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Optical Microscopy
• Introduction
• Lens formula, Image formation and
Magnification
• Resolution and lens defects
• Basic components and their functions
• Common modes of analysis
• Specialized Microscopy Techniques
• Typical examples of applications
http://www.youtube.com/watch?v=P2teE17zT4I&list=PLKstG-8VPWKzOe4TkvA7F6qMlG2HH8meX at~0:46-1:33
Review Problems on Optical Microscopy
1. Compare the focal lengths of two glass converging lenses,
one with a larger curvature angle and the other with a smaller
curvature angle.
2. List the parameters that affect the resolution of optical
microscopes.
3. A student finds that some details on the specimen cannot
be resolved even after the resolution of the microscope was
improved by using the oil immersion objective. The student
thinks that the details can be resolved by enlarging a
photograph taken with the microscope at maximum
magnification. Do you agree? Justify your answer.
http://www.doitpoms.ac.uk/tlplib/optical-microscopy/questions.php
Resolution of Microscope –
Numerical Aperture
 If the space between the specimen and the objective is filled
with a medium of refractive index n, then wavelength in
medium n = /n
 The dmin = /2n sin = /2(N.A.)
 For circular aperture
dmin= 1.22/2(N.A.)=0.61/(N.A.)
where N.A. = n sin is called numerical aperture
Immersion oil n=1.515
http://www.youtube.com/watch?v=H8PQ9RMUoA8 at~6:25-7:50
http://www.youtube.com/watch?v=n2asdncMYMo at~5:12-6:00
Air n=1.0
specimen glass
http://www.youtube.com/watch?v=RSKB0J1sRnU
-oil immersion objective use in microscope at~0:33
NA of an objective is a measure
of its ability to gather light and
resolve fine specimen detail at a
fixed object distance.
Depth of focus (f mm)
The axial range through which
an object can be focused without
any appreciable change in image
sharpness
(F mm)
M NA F
M NA F
Axial resolution – Depth of Field
Depth of Field Ranges (F mm)
F is determined by NA.
NA f F
0.1 0.13 15.5
0.4 3.8 5.8
.95 80.0 0.19
http://micro.magnet.fsu.edu/primer/java/nuaperture/index.html
Small F Large F
Basic components and their functions
http://www.youtube.com/watch?v=RKA8_mif6-E
Microscope Review (simple, clear)
http://www.youtube.com/watch?v=b2PCJ5s-iyk
Microscope working in animation (How to use a microscope)
http://www.youtube.com/watch?annotation_id=annotation_100990&featur
e=iv&src_vid=L6d3zD2LtSI&v=ntPjuUMdXbg (I)
http://www.youtube.com/watch?v=VQtMHj3vaLg (II)
Parts and Function of a Microscope (details)
http://www.youtube.com/watch?v=X-w98KA8UqU&feature=related
How to use a microscope (specimen preparation at~1:55-2:30)
http://www.youtube.com/watch?v=bGBgABLEV4g
How to care for and operate a microscope
Basic components
and their functions
(1) Eyepiece (ocular lens)
(2) Revolving nose piece (to hold
multiple objective lenses)
(3) Objective lenses
(4) And (5) Focus knobs
(4) Coarse adjustment
(5) Fine adjustment
(6) Stage (to hold the specimen)
(7) Light source (lamp)
(8) Condenser lens and
diaphragm
(9) Mechanical stage (move the
specimen on two horizontal axes
for positioning the specimen)
Functions of the Major Parts of a
Optical Microscope
 Lamp and Condenser: project a parallel beam
of light onto the sample for illumination
 Sample stage with X-Y movement: sample is
placed on the stage and different part of the
sample can be viewed due to the X-Y movement
capability
 Focusing knobs: since the distance between
objective and eyepiece is fixed, focusing is
achieved by moving the sample relative to the
objective lens
Light Sources
Condenser
Light from the microscope light source
Condenser gathers light and concentrates it into a
cone of light that illuminates the specimen with
uniform intensity over the entire viewfield
http://www.youtube.com/watch?annotation_id=annotation_100990&feature=iv&src_vid=L6d3zD2LtSI&v=ntPjuUMdXbg ~6:30 to 9:40
http://micro.magnet.fsu.edu/primer/java/kohler/contrast/index.html
Specimen Stage
http://micro.magnet.fsu.edu/primer/flash/stage/index.html
 Objective: does the main part of
magnification and resolves the fine
details on the samples (mo ~ 10 – 100)
 Eyepiece: forms a further magnified
virtual image which can be observed
directly with eyes (me ~ 10)
 Beam splitter and camera: allow a
permanent record of the real image
from the objective be made on film
(for modern research microscope)
Functions of the Major Parts of a
Optical Microscope
Olympus
BX51
Research
Microscope
Cutaway
Diagram
Beam
splitter
camera
Reflected light
Transmitted light
http://micro.magnet.fsu.edu/primer/java/microassembly/index.html
Objective specifications
Objectives are the most important components of a
light microscope: image formation, magnification, the
quality of images and the resolution of the microscope
Objective Lens
Anatomy of an objective
rical
ture
dmin = 0.61/NA
http://www.youtube.com/watch?v=P0Z4H2O_Stg Objectives to~5:26
http://www.youtube.com/watch?v=H8PQ9RMUoA8 Grades of objectives to~2:30 & 3:25-4:50
DIC-differential interference contrast
(Diaphragm)
Eyepieces (Oculars) work in combination with microscope
objectives to further magnify the intermediate image
Eyepiece Lens
M=(L/fo)(25/fe)
http://micro.magnet.fsu.edu/primer/anatomy/oculars.html
Olympus
BX51
Research
Microscope
Cutaway
Diagram
Beam
splitter
camera
http://micro.magnet.fsu.edu/primer/java/microassembly/index.html
Common Modes of Analysis
• Transmitted OM - transparent specimens
thin section of rocks, minerals and single crystals
• Reflected OM - opaque specimens
most metals, ceramics, semiconductors
Specialized Microscopy Techniques
• Polarized LM - specimens with anisotropic optical
character
Characteristics of materials can be determined
morphology (shape and size), phase distribution
(amorphous or crystalline), transparency or opacity,
color, refractive indices, dispersion of refractive
indices, crystal system, birefringence, degree of
crystallinity, polymorphism and etc.
