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Logo of nihpaAbout Author manuscriptsSubmit a manuscriptNIH Public Access; Author Manuscript; Accepted for publication in peer reviewed journal;
Opt Lett. Author manuscript; available in PMC Dec 6, 2007.
Published in final edited form as:
PMCID: PMC2117897
Dual-axis confocal microscope for high-resolution in vivo imaging
Thomas D. Wang, Michael J. Mandella, Christopher H. Contag, and Gordon S. Kino
Thomas D. Wang, Stanford University School of Medicine, 269 Campus Drive, Stanford, California 94305-5187;
We describe a novel confocal microscope that uses separate low-numerical-aperture objectives with the illumination and collection axes crossed at angle θ from the midline. This architecture collects images in scattering media with high transverse and axial resolution, long working distance, large field of view, and reduced noise from scattered light. We measured transverse and axial (FWHM) resolution of 1.3 and 2.1 μm, respectively, in free space, and confirm subcellular resolution in excised esophageal mucosa. The optics may be scaled to millimeter dimensions and fiber coupled for collection of high-resolution images in vivo.
Confocal microscopy provides high-resolution imaging in biological tissue by using the property of optical sectioning.1 This method is commonly used to collect reflectance and fluorescence images ex vivo and potentially can become a powerful tool in vivo if the lenses and scanning mechanisms can be made sufficiently small. A transverse resolution of approximately 1–2 μm with comparable axial resolution is adequate for identification of subcellular structures such as cell nucleus and membrane, which are important structures for medical and biological applications. The transverse resolution Δrs and the axial resolution Δzs between full width at half-power points for uniform illumination of the lenses are given by the following equations2:
equation M1
where λ is the wavelength, n is the refractive index of the medium, α is the maximum convergence angle of the beam, N.A. (=n sin α)is the numerical aperture, and sin αα for low-N.A. lenses.
At present, in vivo confocal imaging is limited to exposed tissue surfaces such as skin and oral mucosa3 because the size of the microscope objective required for achieving high transverse and axial resolution is too large to permit the instrument to be used internally. Equation (1) implies that transverse and axial resolution varies as 1/N.A. and 1/N.A.2, respectively. For an axial resolution of a few micrometers to be achieved, an objective lens must have a large N.A. and a size on a scale of centimeters. The optics cannot be reduced to a millimeter scale without sacrificing resolution, field of view (FOV), or working distance (WD). Also, the scanning mechanism must be located behind the objective, which restricts the FOV and increases sensitivity to aberrations. A microscope reduced in size to millimeter scale can be used to collect in vivo confocal images by means of an endoscope in human patients or by implantation in small animals. Previously, a laser scanning confocal microscope was miniaturized with microelectromechanical system (MEMS) fabrication techniques.4 This instrument had a single-axis design. It achieved high transverse but poor axial resolution and was not adequately developed for in vivo use.
In this Letter we demonstrate the feasibility of a novel dual-axes confocal microscope by predicting and measuring high transverse and axial resolution and long WD. With dual axes,5,6 two separate low-N.A. lenses are oriented with the illumination and collection axes crossing midline axis zd at an angle θ, as shown in Fig. 1. First, consider the illumination (IO) and the collection (CO) objectives separately. The main lobe of the point-spread function (PSF) of the illumination objective at the focal point is represented in the figure by a dark gray oval. This lobe has a narrow transverse dimension Δxs but a wide axial dimension Δzs. The PSF of the collection objective is similar in shape but symmetrically reflected about zd, as represented by the light gray oval. For the dual-axes system the combined PSF is the product of the individual PSFs. The intersecting region, represented by the small black oval, is characterized by narrow transverse dimensions, Δxd and Δyd (out of the page), and by a significantly reduced axial dimension Δzd, which depends on the transverse rather than on the axial resolution of the individual beams where they intersect.
Fig. 1
Fig. 1
Schematic diagram of the dual-axes design: D, lens diameter; other notation defined in text.
To estimate the combined spot size we first transform the optical axes as follows:
equation M2
For a low-N.A. lens, the depth of focus in the zs direction is large; thus the response along and perpendicular to midline axis zd depends only on Δxs and not on Δzs. Combining Eqs. (1) and (2) yields the following transverse (zd = 0) and axial (xd = 0, yd = 0) resolutions for dual axes:
equation M3
These results are confirmed by a more-detailed diffraction theory analysis.7 Thus, with dual axes, low-N.A. lenses can provide an axial resolution (Δzd) that is proportional to 1/N.A. rather than to 1/N.A.2.
Furthermore, low-N.A. lenses provide a long WD. For a lens with diameter D, the WD is given as follows from geometric arguments:
equation M4
Because the dual-axes beams can achieve an axial resolution of a few micrometers with N.A. of 0.2 or less, lenses with diameters as small as 1 mm can be used to produce a WD of several millimeters. This is sufficient space to allow a MEMS mirror (approximately 300–500 μm) to be placed in front of the objective and to provide beam scanning with the high speeds necessary for in vivo imaging. By comparison, conventional high-N.A. oil-immersion objectives have WDs of only approximately 100–200 μm.
