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BMS 631 - LECTURE 5 Flow Cytometry: Theory J.Paul Robinson Professor of Immunopharmacology & Biomedical Engineering Purdue University. Light Sources & Optical systems. Hansen Hall, B050 Purdue University Office: 494 0757 Fax 494 0517 email; [email protected]

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BMS 631 - LECTURE 5Flow Cytometry: TheoryJ.Paul Robinson Professor of Immunopharmacology & Biomedical Engineering Purdue University

Light Sources & Optical systems

Hansen Hall, B050

Purdue University

Office: 494 0757

Fax 494 0517

email\; [email protected]


Shapiro 97-115

illumination sources
Illumination Sources
  • Lamps
      • Xenon-Mercury
      • Mercury
  • Lasers
      • Argon Ion (Ar)
      • Krypton (Kr)
      • Helium Neon (He-Ne)
      • Helium Cadmium (He-Cd)
      • YAG

3rd Ed. Shapiro p 98

optics light sources epilumination in flow cytometers
Optics - Light SourcesEpilumination in Flow Cytometers
  • Arc-lamps
    • provide mixture of wavelengths that must be filtered to select desired wavelengths
    • provide milliwatts of light
    • inexpensive, air-cooled units
    • provide incoherent light


3rd Ed. Shapiro p 98

arc lamp excitation spectra
Arc Lamp Excitation Spectra

Xe Lamp



Irradiance at 0.5 m (mW m-2 nm-1)

Hg Lamp


   

3rd Ed. Shapiro p 99

optics optical channels
Optics - Optical Channels
  • An optical channel is a path that light can follow from the illuminated volume to a detector
  • Optical elements provide separation of channels and wavelength selection
spot illumination lasers
Spot Illumination - Lasers
  • Advantages are that the pathway is easier to define (you know where the light is going !!)
  • It is usually monochromatic light so excitation filters are not needed
  • Brighter source of light than arc lamps (higher radiance)
  • Spot size (d) can be calculated by formula
    • d=1.27(F/D) where D is the beam diameter in mm and F is the focal distance from the lens
  • For a 125 mm focal length spherical lens at 515 nm is 55 um and 61 um at 458 nm

3rd Ed. Shapiro p 103

  • Coherent Enterprise laser - UV-visible
  • Air cooled laser (Argon)
laser power noise l ight a mplification by s timulated e mission of r adiation
Laser Power & NoiseLight Amplification by Stimulated Emission of Radiation
  • Laser light is coherent and monochromatic (same frequency and wavelength)
  • this means the emitted radiation is in phase with and propagating in the same direction as the stimulating radiation
  • ION lasers use electromagnetic energy to produce and confine the ionized gas plasma which serves as the lasing medium.
  • Lasers can be continuous wave (CW) or pulsed (where flashlamps provide the pulse)
  • Laser efficiency is variable - argon ion lasers are about 0.01% efficient (1 W needs 10KW power)

3rd Ed. Shapiro p 106


Images only available for in-house use

Not for publication purposes

argon krypton lasers
Argon & Krypton Lasers

Kr-Ar laser (488, 568, 647 nm lines) (Front)

3rd. Ed. Shapiro p 108

dye lasers
Dye Lasers
  • Dye lasers use a source laser known as the pump laser to excite another laser known as the dye laser.
  • The dye laser consists of a flowing dye which exhibits desirable properties such as excitation and emission.
  • The lasing medium is a fluorescent dye (e.g. Rhodamine 6G) which is dissolved in an organic solvent such as ethanol or ethylene glycol
  • The laser can be tuned, usually by a rotatable filter or prism
  • The dye must be circulated and cooled to prevent it being bleached or over-heated

3rd. Ed.Shapiro p 110

helium neon lasers
Helium-Neon Lasers
  • He-Ne - low power, no cooling needed
  • Cheap, mostly emit red light at 633 nm
  • Generally 0.1 W to 50 mW power
  • Lines available include green (543nm) and red 633 nm, 594nm or 611 nm.

