• Proceedings of the KIEE Conference
• /
• 2008.07a
• /
• pp.1218-1219
• /
• 2008

Thin films (< 30 nm) of titanium carbide (TiC) are coated on carbon nanotubes (CNTs), which are directly grown on nano-sized ($\sim$ 500 nm in diameter) conical-type tungsten (W) tips, by employing an inductively coupled plasma-chemical vapor deposition (ICP-CVD) technique. Any modification in structural properties (such as length to diameter ratio, crystal quality, and growth behavior) of CNTs due to TiC-coating has been monitored by using high-resolution TEM, field-emission SEM, and Raman spectroscopy. Driving voltage for obtaining the same level of emission current in CNTs-emitter is significantly reduced by TiC-coating. It is also worthy of being noted that the degradation of emission current due to prolonged operation (up to 30 h) is remarkably suppressed by TiC-coating.

• 한국정보디스플레이학회:학술대회논문집
• /
• 2002.08a
• /
• pp.1035-1038
• /
• 2002

The electrical properties of Porous polycrystalline silicon Nano-Structure (PNS) as a cold cathode were investigated as a function of anodizing condition, the thickness of Au film as a top electrode and the substrate temperature. Non-doped 2${\mu}m$-polycrystalline silicon was electrochemically anodized in HF: ethanol (=1:1) mixture as a function of the anodizing condition including a current density and anodizing time. After anodizing, the PNS was thermally oxidized for 1 hr at 900 $^{\circ}C$. Then, 20nm, 30nm, 45nm thickness of Au films as a top electrode were deposited by E-beam evaporator. Among the PNSs fabricated under the various kinds of anodizing conditions, the PNS anodized at a current density of 10mA/$cm^2$ for 20 sec has the lowest turn-on voltage and the highest emission current than those of others. Also, the electron emission properties were investigated as functions of measuring temperature and the different thickness of Au film as a top-electrode.

• Proceedings of the Korean Vacuum Society Conference
• /
• 2011.08a
• /
• pp.313-313
• /
• 2011

최근, 산화물 반도체를 통한 나노선 연구가 활발히 진행되고 있다. 1차원 나노선은 넓은 표면적을 가지며 다양한 특성을 지녀 미래 nanodevice로의 중요한 building block 소자로의 활용이 가능하다. 본 연구에서는 이종의 나노선을 합성하여 hierarchical nanojunction structure를 제작, 특성을 확인하였다. 이러한 구조는 나노선이 가지는 넓은 표면적의 특성과 동시에, multi-component fuctional nanodevice를 구현하는데에 적합한 구조이다. 본 연구는 텅스텐 기판 위에 고온의 열증착 방식을 이용하여 텅스텐 산화물 나노선을 제작시켜 그 위에 저온의 수열합성을 통한 산화아연 나노선을 제작한 후 향상된 field emission emitter로서의 특성을 살펴보았다. 합성된 텅스텐 산화물 나노선은 quasi-allign된 구조를 가지며, 이러한 구조 위에 ZnO를 스퍼터링하여 seed layer를 형성시키고, 암모니아수와 아연염을 이용한 수열합성법을 통하여 합성된 나노선 위에 nanobranch의 산화아연 나노선을 형성하였다. 이러한 성장특성은 SEM, TEM을 통하여 확인하였고 각각의 특성과 계면을 살펴보았다. 또한 이러한 구조를 이용하여 전계방출특성을 확인하였는데, 약 5.7 eV의 일함수를 갖는 텅스텐 산화물 나노선 위에 더 작은 값의 일함수를 갖는 산화아연 나노선을 합성하여 전계방출특성을 보았으며, 더 향상된 결과를 얻을 수 있었다. 또한 산화아연의 합성방법에 따른 전계방출 특성의 차이도 비교하였다.

