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Applying Dynamic Strain on Thin Oxide Films Immobilized on a Pseudoelastic Nickel-Titanium Alloy
Published on: July 28, 2020
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Ultrafast laser-induced strain waves in thin ruthenium layers.
Optics Express
|October 7, 2021
Summary
We observed ultra-high frequency acoustic waves in thin ruthenium films, showing thickness-dependent sound speed and optical responses dominated by thermo-optic and strain-optic effects. Initial phase suggests dynamic changes in the acoustic wave post-excitation.
Area of Science:
- Materials Science
- Acoustics
- Optics
Background:
- Laser-induced acoustic waves are crucial for material characterization.
- Understanding material properties at the nanoscale requires advanced probing techniques.
- Ruthenium thin films have applications in electronics and catalysis.
Purpose of the Study:
- To investigate time-dependent optical diffraction from laser-induced acoustic waves in ruthenium thin films.
- To analyze the thermo-optic and strain-optic effects in ruthenium layers.
- To study the generation and detection of ultra-high frequency acoustic waves (130-750 GHz) in ultra-thin films (1.2-20 nm).
Main Methods:
- Time-dependent optical diffraction measurements.
- Generation and detection of longitudinal acoustic waves using pulsed lasers.
- Analysis of acoustic wave propagation in ruthenium thin films on glass substrates.
Main Results:
- Thermo-optic and strain-optic effects were identified as dominant optical responses.
- A strong dependency of the speed of sound on layer thickness (and thus frequency) was observed.
- A faster signal decay at higher frequencies due to acoustic impedance mismatch was measured.
- Acoustic wave frequency and phase remained constant for >2 ps, with an extrapolated initial phase of -π/2.
Conclusions:
- The study demonstrates the feasibility of generating and detecting THz acoustic waves in nm-thick ruthenium films.
- Thickness-dependent sound speed and acoustic impedance mismatch influence wave propagation and signal decay.
- The observed initial phase suggests potential dynamic phase/frequency changes within the first 2 ps post-excitation.

