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Bi177 - Lecture 13 Microscopy Outside the Box Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALM

Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

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Page 1: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

Bi177 - Lecture 13 Microscopy Outside the Box

Fluorescence Nanoscopy

TIRF

4-pi

STED

STORM/PALM

Page 2: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

The diffraction limit: Abbe’s law

Page 3: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

Diffraction limit 100x larger than molecular scale!

1 nm

Green Fluorescent Protein Diffraction Limited Spot

100 nm

The Problem…

Page 4: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

Can we improve the resolution when focusing light with an objective?

First, improving z resolution?

Why Z << XY ?Because the process of focusing is not optimal with an obvious asymmetry resulting from the main direction of light propagation.

2 ways to improve z-resolution:

- near-field approach: evanescent wave microscopy or TIRF

- far-field approach: with an optimal illumination (4 solid angle): Z = XY

Page 5: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

Total Internal Reflection

Page 6: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

How far does the evanescent wave propagate?

221

221 sin41 nn

d

d

zeIzI

0)(

5.6233.15.1 21 cnn et

Angle critique : )/arcsin( 12 nnc

et 8.410.15.1 21 cnn

d62.5 65 170 nm70 100 nm75 83 nm

d41.8 50 84,4 nm60 57,6 nm65 51,8 nm

nm) ( 600

Page 7: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

Epifluorescence Evanescent only

Total Internal Reflection Fluorescence (TIRF) imaging

Like other near-field imaging: limited to the surface, no 3D imaging!

Problem 2: “Frustrated TIRF” (higher cell index of refraction deeper)

Page 8: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

4Pi microscopy: the principle

Engineering the focal volume using interference

Page 9: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

Up to 7x better axial resolutioneg: 4Pi-TPLSM up to 80nm z-resolution!

Required to squeeze the sample between two objectives… thin sample only!

4Pi microscopy: the setup

Page 10: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

(a) MMM-4Pi microscopy(b) GFP labeled compartments of Saccharomyces cerevisiae(c) Golgi apparatus in a live Vero cell

Hell SW, Nature Biotechnology (2003)

4Pi microscopy: applications

Page 11: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

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STED is based on stimulated emission

Spontaneous fluorescence emission Stimulated fluorescence emission

The perturbing photon with the correct energy is seemingly unchanged in the process, and the stimulated emission generate a second

photon with the same phase, frequency/energy, polarization, and direction of

travel as the first one.

Slide from Michael Liebling, UCSB

Page 12: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

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STED: breaking the resolution limit by shaving the PSF

Hell SW, Nature Biotechnology (2003)

Page 13: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

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STED: breaking the resolution limit by shaving the PSF

Page 14: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

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STED can break the diffraction limit!

Page 15: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

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STED microscopy summary

Slide from Michael Liebling, UCSB

Page 16: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

STochastic Optical Reconstruction Microscopy(STORM)

and/or

Photo-Activated Localization Microscopy (PALM)

and/or

Fluorescent Photo-Activated Localization Microscopy (FPALM)

Page 17: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

σ σPSF / N1/2

Thompson at al., Biophys. J., 2002

Finding out the position of a molecule

Yildiz et al., Science, 2003

Fluorescence Imaging with One-Nanometer Accuracy (FIONA)

= single molecule detection

By fitting the signal profile from a single molecule, its position can be estimated

with an accuracy higher than the resolution of the microscope!

Note: resolution localization precision

Hari Shroff, Janelia Farm Reseach Campus, HHMI

Page 18: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

The principle of STORM

How to excite only a few fluorophores at a time???By using low level photo-activation = ability to turn molecules on/off

Page 19: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

Activation

Imaging laser (657 nm)

Activation laser (532 nm)

Cy3 Cy5

Cy3 Cy5Cy3 Cy5

20151050

Activation laser pulses

Cy5 fluorescence

Time (s)

Activator Reporter

6000 photons

STORM requires photo-switchable probes

Page 20: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

STORM use Cy3 to rejuvenate Cy5Cycles of low level activation / imaging / localization / desactivationAt each cycle, only a few molecules are activated within the field of view: the density is low enough to avoid overlap between fluorophores

Page 21: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

Activ

ator

abs

orpt

ion

(nm

)

Reporter emission (nm)

Alexa 405

Cy2

Cy3

Cy5 Cy5.5 Cy7

665 690 775

550

490

400

Alexa 647

20151050

time (s)

3020100time (s)

Activation pulses

Activation pulses

Activation pulses

Fluo

resc

ence

Fluo

resc

ence

Fluo

resc

ence

405 nm532 457

Bates et al, Science 317, 1749 – 1753 (2007)

More colors?

Page 22: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

STORM resolution validated by DNA yardstick

Page 23: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

200 nm

PALM: Photo-Activated Localization MicroscopyFPALM: Fluorescent Photo-Activated Localization Microscopy

Exactly the same concept but using photo-activated fluorescent proteins

Good: genetically encoded approachBad: photo-activation is not reversible! It requires to bleach the molecule after each cycle (photo-toxicity, loss of signal,…)…but reversible photo-switchable proteins can be used now!

STORM-PALM-FPALM imaging

PALMBetzig E, et al: Imaging intracellular fluorescent proteins at nanometer resolution, Science (2006)

FPALMHess ST, et al: Ultra-high resolution imaging by fluorescence photoactivation localization microscopy, Biophysical J. (2006)

STORM:Rust MJ, et al: Sub-diffraction-limit imaging by stochastic optical reconstruction microscopy (STORM), Nature Methods (2006)

Page 24: Fluorescence Nanoscopy TIRF 4-pi STED STORM/PALMbi177/private/L13_handout.pdf · Microsoft PowerPoint - L13_0227_STED_STORM.ppt [Compatibility Mode] Author: dani Created Date: 2/29/2012

Conclusions:

Statistical approaches to reconstruct images: these techniques permit to reconstruct the distribution of fluorophores within an image with ultra-high accuracy (<<resolution of the microscope).

They require many cycles of activation/localization (several thousands of images acquired for one reconstruction!)= low time resolution!

STORM-PALM-FPALM imaging