Title: Announcements, Agenda Week 3
1Announcements, Agenda Week 3
- Reading for today Ch. 1, 2 in Hibbs, Zucker 2006
- Start up your computers you will need them for
some in-class exercises. - Open todays Power point slides and Internet
Explorer
- Lecture Intro to Confocal, optics
- Paper discussion Zucker 2006
- TBA Collect Z-series of Artemia samples
- Assignment due Jan. 29
2TBA times with Dr. Hertzler Spring 2007
3Outline Understanding Microscopy
- Introduction to Confocal Microscopy
- Confocal versus conventional (widefield)
fluorescence - Optical sectioning
- Imaging modes and applications
- Advantages, limitations of confocal
- Essential Optics
- Wave/particle nature of Light
- Diffraction
- Numerical aperture
- Lateral resolution
- Axial resolution
- Useful resource Molecular Expression Microscopy
Primer - http//micro.magnet.fsu.edu/primer/index.html
4Laser Scanning Confocal Microscope Components
Scan Head
Microscope
Controller box
Laser
Computer, display
51. Conventional versus confocal fluorescence
Conventional epifluorescence
Confocal epifluorescence
Sea urchin eggs (100 µm diameter) stained with
antibody to tubulin.
6Widefield
Confocal
Sunflower pollen grain
Human brain slice
Rabbit muscle fibers
7Wide-field fluorescence dichroic (dichromatic)
mirror
8Confocal Light Path
- Confocal means having the same focus.
- Basis of optical sectioning coherent light
emitted by the laser system (excitation source)
passes through a pinhole aperture that is
situated in a conjugate plane (confocal) with a
scanning point on the specimen and a second
pinhole aperture positioned in front of the
detector (a photomultiplier tube).
92. Optical slicing
103. Imaging Capabilities
- XY fluorescence imaging
- Single
- Double
- Single or Double transmitted (not confocal)
- 3-channel (need 3 lasers)
- XYZ imaging, 3-D reconstruction
- Time-lapse
- Including 4D
11Applications
- Immunolabelling
- Organelle ID
- Protein trafficking
- Locating genes on chromosomes
- Analysis of molecular mobility
- Multiple labeling
- Live cell imaging
- Transmission imaging
- Measurement of subcellular functions and ion
concentrations
124. Advantages, limitations of confocal microscopy
- Optical sectioning ability
- Can image cells/tissues internally
- 3D reconstruction
- Improved spatial relationships of structures
- Excellent resolution
- Close to theoretical limit of LM 0.2 µm
- Improved multiple labeling
- Since specific wavelengths of light used by
lasers - Very high sensitivity
- Capable of collecting single fluorescent molecule
- Easy manipulation and merging of images
- Since they are digital
- Computer controlled
- Complex settings can be programmed and recalled.
- Expensive to buy and maintain.
- 250,000
- Difficult to operate.
- Fixed material easy, live difficult.
- Fluorescent tag usually required.
- May be bulky or toxic
- Objects smaller than 0.2 not resolved
- Need to use EM.
- Damaging high intensity laser
- Need to minimize exposure, especially in live
cells. - Digital images are easily mishandled.
- Honesty in imaging very important.
13B. Basic Optics1. The nature of light
- Light behaves as both a particle and a wave.
- Can bounce (reflect) and bend (diffract or
refract) - Has wave properties
- Amplitude
- Wavelength visible is between 400-700 nm
- White light carries all visible wavelengths
- Frequency
- Direction of travel
- Direction of vibration
14- Relation between Wavelength, Frequency, Energy
Blue light 488 nm short wavelength high
frequency high energy (2 times the red)
Photon as a wave packet of energy
Red light 650 nm long wavelength low
frequency low energy
15Light-Matter Interactions
- Absorption
- Reflection
- Refraction bending of light as it passes, at an
angle, from one material to another - Diffraction bending of light as it passes an
edge - Fluorescence spontaneous emission of light after
excitation - Polarization
- Dispersion
162. Diffraction Bending of light as it passes an
edge
One long continuous wave, unlike light from a
lamp or the sun.
? lt d
? gt d
See Microscopy primer,
17Diffraction Pattern from SlitResults from
Interference
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19Java Tutorial Diffraction Patterns
- http//micro.magnet.fsu.edu/primer/java/diffractio
n/basicdiffraction/index.html - How does the width of the central maximum vary
with the wavelength?
