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Measurement of Thermal Properties at the Interface of Graphene and Bi2Te3 Substrate

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dc.contributor.advisor고승환-
dc.contributor.author편경록-
dc.date.accessioned2018-12-03T01:46:54Z-
dc.date.available2018-12-03T01:46:54Z-
dc.date.issued2018-08-
dc.identifier.other000000153084-
dc.identifier.urihttps://hdl.handle.net/10371/143969-
dc.description학위논문 (석사)-- 서울대학교 대학원 : 공과대학 기계항공공학부, 2018. 8. 고승환.-
dc.description.abstractGraphene, a two-dimensional hexagonal honey comb lattice, has been attracted tremendous attentions due its extremely high thermal and electrical, mechanical properties. Owing to these superior properties, there have been many attempts to exploit graphene to practical applications since it was discovered in 2004.Among many research area, thermoelectric field is known as one of the promising research field that graphene can be applied.

On the other hand, bismuth telluride (Bi2Te3) is one of the representative thermoelectric materials due to the high thermoelectric performance at the room temperature. For this reason, Bi2Te3has been already used in various research area and commercial devices, such as thermoelectric generator, peltier cooler.

Recently, a Graphene-Bi2Te3composite, synthesized in the thermoelectric field, has been experimentally proved to exhibit an enhanced thermoelectric performance. This is due to the reduced overall thermal conductivity at the composites. The additional phonon-scattering at the interface of graphene and Bi2Te3is thought to be a possible factor for this reduced thermal conductivity. However, the concrete mechanism why overall thermal conducivity of composites was ruduced is not fully understaned.

Generally, thermal properties at the interface of composite are believed to play an important role in the thermal transport in composite materials. Therefore, it is important to know thermal properties at the interface to understand thermal transport in the composite. In this paper, the thermal properties, particularly thermal contact conductance (Gc) and graphene thermal conductivity (kg),considered as important factors to the reduced thermal conductivity in the composite, were measured.

In many study pertaining to the supported graphene, they empolyed an optothermal Raman technique to measure thermal properties of supported graphene. One of the major difficulties of the optothermal Raman technique for supported graphene is how to obtain the absorptivity of graphene and the substrate. For many studies, the absorptivity of suspended graphene was equally used as the absorptivity of supported graphene. However, absorption value can be changed depending on the type of substrate like semi-conductor or conductor. This is because the electric field inside the material can be changed and influence on the absoprtion values of sample. Therefore, the absorption values should be estimated exactly for the supported graphene. We estimated absorptivities using the Fresnels equation from the refractive index of each matrial. This obtained absoprtion values were used in our experiment.

In short, measusring thermal contact conductance between graphene and Bi2Te3andthermal conductivity, we expected that these result values would be applied to further reasearch in designingoptimizinggraphene-Bi2Te3compositesand optimizing its performance.
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dc.description.tableofcontentsChapter 1. Introduction 1

1.1 Backgrounds 1

1.2 Review of previous studies about thermal properties of 2D materials 4

1.2.1 Previous method for thermal properties of 2D materials 4

1.2.2 Measurement thermal properties of 2D materials using a Raman Spectroscopy 4

1.3 Overview 5

Chapter 2. Sample preparation and Characterization 7

2.1 Synthesis of graphene 7

2.1.1 CVD system 7

2.1.2 CVD synthesis of graphene 8

2.2 Synthesis of bismuth telluride 9

2.2.1 Bridgman synthesis of bismuth telluride 9

2.3 Graphene transfer to the bismuth telluride substrate 11

2.4 Vacuum annealing 11

2.5 Characterization 12

2.5.1 Scanning electron microscopy (SEM) 13

2.5.2 Raman spectroscopy 13

2.5.3 Raman mapping 14

2.5.4 Optical microscopy 15

2.6 Conclusion 16

Chapter 3.Experimental method 24

3.1 Introduction 24

3.2 Opto-thermal Raman techniquewith two different objectives 25

3.2.1 Raman thermometry 26

3.2.2 Numerical calculation 27

3.3 Absorption value of supported graphene and Bi2Te3substrate 30

3.4 Conclusion 32

Chapter 4. Results and Discussion 38

4.1 Introduction 38

4.2 Position of Raman 2D peak depending on temperature 38

4.2.1 Temperature of graphene during the calibration 39

4.2.2 Temperature coefficient of Raman 2D peak 40

4.3 Position of Raman 2D peak depending on laser power 40

4.4 Result of the opto-thermal Raman technique 41

4.5 Repeatability and accuracy of the method 42

4.6 Combination of objectives 44

4.7 Limitation of laser power 45

4.8 Conclusion 45

Chapter 5. Summary and Conclusions 54

References 57

Appendix MATLAB codesfor numerical calculations 66

Abstract (in Korean) 78
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dc.formatapplication/pdf-
dc.format.mediumapplication/pdf-
dc.language.isoen-
dc.publisher서울대학교 대학원-
dc.subject.ddc621-
dc.titleMeasurement of Thermal Properties at the Interface of Graphene and Bi2Te3 Substrate-
dc.typeThesis-
dc.description.degreeMaster-
dc.contributor.affiliation공과대학 기계항공공학부-
dc.date.awarded2018-08-
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