BMS 524 - “Introduction to Confocal Microscopy and Image Analysis”
Department of Basic Medical Sciences,
School of Veterinary Medicine
Weldon School of Biomedical Engineering
Purdue University
J. Paul Robinson, Ph.D.
SVM Professor of Cytomics
Professor of Immunopharmacology & Biomedical Engineering
Director, Purdue University Cytometry Laboratories, Purdue University
These slides are intended for use in a lecture series. Copies of the slides are distributed and students encouraged to take their notes on these graphics. All material copyright J.Paul Robinson unless otherwise stated. No reproduction of this material is permitted without the written permission of J. Paul Robinson. Except that our materials may be used in not-for-profit educational institutions ith appropriate acknowledgement.
You may download this PowerPoint lecture at http://tinyurl.com/2dr5p
This lecture was last updated in January, 2007
Find other PUCL Educational Materials at http://www.cyto.purdue.edu/class
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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At the conclusion of this lecture you should:
• Understand the nature of fluorescence
• The restrictions under which fluorescence occurs
• Nature of fluorescence probes
• Spectra of different probes
• Resonance Energy Transfer and what it is
• Features of fluorescence
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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Lamps
Xenon
Xenon/Mercury
Lasers
Argon Ion (Ar)
Krypton (Kr)
Violet 405nm, 380 nm
Helium-Neon (He-Ne)
Helium-Cadmium (He-Cd)
Krypton-Argon (Kr-Ar)
Laser Diodes
400nm - NIR
2004 sales of approximately 733 million diode laser; 131,000 of other types of lasers
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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• Chromophores are components of molecules which absorb light
• e.g. from protein most fluorescence results from the indole ring of tryptophan residue
• They are generally aromatic rings
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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S
2
Singlet States
Jablonski Diagram
Triplet States
Vibrational energy levels
Rotational energy levels
Electronic energy levels
T
2
S
1
ABS
IsC
FL fast
I.C.
PH
T
1
Triplet state
IsC slow (phosphorescence)
Much longer wavelength ( blue ex
– red em)
[Vibrational sublevels]
S
0
ABS - Absorbance
FL - Fluorescence
S 0.1.2 - Singlet Electronic Energy Levels
T 1,2 - Corresponding Triplet States
I.C.- Nonradiative Internal Conversion IsC - Intersystem Crossing PH - Phosphorescence
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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1
S’
S
1 hv ex hv em
S
0
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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– is the energy difference between the lowest energy peak of absorbance and the highest energy of emission
Fluorescein molecule
Stokes Shift is 25 nm
495 nm 520 nm
Wavelength
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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related to the probability of the event
the energy of the light absorbed or emitted
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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The longer the wavelength the lower the energy
The shorter the wavelength the higher the energy e.g. UV light from sun causes the sunburn not the red visible light
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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632.5 nm (HeNe ) Protein
300 nm 400 nm 500 nm 600 nm 700 nm
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
Excitation Emission
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350
300 nm 400 nm
457 488 514 610 632
500 nm 600 nm 700 nm
Common Laser Lines
PE-TR Conj.
Texas Red
PI
Ethidium
PE
FITC cis-Parinaric acid
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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(He-Cd light difficult to get 325 nm band through some optical systems – need quartz)
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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Xe Lamp
Hg Lamp
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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Fluorophore
FITC
Bodipy
Tetra-M-Rho
L-Rhodamine
Texas Red
CY5
EX peak
EM peak
% Max Excitation at
488 568 647 nm
496 518 87 0 0
503 511 58 1 1
554 576 10 61 0
572 590 5 92 0
592 610 3 45 1
649 666 1 11 98
Note: You will not be able to see CY5 fluorescence under the regular fluorescent microscope because the wavelength is too high.
