Lasers and Confocal
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Lasers and Confocal
Laser
• Acronym: Light Amplification by Stimulated
Emission of Radiation
• Ordinary light emission: Comes from
spontaneous decay of excited state to
ground levels
• Stimulated emission: molecule remains in
excited state until stimulated to emit by
incoming light that is insufficient to raise it
to the next higher excited state
Simulation
• http://micro.magnet.fsu.edu/primer/java/las
ers/electroncycle/index.html
Design of a laser
• Medium (such as ruby crystal) that has reflective mirrors
at both ends
• Mechanism to pump energy (stimulated absorption) in
(flashtube, accelerating coils, pump laser) so that we get
a population inversion: circumstyance in which there are
more (atoms, molecules) in the excited state than the
ground state
• Under these circumstances, additional light is more likely
to generate stimulated emission than stimulated
absorption
• At that point, further pulses give stimulated emission.
Design of a laser (cont’d)
• This phenomenon of stimulated emission gives
rise to a standing wave
• That standing wave can generate constructive
interference to escape from the end of the
crystal
Different lasers with different
pumps
Ruby laser
• Ruby laser
• Length of cavity, index of refraction of
material determines wavelength
Note that emission is:
Phase coherent
Nearly
monochromatic
Cavity resonance modes and gain
bandwidth
• Multimode lases are not monochromatic
• Wavelengths of light are extremely small
compared to size of cavity
• Laser modes are distibuted over a narrow
range of frequencies, termed gain
bandwidth
Varying cavity modes can affect
gain bandwidth
• http://micro.magnet.fsu.edu/primer/java/las
ers/gainbandwidth/index.html
Types of lasers
• Argon ion laser – ionize argon gas to produce excited
state
• Continuous wave emission
• http://micro.magnet.fsu.edu/primer/java/lasers/gainband
width/index.html
• Argon ion lasers can produce approximately 10
wavelengths in the ultraviolet region and up to 25 in the
visible region, ranging from 275 to 363.8 nanometers
and 408.9 to 686.1 nanometers, respectively. In the
visible light spectral region
• Typically most power at 458, 488, 514 are in visible
range
Ion laser spectra
Semiconductor diode laser
• Electrical pumping
• Wide variety of wavelengths
Beam shaping in diode lasers
• http://micro.magnet.fsu.edu/primer/java/las
ers/diodelasers/index.html
Ti-sapphire
mode-locked
lasers
Ti-sapphire lasers
• Wavelength adjustable by
changing cavity length
• Modelocking ensures
better monochromacity
• Tunable over a broad
range using prism to
spread spectrum and slit
to select wavelength
Laser illuminators for widefield
fluorescence
• Because lasers are phase coherent, you
set up standing wavers between optical
components
• Results in fringes when you try to image
• Solution: optical fiber mode scramblers
Optical fibers total internal
reflection
Scramblers work by curving optical
fibers to remove phase coherence:
Advantages of laser sources for
widefield fluorescence:
- Monochromacity
- Intense illumination in a
small spot
Confocal laser scan microscopy
• Instead of defocussing source over the
image plane, focus it to a point
• Scan that point over the specimen to buld
up an image
Advantage: Out of focus loght may
be rejected by a paired emission
aperture
Result: Optical sections
Pollen grain optical sections
Reconstruction of optical stacks
Confocal technologie
• Specimen scan confocal
– Use a Piezo device to scan specimen as you
build up images
– Advantage: can be used in transmission
– Major disadvantages:
• specimen size limitation
• Shear on specimen
Laser scan confocal microscope
Advantages:
Flexibility
Ease of use
Disadvantages
Speed
Monochromacity
Cannot be used for
transmitted-light
confocal
Spinning disc confocal
Advantages:
White light
Speed
Disadvantages
Lack of
sensitivity
Intermediate techniques
• Slit scan confocal – Use a cylindrical lens
to spread beam into a fan bean
• Scan that beam across specimen
• Instead of pinhole, use a slit to reject out-
of-focus information, and use a line
detector
– Real time speed
– However, resolution, contrast, and optical
sectioning are nonisotropic
Confocal caveats
• The meaning of optical sections: no
sharply defined boundaries; Gaussian
intensity distribution
• Means that very bright objects can “spill
over”
• Importance of setting black level and gain
• In X and Y, maximum resolution is ~0.1
µm; in Z, approximately 0.8 µm. Problems
for colocalization
The problem of chromatic
aberration
• Lenses that have chromatic abberration
bring different wavelengths to focus at
different points
• Even apchromats are only corrected at blue, green and
red; we often use purple (DAPI) or near infrared (Cy5) dyes
Problems (continued)
• Spherical aberration
– As we focus into a specimen, we are focusing though aqueous
medium.
– If we are using an oil immersion lens, we will get spherical
aberration, because η is wrong
– One solution: High NA water-immersion objectives
• Signal-to-noise: much worse for confocal than
deconvolved widefield
• Fluorophore overlap: rhodamine, for example, is excited
by 488, as well as 514
– Detection: turn of 514 excitation
– Fix
• 1. Use other dyes
• 2. Sequential scanning
• Multispectral analysis to deconvolve overlapping fluorophores
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