3rd. Ed. Shapiro p 110

helium cadmium lasers
Helium-Cadmium Lasers
  • He-Cd laser
  • 5-200mW power usually at 325 nm (UV) or 441 nm (blue)
  • Wall power, air cooled
  • Uses cadium vapor as the lasing medium
  • Major problem is noise (plasma noise between 300-400 kHz)
  • RMS noise mostly about 1.5%
  • Good for ratio measurements (pH or calcium) because power fluctuations don’t matter here – these lasers do have power fluctuation problems eventually.

He-Cd laser

3rd. Ed. Shapiro p 111

diode lasers
Diode Lasers
  • Small, efficient, cheap
  • Only red wavelengths available at reasonable prices (blue works, but still problems)
  • Mostly made of Gallium aluminum arsenide (GaAlAs)
  • Emission ratio is varied by changing the ration of gallium to aluminum in the semiconductor
  • Main use is CD players (now 2 in every household!! One in the stereo and one in the computer! And maybe one in the laser printer!)
  • Biggest problem is not power - but lack of fluorescent probes to be excited at 650-900 nm
  • Problem is poor beam profiles for diode lasers
  • Noise levels are generally 0.05% or less compared to 1% for air cooled argon and .02% with water cooled argon lasers

3rd Ed. Shapiro p113

solid state lasers
Solid State Lasers
  • Neodynymium-YAG (Yttrium aluminum garnet) lasers
  • Lasing medium is a solid rod of crystalline material pumped by a flashlamp or a diode laser
  • 100s mWs at 1064 nm
  • can be doubled or tripled to produce 532 nm or 355 nm
  • Noisy - and still reasonably expensive (particularly the double and tripled versions)
lasers hazards
Lasers Hazards
  • Laser light is very dangerous and should be treated as a significant hazard
  • Water cooled lasers have additional hazards in that they require high current and voltage in addition to the water hazard
  • Dye lasers use dyes that can be potentially carcinogenic

3rd. Ed. Shapiro p 114

summary so far
Summary so far….
  • Arc lamps are useful for flow cytometry because of low cost and wide spectral characteristics
  • Arc lamps require more complex optical trains
  • Lasers provide light at high radiance
  • Lasers are essentially monochromatic, coherent
  • Lasers represent a significant hazard
goals of light collection
Goals of Light Collection
  • Maximum signal, minimum noise
  • Maximum area of collection
  • Inexpensive system if possible
  • Easy alignment
  • Reduced heat generation
  • Reduced power requirement
optical collection systems
Optical Collection systems

2nd Argon Laser

He-Ne Laser

Argon Laser

He-Cd Laser

Optical layout of an Elite sorter at Purdue University

  • 1.3 NA objective


Harald Steen’s Bryte Cytometer

field stops obscuration bars
Field stops & obscuration bars
  • Obscuration bar is placed along the path of the illuminating beam
  • It blocks the direct light but allows the fluorescence signal (which is going in all directions)
  • In a capillary or cuvet system, a field stop which is placed in the image plane achieves the same result
optical translators
Optical translators

No cytometer should be without one!!!

The laser beam remains parallel, but horizontally translated. This reduces the difficulty in aligning the laser.

the point of a good optical system is to obtain a good signal vs noise
The point of a good optical system is to obtain a good Signal Vs Noise
  • Good optical filters
  • Remove as much excitation signal as possible
  • Collect as much fluorescence as possible (use concave spherical mirrors)
spectral selection next lecture
Spectral Selection(Next lecture)
  • Monochromators Vs Filters
  • Filters are reasonably inexpensive
lecture summary
Lecture Summary
  • After completing this lecture you should understand:
  • Excitation light sources and their properties
  • Each light source has unique utility
  • Optical components together with light source creates an optical system
  • The general nature of optical systems in typical cytometers