20Diffraction Through a Circular Aperture creates
an Airy Disk
- The radius of the Airy disk is the distance r
from the center to the first dark ring, given by
the resolution equation.
Increasing resolution of lens
21Resolution and Airy disk patterns
22Java Tutorial Airy Pattern Basics
- http//micro.magnet.fsu.edu/primer/java/imageforma
tion/airydiskbasics/index.html - How does resolution vary with wavelength and
numerical aperture? - http//micro.magnet.fsu.edu/primer/java/imageforma
tion/airyna/index.html - What is the effect of higher NA?
- http//micro.magnet.fsu.edu/primer/java/imageforma
tion/rayleighdisks/index.html - What is the Rayleigh criterion?
233. Numerical aperture (NA)
NA n sin ? where n refractive index and ?
the collecting angle. nair 1.00 and noil
1.515.
W.D.
24Maximum theoretical NA
- Maximum collecting angle is 90o
- sin 90o 1.00.
- For dry objective, max. NA (1.00)(1.00) 1.0
- In practice, it is 0.95.
- All dry objectives have NA lt 1.00
- For oil objective, max NA (1.515)(1.00) 1.5.
- In practice, it is 1.4.
- All oil objectives have NA gt 1.00
254. Lateral Resolution (XY or rlateral)
- The smallest distance two objects can be imaged
as two. Depends on wavelength and NA.
26Optimal Resolution for LM
- Visible light ranges from 400-700 nm
- Best NA lens is 1.4
- Calculate best theoretical resolution using 520
nm emission of fluorescein - (Footnote for confocal, the resolution equation
is slightly better rlateral 0.4?/NA so best
resolution is closer to 0.15 µm).
27XY under- and over-sampling
- Optimal zoom settings (for full xy resolution)
for 512 X 512 pixel box are given for various
lenses on p. 126. - You dont need to operate at these settings
unless you want to push the resolution limit. - Rules of thumb for 1024 X 1024 box
- 60X 1.4 NA 4X max zoom
- 40X 0.75 NA 5X max zoom
- 20X 0.7 NA 6X max zoom
- Zooming higher than this creates empty
magnification.
28Zooming for maximum XY resolution
2X Zoom
No Zoom
29Java Tutorial 3D Airy disk is the Point Spread
Function
- http//micro.magnet.fsu.edu/primer/java/imageforma
tion/depthoffield/index.html
This Z step will not resolve the objects in Z
axis.
This Z step will resolve the objects in Z axis.
305. Axial Resolution (Z or raxial)
- Minimum distance between the 3D diffraction
patterns of two points along the Z axis that can
still be seen as two. - Depends on wavelength and NAobj as follows
- Rule of thumb step size ½ Z resolution. See
also http//www2.bitplane.com/sampling/index.cfm
and http//www.cemedigital.com/clients/brand_aic_l
rg/support/presentation04.shtml -
31Ideal step sizes
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33Z axis under- and over-sampling
Oversampled Overlapping sections add no
additional information since full Z resolution is
realized just makes a bigger file.
Undersampled Too few sections for full Z
resolution But full Z resolution may not be
needed.
34XY and Z resolutions (µm)
35The bottom line on optimal step size
- The Nyquist Sampling Theorem states that the
pixel size should be 2.3X smaller than the
resolution limit of the microscope (p. 126). - So 1.4 NA objective with rlateral 0.2 µm
requires xy pixel size of 0.08 µm, optimal zoom
of 3.7X at 512 X 512. - Step size should be 3X xy pixel size 0.24 µm
for 1.4 NA objective with raxial 0.6 µm
36Week 3 TBA
- Assignment (each person)
- Collect Z-series of one of your Artemia samples,
using the 20X lens and a step size of 1 or 2 um. - Display the sections in tile mode.
- Save (as a normal TIFFs) extended focus images in
black and white, showing (a) every section of the
Z-series, (b) the top 1/3, (c) the middle 1/3,
and d) the bottom 1/3. - Always include a scale bar on your images.
- Save in the BIO553 file on the imaging computer.
- Turn in a description of your images using the
form available on Blackboard.
37Paper discussion
- Today, Jan. 22 Zucker 2006 (Hertzler)
- Jan. 29 (Hertzler)
- Feb. 5
- Feb. 12
- Feb. 19
- Feb. 26