OA 학술지
A Compact Top-View Conformal Optical System Based on a Single Rotating Cylindrical Lens with Wide Field of Regard
  • cc icon
  • cc icon

A new compact conformal dome optical system was established, and the aberration characteristics of the dome were investigated using Zernike aberration theory. The aberrations induced by the dome at different fields of regard (FORs) from 30° to 100° were effectively balanced by a rotating cylindrical lens. This kind of optical system can be widely used in top-view optical searching devices. A design method was introduced and the optimization results analyzed in detail. The results showed that the Zernike aberrations produced by the conformal dome were decreased dramatically. Also, a complete conformal optical system was designed, to further illustrate the aberration correction effect of the rotating cylindrical lens. Using a cylindrical lens not only provided a large FOR, but also simplified enormously the structure of the conformal optical system.

Optical design , Conformal dome , Infrared catadioptric , Aspherical

    The missile domes of today leave much to be desired in the realm of aerodynamic performance. The exterior spherical surface of a conventional missile dome creates up to 50% of the missile’s drag [1, 2]. Optimizing this exterior surface for aerodynamic performance can dramatically decrease the drag, with resulting increases in range, payload, or velocity. Otherwise, aerodynamic heating will produce a thermal barrier, impacting target recognition.

    A conformal aircraft uses a streamlined surface that can well overcome the above drawbacks, but the curvature of the conformal dome varies with the field of regard (FOR), leading to dynamic aberration that will increase the difficulty of designing an optical imaging system. A variety of aberration correction methods were proposed for narrow FORs, including a fixed aberration-correcting plate based on the Wassermann-Wolf equation, a pair of counter-rotating wedges, two axially movable cylindrical lenses, deformable mirrors, etc. [3-7]

    A new compact conformal optical system based on a single rotating cylindrical lens is adopted in this paper. This optical system provides a wide FOR from 30° to 100°, and can especially be used in top-view optical search devices. The aberration of the ellipsoidal dome is discussed first. We present a detailed rotating-cylindrical-lens design theory and method, based on a conformal system. An optical design with wide FOR is presented. The imaging quality is close to the diffractive limit.


    The aerodynamic performance of an ellipsoidal dome depends mainly on the length to diameter ratio. The face form of the inner surface is more or less arbitrary. To simplify the complexity of the analysis, the internal and external surfaces are set to be ellipsoidal and concentric, as shown in Fig. 1.

    The radius r and conic constant k are used to parametrize the structure ofa conformal dome. The equations used to determine the radius of curvature and conic constant from the fineness ratio are [8]


    where L is the length of the dome, D is its diameter, and F is the fineness ratio. An ellipsoidal dome can be established by the radius r and conic constant k.

    A conformal dome model is built to analyze the static and dynamic aberration properties for different FORs, as shown in Table 1. The outer surface of a conformal dome is continuous, so a conformal dome can provide an FOR far greater than a conventional spherical dome, without vignetting. We put a perfect lens 120 mm behind the dome as the imaging system. The circumrotation node is located at the center of the perfect lens; the rotation step of the gimbal is 10°, and the FOR is 100°.

    In this paper, Zernike polynomials are used to analyze the aberrations generated by an ellipsoidal dome. The mathematical expression for a Zernike polynomial is


    where m and n are integers, n-m ≥ 0 and is an even number, and ρ is the normalized pupil radius. We use terms Z5-Z9 of the Zernike polynomial expansion; the names of which are shown in Table 2.

    Astigmatism (Z5), coma (Z8), and spherical aberration (Z9) induced in the optical system by the dome are shown in Fig. 2. They vary with FOR. For narrow FOR, the ellipsoidal dome is similar to a sphere, while for wide FOR it loses spherical symmetry and gradually becomes similar to the structure of a cylinder, causing large coma and astigmatism. The spherical aberration stays at the level of -0.07 times the wavelength for any FOR, and can be ignored. The coma becomes most serious at 20°; when the FOR is greater than 30°, the coma is reduced to one wavelength and remains nearly constant. Compared to coma, astigmatism is more serious, especially when the FOR is greater than 30° and the value of astigmatism is nearly eight wavelengths, and varies with FOR. Thus astigmatism is the main dynamic aberration that needs to be corrected.


