研究目的
To investigate the influence of optical excitation intensity on the electrical, ferroelectric, and pyroelectric properties of ferroelectric-semiconductor composites, specifically focusing on polarization depth profiles and extending the 'three phase model'.
研究成果
Optical excitation significantly enhances the polarization and pyroelectric properties of the composites, allowing control over polarization depth profiles. The extended 'three phase model' explains the spatially dependent conductivity and polarization, enabling future applications in modulating polarization profiles with optical excitation.
研究不足
The study is limited to specific composite compositions and optical excitation conditions. The temporal decay of pyroelectric coefficient and inhomogeneities in particle dispersion may affect results. The LIMM method has a broad thermal scanning function, limiting spatial resolution. Absolute calibration of pyroelectric profiles was not performed for sample 2 due to mounting constraints.
1:Experimental Design and Method Selection:
The study involved fabricating composite thin films with 10 vol% (Cd:Zn)S particles in P(VDF-TrFE) matrix. Methods included I-V and polarization measurements using Sawyer-Tower circuit, pyroelectric coefficient measurement via an AC method, Laser Intensity Modulation Method (LIMM) for depth profiling, and photo-acoustic spectroscopy for thermal properties.
2:Sample Selection and Data Sources:
Two samples (sample 1 and sample 2) were prepared with specific thicknesses and electrode configurations. Data were collected from electrical, ferroelectric, pyroelectric, and thermal measurements.
3:List of Experimental Equipment and Materials:
Equipment included LED for optical excitation, power supply, power meter, Sawyer-Tower circuit, Peltier element, lock-in amplifier, laser diode for LIMM, photo-acoustic cell, chopper, and various materials like P(VDF-TrFE), (Cd:Zn)S particles, methyl ethyl ketone, gold electrodes.
4:Experimental Procedures and Operational Workflow:
Samples were polarized under different optical excitation intensities and peak-to-peak voltages. Pyroelectric measurements were conducted after polarization with time delays. LIMM measurements were performed from both sides of the sample. Photo-acoustic measurements were done at specific frequencies.
5:Data Analysis Methods:
Data were analyzed using rule of mixtures for thermal properties, RG-theory for photo-acoustic signals, and frequency dependency in LIMM for depth profiling. Statistical analysis included comparing signal amplitudes and fitting exponential decays.
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LED
LXML-PB01-0023
LUMILEDS
Optical excitation source with central wavelength of 470 nm for polarization and pyroelectric measurements.
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Power Meter
S130VC
Thorlabs
Measurement of optical power at specific wavelengths.
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Optical Density Filter
NE10A
Thorlabs
Prevent overload during optical measurements.
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Chopper
MC 2000
Thorlabs GmbH
Light modulation for photo-acoustic measurements.
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Power Supply
PS 2403d
Voltcraft
Control unit for adjusting LED intensity.
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Peltier Element
TEC1-12706
Ro?mann Electronic GmbH
Temperature modulation for pyroelectric coefficient measurement.
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Laser Diode
Used in LIMM for modulated intensity irradiation at wavelength of 685 nm.
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Lock-in Amplifier
Phase-sensitive measurement of pyroelectric current.
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Sputtering System
Deposition of gold electrodes on composite films.
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Ultrasonic Bath
Dispersion of materials in methyl ethyl ketone.
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Magnetic Stirrer
Stirring of composite solution at 50 °C.
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Compression Molding Machine
Fabrication of composite foils by compression molding.
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Photoacoustic Cell
Measurement of thermal properties using photo-acoustic spectroscopy.
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Brass Cylinder
Placed inside photoacoustic cell to reduce chamber volume.
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Sawyer-Tower Circuit
Measurement of ferroelectric hysteresis loops.
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