Presentation slides

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Sergey Kucheryavski
svk@bio.aau.dk
Raman spectroscopy
Acquisition, preprocessing and analysis of spectra
Raman spectrometer scheme
Credits: http://www.doitpoms.ac.uk/tlplib/raman/method.php
Acquisition, preprocessing and analysis of Raman spectra
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Raman spectrometer
Acquisition, preprocessing and analysis of Raman spectra
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Raman spectrometer
Acquisition, preprocessing and analysis of Raman spectra
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Probes and fibers
Acquisition, preprocessing and analysis of Raman spectra
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Non contact probe
Acquisition, preprocessing and analysis of Raman spectra
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Acquisition of Raman spectra
Acquisition, preprocessing and analysis of Raman spectra
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Raman signal is weak
Only around 1 in every 30 million photons is Raman scattered
Acquisition of Raman spectra
Issues
Parameters
Preprocessing
•
Cosmic rays
•
Laser frequency
•
Spectral truncation
•
Noise
•
Laser power
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Noise reduction
•
Detection limits
•
Exposure time
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Baseline correction
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Fluorescence
•
Number of scans
•
Derivatives
Acquisition, preprocessing and analysis of Raman spectra
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Preprocessing
Preprocessing – a way to improve signal for further analysis
What can be improved
– Noise reduction
– Correction of baseline
– Resolving merged meaks
– Removing physical effects
How it works:
– X’ = F(X)
– xij = fj(xij)
6. Data preprocessing
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Cosmic spikes
Noise and detection limits
Fluorescence and background correction
Cosmic spikes
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occasionally appears in spectra as very narrow peaks
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caused by high energy cosmic rays
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typical issue for CCD based instruments
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most of the acquisition software include algorithms to remove the effect
Credits: Confocal Raman Microscopy. ed. Thomas Dieing, et al.
Acquisition, preprocessing and analysis of Raman spectra
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Cosmic spikes
Noise and detection limits
Fluorescence and background correction
Noise and detection limits
CCD detectors have photon noise, dark noise and read noise
Raman signal is weak
To get a good signal/noise ratio
• cool CCD
• higher concentration
• longer exposure time
• more scans for the same sample
• de-noising preprocessing
Acquisition, preprocessing and analysis of Raman spectra
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Noise and detection limits
CCD detectors have photon noise, dark noise and read noise
Raman signal is weak
To get a good signal/noise ratio
• cool CCD
• higher concentration
• longer exposure time
• more scans for the same sample
• de-noising preprocessing
Acquisition, preprocessing and analysis of Raman spectra
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Acquisition parameters and concentration
25% ethanol
t = 5s
t = 3s
t = 1s
Acquisition, preprocessing and analysis of Raman spectra
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Acquisition parameters and concentration
10% ethanol
t = 3s
t = 1s
t = 1s
Acquisition, preprocessing and analysis of Raman spectra
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Acquisition parameters and concentration
10% ethanol
t = 3s
t = 1s
Acquisition, preprocessing and analysis of Raman spectra
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Acquisition parameters and concentration
1% ethanol
t = 5s
t = 3s
t = 1s
Acquisition, preprocessing and analysis of Raman spectra
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Trancating spectra
1% ethanol
t = 5s
t = 3s
t = 1s
Acquisition, preprocessing and analysis of Raman spectra
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Acquisition parameters and concentration
1% ethanol
t = 5s
t = 3s
t = 1s
Acquisition, preprocessing and analysis of Raman spectra
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Acquisition parameters and concentration
Butter
t = 1s, 5 scans
t = 1s, 3 scans
t = 1s, 1 scan
Acquisition, preprocessing and analysis of Raman spectra
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Acquisition parameters and concentration
Butter
t = 1s, 5 scans
t = 1s, 3 scans
t = 1s, 1 scan
Acquisition, preprocessing and analysis of Raman spectra
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Playing with acquisition parameters
Butter
t = 3s, 5 scans
t = 1s, 1 scan
Acquisition, preprocessing and analysis of Raman spectra
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Using filters for noise removal
• Linear filters: moving average, gaussian
• Wavelet decomposition
• Savitzky-Golay smoothing
1100
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w=5
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d=1
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Acquisition, preprocessing and analysis of Raman spectra
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1195
1200
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Using filters for noise removal
SG filtered
noised
original
Acquisition, preprocessing and analysis of Raman spectra
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Cosmic spikes
Noise and detection limits
Fluorescence and background correction
Fluorescence
Mechanism
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appears if molecules can absorb the laser
radiation at particular wavelength
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the absorbed light excites electrons to higher
energy levels
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electrons return to the ground state by emitting
light of longer wavelength
Acquisition, preprocessing and analysis of Raman spectra
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Fluorescence
Features
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very common for colored (especially dark) samples
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several orders of magnitude stronger than Raman scattering
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has a broad emission
How decrease/get rid of fluorescence:
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remove impurities from solid samples
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using microprobes or confocal Raman microscopy (for solid samples)
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using lasers with wavelength in NIR range
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proper preprocessing (baseline correction)
Acquisition, preprocessing and analysis of Raman spectra
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Fluorescence
Color of samples
Acquisition, preprocessing and analysis of Raman spectra
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Laser wavelength
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Visible — higher energy, stronger signal, deeper penetration, better
resolution, fluorescence (good for inorganic materials)
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NIR — lower energy, weaker signal, worse resolution, smaller fluorescence
effect (suitable for organic materials)
Credits: http://www.horiba,com
Acquisition, preprocessing and analysis of Raman spectra
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Baseline correction
Baseline shift and curvature caused by noise, fluorescence, CCD
background, interference, etc.
Automatic baseline correction
Acquisition, preprocessing and analysis of Raman spectra
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Baseline correction
Automatic baseline correction
d=4
Acquisition, preprocessing and analysis of Raman spectra
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Baseline correction
Automatic baseline correction
d=6
Acquisition, preprocessing and analysis of Raman spectra
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Baseline correction
Semi-automatic baseline correction
Acquisition, preprocessing and analysis of Raman spectra
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Conclusions
Issues
Parameters
Preprocessing
• Cosmic rays
• Laser frequency
• Spectral truncation
• Noise
• Laser power
• Noise reduction
• Detection limits
• Exposure time
• Baseline correction
• Fluorescence
• Number of scans
• Derivatives
Acquisition, preprocessing and analysis of Raman spectra
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