    Astigmatism is generated by a difference in optical powers in the tangential and sagittal planes, resulting in two separated line foci. It is well known that cylindrical elements can be introduced to an optical system to provide single-axis power compensation, to balance the relative mismatch in focal lengths, but a fixed cylindrical lens can only provide a certain astigmatism, and cannot correct the variable astigmatism at different FORs introduced by a conformal dome. This paper puts forward the use of a rotating cylindrical lens for variable astigmatism correction. When we rotate a cylindrical lens about the optical axis, the powers along the x’ and y’ axes projected from the cylindrical lens will change. This introduces a variable astigmatism to balance the astigmatism caused by the dome at different FORs.

    The underlying rationale for this correction technique is derived from the paraxial power relation for a system of two separated, thick lenses, given by Eq. (5) [9-11]:


    where ϕ is the total system power,

    τ the distance between elements, and

    ϕsi the individual element power.

    Each of these power relations is separable in x and y, as shown in Eqs. (6)~(7).


    where ϕy is the total system power along the y axis, and likewise ϕx the total system power along the x axis.

    The powers of the dome along the x and y axes are ϕxs1 and ϕys1, varying with FOR. The cylindrical lens can provide a single axis power, defined as ϕs2; the power along the vertical axis is zero. As shown in Fig. 3, the powers of the cylindrical lens along the x and y axes can be expressed as


    When the FOR changes, the cylindrical lens will be rotated about the Z’ axis. ϕxs2 and ϕys2 will consequently change to compensate the variable power of the dome. The total system power along the x’ axis should equal that along the y’ axis, then we have


    To achieve this, a correction structure is put forward, as shown in Fig. 4. L1 is an ellipsoidal dome, L2 is a cylindrical lens, and L3 is a perfect lens for imaging. At different FOR, the cylindrical lens rotates β degrees about the optical axis z’, and β can be derived from Eqs. (5)~(10).

    When correcting aberrations using a rotating cylindrical lens, the error function based on Zernike aberrations was found to converge rapidly and the value of the error function to be substantially reduced. The aberrations were obviously corrected. Since the error function has a few minima, the rotation angle must be appropriately adjusted according to the values and types of residual aberrations, in an optimization process. The weights of different FOR should also be appropriately distributed, according to the residual aberrations of each FOR. Sequentially, optimizing the optical system again achieves the minimal value of the error function.

    Figure 5 shows the curves for the astigmatism and coma of the conformal optical system, after correction. For FOR below 30°, the residual astigmatism and coma are still more than one wavelength, but this is not encountered in a top-view optical system. For FOR over 30°, the residual aberration is less than half of a wavelength, and the fluctuation range is very small, less than 0.75 of a wavelength. Therefore, the astigmatism induced by a conformal dome is well compensated by the rotating cylindrical lens from 30° to 100°.


    To illustrate that the rotating cylindrical lens has a better aberration correction effect, a complete cooled conformal optical system is designed by replacing the perfect lens with a solid catadioptric system. The whole conformal optical system consists of only three optical elements, as shown in Fig. 6. The optical system FOV is circular and of value 2 ω = 4.88°. The total length of the system from the apex of the dome to the image plane is 120 mm, less than the dome length. The aperture stop is placed at 19.8 mm from the image plane, and the diameter of the exit pupil is set 10.6 mm, to bring the cold aperture efficiency to 100%.

    The imaging part of the system behind the dome is a solid catadioptric structure. This optical system can effectively shorten the light path and make the system more compact. To correct other aberrations, all of the surfaces are chosen to be aspherical, with a profile expressed via Eq. (11):


    where c is the curvature (the reciprocal of the radius), r is the radial coordinate in lens units, k is the conic constant, and αi is the coefficient.

    The relationship between FOR and the rotation angle of the cylindrical lensafter optimization is show in Fig. 7. The curve is smooth and easy for a servo to implement. The function after curve fitting can be written as follows:


    Figure 7 is the modulation transfer function (MTF) curve of the optical system for different FOR, wherein most MTF values are close to the diffraction limit, and a few are nearly 0.41 at the Nyquist frequency of 16.67 lp/mm. The optical system offers excellent image quality.


    This paper has presented a conformal top-view seeker optical system based on a rotating cylindrical lens, with simple structure and excellent imaging quality. The aberration characteristics of the ellipsoidal dome were well investigated. The results showed that the Zernike aberrations introduced by the dome from 30° to 100° were decreased dramatically. Finally, an optical design with only three optical elements was presented. Compared to the traditional aberration correction method, the method presented in this paper not only improved the imaging quality, but also simplified the structure of the conformal optical system.

