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Investigation into Germanium thin films formed by a recrystallisation method Acknowledgements: Vishesh Sharma, Dr Peter Gammon, Chunwa Chan, Dr Vishal Shah, Dr Mark Crouch, Dr David Walker, Corrine Maltby Motivation Thin films of germanium on silicon carbide have previously been formed using a conventional epitaxial method, which resulted in imperfect layers of high surface roughness and 1 Polycrystallinity. 2 However, it showed lower turn on voltage. Germanium on silicon carbide can be used to produce hybrid devices, which can have control and power devices on one chip. Photonics, low band gap of Germanium and wide band gap of Silicon carbide means one photodiode can be used to cover the whole solar spectrum. Source N+ Gate Drain N+ Ge P+ Substrate Power device School of Engineering SiC Substrate Fig1: A sketch of a power device in SiC controlled by a CMOS in Ge Ge 100 Ge 111 Ge 120 Why are we using Silicon instead of SiC in this project? Silicon carbide is very expensive. Several new techniques are being investigated including Ge evaporation and thermal annealing, so cheap Si is used to learn these processes. Furthermore, analysis equipment like the Profile-o-meter, interferometer and XRD are being used. SiC Substrate Germanium Peak Fig2: A Sketch of Polycrytsalline Germanium on Silicon Carbide Results XRD X-ray diffraction(XRD) tells us how crystalline the layer is and its orientation. Silicon Peak 500nm 900°C (Blue) have a very well defined Germanium peak. Decreasing the annealing temperature results in a less crystalline layer, reducing peak intensity. This can be seen in the 800°C film (Red) of the same thickness with a reduced intensity, doublet peak. A thinner film also produces a less defined Germanium peak because it is thinner. This is shown by the 100nm film (Green) annealed at 900°C. Fig3. A rocking curve obtained via X-Ray Diffract-o-meter Ge film was amorphous for all thin films annealed at or below 700°C. Results Interferometer Interferometer can scan and show the texture of the surface and give us a RMS Surface roughness reading. Thickest layer of 900°C annealed sample was too dull to take a roughness reading. Samples annealed at 800°C or below produced a very consistent Ge thin film. However at 900°C Ge thin film got more rough with increasing film thickness. Log of Ge film thickness (nm) Fig4: A plot of surface roughness of Ge thin film Fabrication/Experimental 25 Ge thin films on Si substrate were deposited. 5 samples per thickness were made. Thicknesses were 500nm, 200nm, 100nm, 50nm, 20nm. Samples from each thickness were annealed at 5 different temperatures. Annealing temperatures and dwell times were 900°C, 800°C, 700°C with dwell time of 1 minute, 500°C with 5 minutes dwell time and finally 300°C with one hours dwell time. Ge thin films were deposited using Electron Beam Evaporator. Afterwards, they were annealed in a Rapid Thermal Annealer. However for 1 hour dwell time a Tube Furnace was used instead. To verify thickness of Ge film a Profile-o-meter was used. Interferometer was used to measure surface roughness Finally, Crystallinity and crystal orientation of the Ge thin film were analysed using X-Ray Difractometer. Future work Annealing the sample past the melting point of Ge to analyse the effects on crystallinity, which is at 928°C. Samples can be annealed at higher temperatures for longer period of time in a tube furnace. References 1. P. M. Gammon, Development of SiC Heterojunction Power Devices, May 2011, Warwick University.Page 83 2. P. M. Gammon, Development of SiC Heterojunction Power Devices, May 2011, Warwick University.Page 122