Depending on the nature of samples, different illumination
methods must be used
Anatomy of a modern OM
Illumination System
Transmitted
OM
Reflected
OM
Illumination System
http://www.youtube.com/watch?v=zq13e36cs3s at~0:20-1:40 Field diaphragm
http://www.youtube.com/watch?v=7-Tlyd7piSM Trans OM to~1:37
Refle OM from 1:38-end
Polarized Light Microscopy
Polarized light microscope is designed to observe specimens that are
visible primarily due to their optically anisotropic character
(birefringent). The microscope must be equipped with both a polarizer,
positioned in the light path somewhere before the specimen, and an
analyzer (a second polarizer), placed in the optical pathway between the
objective rear aperture and the observation tubes or camera port.
birefringent - doubly refracting
When the electric field vectors of light are restricted to a
single plane by filtration, then the the light is said to be
polarized with respect to the direction of propagation and
all waves vibrate in the same plane.
Polarization of Light
http://micro.magnet.fsu.edu/primer/java/polarizedlight/filters/index.html
http://www.youtube.com/watch?v=lZ-_i82s16E&feature=endscreen&NR=1 to~3:30min
http://www.youtube.com/watch?v=E9qpbt0v5Hw
http://www.youtube.com/watch?v=rbx3K1xBxVU polarized light
Birefringence
Isotropic
anisotropic
CaCO3
Double Refraction (Birefringence)
Birefringence is optical property of a material
having a refractive index that depends on the
polarization and propagation direction of light.
Anisotropic
http://www.youtube.com/watch?v=WdrYRJfiUv0
(Birefringence)
Crystals are classified as being either isotropic or anisotropic depending
upon their optical behavior and whether or not their crystallographic axes
are equivalent. All isotropic crystals have equivalent axes that interact
with light in a similar manner, regardless of the crystal orientation with
respect to incident light waves. Light entering an isotropic crystal is
refracted at a constant angle and passes through the crystal at a single
velocity without being polarized by interaction with the electronic
components of the crystalline lattice.
Anisotropic crystals have crystallographically distinct axes and
interact with light in a manner that is dependent upon the orientation of the
crystalline lattice with respect to the incident light. When light enters the
optical axis (c) of anisotropic crystals, it acts in a manner similar to
interaction with isotropic crystals and passes through at a single velocity.
However, when light enters a non-equivalent axis (a), it is refracted into
two rays each polarized with the vibration directions oriented at right
angles to one another, and traveling at different velocities. This
phenomenon is termed "double" or "bi" refraction and is seen to a
greater or lesser degree in all anisotropic crystals.
Cubic a
tetragonal c
a
Anisotropic Optical Character
http://micro.magnet.fsu.edu/primer/java/polarizedlight/crystal/index.html
Polarized Optical Microscopy (POM)
(a)Surface features of a microprocessor integrated circuit
(b)Apollo 14 Moon rock
Reflected POM Transmitted POM
http://micro.magnet.fsu.edu/primer/virtual/polarizing/index.html
Specialized OM Techniques
• Enhancement of Contrast
Darkfield Microscopy
Phase contrast microscopy
Differential interference contrast microscopy
Fluorescence microscopy-medical & organic materials
• Scanning confocal optical microscopy
(relatively new)
Three-Dimensional Optical Microscopy
inspect and measure submicrometer features in
semiconductors and other materials
• Hot- and cold-stage microscopy
melting, freezing points and eutectics, polymorphs, twin
and domain dynamics, phase transformations
• In situ microscopy
E-field, stress, etc.
