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Investigation of metal-insulator transition in magnetron sputtered samarium nickelate thin films

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Investigation of metal-insulator transition in magnetron sputtered samarium nickelate thin films ( investigation-metal-insulator-transition-magnetron-sputtered )

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2.6 Raman Spectroscopy Figure 2.13: Transitions in vibrational spectroscopy - Raman non-elastic scattering is compared to other transitions. ν0 is the frequency of exciting incident radiation and ν is vibrational quantum number. As featured in (75) p.2. fiber with a 50 mm diameter. An air Olympus MPLAN (100x/0.90NA) objec- tive was used. Raman scattered light was focused on a multi-mode fiber (100 mm diameter) and monochromator with a 600 line/mm grating. The excitation power of laser was 1 mW on the sample. Raman spectra were accumulated by 20 scans with an integration time of 20 s and a resolution of 3 cm−1. The spectrom- eter monochromator was calibrated using the Raman scattering line of a silicon plate (520.7 cm−1). The baseline correction, cosmic ray removal were done us- ing WitecProjectFour software, while peak fitting analysis was performed using GRAMS software package. 57

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Investigation of metal-insulator transition in magnetron sputtered samarium nickelate thin films

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