Topics • Acoustic Optical Modulator • Faster scanning methods • Laser trapping • Fluorescence lifetime imaging
Dec 15, 2015
Topics
• Acoustic Optical Modulator
• Faster scanning methods
• Laser trapping
• Fluorescence lifetime imaging
Acousto-optic modulator
Bragg Diffraction: sound waves diffract lightCan achieve ~90% diffraction efficiency into 1st order spot
RF (100 MHz) onTransducer sets upAcoustic wave inSecond crystal,Forms grating0th order
Condition for Constructive interference:
Double-slit Experiment
a sinθ = nλ
n = 0, 1, 2, 3 …
After focusing:
d = f λ / a
Applications of Acousto-optic Modulators in microscopes
1) Select Wavelength (tunable filter AOTF): vary drive frequency:Achieve same angle of deflection (wavelength dependent, spacing of grating)
2) Control Laser Power: vary RF power to change diffraction fraction
3) Control Beam angle for fast scanning: vary frequency for same , fixed power (achieves different deflected angle)
AOTF to select laser line and power(drive frequency and RF power, respectively)
Laser line selection
Acousto-optic beam deflector
Scanning in a confocal microscope: very fastCompared to galvo mirrors ~100 fold (paper next week)
Sweep beam byChanging deflection(linearized)
Faster Imaging than with two galvos: line scanning + one galvo
Linear CCDSlit pinholes
Detection on line-scanning microscope
Scanning via spinning disk
Spinning disk microscopy
Uses White light: convenient but very poor light budget
Microlens focuses onPinholes, conjugateTo specimen plane
CCD detection,Much higherquantum efficiencyThan PMT
Modern Design
Light contamination between adjacent pinholes
Spinning disk microscopy
Advantages:1. Can image very rapidly ( image collection not limited
by scanning mirrors
2. Use of cooled CCD camera yields lower noise than PMT (un-cooled) higher quantum yield
Disadvantages:
1. Light path not efficient (need powerful light source)2. Fixed pixel size3. Disk needs to match objective4. Lose spatial control of excitation field5. Problem with very thick samples
Laser Trapping
Light Can Be Bent by Air
• Dielectric material
• n > n(surroundings)
• Force range is in pN
How to measure the force?
xxxF )(Langevin equationStochastic force
xxxF )(Langevin equation
power spectrum )(
)(222c
B
ff
TkfS
Position sensing with Quadrant photodiodes
x = [(B+D) - (A+C)] / [A+B+C+D]y = [(A+B) - (C+D] / [A+B+C+D]
Direct observation of base-pair stepping by RNA polymerase
Nature. 2005 Nov 24;438(7067):460-5
Abbondanzieri EA, Greenleaf WJ, Shaevitz JW, Landick R, Block SM
www.bact.wisc.edu/landick/research.htm
Simple
But low resolution
Stepping size per base pair = 3.4 Å
The Dumbbell Setup
The Concept of Force Clamp
Summary:
1. Decouple from stage
2. Helium environment
3. Passive force clamp
HOT
HolographicOpticalTweezers
Sensitive to environment: pH, ions, potentialSNARF, Calcium Green, CameleonsPerform in vitro calibrations
• Results Not sensitive to bleaching artifacts
• Not sensitive to uneven staining (unless self-quenched)
• Not sensitive to alignment (intensity artifacts)
Fluorescence Lifetime Imaging
iscf
f
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k
nonradiscf
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Fluorescence Quantum Yield φ: important for dyesRatio of emitted to absorbed photons
Measured lifetime is sum ofRates of natural lifetime and non radiative decay paths
(k is rate,(k is rate,Inverse of time)Inverse of time)
Quantum Yield:Quantum Yield:
fk 1
0 Natural lifetime
Unquenched emission:Normal QY, lifetime
Quenched emissionDecreased QY, lifetimee.g. metals, aggregation
Unquenched and Quenched Emission
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2 general approaches: time domain and frequency domain
Short pulse laser modulate CW laser
Frequency Domain Methods for Lifetime Measurements:Modulate laser and measure phase change of fluorescence
Use cw laser (e.g. argon ion)Modulate at rate nearInverse of emission lifetime10-100 MHz
Measure phase changewith Lockin amplifier
Time-domain Widefield Lifetime imaging with ICCD
Variable delayed gate is scannedTo sample exponential decay:Many frames
ICCD has no time intrinsic response: slow readoutGated gain
Two-photon has short pulse laser for time-gating
Time-correlated single photon counting:•most flexibility, most accurate,•samples whole decay•Best time response
Measures time of flight of photonsAfter excitation pulse
Bins data at each time intervalRather than gating
Collect enough photons to approximate exponential:
Slower than gating butBetter measurement, Can separate biexponentials: Multiple components
Principles of time-correlated single photon counting
TAC or TDC measures time of flight, bins photons
B&H addon to Zeiss Laser scanning confocal
Electronics all in one PCI board, ~50K addon
Time gating measurements of fluorescence decayTemporal Resolution defined by IRF (laser, detector, electronics)
IRF=instrument response function,Must be (much) shorter than fluorescence lifetime (delta function)to avoid convolution
Measure IRF with reflectionor known short lifetimee.g. Rose Bengal (90 ps)
Ideal IRF Real IRF
Gate away from IRF (laser pulse, PMT response)Lose photons
PMT Detectors for Lifetime measurements
~300 picosecond resolutionBetter with deconvolutionCost ~$500
~30 picosecond resolutionNo dispersionCost ~$15000fragile
PMTS have low quantum yield(10-20%), MCP worse ~5%
Microchannel plate photomultiplier: full of holes, kick off electrons
Dispersion in time of flightacross 14 dynodesLimits time response
Intensity vs fluorescence lifetime image
Same dye, different lifetime because of environment
FRET Outcomes
Donor decreases
Acceptorincreases
LifetimeIntensity
CFP and YFP FRET by Lifetime Imaging
Channel changes conformation, distance changes, Donor quenching occurs due to FRET
Short lifetime is FRET from DonorFor given pixel Ratio of fast to slow decay coefficientsis estimate of FRET efficiency
FLIM as Diagnostic of Joint Disorder
H&E staining
Widefieldfluorescence
WidefieldFLIM
Little info
Detail revealed by FLIM
Fixed, thin sections
Effects of Pinhole Size
Intensity and lifetime measurements
CFP-YFP linked by short peptide chainEnergy is transferred from CFP to YFPLifetime reveals info intensity does not