• Special environmental stages-vacuum or gases
Contrast
Contrast is defined as the difference in light intensity
between the specimen and the adjacent background
relative to the overall background intensity.
Image contrast, C is defined by
Sspecimen-Sbackgroud S
C = =
Sspecimen SA
Sspecimen and Sbackgroud are
intensities measured from specimen
and backgroud, e.g., A and B, in the
scanned area.
Cminimum ~ 2% for human eye to
distinguish differences between the
specimen (image) and its background.
http://www.youtube.com/watch?v=SVK4OkUK0Yw at~1:47-3:04
http://micro.magnet.fsu.edu/primer/techniques/contrast.html
Contrast produced in the specimen by the
absorption of light (directly related to the chemical
composition of the absorber) and the predominant
source of contrast in the ordinary optical
microscope, brightness, reflectance, birefringence,
light scattering, diffraction, fluorescence, or color
variations have been the classical means of
imaging specimens in brightfield microscopy.
Contrast in Optical Microscope
http://micro.magnet.fsu.edu/primer/virtual/virtualzoo/index.html
Enhancement of contrast by darkfield microscopy
Darkfield microscopy is a specialized illumination technique
that capitalizes on oblique illumination to enhance contrast
in specimens that are not imaged well under normal
brightfield illumination conditions.
http://www.youtube.com/watch?v=P2teE17zT4I&list=PLKstG-8VPWKzOe4TkvA7F6qMlG2HH8meX at~1:33-2:21
https://www.youtube.com/watch?v=L3SsxIUm0As at~2:17-3:46
Interaction of light with matter
Angle of Illumination
 Bright filed illumination – The normal method of illumination,
light comes from above (for reflected OM)
 Oblique illumination – light is not projected along the optical
axis of the objective lens; better contrast for detail features
 Dark field illumination – The light is projected onto specimen
surface through a special mirror block and attachment in the
objective – the most effective way to improve contrast.
Light stop
Imax
Imin
C=
Imax-Imin
Imax
C-contrast
http://www.youtube.com/watch?v=d6jsnLIsNwI at~3:40-5:20
http://www.youtube.com/watch?v=7V3nyRGeha4 Dark field microscopy
Condenser
Light from the microscope light source
Condenser gathers light and concentrates it into a
cone of light that illuminates the specimen with
uniform intensity over the entire viewfield
http://www.youtube.com/watch?annotation_id=annotation_100990&feature=iv&src_vid=L6d3zD2LtSI&v=ntPjuUMdXbg at~9:00-10:10
Transmitted Dark Field Illumination
specimen
I I
distance distance
Oblique rays
http://micro.magnet.fsu.edu/primer/java/darkfield/cardioid/index.html
http://micro.magnet.fsu.edu/primer/techniques/darkfieldreflect.html reflected DF
http://www.youtube.com/watch?v=I4ZQm-CAgL8 at~5:24-8:14
Reflected beam
Parallel beam
Contrast Enhancement
OM images of the green alga Micrasterias
Phase Contrast Microscopy
http://www.youtube.com/watch?v=I4ZQm-CAgL8 at~0:50-5:20
http://www.youtube.com/watch?v=WvyCg1uzG5c
Phase contrast microscopy is a contrast-enhancing optical
technique that can be utilized to produce high-contrast images
of transparent specimens, such as living cells, thin tissue slices,
lithographic patterns, fibers, latex dispersions, glass fragments,
and subcellular particles (including nuclei and other organelles).
http://www.microscopyu.com/articles/phasecontrast/phasemicroscopy.html
Crystals Growth by Differential
Interference contrast microscopy (DIC)
Growth spiral on
cadmium iodide
crystals growing
From water
solution (1025x).
http://www.youtube.com/watch?v=P2teE17zT4I at~23:05-30:50
http://micro.magnet.fsu.edu/primer/techniques/dic/dichome.html
Fluorescence microscopy - medical & organic materials
http://www.youtube.com/watch?v=iPrZ84kHH2U at~1:50-3:15
http://micro.magnet.fsu.edu/primer/techniques/fluorescence/fluorhome.html
Scanning Confocal Optical Microscopy
Confocal microscopy is an optical
imaging technique used to increase
optical resolution and contrast of a
micrograph by adding a spatial pinhole
placed at the confocal plane of the lens
to eliminate out-of-focus light.
Scanning confocal optical microscopy
(SCOM) is a technique for obtaining
high-resolution optical images with
depth selectivity. (a laser beam is
used) The key feature of confocal
microscopy is its ability to acquire in-
focus images from selected depths, a
process known as optical sectioning.
