研究目的
Investigating the hot carrier dynamics in a dispersionless plasmonic system using pump-probe measurements to understand the influence of pump generated carriers on the probe generated plasmons and the role of the bulk metal band structure in these dynamics.
研究成果
The study demonstrates that hot carrier dynamics in a dispersionless plasmonic system are governed by the bulk metal band structure. The dependence of decay time on pump fluence varies linearly or quadratically depending on the excitation mechanism. The findings highlight the importance of the metal band structure in plasmon-mediated hot carrier generation and relaxation processes.
研究不足
The study is limited by the time resolution of the pump-probe measurements (45 fs) and the specific geometry of the plasmonic quasicrystal structure. The interpretation of results relies on theoretical models that may not fully capture all physical processes involved.
1:Experimental Design and Method Selection:
The study uses pump-probe measurements with 45 fs time resolution to investigate hot carrier dynamics in a plasmonic quasicrystal structure. The methodology includes simultaneous measurement of differential transmittance and reflectance.
2:Sample Selection and Data Sources:
The sample is a quasiperiodic array of air holes in a 50 nm thick sputtered gold film on a quartz substrate, fabricated using electron beam lithography.
3:List of Experimental Equipment and Materials:
Equipment includes a Spectra Physics Spitfire amplifier laser, TOPAS Optical Parametric Amplifier, photodiodes (Hamamatsu), lock-ins (SRS830), and interference filters (Semrock).
4:Experimental Procedures and Operational Workflow:
The pump and probe beams are focused and spatially overlapped at the sample surface. Differential transmission and reflection are measured as a function of delay between pump and probe pulses.
5:Data Analysis Methods:
Data are fitted with a two-temperature model to extract rise and decay times. Density matrix calculations are used to estimate the dipole matrix element for each transition.
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