To demonstrate proof of principle for a dual-axes system and to check our simple theory of operation, we built the breadboard device shown in Fig. 2, which uses readily available lenses and scans with micrometer stages rather than with a MEMS mirror. The output at 488 nm from a frequency-doubled semiconductor laser (Coherent Sapphire OEM) was passed through a neutral-density filter (ND) and was coupled into a single-mode polarization-maintaining optical fiber (F/O1) with a mean field diameter of 2.9 μm and a N.A. of 0.11. The polarized light coming out of the fiber was collimated by a 9-mm-diameter axial gradient index lens (L1), N.A. of 0.15, to a 5-mm-diameter beam and then focused by a 5-mm-diameter aspheric lens (L2), with a N.A. of 0.16 and a WD of 14.0 mm, to a spot size with a FWHM of 1.22 μm. The optical axis of illumination was oriented at θ = 30° to the midline axis. Approximately 400 μW of power was incident upon the scanning stage (XYZ). The reflected light was collected and collimated by a microscope objective (O1; Coherent 24–8690), f = 14 mm, N.A. of 0.17, WD of 12.3 mm, and entrance aperture 4.76 mm, which collimated the collected light. A second objective (O2; Nikon CF Plan EPI SLWD 10×, f = 20 mm, N.A. of 0.12, WD of 20.3 mm, entrance aperture 8.4 mm, focused the light into a second single-mode PM fiber (F/O2) with a mean field diameter of 3.4 μm and N.A. of 0.11. Achromatic objectives were used to accommodate the collection of broadband fluorescence. The output of the collection fiber was connected to a silicon detector. The WD of the complete optical system was measured to be 10.6 mm. Reflectance images were collected at 25 s per frame, digitized, and displayed. The image acquisition time was limited by the maximum speed of the scanning stages.
Fig. 2
Fig. 2
Schematic of the optical setup: D, detector; ADC, analog-to-digital converter; PC, personal computer; other abbreviations defined in text.
Figure 3(a) shows the response in free space to a chrome edge taken in the transverse direction with a measured 20–80% edge width of 1.06 μm. The edge response may be estimated by integration of the PSF.2 This process yields an estimated 20–80% edge width as follows:
equation M5
or an edge width of 0.75 μm from Eq. (5), with a N.A. of 0.165. Figure 3(b) shows the response to the chrome surface taken in the axial direction with a FWHM of 2.1 μm, which should be compared to the estimated value of 2.2 μm from Eq. (3).
Fig. 3
Fig. 3
(a) Transverse response to chrome edge; measured 20–80% width, 1.06 μm. (b) Axial response to chrome; measured FWHM spot length, 2.1 μm.
Reflectance images were collected from fresh biopsy specimens of normal human esophagus, a tissue accessible by endoscopy. Informed consent was obtained from the patient before the routine procedure. Specimens approximately 1 mm3 in size were resected with biopsy forceps, and the mucosal surface was oriented normal to the midline axis. Approximately 1 ml of 6% acetic acid was applied to enhance contrast.7 After image acquisition, the specimens were evaluated by routine histology. Figure 4 shows an image in a FOV of 200 μm at a depth of 10 μm; the scale bar is 20 μm. The cell nuclei (arrows) and membrane (arrowhead) can be clearly distinguished. These structures were confirmed by direct comparison with histology. We used the Adobe Photoshop 6.0 program to determine the average areas of the nucleus and of the cytoplasm of 12 epithelial cells and found them to be 71 ± 16 μm2 and 1000 ± 290 μm2, respectively, resulting in an average nuclear-to-cytoplasm ratio of 0.07 ± 0.02. These values are comparable to those measured from the corresponding histology sections.
Fig. 4
Fig. 4
This reflectance image of normal esophageal mucosa collected ex vivo reveals cell nuclei and membrane; scale bar, 20 μm.
The dual-axes design demonstrates several advantages over the single-axis design for purposes of miniaturization and in vivo imaging. First, sub-cellular resolution can be achieved easily in the axial as well as in the transverse dimension. Second, low-N.A. lenses that we use are relatively less sensitive to aberrations and are easy to fabricate with small dimensions. Third, a long WD is created that allows for a miniature mirror to be placed on the focused beam side of the objective to provide a large FOV. Fourth, light scattered along the illumination path outside the focal volume is less likely to be collected, thus enhancing detection sensitivity and dynamic range. The multiple scattering events required for the returning photons that originate outside the focal volume to arrive at the proper trajectory for detection occur with low probability. Finally, this method of imaging, unlike optical coherence tomography, can be used for collection of noncoherent light such as fluorescence.
In conclusion, we have presented a novel confocal microscope design that uses two low-N.A. lenses oriented in a dual-axes configuration and demonstrated sub-cellular transverse and axial resolution, long working distance, and large field of view. We have confirmed subcellular resolution is freshly resected human tissue. The illumination and collection optics are fiber coupled and scalable to millimeter dimensions. Future development of this microscope involves miniaturization with MEMS fabrication techniques followed by in vivo medical and biological imaging with reflectance and fluorescence.
We thank Mark H. Garrett and Matthew P. Scott for insightful discussions and George Triadafilopoulos for his technical assistance. This research was supported, in part, by grants from the National Institutes of Health including T32DK07056-27 (T. D. Wang), 1 R43 GM64028-01” (M. J. Mandella), CA88303, CA92862, and CA86312 (C. H. Contag), and unrestricted gifts from the Bio-X program at Stanford University and the Johnson Center for Perinatal Research as part of the Lucille Packard Foundation’s Child Health Initiative. T. D. Wang’s e-mail address is tdwang/at/
Contributor Information
Thomas D. Wang, Stanford University School of Medicine, 269 Campus Drive, Stanford, California 94305-5187.
Michael J. Mandella, Optical Biopsy Technologies, Inc., 235 Alma St., Palo Alto, California 94301.
Christopher H. Contag, Stanford University School of Medicine, 300 Pasteur Drive, Stanford, California 94305-5208.
Gordon S. Kino, Edward L. Ginzton Laboratory, Stanford University, Stanford, California 94305.
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