• Proceedings of the Materials Research Society of Korea Conference
• /
• 2012.05a
• /
• pp.99.2-99.2
• /
• 2012

현재 양산 중인 대부분의 결정질 실리콘 태양전지는 p-type 실리콘 기판의 전면에 인 (phosphorus) 을 확산시켜 에미터로 사용한 스크린 프린티드 태양전지 (Screen Printed Solar Cells) 이다. 위 태양전지의 단점은 p-type 기판의 광열화현상 (Light Induced Degradation) 문제와 후면 알루미늄 금속 전극으로 인한 휨 현상 등이 있다. 이러한 단점을 해결하기 위해 n-type 기판의 전면에 보론 (Boron) 을 도핑하여 에미터로 사용하고, 후면 전계 (Back Surface Field) 로 인 (Phosphorus)을 도핑한 태양전지에 대한 연구가 활발히 진행 중이다. 본 연구에서는, 튜브 전기로 (tube furnace) 를 이용해 n-type 실리콘 웨이퍼 전면에 보론 도핑을 하고 이와 마찬가지로 웨이퍼 후면에 인 도핑을 실시하였다. 그리고 전면과 후면의 패시베이션을 위해 얇게 산화막을 형성한 후 실리콘 질화막 (SiNx) 을 증착하였다. 에미터와 후면 전계 그리고 패시베이션 층의 특성을 평가하기 위해 QSSPC (Quasi-Steady-State PhotoConductance) 로 소수반송자 수명 (Minority Carrier Lifetime) 과 포화 전류 (Saturation current) 값을 측정하였다.

• JSTS:Journal of Semiconductor Technology and Science
• /
• v.13 no.1
• /
• pp.1-7
• /
• 2013

In this paper, a biosensor based on a gated lateral bipolar junction transistor (BJT) is proposed. The gated lateral BJT can function as both a metal-oxide-semiconductor field-effect transistor (MOSFET) and a BJT. By using the self-assembled monolayer (SAM) method, the C-reactive protein antibodies were immobilized on the floating gate of the device as the sensing membrane. Through the experiments, the characteristics of the biosensor were analyzed in this study. According to the results, it is indicated that the gated lateral BJT device can be successfully applied as a biosensor. Additionally, we found that the sensitivity of the gated lateral BJT can be varied by adjusting the emitter (source) bias.

• Proceedings of the Korean Magnestics Society Conference
• /
• 2003.06a
• /
• pp.24-24
• /
• 2003

Metallic magnetoelectronic devices have studied intensively and extensively for last decade because of the scientific interest as well as great technological importance. Recently, the scientific activity in spintronics field is extending to the hybrid devices using ferromagnetic/semiconductor heterostructures and to new ferromagnetic semiconductor materials for future devices. In case of the hybrid device, conductivity mismatch problem for metal/semiconductor interface will be able to circumvent when the device operates in ballistic regime. In this respect, spin-valve transistor, first reported by Monsma, is based on spin dependent transport of hot electrons rather than electron near the Fermi energy. Although the spin-valve transistor showed large magnetocurrent ratio more than 300%, but low transfer ratio of the order of 10$\^$-5/ prevents the potential applications. In order to enhance the collector current, we have prepared magnetic tunneling transistor (MTT) with single ferromagnetic base on Si(100) collector by magnetron sputtering process. We have changed the resistance of tunneling emitter and the thickness of baser layer in the MTT structure to increase collector current. The high transfer ratio of 10$\^$-4/ range at bias voltage of more than 1.8 V, collector current of near l ${\mu}$A, and magnetocurrent ratio or 55% in Si-based MTT are obtained at 77K. These results suggest a promising candidate for future spintronic applications.

• Journal of the Korean Society for Nondestructive Testing
• /
• v.28 no.1
• /
• pp.16-24
• /
• 2008

Near-field scanning microwave microscope (NSMM) has been used to characterize the electromagnetic properties of samples based on a cavity perturbation technique. We used a NSMM using a waveguide cavity to couple a metallic probe tip as a point like evanescent field emitter. We explained the quality of our NSMM system by applying the cavity perturbation theory. First, to make a shape perturbation, we inserted linear and loop probes in the waveguide resonator. To check up electric and magnetic field distribution inside the waveguide resonator by shape perturbation, we confirmed the field distribution by using a HFSS simulation. Second, to make material perturbation, we located a dielectric sample in front of the probe tip and measured reflection coefficient $(S_{11})$. We found that the resonance frequency$(f_r)$ was changed linearly as the dielectric constant of resonator$({\varepsilon}_r)$ increased when ${\Delta}{\varepsilon}\;and\;{\Delta}{\mu}$ were small.

