Bringing light into the chaos: A general introduction to optics and light microscopy Juliana Schwarz 19/03/07

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Bringing light into the chaos: A general introduction to optics and light microscopy Juliana Schwarz 19/03/07 Slide 2 Overview Part one: The root of all evil Basic terms and applications in light microscopy Part two: Bringing colour into the light Fluorescence microscopy and special applications: Widefield, Confocal microscopy, Multiphoton, FRET, FLIM,FRAP, Photoactivation, TIRF Slide 3 What is light? Light is electromagnetic radiation. What we usually describe as light is only the visible spectrum of this radiation with wavelengths between 400nm and 700nm. The elementary particle that defines light is the photon. There are 3 basic dimensions of light a)Intensity (amplitude) which is related to the perception of brightness b)Frequency (wavelength), perceived as colour c)Polarization (angle of vibration) which is not or weakly perceptible to humans a) b) Slide 4 What is a microscope? Slide 5 Theoretically a microscope is an array of two lenses. Objective lens Tube lens Eyepiece lens Focal planeImage plane Classic compound microscope Modern microscope with ICS (Infinity Colour corrected System) Image plane Slide 6 Your friend - the objective Objectives can be classified into transmitted light and reflected-light (Epi) versions. Slide 7 Flat-field correction and aberration correction Flatness of the intermediate image Elimination of chromatic errors Describe two main criteria for the quality of an objective: Slide 8 Spherical aberration Spherical aberration causes beams parallel to but away from the lens axis to be focussed in a slightly different place than beams close to the axis. This manifests itself as a blurring of the image. Slide 9 Flat-field correction and aberration correction Flatness of the intermediate image Elimination of chromatic errors Describe two main criteria for the quality of an objective: Slide 10 Chromatic aberration Chromatic aberration is caused by a lens having different refractive indexes for different wavelengths. Since the focal length of a lens is dependent on the refractive index, different wavelengths will be focused on different positions in the focal plane. Chromatic aberration is seen as fringes of colour around the image. It can be minimised by using an achromatic doublet (= achromat) in which two materials with differing dispersion are bonded together to form a single lens. Slide 11 Objective types CP-Achromat Good colour correction exactly for two wavelengths. Field flatness in the image center, refocusing also covers the peripheral areas. For fields of view up to dia. 18 mm. Versions for phase contrast. Achroplan Improved Achromat objectives with good image flatness for fields of view with dia. 20 or even 23 mm. Achroplan for transmitted light and Achroplan Ph for phase contrast. Plan-Neofluar Excellent colour correction for at least three wavelengths. Field flattening for the field of view with dia. 25 mm. Highly transmitting for UV excitation at 365 nm in fluorescence. All methods possible, special high-quality variants are available for Pol and DIC. Plan-Apochromat Perfect colour rendition (correction for four wavelengths!). Flawless image flatness for fields of view with dia. 25 mm. Highest numerical apertures for a resolving power at the very limits of the physically possible. elimination of chromatic errors flatness of the intermediate image Slide 12 Still your friend - the objective Slide 13 What is magnification? Magnification is defined by the magnification by the objective x the magnification by eyepiece BUT maximum magnification does not mean maximum resolution! Slide 14 What is resolution? Resolution describes the minimal distance of two points that can be distinguished. Picture taken from http://microscopy.fsu.edu/primer/anatomy/numaperture.html Slide 15 NA = n sin What is the numerical aperture? NA is an estimate of how much light from the sample is collected by the objective 11 22 Coverslip (n = 1.5) Glass slide (n = 1.5) Oil (n = 1.5) Air (n = 1.0) n = refractive index = angle of incident illumination Objective lens Slide 16 Numerical aperture, NOT magnification determines resolution! Increasing NA A lens with a larger NA will be able to visualize finer details and will also collect more light and give a brighter image than a lens with lower NA. Slide 17 Your tricky friend - the objective Slide 18 How can we use the properties of light to create contrast? Which properties can be used? Absorption Scattering Refraction Phase Polarization Slide 19 Contrasting techniques Brightfield Darkfield Phase contrast DIC Taken from: http://fig.cox.miami.edu/~cmallery/150/Fallsyll.htmhttp://fig.cox.miami.edu/~cmallery/150/Fallsyll.htm Slide 20 Contrasting