Images are acquired point-by-point
and reconstructed with a computer,
allowing three-dimensional
reconstructions of topologically complex
objects.
http://www.youtube.com/watch?v=mrjgNyKX8-w Why confocal? to~3:10
http://www.youtube.com/watch?v=puT1ccMWKyQ at~0:40-1:36 & 2:40-2:56
http://www.youtube.com/watch?v=Axrst4T__YY scanning
Scanning Confocal Optical Microscopy
Critical dimension measurements
in semiconductor metrology
Cross-sectional image with line scan
at PR/Si interface of a sample
containing 0.6mm-wide lines and
1.0mm-thick photoresist on silicon.
The bottom width, w, determining
the area of the circuit that is
protected from further processing,
can be measured accurately by
using SCOP.
Measurement of the patterned
photoresist is important because it
allows the process engineer to
simultaneously monitor for defects,
misalignment, or other artifacts that
may affect the manufacturing line.
w
Three-Dimensional Optical Microscopy
http://www.youtube.com/watch?v=oluJW7uK7rw&index=12&list=PL200E1A86911B0422 to~2.44 coral under confocal
http://micro.magnet.fsu.edu/primer/virtual/confocal/index.html interactive tutorial
http://www.olympusconfocal.com/theory/confocalintro.html Introduction
Typical Examples of
OM Applications
Grain Size Examination
A grain boundary intersecting a polished surface is not in
equilibrium (a). At elevated temperatures (b), surface
diffusion forms a grain-boundary groove in order to
balance the surface tension forces.
a
b
Thermal Etching
20mm
1200C/30min
1200C/2h
Grain Size Examination
Objective Lens
x100
Reflected OM
Grain Growth - Reflected OM
Polycrystalline CaF2
illustrating normal grain
growth. Better grain size
distribution.
Large grains in polycrystalline
spinel (MgAl2O4) growing by
secondary recrystallization
from a fine-grained matrix
30mm
5mm
Liquid Phase Sintering – Reflective OM
Microstructure of MgO-2% kaolin body resulting
from reactive-liquid phase sintering.
Amorphous
phase
40mm
Image of Magnetic Domains
Magnetic domains and walls on a (110)-oriented
garnet crystal (Transmitted LM with oblique
illumination). The domains structure is illustrated in
(b).
Phase Identification by Reflected
Polarized Optical Microscopy
YBa2Cu307-x superconductor material: (a) tetragonal phase and
(b) orthorhombic phase with multiple twinning (arrowed) (100 x).
Specialized OM Techniques
• Enhancement of Contrast
Darkfield Microscopy
Phase contrast microscopy
Differential interference contrast microscopy
Fluorescence microscopy-medical & organic materials
• Scanning confocal optical microscopy
(relatively new)
Three-Dimensional Optical Microscopy
inspect and measure submicrometer features in
semiconductors and other materials
• Hot- and cold-stage microscopy
melting, freezing points and eutectics, polymorphs, twin
and domain dynamics, phase transformations
• In situ microscopy
E-field, stress, etc.
• Special environmental stages-vacuum or gases
http://www.nature.com/nmeth/journal/v12/n6/full/nmeth.3400.html
Hot-stage POM of Phase Transformations
in Pb(Mg1/3Nb2/3)O3-PbTiO3 Crystals
(a) and (b) at 20oC, strongly
birefringent domains with extinction
directions along <100>cubic,
indicating a tetragonal symmetry;
(c) at 240oC, phase transition from
the tetragonal into cubic phase with
increasing isotropic areas at the
expense of vanishing strip domains.
n
T(oC)
E-field Induced Phase Transition in
Pb(Zn1/3Nb2/3)O3-PbTiO3 Crystals
Schematic diagram for
in situ domain observa-
tions.
Domain structures of PZN-PT
crystals as a function of E-field;
(a)E=20kV/cm, (b) e=23.5kV/cm
(c) E=27kV/cm
Rhombohedral at E=0 and
Tetragonal was induced at E>20kV/cm
a b c
Single domain
Review - Optical Microscopy
• Use visible light as illumination source
• Has a resolution of ~o.2mm
• Range of samples characterized - almost
unlimited for solids and liquid crystals
• Usually nondestructive; sample preparation
may involve material removal
•Main use – direct visual observation;
preliminary observation for final charac-
terization with applications in geology, medicine,
materials research and engineering, industries,
and etc.
• Cost - $15,000-$390,000 or more
Characteristics of Materials
Can be determined By OM:
Morphology (shape and size), phase distribution
(amorphous or crystalline), transparency or opacity,
color, refractive indices, dispersion of refractive
indices, crystal system, birefringence, degree of
crystallinity, polymorphism and etc.
Limits of Optical Microscopy
• Small depth of field <15.5mm
Rough surface
• Low resolution ~0.2mm
• Shape of specimen
Thin section or polished surface
Glass slide
specimen
Cover glass
resin
20mm
• Lack of compositional and
crystallographic information
Optical Microscopy vs Scanning
Electron Microscopy
25mm
OM SEM
Small depth of field
Low resolution
Large depth of field
High resolution
radiolarian
http://www.mse.iastate.edu/microscopy/
Radiolarian – marine protozoan
Scanning Electron Microscopy (SEM)
•What is SEM?
