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Ultrafast in-situ null-ellipsometry for studying pulsed laser – Silicon surface interactions
•A pump and probe imaging ellipsometer setup is described.•Laser excitation of silicon is analyzed by pump-probe ellipsometry.•Time evolution of Ψ and Δ values are presented in the range of 2–146ps.•Changes are discussed in the frame of two-temperature model. The measurement of transient optical pro...
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Published in: | Applied surface science 2017-11, Vol.421, p.325-330 |
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Main Authors: | , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | •A pump and probe imaging ellipsometer setup is described.•Laser excitation of silicon is analyzed by pump-probe ellipsometry.•Time evolution of Ψ and Δ values are presented in the range of 2–146ps.•Changes are discussed in the frame of two-temperature model.
The measurement of transient optical properties due to pulsed laser excitation allows better understanding of the nature of laser induced processes. Conventional ellipsometry is not capable of following changes in the femto-, pico- or nanosecond timescale. In this work, the pump and probe technique is combined with a single wavelength null-ellipsometry. This enabled us to follow the optical changes of silicon due to sub-ps laser pulse irradiation with ps time resolution. The combination of the 496nm probe pulses with a Polarizer – Compensator – Sample – Analyzer (PCSA) configuration imaging null-ellipsometer provided Ψ and Δ ellipsometric angles of silicon irradiated with 248nm pump pulses. Different laser intensities and delay times between the probe and pump pulses are used in the experiments. It is shown that besides thermal effects, the in depth free charge carrier distribution and their electron-phonon relaxation time has to be taken into account in the frame of the two-temperature model for satisfactory interpretation of the experimental results. |
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ISSN: | 0169-4332 1873-5584 |
DOI: | 10.1016/j.apsusc.2017.03.186 |