EPFL SV PTBIOP LASER SCANNING CONFOCAL MICROSCOPY of confocal II_2015.pdf · Widefield microscopy...
Transcript of EPFL SV PTBIOP LASER SCANNING CONFOCAL MICROSCOPY of confocal II_2015.pdf · Widefield microscopy...
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EPFL–SV–PTBIOP
LASER SCANNING
CONFOCAL
MICROSCOPY PRACTICAL CONSIDERATIONS
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EPFL–SV–PTBIOP
OUTLINE
V. Important Parameters
Pixel dwell time
Zoom/Pixel number
Digital sampling/Pixel size
Pinhole size
Scan mode
VI. Practical Considerations
Light efficiency
Signal to nois ratio
Resolution in practice
VII. Summary
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EPFL–SV–PTBIOPPIXEL DWELL TIME
•How much time signal is collected at every pixel
•Very small values, normally in microseconds range
•Defined either directly or indirectly by scan frequency and image size
•Example: 512x512 pixels, 400 Hz - dwell time 4.910-6 sec
•Important characteristic for signal intensity
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DWELL TIME
Dwell time: 50 µs Dwell time: 6 µs Dwell time: 1.6 µs
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1024x1024 2048x2048512x512
Pixel size is defined by
zoom and pixel number
To change pixel size
1. Change zoom - image size changed,
number of pixels constant
2. Change number of pixel -
image size constant, pixel size changed
ZOOM AND PIXEL NUMBER
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SCANNING MECHANISM
ZOOMING/PIXEL NUMBERS
• Zooming: change the mirror deflection range (=Amplitude of scanner input signal)Zoom in: smaller field of view; higher energy deposition (bleaching)
• Pixel numbers: change the speed of the scanner• Large pixel numbers lower scan speed
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CAMERA BASED
DETECTION
• Fixed physical pixel size (e.g. Sony Interline chip 6.45 µm)
• Adaptation: Increase of effective pixel size via binning (CCD camera)
POINT SCANNING
DETECTION
• No physical pixel size
• Pixel size is determinedby sampling (zoom, number of pixels per image)
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DIGITAL SAMPLING
Digital Image
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EPFL–SV–PTBIOP
DIGITAL SAMPLING
Nyquist–Shannon sampling theorem1
If a function x(t) contains no frequencies higher than B hertz, it is completely determined by giving its ordinates at a series of points spaced 1/(2B) seconds apart.
In other words, a In other words, a bandlimitedfunction can be perfectly reconstructed from an infinite sequence of samples if the bandlimit, B, is no greater than ½ the sampling rate (samples per second). function can be perfectly reconstructed from an infinite sequence of samples if the bandlimit, B, is no greater than ½ the sampling rate (samples per second).
Light microscopy:
Bandlimit: Resolution LimitSampling frequency) 1/2 * resolution limit
1Wikipedia: http://en.wikipedia.org/wiki/Nyquist%E2%80%93Shannon_sampling_theorem 8
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EPFL–SV–PTBIOP
DIGITAL SAMPLING
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80 nm/pixel
160 nm/pixel
5 nm/pixel
320 nm/pixel
488 nm 325 nm 244 nm 195 nm 163 nm
Layer Title
139 nm 122 nm 108 nm 98 nm 89 nm
Wavelength: 488nm; NA=1.4 Rayleigh criterion: 212 nm
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PIXEL SIZE
33 nm 65 nm 130 nm 260 nm
12 MB
t=64x
3 MB
t=16x0.8 MB
t=4x0.2 MB
t=1x
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PIXEL SIZE
33 nm 65 nm 130 nm 260 nm
• Nyquist sampling is as good starting point
• Oversampling can result in better images
but increases probability of photobleaching and decreases temporal resolution.
• Undersampling increases temporal resolution and decreases image file size.
