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論文名稱 Title |
特殊鉭鎢碳化物與石墨烯之脈衝雷射剝熔蝕合成與鑑定 Synthesis and characterization of special Ta/W carbides and graphene by pulsed laser ablation |
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系所名稱 Department |
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畢業學年期 Year, semester |
語文別 Language |
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學位類別 Degree |
頁數 Number of pages |
211 |
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研究生 Author |
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指導教授 Advisor |
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召集委員 Convenor |
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口試委員 Advisory Committee |
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口試日期 Date of Exam |
2017-04-28 |
繳交日期 Date of Submission |
2017-06-06 |
關鍵字 Keywords |
脈衝雷射剝熔蝕、奈米凝聚物、鉭-碳、鎢-碳、亂層石墨烯、晶向關係、聚炔烴 W-C, crystallographic relationship, polyyne, turbostratic graphene, Ta-C, nanocondensate, pulsed laser ablation |
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統計 Statistics |
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中文摘要 |
本研究利用脈衝雷射剝熔蝕靶材於真空中伴隨著基材上的碳或特殊的液態環境中,合成鉭-鎢-碳系統中不同型態的特殊耐火金屬碳化物以及石墨烯,並利用穿透式電子顯微鏡及光譜去做鑑定。 首先是在高能量密度下,於真空中對塊材TaC作脈衝雷射剝熔蝕合成碳化鉭凝聚物。穿透式電子顯微鏡觀察到的顆粒及奈米凝聚物,為有著相當程度的非化學劑量及缺陷之岩鹽結構TaC及六方Ta2C的複合物。TaC的顆粒有著良好發展的{001}、{011}、{111}面伴隨著聚簇所形成的{111}雙晶面。而Ta2C的顆粒則有(0001)、{1010}、{11-20}以及{1-101}的面。周圍的TaC及Ta2C奈米凝聚物則有著{022}TaC // {01-10}Ta2C、<100>TaC // <0001>Ta2C的晶向關係。而吸收光譜顯示雙峰的最小能隙值約3.8 eV及2.3 eV。 再來,於真空中脈衝雷射剝熔蝕鎢金屬靶材,合成出體心立方晶及其衍生物的鎢/碳化鎢凝聚物及顆粒。體心立方晶及序化體心斜方晶的碳化鎢顆粒周圍會被亂層石墨烯層所包圍。體心立方晶結構的鎢奈米凝聚物顯現出{110}及{112}的面以及對稱的[111](110)傾斜界面和非對稱的[111](-110)/(-23-1)傾斜界面。碳參雜的體心斜方晶結構的鎢奈米凝聚物則有{110}的雙晶/疊差、相稱超晶格、(011)[100]/(-101)[010]的特殊界面以及約30°{111}的扭轉界面。 接著,於真空中脈衝雷射剝熔蝕碳化鎢靶材,合成特殊形狀及面缺陷的WC及W2C奈米顆粒。最主要的β-W2C1-x顆粒顯現(0001)、{-1011}面及(0001)的疊差和 [2-1-10](0-113)的雙晶界面。次要的γ-WC1-x則有發展良好的{100}、{110}及{111}面,還有(1-11)的聚片變形雙晶。 此外,於TEOS溶液中脈衝雷射剝熔蝕鎢金屬靶材則主要產生γ-WC及次要的α-W及β-W。對比於先前由於承接基板上的碳過參雜,則形成有序體心斜方晶結構的鎢顆粒。 最後,於液態氮中利用不同能量的脈衝雷射剝熔蝕碳靶材,產生多層的石墨烯奈米緞帶及奈米板以及聚炔烴(polyyne),並利用X光/電子繞射及光譜去做鑑定。 |
Abstract |
This research deals with the synthesis and transmission electron microscopic (TEM) coupled with optical spectroscopic characterizations of some special carbides of refractory metals and graphene with various forms in Ta-W-C based system as fabricated by pulsed laser ablation (PLA) of bulk targets with optional supply of carbon from the substrate in vacuum or from a specific liquid environment. PLA of bulk TaC in vacuum under a peak power density of 1.3 x 1011 W/cm2 were used to fabricate tantalum carbide condensates. TEM observations indicated the resultant particulates and nanocondensates are composite of rocksalt type TaC and hexagonal Ta2C with a considerable extent of nonstoichiometry and defect clusters yet negligible turbostratic graphene. The TaC particulates have well-developed {001}, {011}, {111} faces with occasional twinned bicrystal following {111} twin plane due to coalescence event, whereas the Ta2C particulates have (0001), {10-10}, {11-20} and {1-101} faces but hardly twinned. The surrounding TaC and Ta2C nanocondensates were found to follow almost the crystallographic relationship {022}TaC//{01-10}Ta2C; <100>TaC//<0001>Ta2C which can be rationalized by their coalescence over the well-developed (100)TaC and (0001)Ta2C surface for further twisting toward an energy cusp with a fair coincidence site lattice. The TaC and Ta2C composite particulates/condensates have a bimodal minimum band gap of ~3.7 and ~2.3 eV for potential optoelectronic applications. PLA of bulk α-W target in vacuum under a peak power density of 1.3 x 1011 W/cm2 