  • 1. Zhao N. (2008) “Summarize of conformal optics,” [Proc. SPIE] Vol.6624 P.1-7 google
  • 2. Chang J., Liu L. P., Cheng D. W., Zhao N. (2009) “Design of infrared optical system with special dome,” [J. Infrared Millim. Waves] Vol.28 P.204-206 google doi
  • 3. Sparrold S. W. (2000) “Conformal dome correction with counterrotating phase plates,” [Opt. Eng.] Vol.39 P.1822-1829 google doi
  • 4. Knapp D. (2002) “Fundamentals of conformal missile dome design,” [OSA/IODC] Vol.IWB1 P.168-169 google
  • 5. Leroux C. E., Tzschachmann A., Dainty J. C. (2010) “Pupil matching of Zernike aberrations,” [Opt. Express] Vol.18 P.21567-21572 google doi
  • 6. Liu Y. M., Ma J., Ma H. P., Jiang X. Z. (2010) “Zernike aberration characteristics of precision conformal optical windows,” [Proc. SPIE] Vol.7544 P.1-7 google
  • 7. Li Y., Li L., Huang Y. F., Liu J. G. (2009) “Conformal optical design with combination of static and dynamic aberration corrections,” [Chin. Phys. B] Vol.18 P.565-570 google doi
  • 8. Sparrold S. W. (1999) “Arch corrector for conformal optical systems,” [Proc. SPIE] Vol.3705 P.189-203 google
  • 9. Whalen M. R. (1999) “Correcting variable third order astigmatism introduced by conformal aspheric surfaces,” [Proc. SPIE] Vol.3482 P.32-37 google
  • 10. Liebetraut P., Petsch S., Liebeskind J., Zappe H. (2013) “Elastomeric lenses with tunable astigmatism,” [Light: Science & Applications] Vol.2 P.e98 google
  • 11. Pechprasarn S., Zhang B., Albutt D., Zhang J., Somekh M. (2014) “Ultrastable embedded surface plasmon confocal interferometry,” [Light: Science & Applications] Vol.3 P.e187 google
이미지 / 테이블
  • [ FIG. 1. ]  Geometrical model of an ellipsoidal dome.
    Geometrical model of an ellipsoidal dome.
  • [ ] 
  • [ ] 
  • [ ] 
  • [ TABLE 1. ]  Parameters of an ellipsoidal dome
    Parameters of an ellipsoidal dome
  • [ ] 
  • [ TABLE 2. ]  Terms Z5-Z9 of a Zernike polynomial expression
    Terms Z5-Z9 of a Zernike polynomial expression
  • [ FIG. 2. ]  Astigmatism and coma versus FOR.
    Astigmatism and coma versus FOR.
  • [ ] 
  • [ ] 
  • [ ] 
  • [ FIG. 3. ]  Powers of the cylindrical lens along x’ and y’ axes.
    Powers of the cylindrical lens along x’ and y’ axes.
  • [ ] 
  • [ ] 
  • [ ] 
  • [ FIG. 4. ]  Conformal optical system with rotating cylindrical lens.
    Conformal optical system with rotating cylindrical lens.
  • [ FIG. 5. ]  Aberration characteristics of the conformal optical system, after optimization.
    Aberration characteristics of the conformal optical system, after optimization.
  • [ FIG. 6. ]  Schematic diagram of a cooled conformal optical system.
    Schematic diagram of a cooled conformal optical system.
  • [ ] 
  • [ FIG. 7. ]  Rotation angle of the cylindrical lens versus FOR.
    Rotation angle of the cylindrical lens versus FOR.
  • [ ] 
  • [ FIG. 8. ]  Modulation transfer function (MTF) of the conformal optical system, for FOR of (a) 30°, (b) 40°, (c) 50°, (d) 60°, (e) 70°, (f) 80°, (g) 90°, and (h) 100°.
    Modulation transfer function (MTF) of the conformal optical system, for FOR of (a) 30°, (b) 40°, (c) 50°, (d) 60°, (e) 70°, (f) 80°, (g) 90°, and (h) 100°.
(우)06579 서울시 서초구 반포대로 201(반포동)
Tel. 02-537-6389 | Fax. 02-590-0571 | 문의 : oak2014@korea.kr
Copyright(c) National Library of Korea. All rights reserved.