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Thermal Conductivity Reduction of Polycrystalline CVD Graphene by Grain Boundary and Hole Defect : 결정 경계와 구멍 결함에 의한 다결정 CVD 그래핀의 열전도도 감소

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dc.contributor.advisor고승환-
dc.contributor.author이우민-
dc.date.accessioned2018-11-12T01:01:14Z-
dc.date.available2018-11-12T01:01:14Z-
dc.date.issued2018-08-
dc.identifier.other000000152251-
dc.identifier.urihttps://hdl.handle.net/10371/143314-
dc.description학위논문 (박사)-- 서울대학교 대학원 : 공과대학 기계항공공학부, 2018. 8. 고승환.-
dc.description.abstractGraphene, a two-dimensional material consisting of carbon atoms, has attracted great interest due to its novel physical properties, such as high electrical mobility, optical transparency, and superior mechanical strength. Especially, graphene has exceptionally outstanding thermal properties owing to long mean free path of phonon in two-dimensional lattices. The extraordinarily high thermal conductivity of graphene can be remarkably reduced by some defects, such as grain boundary, vacancy, and foreign atom. Therefore, Grain boundary effects on thermal transport in CVD grown graphene that has many grain boundaries should be investigated.

In this study, graphene samples with different grain sizes were synthesized by chemical vapor deposition (CVD) system to investigate the grain boundary effect on thermal transport in polycrystalline graphene. Manipulation of the CVD synthesis conditions allowed for synthesis of polycrystalline single-layered graphene with controlled grain sizes. Thermal conductivities of 3 graphene with different grain sizes were measured by the optothermal Raman technique, using the temperature-dependent 2D peak shift in Raman spectra. At first, the optical absorption was measured to define the absorbed power of defected graphene by Raman laser irradiation. Then, the temperature coefficient of Raman 2D peak positions and 2D peak shifts as the absorbed power were measured. Finally, thermal conductivities of defected graphene were obtained by solving the heat diffusion equation where experimental data were used. Furthermore, the effect of air convection losses and the hole edge temperature of suspended graphene were analyzed by numerically solving the full energy balance. Thermal conductivities of the single-crystal graphene as temperature were estimated by extrapolation/fitting of the experimental data. And the temperature discrepancies between the measured temperature from G peak and 2D peak shifts were compared to confirm noneuqilibrium phonons.

Although defects in graphene have a detrimental effect on thermal conductivity of graphene, the thermal conductivity suppression of graphene by defects can be useful for various applications. For the quantitative study of thermal conductivity of graphene as defects concentrations and for the more effective thermal conductivity suppressions, thermal conductivity reductions of holey graphene (HG) as porosity were measured by optothermal Raman method. HG samples were obtained by focused ion beam (FIB) processing for the study. The hole defects were precisely fabricated and controlled by direct FIB milling which does not require any masking or post processing. After graphene samples were transferred on the substrate by PMMA, all samples were characterized by diverse technique (e.g. Raman spectroscopy, SEM, optical microscope) Finally, the measured thermal conductivity reductions of holey graphene as porosity were compared to other reference experimental data and calculation results.
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dc.description.tableofcontentsChapter 1. Introduction 1

1.1 Background 1

1.2 Review of previous studies 2

1.2.1 Polycrystalline CVD Graphene 2

1.2.2 Holey Graphene with Hole-Shaped Defects 3

1.2.3 Thermal conductivity measurement of graphene 4

1.3 Objective of the present study 6

Chapter 2. Grain Size Effects on k of Polycrystalline Graphene 13

2.1 Introduction 13

2.2 Sample preparation 14

2.2.1 Control of the grain sizes of polycrystalline graphene 14

2.2.2 Graphene transfer (the suspended graphene) 16

2.3 Characterization 18

2.3.1 Scanning electron microscopy (SEM) 18

2.3.2 Optical microscopy 19

2.3.3 Definition of grain sizes 20

2.3.4 Raman spectroscopy 20

2.4 k measurements of polycrystalline graphene 22

2.4.1 Heat diffusion equation 23

2.4.2 Optical absorption of graphene 24

2.4.3 The correlation between 2D peak positions and temperature 26

2.4.4 The temperature rises as the absorbed laser power 27

2.4.5 Grain size dependent k of polycrystalline graphene 27

2.5 Analysis of experimental results 30

2.5.1 Uncertainty of k measurements 31

2.5.2 Hole edge temperature of suspended graphene 32

2.5.3 The effect of air convection losses 34

2.5.4 Thermal conductivity of the single-crystal graphene 36

2.5.5 Temperature discrepancies by nonequilibrium of phonons 40

2.6 Conclusion 41

Chapter 3. k Reductions of Holey Graphene as Hole-Defect Porosity 68

3.1 Introduction 68

3.2 Sample preparation 69

3.2.1 Graphene transfer (the supported graphene) 69

3.2.2 Fabrication of hole defects in graphene 69

3.3 Characterization 72

3.3.1 Scanning electron microscopy (SEM) 72

3.3.2 Optical microscopy 73

3.3.4 Definition of porosity 73

3.3.5 Raman spectroscopy 74

3.4 k measurements of holey graphene 74

3.4.1 Heat diffusion equation 75

3.4.2 Optical absorption of graphene 76

3.4.3 The correlation between 2D peak positions and temperature 77

3.4.4 The temperature rises as the absorbed laser power 78

3.4.5 k reductions of holey graphene as porosity 78

3.5 Conclusion 81

Chapter 4. Summary and Conclusions 97

References 100

Abstract (in Korean) 111
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dc.language.isoen-
dc.publisher서울대학교 대학원-
dc.subject.ddc621-
dc.titleThermal Conductivity Reduction of Polycrystalline CVD Graphene by Grain Boundary and Hole Defect-
dc.title.alternative결정 경계와 구멍 결함에 의한 다결정 CVD 그래핀의 열전도도 감소-
dc.typeThesis-
dc.contributor.AlternativeAuthorWoomin Lee-
dc.description.degreeDoctor-
dc.contributor.affiliation공과대학 기계항공공학부-
dc.date.awarded2018-08-
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