• Sampling frequency should match the biological question
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PINHOLE SIZE
Pinhole: 10 AU Pinhole: 5 AU Pinhole: 1 AU
Closing the pinhole increases the z-sectioning capabilities because light from out of focus
planes is suppressed, but also decreases the SNR/contrast
(less photons are detected also from the focal plane).
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SPECTRAL OVERLAP
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• Spectral overlap depends on the emisson-spectra of the fluorophores.
• Amount of bleed through depends on the spectral overlap the concentration of the fluorophores and the excitation intensity.
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EPFL–SV–PTBIOP
SCAN MODEBLEED-THROUGH
Sequential scanning : minimizes bleedthrough, less temporal resolution
Simultaneous scanning : optimizes temporal resolution
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EPFL–SV–PTBIOP
OUTLINE
V. Important Parameters
Pixel dwell time
Zoom/Pixel number
Digital sampling/Pixel size
Pinhole size
Scan mode
VI. Practical Considerations
Light efficiency
Signal to nois ratio
Resolution in practice
VII. Summary
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EPFL–SV–PTBIOP
LIGHT EFFICIENCY
Photons emitted by a single fluorophore
- How many photons can one obtain from a
typical fluorophore in confocal microscopy?
- How does can we influence the photon flux?
- Why is the photo flux important for (Laser
scanning confocal) microscopy?
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EPFL–SV–PTBIOP
ba
a
tot kk
k
S
S
][
][ 1
LIGHT EFFICIENCYPHOTONS EMITTED BY A SINGLE FLUOROPHORE
ka = s * I
kb = 1/tF tF =fluorescent
lifetime
Photon output (steady state)
= kb*[S1]
kbka
S0
S1
very fast
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EPFL–SV–PTBIOP
LIGHT EFFICIENCYPHOTONS EMITTED BY A SINGLE FLUOROPHORE
1mW @488 nm foccused to a radius of 0.25 mm
(e.g. objective NA 1.25)
I = 5.1 *105 W/cm2 = 1.25*1024 photons/(cm2*s)
Fluoresceine: e = 80 000 l*mol-1*cm-1
Cross section/molecule = 3.06 * 10 -16 cm2/molecule
ka = s * I = 3.8 * 108 s-1
kb = 1/tF
tF = 4.5 ns kb = 2.2*108 s-1
S1
kbka
S0
very fast
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EPFL–SV–PTBIOP
ba
a
tot kk
k
S
S
][
][ 10 2 4 6 8 10
0,0
0,2
0,4
0,6
0,8
1,0
0,0
0,2
0,4
0,6
0,8
1,0
S
1/S
tot
S
0/S
tot
ka/k
b
LIGHT EFFICIENCYPHOTONS EMITTED BY A SINGLE FLUOROPHORE
kbka
S0
S1
very fast
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EPFL–SV–PTBIOP
LIGHT EFFICIENCYPHOTONS EMITTED BY A SINGLE FLUOROPHORE
Photon output: Qe*kb*[S1] = 0.9 * 0.63 * 2.2*108 s-1 =
1.3* 108 photons/s
512*512 pixel / s = 3.8 ms/pixel ~ 500 photons/pixel
(for fluoresceine excited with 488 nm)
ka = s * I = 3.8 * 108 s-1
kb = 1/tF
tF = 4.5 ns kb = 2.2*108 s-1
S1
kbka
S0
very fast
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EPFL–SV–PTBIOP
LIGHT EFFICIENCYPHOTONS EMITTED BY A SINGLE FLUOROPHORE
Single Fluorophore (Fluoresceine):
512*512 pixel / s = 3.8 µs/pixel ~ 500 photons/pixel
But losses due to
- Geometry (fluorophore emitting in all directions)
-NA 1.4 40% efficiency
-NA 0.3 5% efficiency
- Scattering
- Optical elements
- Objective
- mirrors, filters
- pinhole
- Detector efficiency 10-30%
Each fluorescent molecule contributes on the order of only one
photoelectron/pixel/sweep
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SIGNAL TO NOISE
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Layer Title
Layer Title
Layer Title
No Noise
Gaussian Noise: 1 STDV
Gaussian Noise: 2 STDV
Noise reduces
Modulation/Contrast
Decreases Resolution
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EPFL–SV–PTBIOP
NOISE REDUCTION
Strategies to reduce image noise
• reduce scan speed
increases pixel dwell time=more photons
• Averaging
• line averaging
• frame averaging
• Integrate
• Photon output
• increase laser intensity
• Limitation: fluorophore saturation
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EPFL–SV–PTBIOP
BLEACHING
Excitation
- Cone of light
- Bleaching occurs above
and below focal plane
- z-sampling affects
bleaching
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EPFL–SV–PTBIOP
BLEACHING MECHANISMS
Photon output: 1.3* 108 photons/s =
1.3* 108 cycles/s
High energy density
High cycle time
High bleaching probability
- Photochemistry of bleaching poorly
understood.