•Working principles of SEM
•Major components and their functions
•Electron beam - specimen interactions
•Interaction volume and escape volume
•Magnification, resolution, depth of field and
image contrast
•Energy Dispersive X-ray Spectroscopy (EDS)
•Wavelength Dispersive X-ray Spectroscopy
(WDS)
•Orientation Imaging Microscopy (OIM)
•X-ray Fluorescence (XRF)
http://www.mse.iastate.edu/microscopy/

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optical microscope and its details working.ppt

  • 1. Optical Microscopy • Introduction • Lens formula, Image formation and Magnification • Resolution and lens defects • Basic components and their functions • Common modes of analysis • Specialized Microscopy Techniques • Typical examples of applications http://www.youtube.com/watch?v=P2teE17zT4I&list=PLKstG-8VPWKzOe4TkvA7F6qMlG2HH8meX at~0:46-1:33
  • 2. Review Problems on Optical Microscopy 1. Compare the focal lengths of two glass converging lenses, one with a larger curvature angle and the other with a smaller curvature angle. 2. List the parameters that affect the resolution of optical microscopes. 3. A student finds that some details on the specimen cannot be resolved even after the resolution of the microscope was improved by using the oil immersion objective. The student thinks that the details can be resolved by enlarging a photograph taken with the microscope at maximum magnification. Do you agree? Justify your answer. http://www.doitpoms.ac.uk/tlplib/optical-microscopy/questions.php
  • 3. Resolution of Microscope – Numerical Aperture  If the space between the specimen and the objective is filled with a medium of refractive index n, then wavelength in medium n = /n  The dmin = /2n sin = /2(N.A.)  For circular aperture dmin= 1.22/2(N.A.)=0.61/(N.A.) where N.A. = n sin is called numerical aperture Immersion oil n=1.515 http://www.youtube.com/watch?v=H8PQ9RMUoA8 at~6:25-7:50 http://www.youtube.com/watch?v=n2asdncMYMo at~5:12-6:00 Air n=1.0 specimen glass http://www.youtube.com/watch?v=RSKB0J1sRnU -oil immersion objective use in microscope at~0:33 NA of an objective is a measure of its ability to gather light and resolve fine specimen detail at a fixed object distance.
  • 4. Depth of focus (f mm) The axial range through which an object can be focused without any appreciable change in image sharpness (F mm) M NA F M NA F Axial resolution – Depth of Field Depth of Field Ranges (F mm) F is determined by NA. NA f F 0.1 0.13 15.5 0.4 3.8 5.8 .95 80.0 0.19 http://micro.magnet.fsu.edu/primer/java/nuaperture/index.html Small F Large F
  • 5. Basic components and their functions http://www.youtube.com/watch?v=RKA8_mif6-E Microscope Review (simple, clear) http://www.youtube.com/watch?v=b2PCJ5s-iyk Microscope working in animation (How to use a microscope) http://www.youtube.com/watch?annotation_id=annotation_100990&featur e=iv&src_vid=L6d3zD2LtSI&v=ntPjuUMdXbg (I) http://www.youtube.com/watch?v=VQtMHj3vaLg (II) Parts and Function of a Microscope (details) http://www.youtube.com/watch?v=X-w98KA8UqU&feature=related How to use a microscope (specimen preparation at~1:55-2:30) http://www.youtube.com/watch?v=bGBgABLEV4g How to care for and operate a microscope
  • 6. Basic components and their functions (1) Eyepiece (ocular lens) (2) Revolving nose piece (to hold multiple objective lenses) (3) Objective lenses (4) And (5) Focus knobs (4) Coarse adjustment (5) Fine adjustment (6) Stage (to hold the specimen) (7) Light source (lamp) (8) Condenser lens and diaphragm (9) Mechanical stage (move the specimen on two horizontal axes for positioning the specimen)
  • 7. Functions of the Major Parts of a Optical Microscope  Lamp and Condenser: project a parallel beam of light onto the sample for illumination  Sample stage with X-Y movement: sample is placed on the stage and different part of the sample can be viewed due to the X-Y movement capability  Focusing knobs: since the distance between objective and eyepiece is fixed, focusing is achieved by moving the sample relative to the objective lens
  • 9. Condenser Light from the microscope light source Condenser gathers light and concentrates it into a cone of light that illuminates the specimen with uniform intensity over the entire viewfield http://www.youtube.com/watch?annotation_id=annotation_100990&feature=iv&src_vid=L6d3zD2LtSI&v=ntPjuUMdXbg ~6:30 to 9:40 http://micro.magnet.fsu.edu/primer/java/kohler/contrast/index.html
  • 11.  Objective: does the main part of magnification and resolves the fine details on the samples (mo ~ 10 – 100)  Eyepiece: forms a further magnified virtual image which can be observed directly with eyes (me ~ 10)  Beam splitter and camera: allow a permanent record of the real image from the objective be made on film (for modern research microscope) Functions of the Major Parts of a Optical Microscope
