Fluorescence and Fluorescent Probes

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BMS 524 - “Introduction to Confocal Microscopy and Image Analysis”

Lecture 5: Fluorescence

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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Overview

• Fluorescence

• The fluorescent microscope

• Types of fluorescent probes

• Problems with fluorochromes

• General applications

© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories

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Learning Objectives

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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Excitation Sources

Excitation Sources

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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Fluorescence

• What is it?

• Where does it come from?

• Advantages

• Disadvantages

© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories

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Fluorescence

• 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

Fluorescence

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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Simplified Jablonski Diagram

1

S’

S

1 hv ex hv em

S

0

© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories

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Fluorescence

Stokes Shift

– 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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Fluorescence Excitation Spectra

Intensity

related to the probability of the event

Wavelength

the energy of the light absorbed or emitted

© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories

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Fluorescence

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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Allophycocyanin (APC)

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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Laser

Light Sources - Lasers

Abbrev.

Excitation Lines

• Argon

• Violet Diode

Ar 353-361, 488, 514 nm

380-405 nm

• Krypton-Ar

Kr-Ar 488, 568, 647 nm

• Helium-Neon He-Ne

543 nm, 633 nm

• He-Cadmium He-Cd

325 - 441 nm

(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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 

 

Arc Lamp Excitation Spectra

Xe Lamp

Hg Lamp

 

  

© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories



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Excitation - Emission Peaks

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

Slide 17 t:/classes/BMS524/524lect003.ppt

Parameters

• 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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Absorbance

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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Relative absorbance of phycobiliproteins

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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Excitation Saturation

• 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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How many Photons?

• 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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Raman Scatter

• 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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Photobleaching

• 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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Quenching

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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Antifade Agents

• 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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Photobleaching example

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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Fluorescent Microscope

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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Fluorescence Microscope

upright inverted

© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories

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Cameras and emission filters

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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Probes for Proteins

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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Probes for Nucleic Acids

• 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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DNA Probes

• AO

– Metachromatic dye

• concentration dependent emission

• double stranded NA - Green

• single stranded NA - Red

• AT/GC binding dyes

– 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

Probes for Ions

• 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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pH Sensitive Indicators

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

Probes for Oxidation States

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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Specific Organelle Probes

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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Other Probes of Interest

• 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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Multiple Emissions

• 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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Filter combinations

• 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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Fluorescence Overlap

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

• 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

FRET properties

Isolated donor

Donor distance too great

Donor distance correct

© 1993-2007 J. Paul Robinson - Purdue University Cytometry Laboratories

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Energy Transfer

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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Resonance Energy Transfer

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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Fluorescence

• 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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Mixing fluorochromes

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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Mixing fluorochromes

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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Mixing fluorochromes

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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Conclusions

• 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

Slide 52 t:/classes/BMS524/524lect003.ppt

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