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Raman spectroscopyAcquisition, preprocessing and analysis of spectra

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(1)

Sergey Kucheryavski

svk@bio.aau.dk

Raman spectroscopy

Acquisition, preprocessing and analysis of spectra

(2)

Raman spectrometer scheme

Acquisition, preprocessing and analysis of Raman spectra 2

Credits: http://www.doitpoms.ac.uk/tlplib/raman/method.php

(3)

Raman spectrometer

Acquisition, preprocessing and analysis of Raman spectra 3

(4)

Raman spectrometer

Acquisition, preprocessing and analysis of Raman spectra 4

(5)

Probes and fibers

Acquisition, preprocessing and analysis of Raman spectra 5

(6)

Non contact probe

Acquisition, preprocessing and analysis of Raman spectra 6

(7)

Acquisition of Raman spectra

Acquisition, preprocessing and analysis of Raman spectra 7

(8)

Raman signal is weak

Only around 1 in every 30 million photons is Raman scattered

(9)

Acquisition of Raman spectra

Acquisition, preprocessing and analysis of Raman spectra 9

Issues

• Cosmic rays

• Noise

• Detection limits

• Fluorescence

Parameters

• Laser frequency

• Laser power

• Exposure time

• Number of scans

Preprocessing

• Spectral truncation

• Noise reduction

• Baseline correction

• Derivatives

(10)

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)x

ij

= f

j

(x

ij

)

10 6. Data preprocessing

(11)

Cosmic spikes

Noise and detection limits

Fluorescence and background correction

(12)

Cosmic spikes

• occasionally appears in spectra as very narrow peaks

• caused by high energy cosmic rays

• typical issue for CCD based instruments

• most of the acquisition software include algorithms to remove the effect

Acquisition, preprocessing and analysis of Raman spectra 12

Credits: Confocal Raman Microscopy. ed. Thomas Dieing, et al.

(13)

Cosmic spikes

Noise and detection limits

Fluorescence and background correction

(14)

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 14

(15)

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 15

(16)

Acquisition parameters and concentration

Acquisition, preprocessing and analysis of Raman spectra 16

25% ethanol

t = 5s

t = 3s

t = 1s

(17)

Acquisition parameters and concentration

Acquisition, preprocessing and analysis of Raman spectra 17

10% ethanol

t = 3s

t = 1s

t = 1s

(18)

Acquisition parameters and concentration

Acquisition, preprocessing and analysis of Raman spectra 18

10% ethanol

t = 3s

t = 1s

(19)

Acquisition parameters and concentration

Acquisition, preprocessing and analysis of Raman spectra 19

1% ethanol

t = 5s

t = 3s

t = 1s

(20)

Trancating spectra

Acquisition, preprocessing and analysis of Raman spectra 20

1% ethanol

t = 5s

t = 3s

t = 1s

(21)

Acquisition parameters and concentration

Acquisition, preprocessing and analysis of Raman spectra 21

1% ethanol

t = 5s

t = 3s

t = 1s

(22)

Acquisition parameters and concentration

Acquisition, preprocessing and analysis of Raman spectra 22

Butter

t = 1s, 5 scans

t = 1s, 3 scans

t = 1s, 1 scan

(23)

Acquisition parameters and concentration

Acquisition, preprocessing and analysis of Raman spectra 23

Butter

t = 1s, 5 scans

t = 1s, 3 scans

t = 1s, 1 scan

(24)

Playing with acquisition parameters

Acquisition, preprocessing and analysis of Raman spectra 24

Butter

t = 3s, 5 scans

t = 1s, 1 scan

(25)

Using filters for noise removal

Linear filters: moving average, gaussian

Wavelet decomposition

Savitzky-Golay smoothing

Acquisition, preprocessing and analysis of Raman spectra 25

1150 1155 1160 1165 1170 1175 1180 1185 1190 1195 1200

400 500 600 700 800 900 1000 1100

1150 1155 1160 1165 1170 1175 1180 1185 1190 1195 1200

400 500 600 700 800 900 1000 1100

1150 1155 1160 1165 1170 1175 1180 1185 1190 1195 1200

400 500 600 700 800 900 1000 1100

w = 5 d = 1

(26)

Using filters for noise removal

Acquisition, preprocessing and analysis of Raman spectra 26

SG filtered

noised

original

(27)

Cosmic spikes

Noise and detection limits

Fluorescence and background correction

(28)

Fluorescence

Mechanism

• appears if molecules can absorb the laser radiation at particular wavelength

• the absorbed light excites electrons to higher energy levels

• electrons return to the ground state by emitting light of longer wavelength

Acquisition, preprocessing and analysis of Raman spectra 28

(29)

Fluorescence

How decrease/get rid of fluorescence:

• remove impurities from solid samples

• using microprobes or confocal Raman microscopy (for solid samples)

• using lasers with wavelength in NIR range

• proper preprocessing (baseline correction)

Acquisition, preprocessing and analysis of Raman spectra 29

Features

• very common for colored (especially dark) samples

• several orders of magnitude stronger than Raman scattering

• has a broad emission

(30)

Fluorescence Color of samples

Acquisition, preprocessing and analysis of Raman spectra 30

(31)

Laser wavelength

Visible — higher energy, stronger signal, deeper penetration, better resolution, fluorescence (good for inorganic materials)

NIR — lower energy, weaker signal, worse resolution, smaller fluorescence effect (suitable for organic materials)

Acquisition, preprocessing and analysis of Raman spectra 31

Credits: http://www.horiba,com

(32)

Baseline correction

Acquisition, preprocessing and analysis of Raman spectra 32

Baseline shift and curvature caused by noise, fluorescence, CCD background, interference, etc.

Automatic baseline correction

(33)

Baseline correction

Acquisition, preprocessing and analysis of Raman spectra 33

Automatic baseline correction

d = 4

(34)

Baseline correction

Acquisition, preprocessing and analysis of Raman spectra 34

Automatic baseline correction

d = 6

(35)

Baseline correction

Acquisition, preprocessing and analysis of Raman spectra 35

Semi-automatic baseline correction

(36)

Conclusions

Issues

• Cosmic rays

• Noise

• Detection limits

• Fluorescence

Acquisition, preprocessing and analysis of Raman spectra 36

Parameters

• Laser frequency

• Laser power

• Exposure time

• Number of scans

Preprocessing

• Spectral truncation

• Noise reduction

• Baseline correction

• Derivatives

Referencer

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