研究目的
To demonstrate that the highest signal-to-noise ratio (SNR) in Stimulated Raman Scattering (SRS) microscopy with shot noise limited detection is achieved with a time-averaged laser power ratio of 1:2 of the unmodulated and modulated beam, and to validate this theoretically and experimentally.
研究成果
Shot noise limited detection is achieved over a broad range of biologically relevant laser powers (0.45-60 mW total power on sample). The optimal SNR in SRS microscopy with shot noise limited detection is confirmed to be at a 1:2 time-averaged laser power ratio of unmodulated to modulated beams for linear photodamage, providing an 8% improvement over the 1:1 ratio. For non-linear photodamage, the optimal ratio converges to 1:1 with increasing damage order. This optimization enhances image quality without hardware changes, particularly beneficial for low signal levels in biological samples.
研究不足
The shot noise limited detection window is from 0.45 to 60 mW total power on the sample, limited by electronic noise at the lower end and photodiode saturation at the upper end. The improvement in SNR is small (8%), and the optimal power ratio depends on the photodamage mechanism, which may vary with sample type. Non-linear damage mechanisms shift the optimal ratio towards 1:1, requiring knowledge of the damage order for precise optimization.
1:Experimental Design and Method Selection:
The experiment is designed to validate the theoretical prediction of optimal laser power ratio for SNR in SRS microscopy. The method involves Stimulated Raman Loss (SRL) microscopy with shot noise limited detection, using amplitude modulation and lock-in detection to measure the modulation transfer between laser beams.
2:Sample Selection and Data Sources:
Samples include 2 μm polystyrene beads in water and adult C. Elegans roundworms. Polystyrene beads are used for controlled validation, and C. Elegans for biological relevance. Data are collected from regions of interest in images.
3:List of Experimental Equipment and Materials:
Equipment includes an 80 MHz laser (Lumera Plecter Duo), Optical Parametric Oscillator (APE Levante Emerald), acousto-optic modulator (Crystal Technology 3080194), Zeiss laser scanning microscope (LSM 7MP) with 32× objective (C-Achroplan W, NA=0.85), Si photodiode (Thorlabs DET36A), home-built transimpedance amplifier (using Texas Instruments OPA656), and lock-in amplifier (Stanford Research Systems SR844). Materials include half-wave plates, polarizing beamsplitters, optical filters, glass slides, coverslips, polystyrene beads, C. Elegans worms, M9 buffer, levamisole, and agarose.
4:85), Si photodiode (Thorlabs DET36A), home-built transimpedance amplifier (using Texas Instruments OPA656), and lock-in amplifier (Stanford Research Systems SR844). Materials include half-wave plates, polarizing beamsplitters, optical filters, glass slides, coverslips, polystyrene beads, C. Elegans worms, M9 buffer, levamisole, and agarose. Experimental Procedures and Operational Workflow:
4. Experimental Procedures and Operational Workflow: The set-up involves overlapping pump (816.7 nm) and Stokes (1064 nm) beams in space and time, modulating the Stokes beam at 3.636 MHz, focusing on the sample with the microscope objective, detecting the pump beam with the photodiode, amplifying the signal with the transimpedance amplifier, and demodulating with the lock-in amplifier. Images are recorded at specific pixel dwell times and frames averaged.
5:7 nm) and Stokes (1064 nm) beams in space and time, modulating the Stokes beam at 636 MHz, focusing on the sample with the microscope objective, detecting the pump beam with the photodiode, amplifying the signal with the transimpedance amplifier, and demodulating with the lock-in amplifier. Images are recorded at specific pixel dwell times and frames averaged. Data Analysis Methods:
5. Data Analysis Methods: SNR is calculated as signal divided by the sum of electronic and shot noise. Data points are mean intensities from regions of interest, with error bars as standard deviations. Theoretical curves are fitted to data, and improvements in SNR are quantified.
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photodiode
DET36A
Thorlabs
Detects the pump beam light after filtering, converting optical signals to electrical currents for SRS signal measurement.
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lock-in amplifier
SR844
Stanford Research Systems
Demodulates the amplified signal at the modulation frequency to extract the SRS signal from noise.
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Optical Parametric Oscillator
Levante Emerald
APE
Generates tunable wavelength output (775-990 nm) used as the pump beam in SRS microscopy.
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laser scanning microscope
LSM 7MP
Zeiss
Used for imaging samples with laser scanning, providing sub-micrometre resolution in SRS microscopy.
ZEISS LSM 990 Spectral Multiplex
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objective
C-Achroplan W
Zeiss
Focuses laser beams on the sample and collects light for imaging in the microscope.
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laser
Plecter Duo
Lumera
Provides 80 MHz laser pulses at 532 nm to pump the OPO for generating pump and Stokes beams in SRS microscopy.
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acousto-optic modulator
3080194
Crystal Technology
Modulates the intensity of the Stokes beam at 3.636 MHz for lock-in detection in SRS microscopy.
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transimpedance amplifier
Home-built (using Texas Instruments OPA656)
Amplifies the photodiode current with 86 dB transimpedance gain and includes a bandpass filter for signal conditioning in SRS detection.
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