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1 | (10) |
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1 | (3) |
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4 | (4) |
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Future Prospects for NC-AFM |
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8 | (3) |
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10 | (1) |
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11 | (36) |
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11 | (9) |
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Relation to the Scanning Tunneling Microscope (STM) |
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11 | (4) |
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Atomic Force Microscope (AFM) |
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15 | (3) |
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18 | (2) |
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Scanning Speed, Signal Bandwidth and Noise |
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20 | (1) |
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The Four Additional Challenges Faced by AFM |
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20 | (2) |
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Jump-to-Contact and Other Instabilities |
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21 | (1) |
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Contribution of Long-Range Forces |
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21 | (1) |
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Noise in the Imaging Signal |
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22 | (1) |
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Non-Monotonic Imaging Signal |
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22 | (1) |
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Frequency-Modulation AFM (FM-AFM) |
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22 | (7) |
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22 | (4) |
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26 | (3) |
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Relation between Frequency Shift and Forces |
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29 | (5) |
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29 | (3) |
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Frequency Shift for a Typical Tip--Sample Force |
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32 | (1) |
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Calculation of the Tunneling Current for Oscillating Tips |
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33 | (1) |
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Noise in Frequency-Modulation AFM |
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34 | (5) |
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34 | (1) |
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Noise in the Frequency Measurement |
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34 | (4) |
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Optimal Amplitude for Minimal Vertical Noise |
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38 | (1) |
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A Novel Force Sensor Based on a Quartz Tuning Fork |
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39 | (2) |
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Quartz Versus Silicon as a Cantilever Material |
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39 | (1) |
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Benefits in Clamping One of the Beams (qPlus Configuration) |
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40 | (1) |
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41 | (6) |
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43 | (4) |
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47 | (32) |
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47 | (1) |
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Three-Dimensional Mapping of Atomic Force |
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48 | (4) |
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52 | (3) |
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Imaging Mechanisms for Si(100)2x1 and Si(100)2x1:H |
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55 | (3) |
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Surface Strain on an Atomic Scale |
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58 | (2) |
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Low Temperature Image of Si(100) Clean Surface |
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60 | (1) |
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Mechanical Control of Atom Position |
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61 | (4) |
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Atom Identification Using Covalent Bonding Force |
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65 | (3) |
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Charge Imaging with Atomic Resolution |
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68 | (6) |
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Mechanical Atom Manipulation |
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74 | (5) |
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76 | (3) |
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Bias Dependence of NC-AFM Images and Tunneling Current Variations on Semiconductor Surfaces |
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79 | (14) |
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79 | (1) |
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Bias Dependence of NC-AFM Images for Si(111)7x7 |
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80 | (8) |
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Mechanism of Inverted Atomic Corrugation |
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81 | (3) |
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NC-AFM Imaging and Tunneling Current |
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84 | (4) |
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NC-AFM Images for Ge/Si(111) |
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88 | (3) |
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91 | (2) |
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92 | (1) |
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93 | (16) |
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93 | (2) |
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93 | (1) |
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94 | (1) |
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Imaging of Single Crystals |
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95 | (3) |
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95 | (1) |
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96 | (1) |
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97 | (1) |
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Mixed Alkali Halide Crystals |
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98 | (1) |
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98 | (3) |
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Preparation of Thin Films |
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99 | (1) |
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Atomic Resolution at Low-Coordinated Sites |
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100 | (1) |
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101 | (2) |
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Metallization and Bubble Formation in CaF2 |
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101 | (1) |
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102 | (1) |
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103 | (6) |
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Material and Site-Specific Contrast |
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104 | (1) |
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Using Damping for Distance Control |
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105 | (1) |
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106 | (3) |
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Atomic Resolution Imaging on Fluorides |
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109 | (16) |
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110 | (1) |
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111 | (4) |
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115 | (4) |
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119 | (6) |
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122 | (3) |
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Atomically Resolved Imaging of a NiO(001) Surface |
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125 | (10) |
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Antiferromagnetic Nickel Oxide |
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125 | (2) |
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Experimental Considerations |
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127 | (1) |
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Morphology of the Cleaved Surface |
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128 | (1) |
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Atomically Resolved Imaging Using Non-Coated and Fe-Coated Si Tips |
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129 | (1) |
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Short-Range Magnetic Interaction |
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130 | (1) |
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Analysis of the Cross-Section |
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131 | (2) |
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133 | (2) |
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134 | (1) |
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Atomic Structure, Order and Disorder on High Temperature Reconstructed α-Al2O3(0001) |
