Development of a narrow water-immersion objective for laserinterferometric and electrophysiological applications in cell biology
Introduction
A major part of modern biological and physiological research involves the study of cellular mechanisms inside ``living'' tissue. When working with sections of tissue in which the cells of interest are located directly under a glass cover, optimal resolution can be obtained with conventional, high numerical aperture, oil-immersion objectives corrected for the cover glass. However, the resolution is severely reduced when using these oil-immersion objectives for focusing at depths more than several tenths of micrometers within the tissue; this is due to the difference in refractive indices of glass (1.515) and tissue (1.33–1.35). Under these circumstances, better results can be obtained with water-immersion objectives, which are available for working distances from several tenths of millimeters to several millimeters. Optically optimized long-range objectives of this kind allow sufficient space between the tissue and the objective for many experimental purposes (e.g. patch-clamping) and, in addition, their outer shape is often adapted to the in vitro or in situ situation. Examples of four commercially available water-immersion objectives are given in Fig. 1. However, for in vivo experiments the situation may be less than optimal because lateral access for recording electrodes, for example, is not possible or because optical access is hindered for anatomical reasons.
In our application, an objective is required for focusing the light from a laser Doppler vibrometer onto cellular structures in the cochlea. Although we (Gummer et al., 1996) were able to make successful vibration measurements in a temporal bone preparation of the cochlea using a commercially available objective (Zeiss Acroplan 40x/0.75 WPh2), in vivo vibration experiments proved impossible because, unlike the in vitro situation, it was not possible to remove sufficient overlying tissue to allow access with the Zeiss objective (Fig. 2A). The in vivo experiments, requiring the neuronal and systemic inputs to the inner ear to be left undisturbed, must be conducted with a much smaller ventral opening of the middle-ear cavity or bulla (Fig. 2). This paper describes the objective (Fig. 1C, Fig. 2B) that we designed for the in vivo vibration measurements, giving its theoretical and experimental performance.
Vibration measurements in the apical (low-frequency) region of the in vitro (Khanna et al., 1989, Ulfendahl et al., 1989) and in vivo (Khanna and Hao, 1996) cochlea have made use of long-range air-objectives in combination with a dipping cone. However, the dipping cone is not commercially available. Unfortunately, relevant structures can be discerned only occasionally when using commercially available water-immersion objectives. For vibration measurements, a long-range air-objective without a dipping cone requires a glass window at the interposed fluid-air interface. Generally, a decrease in the signal-to-noise ratio is produced by additional reflections and poor image quality due to the uncompensated change of the refractive index in the optical path. To compensate for a loss of image quality, the endolymphatic space must be opened and under normal in vivo conditions reflective beads must be placed on the vibrating surface (Cooper and Rhode, 1995). It is possible, however, to make vibration measurements of the highly reflecting lipid droplets of Hensen cells without introducing a reflector (Cooper and Rhode, 1996).
To design a dipping cone of high optical quality for a commercially built long-range objective, a knowledge of the detailed parameters of the objective is essential: Unfortunately, they are usually kept secret by the manufacturers. To avoid these disadvantages, we decided to develop a water-immersion objective with a narrow tip-diameter adapted to the special anatomical constraints of our experiments.
We present here an affordable way to develop and construct a custom-designed achromatic objective which is not only suited to our laser vibrometric experiments, but can also be used in other applications where space is a major constraint: for example, in certain types of patch-clamp experiment.
Section snippets
Specifications
Vibration measurements were to be made in the apical region of the cochlea by coupling the beam of a helium-neon (633 nm), laser Doppler vibrometer (Polytec OFV-302) into the side-arm of an epifluorescence microscope (Leitz Aristomet) (Fig. 3). This measurement technique has been used in vivo in the basal half of the cochlea (Ruggero and Rich, 1991, Nuttall et al., 1991) and in a temporal bone preparation in the apical half of the cochlea (Gummer et al., 1996).
Access to the apical end of the
Design and numerical optimization
The performance of the optical system was determined and optimized using two different optical design programs: Code V (Optical Research Associates, CA, USA) and ZEMAX (Optima Research Ltd., UK). Although these programs are highly elaborate, it must be emphasized that the success of a lens' design depends strongly on the quality of the initial estimates of the lens' parameters. The design of an objective from a zero starting point requires much more experience than was available in our group.
Calculated optical performance
Fig. 4 shows the final lens configuration for the objective. The calculation of the reflections (percentages above the lens diagram) showed that only the back-surface of the front lens (L1: 2.5%) and both surfaces of the last plano-convex lens (L6: 3.3%, 5.5%) would contribute reflections in the range of a few percent (if a 100% reflecting surface is assumed). For the quality of the broadband coating specified by the manufacturer (r<0.3%), this would result in a relative reflected intensity of
Conclusion
The key element to the performance of a microscope is the objective lens system. Both theoretical and experimental results have shown that it is possible to handle the challenges arising from the development of a custom-built objective in a small research laboratory. With modern, powerful optical design programs, optical design problems can be solved on a PC platform. If not already available, initial parameters can be obtained from colleagues in University Engineering Departments, patents or
Acknowledgements
This work is supported by the Deutsche Forschungsgemeinschaft, Gu 194/3–1 and SFB 307, C10. The authors gratefully acknowledge Heiko Wasmund from Syncotec Wetzlar for helpful discussions and valuable help in the construction and development; Bernd Packroß from Lamtech GmbH, Stuttgart, for assistance in development and introduction to ZEMAX and for critical reading of the manuscript; Joachim Rienitz for supplying the microscope test objects; Ulrich Rexhausen and Henry Haase for the DIC
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Present address: Hensoldt AG, Wetzlar, Germany.