“Breaking the diffraction barrier in fluorescence microscopy at low light intensities by using...

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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
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Page 1: “Breaking the diffraction barrier in fluorescence microscopy at low light intensities by using reversibly photoswitchable proteins” M. Hoffmann, C. Eggeling,S.

“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 PRESENTATION2/13/2006

Mehmet Dogan

Page 2: “Breaking the diffraction barrier in fluorescence microscopy at low light intensities by using reversibly photoswitchable proteins” M. Hoffmann, C. Eggeling,S.

OUTLINE

• Background:– Resolution,– STED, – RESOLFT

• Photoswitching • Characterization of switch kinetics of protein: asFP595• Demonstration of RESOLFT idea : ~100nm resolution• Conclusions

Page 3: “Breaking the diffraction barrier in fluorescence microscopy at low light intensities by using reversibly photoswitchable proteins” M. Hoffmann, C. Eggeling,S.

Resolution Limit

Abbe’s Diffraction Limit:

sin2n

x

Abbe’s Equation Modified for Fluorescence:

1sin2nx

0 Abbe Limit

0x

Saturation FactorsatIxI /)(

Page 4: “Breaking the diffraction barrier in fluorescence microscopy at low light intensities by using reversibly photoswitchable proteins” M. Hoffmann, C. Eggeling,S.

Requirements for Subdiffraction Resolution

• Large saturation factor– Either large I(x)

– Or small saturation intensity Isat

• Spatial intensity zero

satIxI /)(

Isat

I(x)

x

saturated saturated

Page 5: “Breaking the diffraction barrier in fluorescence microscopy at low light intensities by using reversibly photoswitchable proteins” M. Hoffmann, C. Eggeling,S.

Reversible Saturable Optical Fluorescent Transition (RESOLFT)

A B)(xIk ABAB

BAk BAAB

BAA kk

kN

At Equilibrium:

BAAB

BAA kxI

kN

)(

sat

A

IxI

N)(

1

1

AB

BAsat

kI

dt

dNNkNk

dt

dN BBBAAAB

A

Rate Equations:

tkk

k

k

kk

ktN BAAB

AB

BA

BAAB

ABA exp)(

Normalized Populations:

Page 6: “Breaking the diffraction barrier in fluorescence microscopy at low light intensities by using reversibly photoswitchable proteins” M. Hoffmann, C. Eggeling,S.

Spatial Intensity Zero for Increased Resolution

Page 7: “Breaking the diffraction barrier in fluorescence microscopy at low light intensities by using reversibly photoswitchable proteins” M. Hoffmann, C. Eggeling,S.

A Subset : STEDStimulated Emission Depletion

• State A: Fluorescent State• State B: Non-fluorescent ground state

IkStE

Stimulated Emission vs. Spontaneous Emission

spk

I2/100 cmMW

kI spsat

Too high saturation intensity Photo induced damage

Page 8: “Breaking the diffraction barrier in fluorescence microscopy at low light intensities by using reversibly photoswitchable proteins” M. Hoffmann, C. Eggeling,S.

Alternative Approach: Reduced Isat

)/(1sin2 satIInx

Systems with weak spontaneous interstate conversions

Remember:

spsat kI

Photoswitchable Fluorophores:ssFP595 : Photochromic Fluorescent Protein

ON State (A) : fluorescence-activated

OFF State (B) : fluorescence-inhibited450 nm 560 nm

Page 9: “Breaking the diffraction barrier in fluorescence microscopy at low light intensities by using reversibly photoswitchable proteins” M. Hoffmann, C. Eggeling,S.

Photoswitching

Photoswitching of protein in E-coli with wide field epifluorescence microscope

Photoswitching of thin protein layer on a 0.3 µm focal spot

Iy= 2 W/cm2

Ib=0.1 W/cm2

Iy= 4.4 W/cm2

Ib=3.6 W/cm2

Py=3.3 nW

Pb=2.2 nW

8 orders of magnitude less than STED

Page 10: “Breaking the diffraction barrier in fluorescence microscopy at low light intensities by using reversibly photoswitchable proteins” M. Hoffmann, C. Eggeling,S.

Drawbacks

1) Low quantum yield: <1%

2) Incomplete OFF (15% fluorescence)

3) Photobleaching with cycling

4) Intensity to be adjusted for fluorescence settling

Page 11: “Breaking the diffraction barrier in fluorescence microscopy at low light intensities by using reversibly photoswitchable proteins” M. Hoffmann, C. Eggeling,S.

Effects of Iy and Ib on Inhibition

Isat~ 1 W/cm2

Page 12: “Breaking the diffraction barrier in fluorescence microscopy at low light intensities by using reversibly photoswitchable proteins” M. Hoffmann, C. Eggeling,S.

Effect of Iy

Larger Iy gives larger Residual Fluorescence

Strong inhibition and small fluorescence settling time

Page 13: “Breaking the diffraction barrier in fluorescence microscopy at low light intensities by using reversibly photoswitchable proteins” M. Hoffmann, C. Eggeling,S.

Subdiffraction focal spots

Solid lines: calculated

Dashed lines: measured

Focal spot with two offset peaks using phase plate

y

x

Page 14: “Breaking the diffraction barrier in fluorescence microscopy at low light intensities by using reversibly photoswitchable proteins” M. Hoffmann, C. Eggeling,S.

Effective PSFCalculated effective PSF using experimental values

Calculated Effective PSF using theoretical values

Incomplete inhibition of fluorescence at the periphery:

RESOLFTdiff PSFPSFPSFE )1(

0.3

Page 15: “Breaking the diffraction barrier in fluorescence microscopy at low light intensities by using reversibly photoswitchable proteins” M. Hoffmann, C. Eggeling,S.

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

Page 16: “Breaking the diffraction barrier in fluorescence microscopy at low light intensities by using reversibly photoswitchable proteins” M. Hoffmann, C. Eggeling,S.

scan

a-c

a-f

d-e

20nm steps

50ms dwell time

Iy= 600W/cm2

Ib=30 W/cm2

Page 17: “Breaking the diffraction barrier in fluorescence microscopy at low light intensities by using reversibly photoswitchable proteins” M. Hoffmann, C. Eggeling,S.

Conclusion• Demonstration of resolution increase with

photoswithing at low power• New proteins should be engineered

Challenges• Low quantum yield (1%)• Slow switching requires ms integration• Action cross-talk