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“Breaking the diffraction barrier in fluorescence microscopy at low light intensities by using reversibly photoswitchable proteins”. M. Hoffmann, C. Eggeling,S. Jakobs, S.W. Hell. JOURNAL CLUB PRESENTATION 2/13/2006 Mehmet Dogan. OUTLINE. Background: Resolution, STED, RESOLFT
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“Breaking the diffraction barrier in fluorescence microscopy at low light intensities by using reversibly photoswitchable proteins” M. Hoffmann, C. Eggeling,S. Jakobs, S.W. Hell JOURNAL CLUB PRESENTATION 2/13/2006 Mehmet Dogan
OUTLINE • Background: • Resolution, • STED, • RESOLFT • Photoswitching • Characterization of switch kinetics of protein: asFP595 • Demonstration of RESOLFT idea : ~100nm resolution • Conclusions
Abbe’s Equation Modified for Fluorescence: Abbe Limit Saturation Factor Resolution Limit Abbe’s Diffraction Limit:
Requirements for Subdiffraction Resolution • Large saturation factor • Either large I(x) • Or small saturation intensity Isat • Spatial intensity zero • I(x) • Isat saturated saturated x
At Equilibrium: A B Rate Equations: Normalized Populations: Reversible Saturable OpticalFluorescent Transition (RESOLFT)
Stimulated Emission vs. Spontaneous Emission Too high saturation intensity Photo induced damage A Subset : STEDStimulated Emission Depletion • State A: Fluorescent State • State B: Non-fluorescent ground state
Photoswitchable Fluorophores: ssFP595 : Photochromic Fluorescent Protein ON State (A) : fluorescence-activated OFF State (B) : fluorescence-inhibited 560 nm 450 nm Alternative Approach: Reduced Isat Remember: Systems with weak spontaneous interstate conversions
Photoswitching Photoswitching of thin protein layer on a 0.3 µm focal spot Photoswitching of protein in E-coli with wide field epifluorescence microscope Py=3.3 nW Pb=2.2 nW Iy= 4.4 W/cm2 Ib=3.6 W/cm2 Iy= 2 W/cm2 Ib=0.1 W/cm2 8 orders of magnitude less than STED
Drawbacks • Low quantum yield: <1% • Incomplete OFF (15% fluorescence) • Photobleaching with cycling • Intensity to be adjusted for fluorescence settling
Effects of Iy and Ib on Inhibition Isat~ 1 W/cm2
Effect of Iy Larger Iy gives larger Residual Fluorescence Strong inhibition and small fluorescence settling time
Subdiffraction focal spots Solid lines: calculated Dashed lines: measured x Focal spot with two offset peaks using phase plate y
Effective PSF Calculated Effective PSF using theoretical values Calculated effective PSF using experimental values Incomplete inhibition of fluorescence at the periphery: 0.3
Imaging Test Samples Grooves on test slides with focused ion beam milling 10µm long 100nm wide 0.5-1µm deep Separation: 500nm Immersion into buffer with asFP595: Grooves filled by adsorption
scan 20nm steps 50ms dwell time Iy= 600W/cm2 Ib=30 W/cm2 a-c a-f d-e
Conclusion Challenges • Low quantum yield (1%) • Slow switching requires ms integration • Action cross-talk • Demonstration of resolution increase with photoswithing at low power • New proteins should be engineered