Material Source:
Pawley: Handbook of Confocal Microscopy
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© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
Calibration is accurate and against an easily obtainable calibration lamp
($300 lamp is from Lightform, Inc www.lightform.com)
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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• Extinction Coefficient
– refers to a single wavelength (usually the absorption maximum )
• Quantum Yield
– Q f band is a measure of the integrated photon emission over the fluorophore spectral
• At sub-saturation excitation rates, fluorescence intensity is proportional to the product of
and Q f
=
Number of emitted photons
Number of absorbed photons
• Lifetime 1 –10x10 -9 secs (1-10 ns)
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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ln (I o
/I) = s nd
(B eer –Lambert law)
I o
= light intensity entering cuvet
I=light intensity leaving cuvet s – absorption cross section n molecules d = cross section (cm) or ln (I o a
=absorption coefficient
/I) = a
C d (beer –Lambert law)
C = concentration
• Converting to decimal logs and standardizing quantities we get
•
Log (I
0
/I) =
cd = A
Now
is the decadic molar extinction coefficient
A = absorbance or optical density (OD) a dimensionless quantity
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories d n molecules s – absorption cross section
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Phycobiliproteins are stable and highly soluble proteins derived from cyanobacteria and eukaryotic algae with quantum yields up to 0.98 and molar extinction coefficients of up to 2.4 × 10 6
Protein 488nm
% absorbance
568nm
% absorbance
633nm
% absorbance
B-phycoerytherin
33 97 0
R-phycoerytherin
63 92 0 allophycocyanin
0.5
20 56
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
Data from Molecular Probes Website
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• The rate of emission is dependent upon the time the molecule remains within the excitation state (the excited state lifetime
f
)
• Optical saturation occurs when the rate of excitation exceeds the reciprocal of
f
• In a scanned image of 512 x 768 pixels (400,000 pixels) if scanned in 1 second requires a dwell time per pixel of 2 x 10 -6 sec.
• Molecules that remain in the excitation beam for extended periods have higher probability of interstate crossings and thus phosphorescence
• Usually, increasing dye concentration can be the most effective means of increasing signal when energy is not the limiting factor (ie laser based confocal systems)
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
Material Source:
Pawley: Handbook of Confocal Microscopy
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• Consider 1 mW of power at 488 nm focused to a Gaussian spot whose radius at 1/e 2 intensity is 0.25
m via a 1.25 NA objective
• The peak intensity at the center will be 10 -3 W [
.(0.25 x 10 -4 cm) 2 ]= 5.1 x 10 5 W/cm 2 or 1.25 x 10 24 photons/(cm 2 sec -1 )
• At this power,
FITC would have 63% of its molecules in an excited state and 37% in ground state at any one time
C
21
H
11
NO
5
S
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
Material Source:
Pawley: Handbook of Confocal Microscopy
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• A molecule may undergo a vibrational transition (not an electronic shift) at exactly the same time as scattering occurs
• This results in a photon emission of a photon differing in energy from the energy of the incident photon by the amount of the above energy - this is
Raman scattering.
• The dominant effect in flow cytometry is the stretch of the O-H bonds of water. At 488 nm excitation this would give emission at 575-595 nm
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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• Defined as the irreversible destruction of an excited fluorophore (discussed in later lecture)
• Methods for countering photobleaching
– Scan for shorter times
– Use high magnification, high NA objective
– Use wide emission filters
– Reduce excitation intensity
– Use “ antifade
” reagents (not compatible with viable cells)
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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Not a chemical process
Dynamic quenching =- Collisional process usually controlled by mutual diffusion
Typical quenchers – oxygen
Aliphatic and aromatic amines (IK, NO2, CHCl3)
Static Quenching
Formation of ground state complex between the fluorophores and quencher with a non-fluorescent complex (temperature dependent – if you have higher quencher ground state complex is less likely and therefore less quenching
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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• Many quenchers act by reducing oxygen concentration to prevent formation of singlet oxygen
• Satisfactory for fixed samples but not live cells!
• Antioxidents such as propyl gallate, hydroquinone, pphenylenediamine are used
• Reduce O
2 concentration or use singlet oxygen quenchers such as carotenoids (50 mM crocetin or etretinate in cell cultures); ascorbate, imidazole, histidine, cysteamine, reduced glutathione, uric acid, trolox (vitamin E analogue)
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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•
FITC - at 4.4 x 10 23 photons cm -2 sec -1
FITC bleaches with a quantum efficiency
Q b of 3 x 10 -5
• Therefore
FITC would be bleaching with a rate constant of 4.2 x 10 3 sec -1 so 37% of the molecules would remain after 240
sec of irradiation.