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135 | (12) |
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137 | (2) |
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Defect Formation upon Water Exposure |
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139 | (2) |
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Self-Organized Formation of Nanoclusters |
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141 | (6) |
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143 | (4) |
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NC-AFM Imaging of Surface Reconstructions and Metal Growth on Oxides |
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147 | (20) |
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147 | (1) |
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1x1 to 1x3 Phase Transition of TiO2(100) |
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148 | (3) |
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Surface Reconstructions of TiO2(110) |
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151 | (3) |
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The 1x2 Reconstruction of SnO2(110) |
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154 | (1) |
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Imaging Thin Film Alumina: NiAl(110)-Al2O3 |
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155 | (3) |
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Growth of Cu and Pd on α-Al2O3(0001)-√31 x √31R±9° |
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158 | (2) |
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A Short-Range-Ordered Overlayer of K on TiO2(110) |
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160 | (2) |
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162 | (5) |
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163 | (4) |
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Atoms and Molecules on TiO2(110) and CeO2(111) Surfaces |
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167 | (16) |
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167 | (1) |
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Brief Description of Experiments |
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168 | (1) |
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Surface Structures of TiO2(110) |
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169 | (1) |
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Adsorbed Atoms and Molecules on TiO2(110) |
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170 | (3) |
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Carboxylate Ions on TiO2(110) |
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170 | (2) |
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Hydrogen Adatoms on TiO2(110) |
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172 | (1) |
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Fluctuation of Acetate Ions on TiO2(110) |
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173 | (2) |
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Surface Structures of CeO2(111) |
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175 | (3) |
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178 | (5) |
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179 | (4) |
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NC-AFM Imaging of Adsorbed Molecules |
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183 | (10) |
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Nucleic Acid Bases on a Graphite Surface |
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183 | (4) |
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Double-Stranded DNA on a Mica Surface |
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187 | (2) |
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Alkanethiol on a Au(111) Surface |
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189 | (4) |
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191 | (2) |
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193 | (22) |
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AFM Imaging of Molecular Films |
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194 | (10) |
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195 | (3) |
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198 | (2) |
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Ferroelectric Molecular Films |
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200 | (4) |
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Surface Potential Measurements |
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204 | (5) |
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Technical Developments in NC-AFM Imaging of Molecules |
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209 | (2) |
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211 | (4) |
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212 | (3) |
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215 | (18) |
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215 | (1) |
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216 | (1) |
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217 | (1) |
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Alkyl-Substituted Carboxylates |
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218 | (3) |
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Numerical Simulation of Propiolate Topography |
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221 | (5) |
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223 | (1) |
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Sphere--Carboxylate Force |
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223 | (1) |
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224 | (1) |
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Cluster--Carboxylate Force |
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224 | (1) |
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224 | (2) |
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Fluorine-Substituted Acetates |
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226 | (3) |
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Conclusions and Perspectives |
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229 | (4) |
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230 | (3) |
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Low-Temperature Measurements: Principles, Instrumentation, and Application |
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233 | (24) |
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233 | (1) |
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Microscope Operation at Low Temperatures |
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234 | (3) |
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234 | (2) |
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236 | (1) |
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237 | (2) |
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239 | (3) |
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240 | (1) |
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241 | (1) |
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242 | (2) |
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244 | (5) |
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Δf(z) Curves on Specific Atomic Sites |
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244 | (2) |
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Tip-Dependent Atomic Scale Contrast |
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246 | (2) |
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248 | (1) |
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Magnetic Force Microscopy at Low Temperatures |
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249 | (3) |
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249 | (1) |
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Domain Structure of La0.7Ca0.3MnO3--δ |
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250 | (1) |
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251 | (1) |
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252 | (5) |
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253 | (4) |
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Theory of Non-Contact Atomic Force Microscopy |
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257 | (22) |
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257 | (2) |
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259 | (3) |
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Theoretical Simulation of NC-AFM Images |
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262 | (5) |
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Non-Contact Atomic Force Microscopy Images of Dynamic Surfaces |
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267 | (3) |
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Effect of Tip on Image for the Si(100)2x1:H Surface |
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270 | (4) |
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Effect of Tip on Surface Structure Change and its Relation to Dissipation |
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274 | (3) |
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277 | (2) |
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278 | (1) |
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Chemical Interaction in NC-AFM on Semiconductor Surfaces |
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279 | (26) |
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279 | (1) |
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First-Principles Calculation of Tip--Surface Chemical Interaction |
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280 | (1) |
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Simulation of NC-AFM Images |
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281 | (3) |
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Simulations on Various Surfaces |
