Microscopy Primer
Light and Color
Microscope Basics
Special Techniques
Digital Imaging
Confocal Microscopy
Live-Cell Imaging
Photomicrography
Microscopy Museum
Virtual Microscopy
Fluorescence
Web Resources
License Info
Image Use
Custom Photos
Partners
Site Info
Contact Us
Publications
Home

The Galleries:

Photo Gallery
Silicon Zoo
Pharmaceuticals
Chip Shots
Phytochemicals
DNA Gallery
Microscapes
Vitamins
Amino Acids
Birthstones
Religion Collection
Pesticides
BeerShots
Cocktail Collection
Screen Savers
Win Wallpaper
Mac Wallpaper
Movie Gallery

Differential Interference Contrast
Interactive Java Tutorials

Optical Staining with DIC Microscopy

By introducing birefringent compensator plates into the optical pathway of a differential interference contrast (DIC) microscope, transparent specimens that are otherwise rendered over a limited range of grayscale values can be transformed to display a wide array of colors through the technique known as optical staining. This interactive tutorial explores how varying the amount of bias retardation can affect the appearance and level of staining achieved in the specimen image.

Interactive Java Tutorial
ATTENTION
Our servers have detected that your web browser does not have the Java Virtual Machine installed or it is not functioning properly. Please install this software in order to view our interactive Java tutorials. You may download the necessary software by clicking on the "Get It Now" button below.

 

The tutorial initializes with a randomly selected DIC image appearing in the Specimen Image window having a small bias retardation value (one-twentieth of a wavelength) applied to the optical system. To operate the tutorial, translate the Bias Retardation slider to higher values (to the right) in order to produce higher-order interference colors in the specimen image. This slider has an operational range between 1/20 and a full wavelength of retardation. New specimens can be examined by selecting the appropriate choice in the Choose A Specimen pull-down menu.

Bias retardation between the ordinary and extraordinary wavefronts in differential interference contrast can be manipulated through the use of compensators originally targeted as quantitative retardation measuring devices and contrast-enhancing elements for polarized light microscopy. Compensating plates bestow greater control for adjusting the contrast of specimen details in relation to the background intensity and color values, and also enable more precise tuning of the bias value between wavefronts. These birefringent components are also frequently employed for optical staining of transparent specimens, which are normally rendered over a limited range of grayscale values.

When a standard objective Nomarski prism is translated along the microscope optical axis beyond path differences of one-quarter wavelength, both specimen features and the background acquire a spectrum of Newtonian interference colors similar to those observed in polarized light microscopy. The specimen and background become optically stained with a transition of color that migrates through a series of gray values through white, yellow, red-blue and higher orders. Optical staining produces dramatic and beautifully colored images, but has limited use for scientific applications. Usually, the optimum specimen contrast is limited to the range of one-twentieth to one-quarter wavelength of retardation.

Compensators can be inserted into the optical pathway of a DIC microscope between either the objective prism and the analyzer or the polarizer and the condenser prism. Many microscopes have a slot located in the intermediate tube or substage condenser housing designed for this purpose. Addition of a first-order compensator (often termed a full-wave or first-order red plate) having a retardation value equal to a full wavelength in the green region of visible light (approximately 550 nanometers), introduces a spectrum of interference colors to the specimen and background. With the compensator in place, green light is unable to pass through the analyzer because it emerges from the retardation plate linearly polarized with an electric field vector having the same orientation as the polarizer. However, wavefronts in the red and blue spectral regions experience retardations less than a wavelength and become elliptically polarized, allowing them to pass a component through the analyzer. As a result, these colors become mixed to form a magenta background in the field of view.

Thus, when a specimen is observed in white light with differential interference contrast optics and a first-order compensator, the background appears magenta while image contrast is displayed in the second-order blue and first-order yellow colors (depending on orientation) of the Newtonian interference color spectrum. With the compensator in place, small variations in bias retardation obtained by translation of the Nomarski prism (or rotating the polarizer in a de Sénarmont compensator) yield rapid changes to interference colors observed in structures having large path length gradients. This technique is useful for introducing color (optical staining) to regions having high refractive index boundaries, such as cellular membranes, large intracellular particles, cilia, and the nucleus. The interference colors displayed by specimen features can be compared to the values on a Michel-Levy color chart to obtain an estimate of the optical path difference.

Illustrated in Figure 1 are several transparent specimens that have been optically stained and rendered in pseudo three-dimensional relief through DIC optical techniques. Figure 1(a) depicts projections at the edge of a ctenoid fish scale, while the mouth of a canine hookworm (Ancylostoma caninum) is featured in Figure 1(b). Colorful wing scales of the Great Leopard moth (Ecpantheria scribonia) are presented in Figure 1(c). In all cases, the Nomarski prism was translated across the microscope optical axis to a bias retardation value exceeding a full wavelength. Although these images do not reveal hidden scientific information pertaining to the specimens, they do have the potential to advance the technique of DIC optical microscopy as a legitimate bridge between science and art.

On microscopes equipped with a de Sénarmont compensator for introducing bias into a differential interference contrast optical system, a full-wave retardation plate can be added to optically stain the specimen with Newtonian interference colors and provide more quantitative information about path differences. The de Sénarmont compensator is frequently employed in DIC microscopy to obtain precisely measured levels of bias retardation, but the device is also useful to monitor alignment of the optical components. In video-enhanced DIC (VE-DIC) microscopy, de Sénarmont compensators are often utilized to optimize contrast in specimen detail that lies below the resolution limit of the microscope.

Contributing Authors

Douglas B. Murphy - Department of Cell Biology and Microscope Facility, Johns Hopkins University School of Medicine, 725 N. Wolfe Street, 107 WBSB, Baltimore, Maryland 21205.

Jan Hinsch - Leica Microsystems, Inc., 90 Boroline Road, Allendale, New Jersey, 07401.

Kenneth R. Spring - Scientific Consultant, Lusby, Maryland, 20657.

Matthew J. Parry-Hill and Michael W. Davidson - National High Magnetic Field Laboratory, 1800 East Paul Dirac Dr., The Florida State University, Tallahassee, Florida, 32310.


BACK TO DIFFERENTIAL INTERFERENCE CONTRAST MICROSCOPY

Questions or comments? Send us an email.
© 1998-2013 by Michael W. Davidson and The Florida State University. All Rights Reserved. No images, graphics, scripts, or applets may be reproduced or used in any manner without permission from the copyright holders. Use of this website means you agree to all of the Legal Terms and Conditions set forth by the owners.
This website is maintained by our
Graphics & Web Programming Team
in collaboration with Optical Microscopy at the
National High Magnetic Field Laboratory.
Last modification: Wednesday, Mar 26, 2014 at 02:23 PM
Access Count Since January 17, 2003: 15748
For more information on microscope manufacturers,
use the buttons below to navigate to their websites: