lecture-2 optical microscopy introduction lens formula, image formation and magnification resolution...
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Lecture-2 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
Basic components and their functions
http://www.youtube.com/watch?v=PMIU1fkIPQs Microscope Review (simple, clear)
http://www.youtube.com/watch?annotation_id=annotation_100990&feature=iv&src_vid=L6d3zD2LtSI&v=ntPjuUMdXbg (I)
Parts and Function of a Microscope (details)http://www.youtube.com/watch?v=VQtMHj3vaLg (II)
http://www.youtube.com/watch?v=X-w98KA8UqU&feature=related How to use a microscopehttp://www.youtube.com/watch?v=bGBgABLEV4g
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://micro.magnet.fsu.edu/primer/java/kohler/condensercones/index.html 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
Objective specifications
Objectives are the most important components of alight microscope: image formation, magnification, thequality of images and the resolution of the microscope
Objective Lens
Anatomy of an objective
ricalture
dmin = 0.61/NA
http://www.youtube.com/watch?annotation_id=annotation_100990&feature=iv&src_vid=L6d3zD2LtSI&v=ntPjuUMdXbghttp://micro.magnet.fsu.edu/primer/java/microscopy/immersion/index.htmlhttp://micro.magnet.fsu.edu/primer/java/nuaperture/index.html
(Diaphragm)
Eyepieces (Oculars) work in combination with microscope objectives to further magnify the intermediate image
Eyepiece Lens
M=(L/fo)(25/fe)
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 characterCharacteristics 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
TransmittedOM
ReflectedOM
Illumination System
http://micro.magnet.fsu.edu/primer/java/microscopy/transmitted/index.html
http://micro.magnet.fsu.edu/primer/java/microscopy/diaphragm/index.html
http://micro.magnet.fsu.edu/primer/java/microscopy/reflected/index.html
Polarized Light MicroscopyPolarized 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.htmlhttp://www.youtube.com/watch?v=lZ-_i82s16E&feature=endscreen&NR=1 ~3:30min
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://micro.magnet.fsu.edu/primer/java/polarizedlight/icelandspar/index.html
BirefringenceCrystals 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
http://micro.magnet.fsu.edu/primer/java/polarizedlight/crystal/index.html
Olympus BX51
Research Microscope
Cutaway Diagram
Beam splitter
camera
http://micro.magnet.fsu.edu/primer/java/microassembly/index.html
Specialized OM Techniques• Enhancement of Contrast
Darkfield Microscopy Phase contrast microscopyDifferential 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 microscopymelting, freezing points and eutectics, polymorphs, twin and domain dynamics, phase transformations
• In situ microscopyE-field, stress, etc.
• Special environmental stages-vacuum or gases
ContrastContrast 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 SC = = 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.
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.
Formation of Contrast
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.
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
ImaxImin
C=Imax-Imin
Imax
C-contrast
http://micro.magnet.fsu.edu/primer/java/darkfield/reflected/index.html
Transmitted Dark Field Illumination
specimen
I I
distance distance
Oblique rays
http://micro.magnet.fsu.edu/primer/java/darkfield/cardioid/index.html
Contrast Enhancement
OM images of the green alga Micrasterias
Phase Contrast Microscopy
http://www.microscopyu.com/articles/phasecontrast/phasemicroscopy.html
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).
Crystals Growth by Differential Interference contrast microscopy
Growth spiral on cadmium iodide crystals growingFrom water solution (1025x).
http://micro.magnet.fsu.edu/primer/techniques/dic/dichome.html
Fluorescence microscopy - medical & organic materialshttp://micro.magnet.fsu.edu/primer/techniques/fluorescence/fluorhome.html
Scanning Confocal Optical Microscopy
Critical dimension measurementsin semiconductor metrologyCross-sectional image with line scan at PR/Si interface of a sample containing 0.6m-wide lines and 1.0m-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.olympusconfocal.com/theory/confocalintro.htmlhttp://micro.magnet.fsu.edu/primer/virtual/confocal/index.html
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
20m
1200C/30min
1200C/2h
Grain Size Examination
Objective Lens
x100
Grain Growth - Reflected OM
Polycrystalline CaF2 illustrating normal graingrowth. Better grain size distribution.
Large grains in polycrystallinespinel (MgAl2O4) growing bysecondary recrystallization from a fine-grained matrix
30m5m
Liquid Phase Sintering – Reflective OM
Microstructure of MgO-2% kaolin body resultingfrom reactive-liquid phase sintering.
Amorphousphase
40m
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).
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
Phase Identification by Reflected Polarized Optical Microscopy
YBa2Cu307-x superconductor material: (a) tetragonal phase and (b) orthorhombic phase with multiple twinning (arrowed) (100 x).
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 forin situ domain observa-tions.
Domain structures of PZN-PTcrystals as a function of E-field; (a) E=20kV/cm, (b) e=23.5kV/cm(c) E=27kV/cmRhombohedral at E=0 andTetragonal was induced at E>20kV/cm
a b cSingle domain
Review - Optical Microscopy• Use visible light as illumination source• Has a resolution of ~o.2m• 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 <15.5mRough surface
• Low resolution ~0.2m• Shape of specimen
Thin section or polished surface
Glass slide
specimenCover glass
resin
20m
• Lack of compositional and crystallographic information
Optical Microscopy vs Scanning Electron Microscopy
m
OM SEM
Small depth of field Low resolution
Large depth of field High resolution
radiolarian
http://www.mse.iastate.edu/microscopy/
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