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284 | (2) |
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Tip-Induced Surface Relaxation on the GaAs(110) Surface |
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286 | (7) |
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Vertical Scan Over an As Atom |
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286 | (2) |
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Vertical Scan Over a Ga Atom |
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288 | (3) |
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Relevance to Near-Contact STM Observations |
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291 | (2) |
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Tip-Induced Surface Atomic Processes and Energy Dissipation in NC-AFM |
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293 | (1) |
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Image Contrast on GaAs(110) for a Pure Si Tip: Distance Dependence |
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293 | (4) |
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Effect of Tip Morphology on NC-AFM Images |
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297 | (5) |
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Image Contrast for the Ga/Si Tip |
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299 | (2) |
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Image Contrast for the As/Si Tip |
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301 | (1) |
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302 | (3) |
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303 | (2) |
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Contrast Mechanisms on Insulating Surfaces |
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305 | (44) |
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305 | (1) |
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Model of AFM and Main Forces |
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306 | (7) |
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306 | (1) |
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307 | (6) |
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313 | (7) |
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313 | (1) |
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314 | (3) |
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317 | (2) |
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319 | (1) |
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Generating a Theoretical Surface Image |
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320 | (1) |
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320 | (21) |
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The Calcium Fluoride (111) Surface |
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322 | (14) |
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Calcite: Surface Deformations During Scanning |
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336 | (5) |
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Studying Surface and Defect Properties |
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341 | (2) |
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343 | (6) |
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344 | (5) |
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Analysis of Microscopy and Spectroscopy Experiments |
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349 | (22) |
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349 | (1) |
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349 | (6) |
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349 | (2) |
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Origin of the Frequency Shift |
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351 | (1) |
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Calculation of the Frequency Shift |
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352 | (2) |
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Frequency Shift for Conservative Tip--Sample Forces |
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354 | (1) |
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Simulation of NC-AFM Images |
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355 | (7) |
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Experimental NC-AFM Images of van der Waals Surfaces |
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355 | (3) |
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Basic Principles of the Simulation Method |
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358 | (2) |
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Applications of the Simulation Method |
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360 | (2) |
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Dynamic Force Spectroscopy |
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362 | (5) |
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Determining Forces from Frequencies |
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362 | (4) |
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Analysis of Tip--Sample Interaction Forces |
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366 | (1) |
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367 | (4) |
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368 | (3) |
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Theory of Energy Dissipation into Surface Vibrations |
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371 | (24) |
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371 | (1) |
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Possible Dissipation Mechanisms |
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372 | (3) |
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372 | (3) |
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375 | (1) |
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375 | (1) |
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Brownian Particle Mechanism of Energy Dissipation |
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375 | (7) |
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375 | (2) |
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Fluctuation--Dissipation Theorem |
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377 | (1) |
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Oscillating Tip as a Brownian Particle |
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378 | (2) |
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Energy Dissipated Per Oscillation Cycle |
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380 | (2) |
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Nonequilibrium Considerations for NC-AFM Systems |
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382 | (6) |
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382 | (1) |
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Mixed Quantum--Classical Representation |
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383 | (2) |
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Equation of Motion for the Tip |
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385 | (3) |
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Estimation of Dissipation Energies in NC-AFM |
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388 | (3) |
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391 | (1) |
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Conclusions and Future Directions |
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392 | (3) |
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393 | (2) |
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Measurement of Dissipation Induced by Tip--Sample Interactions |
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395 | (38) |
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395 | (1) |
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Experimental Aspects of Energy Dissipation |
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396 | (2) |
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398 | (1) |
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Apparent Energy Dissipation |
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399 | (5) |
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Velocity-Dependent Dissipation |
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404 | (9) |
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Electric-Field-Mediated Joule Dissipation |
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405 | (3) |
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Magnetic-Field-Mediated Joule Dissipation |
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408 | (1) |
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Magnetic-Field-Mediated Dissipation |
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409 | (3) |
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412 | (1) |
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Hysteresis-Related Dissipation |
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413 | (6) |
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Magnetic-Field-Induced Hysteresis |
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413 | (2) |
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Hysteresis Due to Adhesion |
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415 | (1) |
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Hysteresis Due to Atomic Instabilities |
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416 | (3) |
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Dissipation Imaging with Atomic Resolution |
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419 | (7) |
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426 | (3) |
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429 | (4) |
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429 | (4) |
Index |
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433 | |