• In a single plane, 16 scans would cause 6-
50% bleaching
Material Source:
Pawley: Handbook of Confocal Microscopy
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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EPI-Illumination
Arc Lamp
Excitation Diaphragm
Excitation Filter
Ocular
Dichroic Filter
Objective
Emission Filter
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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upright inverted
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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Camera goes here
Color CCD camera does not need optical filters to collect all wavelengths but if you want to collect each emission wavelength optimally, you need a monochrome camera with separate emission filters shown on the right. Alternatives include AOTF or liquid crystal filters.
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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Probe
FITC
PE
APC
PerCP ™
Cascade Blue
Coumerin-phalloidin
Texas Red ™
Tetramethylrhodamine-amines
CY3 (indotrimethinecyanines)
CY5 (indopentamethinecyanines)
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
Excitation Emission
610
550
540
640
488
488
630
488
360
350
525
575
650
680
450
450
630
575
575
670
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• Hoechst 33342 (AT rich) (uv)
• DAPI (uv)
• POPO-1
• YOYO-1
• Acridine Orange (RNA)
• Acridine Orange (DNA)
• Thiazole Orange (vis)
• TOTO-1
• Ethidium Bromide
• PI (uv/vis)
• 7-Aminoactinomycin D (7AAD)
346
359
434
491
460
502
509
514
526
536
555
460
461
456
509
650
536
525
533
604
620
655
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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– Metachromatic dye
• concentration dependent emission
• double stranded NA - Green
• single stranded NA - Red
– AT rich: DAPI, Hoechst, quinacrine
– GC rich: antibiotics bleomycin, chromamycin A
3
, mithramycin, olivomycin, rhodamine 800
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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Indo-1
• INDO-1
• QUIN-2
• Fluo-3
• Fura -2
E x
350
E x
350
E x
488
E x
330/360
E m
405/480
E m
490
E m
525
E m
510
INDO-1: 1H-Indole-6-carboxylic acid, 2-[4-[bis[2-[(acetyloxy)methoxy]-2- oxoethyl]amino]-
3-[2-[2-[bis[2- [(acetyloxy)methoxy]-2-oxoetyl]amino]-5- methylphenoxy]ethoxy]phenyl]-,
(acetyloxy)methyl ester [
C
47
H
51
N
3
O
22
] (just in case you want to know….!!)
FLUO-3: Glycine, N-[4-[6-[(acetyloxy)methoxy]-2,7- dichloro-3-oxo-3H-xanthen-9-yl]-2-[2-[2-
[bis[2-[(acetyloxy)methoxy]-2- oxyethyl]amino]-5- methylphenoxy]ethoxy]phenyl]-N-[2-
[(acetyloxy)methoxy]-2-oxyethyl]-, (acetyloxy)methyl ester
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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Probe Excitation Emission
• SNARF-1
C
27
H
19
NO
6
• BCECF
C
27
H
20
O
11
488
488
440/488
575
525/620
525
SNARF-1: Benzenedicarboxylic acid, 2(or 4)-[10-(dimethylamino)-3-oxo-3H- benzo[c]xanthene-7-yl]-
BCECF: Spiro(isobenzofuran-1(3H),9'-(9H) xanthene)-2',7'-dipropanoic acid, ar-carboxy-3',6'-dihydroxy-3-oxo-
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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Probe
Oxidant Excitation Emission
• DCFH-DA
• HE
• DHR 123
(H
2
O
2
)
(O
2
-
)
(H
2
O
2
)
488
488
488
525
590
525
DCFH-DA: 2',7'-dichlorodihydrofluorescein diacetate (2',7'-dichlorofluorescin diacetate; H2DCFDA)
C
24
H
16
C l2
O
7
C
21
H
21
N
3
C
21
H
18
N
2
O
3
DCFH-DA
HE
DHR-123
- dichlorofluorescin diacetate
- hydroethidine
3,8-Phenanthridinediamine, 5-ethyl-5,6-dihydro-6-phenyl-
- dihydrorhodamine 123
Benzoic acid, 2-(3,6-diamino-9H-xanthene-9-yl)-, methyl ester
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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Probe Site Excitation Emission
BODIPY
NBD
Golgi
Golgi
505
488
DPH
TMA-DPH
Lipid
Lipid
350
350
Rhodamine 123 Mitochondria 488
DiO Lipid 488 diI-Cn-(5) diO-Cn-(3)
Lipid
Lipid
550
488
511
525
420
420
525
500
565
500
BODIPY - borate-dipyrromethene complexes NBD - nitrobenzoxadiazole
DPH – diphenylhexatriene TMA - trimethylammonium
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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• GFP Green Fluorescent Protein
– GFP is from the chemiluminescent jellyfish Aequorea victoria
– excitation maxima at 395 and 470 nm (quantum efficiency is 0.8) Peak emission at 509 nm