  • 13. Objective specifications Objectives are the most important components of a light microscope: image formation, magnification, the quality of images and the resolution of the microscope Objective Lens Anatomy of an objective rical ture dmin = 0.61/NA http://www.youtube.com/watch?v=P0Z4H2O_Stg Objectives to~5:26 http://www.youtube.com/watch?v=H8PQ9RMUoA8 Grades of objectives to~2:30 & 3:25-4:50 DIC-differential interference contrast
  • 14. (Diaphragm) Eyepieces (Oculars) work in combination with microscope objectives to further magnify the intermediate image Eyepiece Lens M=(L/fo)(25/fe) http://micro.magnet.fsu.edu/primer/anatomy/oculars.html
  • 16. Common Modes of Analysis • Transmitted OM - transparent specimens thin section of rocks, minerals and single crystals • Reflected OM - opaque specimens most metals, ceramics, semiconductors Specialized Microscopy Techniques • Polarized LM - specimens with anisotropic optical character Characteristics of materials can be determined morphology (shape and size), phase distribution (amorphous or crystalline), transparency or opacity, color, refractive indices, dispersion of refractive indices, crystal system, birefringence, degree of crystallinity, polymorphism and etc. Depending on the nature of samples, different illumination methods must be used
  • 17. Anatomy of a modern OM Illumination System Transmitted OM Reflected OM Illumination System http://www.youtube.com/watch?v=zq13e36cs3s at~0:20-1:40 Field diaphragm http://www.youtube.com/watch?v=7-Tlyd7piSM Trans OM to~1:37 Refle OM from 1:38-end
  • 18. Polarized Light Microscopy Polarized light microscope is designed to observe specimens that are visible primarily due to their optically anisotropic character (birefringent). The microscope must be equipped with both a polarizer, positioned in the light path somewhere before the specimen, and an analyzer (a second polarizer), placed in the optical pathway between the objective rear aperture and the observation tubes or camera port. birefringent - doubly refracting
  • 19. When the electric field vectors of light are restricted to a single plane by filtration, then the the light is said to be polarized with respect to the direction of propagation and all waves vibrate in the same plane. Polarization of Light http://micro.magnet.fsu.edu/primer/java/polarizedlight/filters/index.html http://www.youtube.com/watch?v=lZ-_i82s16E&feature=endscreen&NR=1 to~3:30min http://www.youtube.com/watch?v=E9qpbt0v5Hw http://www.youtube.com/watch?v=rbx3K1xBxVU polarized light
  • 20. Birefringence Isotropic anisotropic CaCO3 Double Refraction (Birefringence) Birefringence is optical property of a material having a refractive index that depends on the polarization and propagation direction of light. Anisotropic http://www.youtube.com/watch?v=WdrYRJfiUv0
  • 21. (Birefringence) Crystals are classified as being either isotropic or anisotropic depending upon their optical behavior and whether or not their crystallographic axes are equivalent. All isotropic crystals have equivalent axes that interact with light in a similar manner, regardless of the crystal orientation with respect to incident light waves. Light entering an isotropic crystal is refracted at a constant angle and passes through the crystal at a single velocity without being polarized by interaction with the electronic components of the crystalline lattice. Anisotropic crystals have crystallographically distinct axes and interact with light in a manner that is dependent upon the orientation of the crystalline lattice with respect to the incident light. When light enters the optical axis (c) of anisotropic crystals, it acts in a manner similar to interaction with isotropic crystals and passes through at a single velocity. However, when light enters a non-equivalent axis (a), it is refracted into two rays each polarized with the vibration directions oriented at right angles to one another, and traveling at different velocities. This phenomenon is termed "double" or "bi" refraction and is seen to a greater or lesser degree in all anisotropic crystals. Cubic a tetragonal c a Anisotropic Optical Character http://micro.magnet.fsu.edu/primer/java/polarizedlight/crystal/index.html
  • 22. Polarized Optical Microscopy (POM) (a)Surface features of a microprocessor integrated circuit (b)Apollo 14 Moon rock Reflected POM Transmitted POM http://micro.magnet.fsu.edu/primer/virtual/polarizing/index.html
  • 23. Specialized OM Techniques • Enhancement of Contrast Darkfield Microscopy Phase contrast microscopy Differential interference contrast microscopy Fluorescence microscopy-medical & organic materials • Scanning confocal optical microscopy (relatively new) Three-Dimensional Optical Microscopy inspect and measure submicrometer features in semiconductors and other materials • Hot- and cold-stage microscopy melting, freezing points and eutectics, polymorphs, twin and domain dynamics, phase transformations • In situ microscopy E-field, stress, etc. • Special environmental stages-vacuum or gases