- Differs from fluorophor to fluorophor
-Main Bleaching route: Triplet state
- Absorb another photon
- Energy exchange with triplet
oxygen, which becomes highly
reactive singlet oxygen
S2
S0
S1
t ~ ns
T2
T1
t ~ µs-s
Energ
y
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TRIPLET STATES
0 2 4 6 8 10
0.0
0.2
0.4
0.6
0.8
1.0
0.0
0.2
0.4
0.6
0.8
1.0
S
0/S
tot
S
1/S
tot
ka/k
b
tT=1 µs
kIC
=0.01*(1/tF
S2
S0
S1t ~ ns
T2
T1
t ~ µs-s
Energ
y
Ensemble of molecules: 60% are trapped in triplet state
decrease of fluorescent intensity by 60%
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EPFL–SV–PTBIOPBLEACHING
Parameters affecting bleaching probability- Fluorophore
- Laser intensity
- Pixel Dwell time
- Sampling frequency
Bleaching (Photon)Noise
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EPFL–SV–PTBIOP
LASER SCANNING CONFOAL
MICROSCOPYOUTLOOK
Resolution
• Point Spread Function
•Nyquist Sampling
•Optical Slice thickness
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EPFL–SV–PTBIOP
LASER SCANNING CONFOAL
MICROSCOPYPOINT SPREAD FUNCTION
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EPFL–SV–PTBIOP
OPTICAL RESOLUTION
THEORY/PRAXIS
Example: l500 nm; n=1.518; NAObj =1.4
wf xy-plane resel=217 nm conf. xy-plane
resel=157 nm conf. axial resel=580 nm
0 1 2 3 4
0
500
1000
1500
2000
rel. in
tensity
distance / mm
bead: 170 nm
FWHM: 234 nmIn
ten
sity
optical unit
FWHM
resel
FWHM resel
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SPHERICAL ABBERATIONS
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EPFL–SV–PTBIOPRESOLUTION
• Physical Resolution– Parameters affecting resolution
• Wavelength
• NA of objective
• Refractive index
• Pinhole size
– Difference in lateral and axial resolution
• Digital resolution (Sampling)– Nyquist sampling
– Optical zooming
– Number of pixels
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EPFL–SV–PTBIOP
LASER SCANNING CONFOCAL
MICROSCOPYSUMMARY
Widefield microscopy• Detector efficiency : 60%-80%• Detector noise: 4 RMS electrons/pixel• Pixel Dwell time: 10-1000 ms• Opical sectioning: no• Backgrond supression: no
Laser scanning confocal microscopy• Detector efficiency : 3%-12%• Detector Noise: < 0.01 RMS electrons/pixel• Pixel dwell time: 1-100 µs• Optical sectioning: yes• Background supression: yes
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EPFL–SV–PTBIOP
SUMMARY
Decrease
pinhole size
Increases Resolution(mainly along z-axis,
but also in the xy-plane)
Less photons
Decreases SNR, contrast and
thereby resolution
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