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1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013 Copyright Jim Gipe/Pivot Media

1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Page 1: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Seeing at the NanoscaleNew Microscopies for the Life Sciences

Dr. Jennifer Ross, Department of Physics

University of Massachusetts AmherstJuly 9, 2013

Copyright Jim Gipe/Pivot Media

Page 2: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Biology: Bridging Meters to Nanometers

Page 3: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Brain

Very complicated100 Billion cells10 Trillion+ interconnections

Worse than the internet

Page 4: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Axon of nerve cell, Baas Lab, Drexel

Nerve Cells

Cell Body

Axon

Dendrites

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Page 5: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Structure and Function

Cell Body

Growth ConeAxon

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Page 6: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Bones of the Cell

Microtubules

Page 7: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Girders

Page 8: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Long Distance Support

The nerve of you,Body Worlds

3 fe

et =

1 m

eter

Page 9: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Long Distance Support

Axon

Growth ConeCommunications

Hub

CellBody

Page 10: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Growth ConeCommunications

Hub

Long Distance Communications

Cell Body

Axon

Page 11: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Growth ConeCommunications

Hub

Long Distance Maintenance

Cell BodyFactory

Axon

Page 12: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Long Distance Maintenance

Growth ConeCommunications

HubFinal Destination Cell Body

Factory

AxonThroughway

How can we get from Point A to Point B?

Page 13: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Diffusion

3 feet = 1 meter

Robert BrownBrownian Motion,

1827

Albert EinsteinDiffusion

Equation, 1905

Page 14: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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3000 Years Later...

3 feet = 1 meter

Some neuronal cells can be up to 1 m long to connect your toes to your spinal cord

If particles diffuse with a diffusion coefficient of:

How long will it take a 4 nm protein to diffuse down the 1-meter axon filled with cytoplasm that is 5x more viscous than water?

Hint: What are the units of the diffusion coefficient?

Page 15: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Highways

AxonThroughway

Page 16: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Big Rigs

Page 17: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Big Rigs

Some neuronal cells can be up to 1 m long to connect your toes to your spinal cord

Motor proteins transport goods up and down the axon taking 8 nm steps.

How many steps do they need to take to go from the cell body (soma) to the axon terminals, 1 m away?

If they travel at a velocity of 1 μm/s, how long will the trip take?

Page 18: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Nano Motors

NO: Walking BackwardNO: Turning Around

Feet are stuck to the highway in a specific direction.

Uses ATP as an energy source (1 ATP per step)

Kinesin = Motion protein

Page 19: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Big Rig Cargo

Motors walk cargo:Organelles (mitochondria)Vesicles carrying signaling molecules to talk to the other cells.Protein structures (other microtubules, RNA)

Page 20: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Big Rig Cargo

Multiple Motors bind to cargo

Page 21: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Big Rig Cargo

Multiple Motors bind to cargo

Can have different types of motors that walk in different directions = TUG OF WAR

Dynein = force protein

Page 22: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

QuickTime™ and aGIF decompressor

are needed to see this picture.

Motor ExperimentsFilament Gliding

Page 23: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

QuickTime™ and a decompressorare needed to see this picture.

Motor ExperimentsSingle Molecule

Single MoleculeImaging

Page 24: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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QuickTime™ and aSorenson Video decompressorare needed to see this picture.

Micro-parasol

Black Particles: melanosomes

Dark pigment-filled vesicles (10-100 nm).

Page 25: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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QuickTime™ and aSorenson Video decompressorare needed to see this picture.

Micro-parasol

Black Particles: melanosomes

Dark pigment-filled vesicles (10-100 nm).

Protect your cells’ nuclei from harmful UV rays

Micro-parasol

Page 26: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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QuickTime™ and aSorenson Video decompressorare needed to see this picture.

Micro-parasol

Powered by motor proteins that walk on microtubule and actin filaments

Micro-parasol

Page 27: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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How do we Visualize Single Molecules at Nanoscale?

When you illuminate a sample in epi-fluorescence, a rather large volume is illuminated

Causes background fluorescence

Many molecules in the field

How can we see single molecules?Slide

Cover glass

Inverted objective

Page 28: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Visualizing Single Molecules

1) Dilute the sample

Page 29: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Visualizing Single Molecules

• Dilute the sample

1) We could use a confocal spot with apertures to block out-of-plane fluorescence

Page 30: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Visualizing Single Molecules

• Dilute the sample

• We could use a confocal spot with apertures to block out-of-plane fluorescence

1) Total Internal Reflection Fluorescence

My method of choice

Page 31: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Total Internal Reflection Fluorescence Microscopy

Focus laser on back-focal plane of objective

It comes out collimated

Page 32: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Total Internal Reflection Fluorescence Microscopy

Move focused spot to edge of back focal plane

Collimated beam tilts

Why does the light bend?