  • 24. Contrast Contrast is defined as the difference in light intensity between the specimen and the adjacent background relative to the overall background intensity. Image contrast, C is defined by Sspecimen-Sbackgroud S C = = Sspecimen SA Sspecimen and Sbackgroud are intensities measured from specimen and backgroud, e.g., A and B, in the scanned area. Cminimum ~ 2% for human eye to distinguish differences between the specimen (image) and its background. http://www.youtube.com/watch?v=SVK4OkUK0Yw at~1:47-3:04 http://micro.magnet.fsu.edu/primer/techniques/contrast.html
  • 25. Contrast produced in the specimen by the absorption of light (directly related to the chemical composition of the absorber) and the predominant source of contrast in the ordinary optical microscope, brightness, reflectance, birefringence, light scattering, diffraction, fluorescence, or color variations have been the classical means of imaging specimens in brightfield microscopy. Contrast in Optical Microscope http://micro.magnet.fsu.edu/primer/virtual/virtualzoo/index.html Enhancement of contrast by darkfield microscopy Darkfield microscopy is a specialized illumination technique that capitalizes on oblique illumination to enhance contrast in specimens that are not imaged well under normal brightfield illumination conditions. http://www.youtube.com/watch?v=P2teE17zT4I&list=PLKstG-8VPWKzOe4TkvA7F6qMlG2HH8meX at~1:33-2:21 https://www.youtube.com/watch?v=L3SsxIUm0As at~2:17-3:46 Interaction of light with matter
  • 26. Angle of Illumination  Bright filed illumination – The normal method of illumination, light comes from above (for reflected OM)  Oblique illumination – light is not projected along the optical axis of the objective lens; better contrast for detail features  Dark field illumination – The light is projected onto specimen surface through a special mirror block and attachment in the objective – the most effective way to improve contrast. Light stop Imax Imin C= Imax-Imin Imax C-contrast http://www.youtube.com/watch?v=d6jsnLIsNwI at~3:40-5:20 http://www.youtube.com/watch?v=7V3nyRGeha4 Dark field microscopy
  • 27. Condenser Light from the microscope light source Condenser gathers light and concentrates it into a cone of light that illuminates the specimen with uniform intensity over the entire viewfield http://www.youtube.com/watch?annotation_id=annotation_100990&feature=iv&src_vid=L6d3zD2LtSI&v=ntPjuUMdXbg at~9:00-10:10
  • 28. Transmitted Dark Field Illumination specimen I I distance distance Oblique rays http://micro.magnet.fsu.edu/primer/java/darkfield/cardioid/index.html http://micro.magnet.fsu.edu/primer/techniques/darkfieldreflect.html reflected DF http://www.youtube.com/watch?v=I4ZQm-CAgL8 at~5:24-8:14 Reflected beam Parallel beam
  • 29. Contrast Enhancement OM images of the green alga Micrasterias
  • 30. Phase Contrast Microscopy http://www.youtube.com/watch?v=I4ZQm-CAgL8 at~0:50-5:20 http://www.youtube.com/watch?v=WvyCg1uzG5c Phase contrast microscopy is a contrast-enhancing optical technique that can be utilized to produce high-contrast images of transparent specimens, such as living cells, thin tissue slices, lithographic patterns, fibers, latex dispersions, glass fragments, and subcellular particles (including nuclei and other organelles). http://www.microscopyu.com/articles/phasecontrast/phasemicroscopy.html
  • 31. Crystals Growth by Differential Interference contrast microscopy (DIC) Growth spiral on cadmium iodide crystals growing From water solution (1025x). http://www.youtube.com/watch?v=P2teE17zT4I at~23:05-30:50 http://micro.magnet.fsu.edu/primer/techniques/dic/dichome.html Fluorescence microscopy - medical & organic materials http://www.youtube.com/watch?v=iPrZ84kHH2U at~1:50-3:15 http://micro.magnet.fsu.edu/primer/techniques/fluorescence/fluorhome.html
  • 32. Scanning Confocal Optical Microscopy Confocal microscopy is an optical imaging technique used to increase optical resolution and contrast of a micrograph by adding a spatial pinhole placed at the confocal plane of the lens to eliminate out-of-focus light. Scanning confocal optical microscopy (SCOM) is a technique for obtaining high-resolution optical images with depth selectivity. (a laser beam is used) The key feature of confocal microscopy is its ability to acquire in- focus images from selected depths, a process known as optical sectioning. Images are acquired point-by-point and reconstructed with a computer, allowing three-dimensional reconstructions of topologically complex objects. http://www.youtube.com/watch?v=mrjgNyKX8-w Why confocal? to~3:10 http://www.youtube.com/watch?v=puT1ccMWKyQ at~0:40-1:36 & 2:40-2:56 http://www.youtube.com/watch?v=Axrst4T__YY scanning