– contains a p-hydroxybenzylidene-imidazolone chromophore generated by oxidation of the Ser-Tyr-Gly at positions 65-67 of the primary sequence
– Major application is as a reporter gene for assay of promoter activity
– requires no added substrates
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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• Many possibilities for using multiple probes with a single excitation
• Multiple excitation lines are possible
• Combination of multiple excitation lines or probes that have same excitation and quite different emissions
– e.g. Calcein AM and Ethidium ( ex 488 nm )
– emissions
530 nm and 617 nm
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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• The band width of the filter will change the intensity of the measurement
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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Fluorescein molecule
488 nm
Band pass filter
575 nm
PE molecule
450 500 550
Wavelength (nm)
600 650
Overlap of FITC fluorescence in PE PMT
Overlap of PE fluorescence in FITC PMT
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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• Resonance energy transfer can occur when the donor and acceptor molecules are less than 100 Å of one another
(preferable 20-50 Å )
• Energy transfer is non-radiative which means the donor is not emitting a photon which is absorbed by the acceptor
• Fluorescence RET (FRET) can be used to spectrally shift the fluorescence emission of a molecular combination.
3 rd Ed. Shapiro p 90
4 th Ed. Shapiro p 115
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© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
Isolated donor
Donor distance too great
Donor distance correct
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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Non radiative energy transfer – a quantum mechanical process of resonance between transition dipoles
• Effective between
10-100 Å only
• Emission and excitation spectrum must significantly overlap
• Donor transfers non-radiatively to the acceptor
• PE-Texas Red
™
• Carboxyfluorescein-Sulforhodamine B
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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Molecule 1
Molecule 1
DONOR
Donor
Molecule 2
Molecule 2
ACCEPTOR
Acceptor
Absorbance
Absorbance
Wavelength
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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• The longer the wavelength the lower the energy
• The shorter the wavelength the higher the energy
– eg. UV light from sun - this causes the sunburn, not the red visible light
• The spectrum is independent of precise excitation line but the intensity of emission is not
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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When there are two molecules with different absorption spectra, it is important to consider where a fixed wavelength excitation should be placed. It is possible to increase or decrease the sensitivity of one molecule or another.
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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When there are two molecules with different absorption spectra, it is important to consider where a fixed wavelength excitation should be placed. It is possible to increase or decrease the sensitivity of one molecule or another.
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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When there are two molecules with different absorption spectra, it is important to consider where a fixed wavelength excitation should be placed. It is possible to increase or decrease the sensitivity of one molecule or another.
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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• Fluorescence is the primary energy source for confocal microscopes
• Dye molecules must be close to, but below saturation levels for optimum emission
• Fluorescence emission is longer than the exciting wavelength
• The energy of the light increases with reduction of wavelength
• Fluorescence probes must be appropriate for the excitation source and the sample of interest
• Correct optical filters must be used for multiple color fluorescence emission
Go to the web to download the lecture http://tinyurl.com/2dr5p
© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories
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