techniques Brightfield Darkfield Phase Contrast Polarization Contrast Differential Interference Contrast (DIC) Fluorescence Contrast ( Ireen) Slide 21 Brightfield Piece of artificially grown skin (www.igb.fhg.de/.../dt/PI_BioTechnica2001.dt.html )www.igb.fhg.de/.../dt/PI_BioTechnica2001.dt.html Cross section of sunflower root (http://www.zum.de/Faecher/Materialien/beck/12/bs12-5.htm) Principle: Light is transmitted through the sample and absorbed by it. Application: Only useful for specimens that can be contrasted via dyes. Very little contrast in unstained specimens. With a bright background, the human eye requires local intensity fluctuations of at least 10 to 20% to be able to recognize objects. all our microscopes can be used for brightfield Slide 22 Darkfield Principle: The illuminating rays of light are directed through the sample from the side by putting a dark disk into the condenser that hinders the main light beam to enter the objective. Only light that is scattered by structures in the sample enters the objective. Application: People use it a lot to look at Diatoms and other unstained/colourless specimens Brightfield Darkfield we do not have microscopes set up for darkfield Symbiotic Diatom colony (www1.tip.nl/~t936927/making.html) Slide 23 Phase contrast in theory Principle: Incident light [Io] is out of phase with transmitted light [I] as it was slowed down while passing through different parts of the sample and when the phases of the light are synchronized by an interference lens, a new image with greater contrast is seen. I I0I0 most of our microscopes are set up for phase contrast Phase ring alignednot aligned Phase stops Slide 24 Phase contrast in practice Application: Phase contrast is the most commonly used contrasting technique in this institute. All tissue culture microscopes and the time-lapse microscopes are set up for phase. BUT: MOST OF YOU ARE USING IT IN THE WRONG WAY!! Because you do not use the right phase stop with the corresponding objective! wrong phase stop brightfield right phase stop Slide 25 Polarization Contrast Principle: Polarized light is used for illumination. Only when the vibration direction of the polarized light is altered by a sample placed into the light path, light can pass through the analyzer. The sample appears light against a black background. A lambda plate can be used to convert this contrast into colours. we do not have microscopes set up for polarization contrast Lambda plate Polarizer Analyzer Application: Polarization contrast is used to look at materials with birefringent properties, in which the refractive index depends on the vibration direction of the incident light, e.g. crystals or polymers. BrightfieldPolarization contrast Polarization contrast with Lambda plate Slide 26 D (ifferential) I (nterference) C (ontrast) most of our microscopes are set up for DIC AB C > 0 XX XX XX n1 n2 n3 ~n/x X Principle: Also known as Nomarski microscopy. Uses polarized light for illumination. Synchronizing of the different phases of incident and transmitted light is done by a set of prisms and filters introduced into the light path. Slide 27 Contrasting techniques - a summary Brightfield - absorption Light is transmitted through the sample. Only useful for specimens that can be contrasted via dyes. Very little contrast in unstained specimens. Darkfield - scattering T he illuminating rays of light are directed from the side so that only scattered light enters the microscope lenses, consequently the cell appears as an illuminated object against the view. Phase Contrast- phase interference Incident light [Io] is out of phase with transmitted light [I] and when the phases of the light are synchronized by an interference lens, a new image with greater contrast is seen Polarization Contrast - polarization Uses polarized light for illumination. Only when the vibration direction of the polarized light is altered by a sample placed into the light path, light can pass through the analyzer. The sample appears light against a black background. Differential Interference Contrast (DIC) polarization + phase interference Also known as Nomarski microscopy. Synchronizing of the different phases of incident and transmitted light is done by a set of special condenser lens mounted below the stage of a microscope Fluorescence Contrast (->Ireen) Slide 28 Final words from your friend - the objective Coverslip-types: 1: 0.13 - 0.17 mm 1.5: 0.16 - 0.19 mm 2.0:0.19 - 0.23 mm Objective 10x 20x 40x 60x Slide 29 Useful links Margaret and Tom (ext. 6872)!!! Zeiss Microscopy from the very beginning http://www.zeiss.de/C1256B5E0047FF3F?Open http://www.zeiss.de/C1256B5E0047FF3F?Open Molecular Expressions homepage http://micro.magnet.fsu.edu/index.html http://micro.magnet.fsu.edu/index.html Wikipedia http://en.wikipedia.org/wiki/Main_Page