caused the bcc-type based/derived W/WC condensates/particulates with {110} preferred orientation. The WC particulates with body-centered cubic (B2) and ordered body-centered orthorhombic (OBCO)-type structures tended to be encapsulated/surrounded by turbostratic graphene lamellae rolls due to C uptake from the supporting carbon-coated collodion film. The bcc-type α-W nanocondensates showed ledged {110} and {112} faces for mutual coalescence as special interfaces such as symmetrical [111](-110) tilt boundary and asymmetrical [111](-110)/(-23-1) tilt boundary. The carbon doped body-centered orthorhombic (BCO)-type W nanocondensates have prevailed {110} twinning/faulting, commensurate superstructure and (011)[100]/(-101)[010] special interface as well as {111} ca. 30° twist boundary. As the carbon atoms progressively substitute for tungsten atoms for the composite W/WC condensates/particulates by the C-richer substrate, the minimum band gap decreases from 3.55 to 3.21 eV implying their potential optoelectronic and catalytic applications. PLA of bulk δ-WC in vacuum caused rapid solidification and condensation of tungsten mono- and semi-carbide nanoparticles having high-temperature primitive structures with specific shape and planar defects. The predominant β-type W2C1-x particulates with primitive hexagonal structure (P63/mmc) and hence forbidden (0001) reflection showed (0001), { 011} facets, (0001) fault and a coherent [2-1-10](0-113) twin boundary due to (0-113)-specific coalescence and/or a growth mechanism. The minor high-temperature stabilized γ-WC1-x particulates with rocksalt-type structure showed well-developed {100}, {110} and {111} facets and (1-11) polysynthetic deformation twinning. The nanocondensates ranging from 5 to 20 nm in size were made of β-W2C1-x, γ-WC1-x, and rare W3C (with bcc sublattice of C) all having point defect clusters when mediated by the 2-3 nm sized lamellar phase of amorphous carbon with W dopant. The occurrence of β-W2C1-x and γ-WC1-x rather than C-overdoped BCO-type W and OBCO-type WC indicates that such ordered superstructures can only occur by inward diffusion of C from substrate upon pulsed laser heating in vacuum as shown in previous part. Besides, PLA of bulk W in tetraethyl orthosilicate (TEOS) under free run mode vs vacuum under Q-switch mode were comparatively studied. The W-based nanoparticles less than 20 nm in size thus formed in the former process are mainly γ-WC and minor α-W (bcc) and β-W (simple cubic). By contrast, C-doped W particulates with OBCO structure were formed in the latter process due to carbon overdosage from the supporting substrate. This knowledge sheds light on the kinetic phase selection of the W-based materials in the C-Si-O-H environment for some engineering applications. Finally, multilayer graphene nanoribbons and nanoplates in flat appearance and a byproducts of polyyne molecules as formed by PLA of bulk graphite in liquid nitrogen (LN2) within a peak power density range of 1011 to 107 W/cm2 were characterized by X-ray/electron diffraction and optical spectroscopy. The nanoribbons have unusual in-plane corrugations ca. 5-10 nm periodicity parallel to the flat surface, whereas the nanoplates gave tangential orientation domain boundaries, i.e. glide and twisting stacking faults in terms of A/B sites wrong registration and 30° rotation, respectively of the basal layers. The nanoribbons tended to parallel align on the orthogonal nanoplates to form 90° tilt boundary with 2-D semicoherency constrained by the coherent [11] direction. The graphene nanoribbons/nanoplates with near visible absorbance and polyyne molecules (C2H2 up to C14H2) with multiple UV absorbance have potential bio-medical/optoelectronic applications. The formation mechanism of the graphene nanostructures and the H uptake of polyyne by the PLA process in LN2 are addressed. |
