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The Regulation of VO2 Transition Temperature through Oxygen and Hydrogen Atom Control
| DC Field | Value | Language |
|---|---|---|
| dc.contributor.advisor | Hyungtak Seo | - |
| dc.contributor.author | 고민환 | - |
| dc.date.accessioned | 2019-04-01T16:41:16Z | - |
| dc.date.available | 2019-04-01T16:41:16Z | - |
| dc.date.issued | 2019-02 | - |
| dc.identifier.other | 28585 | - |
| dc.identifier.uri | https://dspace.ajou.ac.kr/handle/2018.oak/15041 | - |
| dc.description | 학위논문(석사)--아주대학교 일반대학원 :에너지시스템학과,2019. 2 | - |
| dc.description.tableofcontents | III. INTRODUCTION 1 A. THE NEED FOR NEXT-GENERATION SEMICONDUCTOR MATERIAL RESEARCH 1 B. BACKGROUND 5 1. Vanadium oxide 5 2. Vanadium dioxide (VO2) 8 3. VO2 Metal-Insulator Transition 10 4. VO2 Nanobeam 12 5. Synthesis of VO2 Nanobeam 14 IV. EXPERIMENTAL DETAIL 16 A. VTC DEPOSITION OF VO2 NANOBEAM 16 1. Substrate preparation 16 2. Source powder preparation 16 3. Thermal CVD condition 18 B. DIRECT DEPOSITION OF VO2 NANOBEAM 20 1. Substrate preparation 20 2. V2O5 Solution preparation 20 3. Spin coating 21 4. Thermal CVD condition 21 C. ELECTRODE FORMATION 22 D. PLASMA DOPING 22 E. OPTICAL MICROSCOPE (OM) 24 F. IMAGEJ SOFTWARE 24 G. X-RAY DIFFRACTOMETER (XRD) 24 H. SCANNING ELECTRON MICROSCOPE (SEM) 24 I. RAMAN SPECTROSCOPY 25 J. TUNNELING ELECTRON MICROSCOPE (TEM) 25 K. X-RAY PHOTOELECTRON SPECTROSCOPY (XPS) 26 L. MEASUREMENT OF ELECTRICAL CHARACTERS 26 M. SECONDARY ION MASS SPECTROMETRY (SIMS) 27 V. RESULT AND DISCUSSION 28 A. OXYGEN REGULATION 28 1. Morphology of VO2 nanobeams 28 2. Room temperature phase of VO2 nanobeam 33 3. MIT temperature of VO2 nanobeams 37 4. Realization of Ti-less VO2 nanobeams 42 5. Surface and bulk analysis of VO2 nanobeams 47 B. HYDROGEN REGULATION 50 1. Effect of Plasma Time on VO2 nanobeams 51 2. Effect of Plasma Power on VO2 nanobeams 54 C. VO2 BEAM GROWTH OPTIMIZATION 57 1. Problem recognition of VTC method 57 2. Effect of solution concentration on formation of VO2 nanobeam 61 3. Characterization of VO2 Nanobeam on SiO2 via DD method 64 VI. CONCLUSION 67 VII. REFERENCE 69 | - |
| dc.language.iso | eng | - |
| dc.publisher | The Graduate School, Ajou University | - |
| dc.rights | 아주대학교 논문은 저작권에 의해 보호받습니다. | - |
| dc.title | The Regulation of VO2 Transition Temperature through Oxygen and Hydrogen Atom Control | - |
| dc.title.alternative | Minhwan Ko | - |
| dc.type | Thesis | - |
| dc.contributor.affiliation | 아주대학교 일반대학원 | - |
| dc.contributor.alternativeName | Minhwan Ko | - |
| dc.contributor.department | 일반대학원 에너지시스템학과 | - |
| dc.date.awarded | 2019. 2 | - |
| dc.description.degree | Master | - |
| dc.identifier.localId | 905316 | - |
| dc.identifier.uci | I804:41038-000000028585 | - |
| dc.identifier.url | http://dcoll.ajou.ac.kr:9080/dcollection/common/orgView/000000028585 | - |
| dc.description.alternativeAbstract | Vanadium dioxide (VO2) is a typical Mott material having a metal-semiconductor transition at 341K, and many researches have been made because it can be used as a selector or transistor of next-generation memory. However, since the transition temperature is close to room temperature, switching reliability is low at the high temperature (i.e., > 341K) at which the device can easily reach during circuit operation so that desired characteristics cannot be obtained. To overcome this technical barrier, various studies have been conducted on the control of transition temperature in VO2 through impurity doping. The recent studies have been conducted using various elemental dopants such as W, Cr, Y, and Ti. However, studies on transition temperature changes through doping in thin film have some limitation that transition temperature varies according to the condition of thin film. In this study, we attempted to achieve a reliable transition temperature control in VO2. A VO2 nanobeam was synthesized by using VTC as a source of powder mixed with V2O5 and TiO2, and the ratio of TiO2 to V2O5 of the source powder was 0, 2, 4, 5, 10 at% Respectively. In addition, to solve the problem of the VTC method, the new VO2 nanobeam method of the DD method was devised and optimized. Then, the VO2 nanobeam fabricated using the DD method was doped with hydrogen using RIE plasma. The VO2 nanobeam formed through VTC and DD method identified the rectangular nanobeam shape through an optical microscope (OM) and the scanning electron microscope (SEM). The X-ray diffraction (XRD), transmission electron microscope (TEM), Energy-dispersive X-ray spectroscopy (EDS) and Secondary-ion mass spectrometry (SIMS) show that the phase and composition of the nanobeam are VO2 monoclinic. Finally, gold electrodes were deposited on both ends of the nanobeam to confirm the electrical characteristics and the transition temperature. It was confirmed that the transition temperature increased constantly as the Ti ratio of the source increased, reached the maximum value at 5 at%, and then decreased again. Since V 2p XPS spectra revealed the oxidation of V oxidation state, Ti precursor played a role in O supplier from surface V-O bonds as forming volatile Ti-O species. Therefore, this result implies that Ti reactants can be used as VO2 nanobeam surface chemical modifier to manipulate MIT transition temperature as maintaining homogenous VO2 phase, which is very useful for Mott device application. The distance dependence problem of the VTC method is solved by the DD method, and the VO2 nanobeam synthesized by the DD method is the same phase structure as the VO2 nanobeam synthesized by the VTC method, but the transition temperature is slightly increased due to the substrate did. Furthermore, hydrogen-doped VO2 nanobeam has been shown to be able to control the conductivity level at room temperature by controlling plasma power and time. This means that the transition temperature can be effectively controlled through the use of plasma-doped hydrogen and oxygen doping using a Ti reactant to use VO2 as a Mott device. | - |
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