• Proceedings of the Korean Vacuum Society Conference
• /
• 2013.02a
• /
• pp.630-630
• /
• 2013

Recently, atomically smooth hexagonal boron nitride(h-BN) known as a white graphene has drawn great attention since the discovery of graphene. h-BN is a III-V compound and has a honeycomb structure very similar to graphene with smaller lattice mismatch. Because of strong covalent sp2bonds like graphene, h-BN provides a high thermal conductivity and mechanical strength as well as chemical stability of h-BN superior to graphene. While graphene has a high electrical conductivity, h-BN has a highly dielectric property as an insulator with optical band gap up to 6eV. Similar to the graphene, h-BN can be applied to a variety of field, such as gate dielectric layers/substrate, ultraviolet emitter, transparent membrane, and protective coatings. However, up until recently, obtaining and controlling good quality monolayer h-BN layers have been too difficult and challenging. In this work, we investigate the controlled synthesis of h-BN layers according to the growth condition, time, temperature, and gas partial pressure. h-BN is obtained by using chemical vapor deposition on Cu foil with ammonia borane (BH3NH3) as a source for h-BN. Scanning Transmission Electron Microscopy (STEM, JEOL-JEM-ARM200F) is used for imaging and structural analysis of h-BN layer. Sample's surface morphology is characterized by Field emission scanning electron microscopy (SEM, JEOL JSM-7100F). h-BN is analyzed by Raman spectroscopy (HORIBA, ARAMIS) and its topographic variations by Atomic force microscopy (AFM, Park Systems XE-100).

• Journal of the Korea Academia-Industrial cooperation Society
• /
• v.18 no.6
• /
• pp.567-575
• /
• 2017

The direction finder is an important device for an electronic support(ES) system because it is responsible for finding the direction of an emitter. The higher the accuracy of the direction finding, the higher the vitality of the weapon system with the ES system. Recently, the direction error occurred in the operating shipboard ES system when direction finding was performed for the signal with a pulse width of 200 ns. Therefore, this paper proposes, an improved method to reduce the direction error for shipboard ES systems. The proposed method was applied to the operating shipboard ES system and a field test was performed. The results of the field test showed that the direction error was reduced significantly for the signal with a pulse width of 200 ns.

• Proceedings of the Materials Research Society of Korea Conference
• /
• 2009.05a
• /
• pp.31.1-31.1
• /
• 2009

Carbon nanotubes (CNTs) are attractive material because of their superior electrical, mechanical, and chemical properties. Furthermore, their geometric features such as a large aspect ratio and a small radius of curvature at tip make them ideal for low-voltage field emission devices including backlight units of liquid crystal display, lighting lamps, X-ray source, microwave amplifiers, electron microscopes, etc. In field emission devices for display applications, the phosphor anode is positioned against the CNT emitters. In most case, light generated from the phosphor by electron bombardment passes through the anode front plate to reach observers. However, light is produced in a narrow depth of the surface of the phosphor layer because phosphor particles are big as much as several micrometers, which means that it is necessary to transmit through the phosphor layer. Hence, a drop of light intensity is unavoidable during this process. In this study, we fabricated a transparent cathode back plate by depositing an ultra-thin film of single walled CNTs (SWCNTs) on an indium tin oxide (ITO)-coated glass substrate. Two types of phosphor anode plates were employed to our transparent cathode back plate: One is an ITO glass substrate with a phosphor layer and the other is a Cr-coated glass substrate with phosphor layer. For the former case, light was radiated from both the front and the back sides, where luminance on the back was ~30% higher than that on the front in our experiments. For the other case, however, light was emitted only from the cathode back side as the Cr layer on the anode glass rolled as a reflecting mirror, improving the light luminance as much as ~60% compared with that on the front of one. This study seems to be discussed about the morphologies and field emission characteristics of CNT emitters according to the experimental parameters in fabricating the lamps emitting light on the both sides or only on the cathode back side. The experimental procedures are as follows. First, a CNT aqueous solution was prepared by ultrasonically dispersing purified SWCNTs in deionized water with sodium dodecyl sulfate (SDS). A milliliter or even several tens of micro-liters of CNT solution was deposited onto a porous alumina membrane through vacuum filtration. Thereafter, the alumina membrane was solvated with the 3 M NaOH solution and the floating CNT film was easily transferred to an ITO glass substrate. It is required for CNT film to make standing CNTs up to serve as electron emitter through an adhesive roller activation.