graphitization, (2)electric field concentration effectively occurred because the surface morphology of carbon film deposited on Pt/si substrates with rough surface, (3)it is showed that annealing induced reaction between Pt film and Si substrate, as a consequence that the interfacial resistance between Pt film and Si substrate was decreased.

• 한국진공학회지
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• 제9권2호
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• pp.122-129
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• 2000

Mo이 코팅된 유리기판 상에 전기영동법으로 도포된 유리화 비정형 탄소분말의 전계방출 특성을 조사하였다. 탄소의 $sp^2$결합만으로 이루어진 유리화 비정형 탄소는 전계방출을 얻기 위한 초기화 공정 없이도 규칙적인 전계방출 거동을 보이고 있었다. 전자의 방출이 시작되는 임계전장의 크기는 3에서 4 MV/m 구간의 값을 가지고 있었으며, Fowler-Nordheim plot로부터 평가된 effective work function은 약 0.06 eV였다. 전류전압거동의 반복측정에 의해 관찰된 바와 같이 전계방출의 안정성 면에서 유리화 비정형 탄소는 Si tip보다 우수하였으며, 도포된 전체면적에서 전면발광의 가능성을 확인할 수 있었다. 이러한 결과는 탄소계 물질에서 관찰되는 전계방출이 탄소의 $sp^3$결합과 밀접하게 관련되어 있지 않으며, 전자가음극물질의 표면으로 이동하는데 필요한 전기전도성, 혹은 기판과 음극물질 계면에서의 전자이동 등이 전계방출의 거동을 결정하는 중요한 요인임을 보여주고 있다.

• 반도체디스플레이기술학회지
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• 제17권4호
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• pp.6-10
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• 2018

Organic light emitting devices have attracted the attention of many people because of their high potential for self-emission and flexible display devices. However, due to limitations in device efficiency and lifetime, partial commercialization is underway. In this paper, we have investigated the electrical conduction mechanism of the organic light emitting device by the temperature and the thickness of the light emitting layer through the current - voltage characteristics with respect to the conduction mechanism directly affecting the efficiency and lifetime of the organic light emitting device. Through the study, it was found that the conduction in the low electric field region is caused by the movement of the heat excited charge in the ohmic region and the tunneling of the electric charge due to the high electric field in the high electric field region.

• International Journal of Automotive Technology
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• 제1권1호
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• pp.9-16
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• 2000

The growing concerns on environmental protection have been constantly demanding cleaner and more energy efficient vehicles without compromising any conveniences provided by the conventional vehicles. The recent significant advances in proton-exchange-membrane (PEM) fuel cell technology have shown the possibility of developing such vehicles powered by fuel cells. Several prototype fuel cell electric vehicles (FCEV) have been already developed by several major automotive manufactures, and all of the favorable features have been demonstrated in the public roads. FCEV is essentially a zero emission vehicle and allows to overcome the range limitation of the current battery electric vehicles. Being motivated by the laboratory and field demonstrations of the fuel cell technologies, variety of fuel cell alliances between fuel cell developers, automotive manufactures, petroleum companies and government agencies have been formed to expedite the realization of commercially viable FCEV. However, there still remain major issues that need to be overcome before it can be fully accepted by consumers. This paper describes the current fuel cell vehicle development status and the staggering challenges for the successful introduction of consumer acceptable FCEVS.

• 반도체디스플레이기술학회지
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• 제15권2호
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• pp.26-31
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• 2016

The Townsend to glow discharge mode transition was investigated in the dielectric barrier discharge (DBD) helium plasma source which was powered by 20 kHz / $4.5 kV_{rms}$ high voltage at atmospheric pressure. The spatial profile of the electric field strength at each modes was measured by using the intensity ratio method of two helium emission lines (667.8 nm ($3^1D{\rightarrow}2^1P$) and 728.1 nm ($3^1S{\rightarrow}2^1P$)) and the Stark effect. ICCD images were analyzed with consideration for the electric field property. The Townsend discharge (TD) mode at the initial stage of breakdown has the light emission region located in the vicinity of the anode. The electric field of the light emitting region is close to the applied field in the system. Immediately, the light emitting region moves to the cathode and the discharge transits to the glow discharge (GD) mode. This mode transition can be understood with the ionization wave propagation. The electric field of the emitting region of GD near cathode is higher than that of TD near anode because of the cathode fall formation. This observation may apply to designing a DBD process system and to analysis of the process treatment results.

• 전기학회논문지
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• 제61권7호
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• pp.1001-1006
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• 2012

This paper presents a carbon nanotube (CNT) triode-structure field emitter as an ion source in a micro time-of-flight mass spectrometer(TOF-MS). In the ion source by field emission, the electrons emitted from cathodes under an electric field accelerated to the anode and ionize gas molecules by impact before arriving the anode. The generated positive ions are to be accelerated to the ion collector. Whereas most of ions are drawn to the cathodes in diode field emitters, a grid in the triode field emitter prevents the ions from being drawn to the cathodes. The triode field emitter is fabricated by micromachining. The cathode is composed of six CNT cylinders. The total size of the fabricated device is $8.0{\times}7.3{\times}1.9mm^3$. The anode and the grid current of the fabricated CNT field emitter were measured for various anode and grid voltages. When the anode and the grid voltages are 1000 V and 990 V, respectively, the emission current passing through the ionization region is 8.6 ${\mu}A$, which is a sufficient emission current for ionization and mass spectrometry.