  • 33. Scanning Confocal Optical Microscopy Critical dimension measurements in semiconductor metrology Cross-sectional image with line scan at PR/Si interface of a sample containing 0.6mm-wide lines and 1.0mm-thick photoresist on silicon. The bottom width, w, determining the area of the circuit that is protected from further processing, can be measured accurately by using SCOP. Measurement of the patterned photoresist is important because it allows the process engineer to simultaneously monitor for defects, misalignment, or other artifacts that may affect the manufacturing line. w Three-Dimensional Optical Microscopy http://www.youtube.com/watch?v=oluJW7uK7rw&index=12&list=PL200E1A86911B0422 to~2.44 coral under confocal http://micro.magnet.fsu.edu/primer/virtual/confocal/index.html interactive tutorial http://www.olympusconfocal.com/theory/confocalintro.html Introduction
  • 34. Typical Examples of OM Applications
  • 35. Grain Size Examination A grain boundary intersecting a polished surface is not in equilibrium (a). At elevated temperatures (b), surface diffusion forms a grain-boundary groove in order to balance the surface tension forces. a b Thermal Etching 20mm 1200C/30min 1200C/2h
  • 36. Grain Size Examination Objective Lens x100 Reflected OM
  • 37. Grain Growth - Reflected OM Polycrystalline CaF2 illustrating normal grain growth. Better grain size distribution. Large grains in polycrystalline spinel (MgAl2O4) growing by secondary recrystallization from a fine-grained matrix 30mm 5mm
  • 38. Liquid Phase Sintering – Reflective OM Microstructure of MgO-2% kaolin body resulting from reactive-liquid phase sintering. Amorphous phase 40mm
  • 39. Image of Magnetic Domains Magnetic domains and walls on a (110)-oriented garnet crystal (Transmitted LM with oblique illumination). The domains structure is illustrated in (b).
  • 40. Phase Identification by Reflected Polarized Optical Microscopy YBa2Cu307-x superconductor material: (a) tetragonal phase and (b) orthorhombic phase with multiple twinning (arrowed) (100 x).
  • 41. Specialized OM Techniques • Enhancement of Contrast Darkfield Microscopy Phase contrast microscopy Differential interference contrast microscopy Fluorescence microscopy-medical & organic materials • Scanning confocal optical microscopy (relatively new) Three-Dimensional Optical Microscopy inspect and measure submicrometer features in semiconductors and other materials • Hot- and cold-stage microscopy melting, freezing points and eutectics, polymorphs, twin and domain dynamics, phase transformations • In situ microscopy E-field, stress, etc. • Special environmental stages-vacuum or gases http://www.nature.com/nmeth/journal/v12/n6/full/nmeth.3400.html
  • 42. Hot-stage POM of Phase Transformations in Pb(Mg1/3Nb2/3)O3-PbTiO3 Crystals (a) and (b) at 20oC, strongly birefringent domains with extinction directions along <100>cubic, indicating a tetragonal symmetry; (c) at 240oC, phase transition from the tetragonal into cubic phase with increasing isotropic areas at the expense of vanishing strip domains. n T(oC)
  • 43. E-field Induced Phase Transition in Pb(Zn1/3Nb2/3)O3-PbTiO3 Crystals Schematic diagram for in situ domain observa- tions. Domain structures of PZN-PT crystals as a function of E-field; (a)E=20kV/cm, (b) e=23.5kV/cm (c) E=27kV/cm Rhombohedral at E=0 and Tetragonal was induced at E>20kV/cm a b c Single domain
  • 44. Review - Optical Microscopy • Use visible light as illumination source • Has a resolution of ~o.2mm • Range of samples characterized - almost unlimited for solids and liquid crystals • Usually nondestructive; sample preparation may involve material removal •Main use – direct visual observation; preliminary observation for final charac- terization with applications in geology, medicine, materials research and engineering, industries, and etc. • Cost - $15,000-$390,000 or more
  • 45. Characteristics of Materials Can be determined By OM: Morphology (shape and size), phase distribution (amorphous or crystalline), transparency or opacity, color, refractive indices, dispersion of refractive indices, crystal system, birefringence, degree of crystallinity, polymorphism and etc.
  • 46. Limits of Optical Microscopy • Small depth of field <15.5mm Rough surface • Low resolution ~0.2mm • Shape of specimen Thin section or polished surface Glass slide specimen Cover glass resin 20mm • Lack of compositional and crystallographic information
  • 47. Optical Microscopy vs Scanning Electron Microscopy 25mm OM SEM Small depth of field Low resolution Large depth of field High resolution radiolarian http://www.mse.iastate.edu/microscopy/ Radiolarian – marine protozoan
  • 48. Scanning Electron Microscopy (SEM) •What is SEM? •Working principles of SEM •Major components and their functions •Electron beam - specimen interactions •Interaction volume and escape volume •Magnification, resolution, depth of field and image contrast •Energy Dispersive X-ray Spectroscopy (EDS) •Wavelength Dispersive X-ray Spectroscopy (WDS) •Orientation Imaging Microscopy (OIM) •X-ray Fluorescence (XRF) http://www.mse.iastate.edu/microscopy/