目次 Table of Contents |
論文審定書 i 誌謝 ii 中文摘要 iii Abstract v Contents ix List of Figures xiii List of Appendixes and Supplements xxii List of Tables xxiv Chapter 1 Research outline and background Chapter 2 Laser ablation synthesis of tantalum carbide particles with specific phase assemblage and special interface 2-1. Introduction 3 2-2. Experimental 6 2-2-1. PLA synthesis 6 2-3. Results 7 2-3-1. XRD 7 2-3-2. SEM 8 2-3-3. TEM-EDX 9 2-3-4. Raman and UV-visible spectra 12 2-4. Discussion 13 2-4-1. Laser parameters of the formation of condensates and particulates 13 2-4-2. Phase selection of tantalum carbide and excess carbon by PLA 15 2-4-3. Special interface of TaC1-x/Ta2C condensates 19 2-4-4. Implications 20 2-5. Conclusions 20 Chapter 3 Pulsed laser synthesis of carbon-overdoped tungsten with a body-centered orthorhombic structure and planar defects 3-1. Introduction 41 3-2. Experimental 45 3-2-1. PLA synthesis 45 3-3-2. Characterization techniques 45 3-3. Results 46 3-3-1. XRD 46 3-3-2. TEM-EDX 48 3-3-2-1. Rapidly solidified particulates 48 3-3-2-2. Condensed nanpparticles 51 3-3-3. Raman probe 53 3-3-4. UV-visible absorbance 54 3-4. Discussion 54 3-4-1. Phase selection of W-C system by the PLA process 54 3-4-2. {110} shuffled superstructures of BCO- and/or OBCO-W nanocondensates 57 4-4-3. Surface and special grain boundaries with fair CSL 58 3-4-4. Engineering Implications 61 3-5. Conclusions 62 Chapter 4 High-temperature primitive tungsten mono/semicarbides with special defects by pulsed laser ablation of bulk WC in vacuum 4-1. Introduction 82 4-2. Experimental 84 4-2-1. PLA synthesis 84 4-2-2. Characterization techniques 85 4-3. Results 86 4-3-1. XRD 86 4-3-2. SEM 86 4-3-3. TEM 87 4-3-3-1. β-W2C1-x particulate 87 4-3-3-2. γ-WC1-x particulate 88 4-3-3-3. Nanocondensates with varied crystal structures 89 4-3-4. Raman spectroscopy and UV-visible absorbance 90 4-4. Discussion 91 4-4-1. Phase selection of W-C system by PLA of bulk δ-WC in vacuum 91 4-4-2. Causes of planar defects of γ-WC1-x and β-W2C1-x 93 4-4-3. Implications 96 4-5. Conclusions 96 Chapter 5 Pulsed laser synthesis of W-based particles C-Si-O-H environment 5-1. Introduction 115 5-2. Experimental 116 5-2-1. PLA synthesis 116 5-2-2. Characterization techniques 117 5-3 Results and discussions 118 5-3-1. PLA of W in TEOS 118 5-3-2. PLA of W in vacuum for particle deposition on a C-supporting substrate 120 5-4. Concluding remarks 120 Chapter 6 On the straight graphene nanoribbons/nanoplates with in-plane corrugations and special boundaries by pulsed laser ablation of graphite in liquid nitrogen 6-1. Introduction 127 6-2. Experimental 129 6-2-1. PLA synthesis 129 6-2-2. Characterization techniques 131 6-3. Results 132 6-3-1. XRD 132 6-3-2. TEM-EDX 133 6-3-2-1. PLA at a high peak power density in LN2 133 6-3-2-2. PLA at a relatively low peak power density in LN2 134 6-3-2-3. PLA at a high peak power density in vacuum 136 6-3-3. Raman spectra 136 6-3-4. UV-visible absorbance 137 6-3-5. XPS 138 6-4. Discussion 139 6-4-1. Rolling of turbostratic graphene with/without co-existing 3-D nanocrystal 139 6-4-2. Bonding configuration and formation mechanism of straight graphene nanoribbon with in-plane corrugations and strain 140 6-4-3. Translation (glide) and rotation (twist) stacking faults of graphene nanoplate 143 6-4-4. Implications 145 6-5. Conclusions 147 References 163 |
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