Page 33: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Total Internal Reflection Fluorescence Microscopy

Move to far edge so that angle > critical angle for total internal reflection

Snell’s Law says: n1 sin (θ1) = n2 sin (θ2)

Calculate:

If nglass = 1.51 and nwater = 1.38, what is the “critical angle” for total internal reflection? (When does θ2 = 90°?)

Page 34: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Total Internal Reflection Fluorescence Microscopy

Zoom in on Evanescent Wave

Decays exponentially in z

Only about 100 nm into sample

Brighter is closer to cover glass

Only molecules within 100 nm are visible

Page 35: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Total Internal Reflection Fluorescence Microscopy

Zoom in on Evanescent Wave

Decays exponentially in z

Only about 100 nm into sample

What does an exponential decay look like?

Plot it.

If it dies off after 100 nm, what does that tell you about the decay

constant??

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Page 36: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Resolution Limits to Imaging Single MoleculesA motor protein takes an 8 nm step, can we measure that in our single molecule assay?

Please vote by holding up the number of fingers you want to vote for: (1) Yes. (2) No.

Page 37: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Resolution Limits to Imaging Single MoleculesA motor protein takes an 8 nm step, can we measure that in our single molecule assay?

Ideally, the motor is only about 4 nm, so an 8 nm step should be visible

But it’s not resolvable…

Page 38: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Resolution Limits to Imaging Single MoleculesWhy?? Why can’t we see the step?

What is resolution??

What is the resolution of our microscope?

Page 39: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Resolution Limits to Imaging Single MoleculesWhy?? Why can’t we see the step?

What is resolution??

The quantifiable ability to resolve or distinguish between two items. In this case, the items are the images of the same molecule at two positions.

Why does it happen??

Because light is a wave, we cannot focus it infinitely well. This is a fundamental physical limit of all imaging systems.

What is the resolution of our microscope?

Microscope resolution:

Distance resolvable:

Page 40: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Resolution Limits to Imaging Single MoleculesWhy?? Why can’t we see the step?

The objective diffracts the light, because it is a wave. Water waves diffract, too:

θ

NA = n*sinθmax

n = index of refraction

This is the diffraction limit

Water waves diffracting through a hole in barrier

Page 41: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Resolution Limits to Imaging Single MoleculesWhy?? Why can’t we see the step?

θ

NA = n*sinθmax

n = index of refraction

Calculate:

What is θmax if the NA of my objective is 1.49 and the index of refraction, n, is 1.51?

Page 42: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Resolution Limits to Imaging Single MoleculesDiffraction limited spot for a high-NA objective

Calculate:

What is d if the NA of my objective is 1.49 and the wavelength of light is 508 nm?

Page 43: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Resolution Limits to Imaging Single MoleculesDiffraction limited spot for a high-NA objective

How can we improve our resolution?

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Super-resolutionUse math tricks!

Intensity of diffraction-limited spot highest at center

Actually a Bessel function, but is well-fit by a 2-D Gaussian

Fit the shape of the intensity to find the center with high accuracyIn

ten

sity

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FIONA: Fluorescence Imaging with One Nanometer Accuracy

Replace the fuzzy spot with a 2-20 nm dot

More photons (brighter spot) leads to better “resolution” and a smaller dot.

Page 46: 1 Seeing at the Nanoscale New Microscopies for the Life Sciences Dr. Jennifer Ross, Department of Physics University of Massachusetts Amherst July 9, 2013

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Large enough to be resolved

Not resolvable

Here, resolution is limited by pixel size - not fundamental properties of light

Effect of pixel size on resolution

Gaussian fitting gives better than 1 pixel accuracy

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FIONA: Fluorescence Imaging with One Nanometer AccuracyFollow the motor for multiple frames

More photons, better fitting

The diffraction limit is broken! 64

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Summary

Thank you for your attention!

Molecular biology exists, organizes, and engineers on the nano-scale

Amazingly, these organizational principles are at the core of all animals from bacteria and yeast to people and elephants!

New optical techniques requiring math tricks are required to see these nano-processes