Achromatic and apochromatic prism element employing prisms and gratings

Abstract: A dispersive optical element employing a grism (34) which is a combination of a grating and a prism. An achromatic grism (34) consists of a prism (36) with a grating (38) attached to its front surface (40). In the preferred embodiment the grating has an Abbe number and partial dispersion coefficient chosen such that the primary angular chromatic spread error is approximately zero. In another embodiment of the present invention, an apochromatic grism (42) includes a first prism (48) with a second prism (50) disposed adjacent to it. A grating (44) is adjacent to the front surface of the first prism (48) and the Abbe number and dispersion coefficient of the grating are chosen such that the primary and secondary angular spread for a given spectral band is approximately zero, The achromatic and apochromatic grisms of the present invention are simple and compact devices with minimal amounts of residual chromatic and anamorphic aberrations.

Description: CROSS REFERENCE TO RELATED APPLICATION The present invention contains subject matter which is related to co-pending U.S. Patent Application entitled "A Grism (Grating-Prism Combination)" Serial No. 07/993,344 (EP-A-0 602 992) which is assigned to the same assignee as the present application. BACKGROUND OF THE INVENTION 1. Technical Field This invention relates to a technique for reducing aberrations in optical systems, and more particularly to a simple and compact optical element employing the combination of a grating and a prism. 2. Discussion The prism has long been one of the very basic optical components in many optical systems. It is a very fundamental optical component for many applications such as for altering beam direction, zooming elements, anamorphic aberration correction, line of sight correction, etc. The applications also include infrared systems (FLIR), head-up displays (HUD), helmet mounted display (HMD) systems, laser radar, commercial cinematography, etc. Unfortunately, the generic dispersion characteristics of a prism limits its applications. That is, because of the variation in index of refraction and dispersion with wavelength, prisms are often not useful in applications involving a wide spectral range of optical radiation. These dispersion characteristics result in optical chromatic aberrations, that is, a departure of the image-forming system from the ideal behavior occurring when a beam passes through a system. In particular, prisms are prone to chromatic aberrations which results from the variation in the index of refraction with wavelength. Chromatic aberration will severely degrade the image quality of an optical system. However, aberration of an optical component has both a positive and a negative contribution, and if these contributions are balanced, the total aberration of the system can be tolerably small. For example, achromatic and apochromatic prisms take advantage of this approach. Achromatic prisms consist of a pair of prisms with different dispersion coefficients and different prism angles. Apochromatic prisms, usually employ two pairs of prisms with at least three different glass materials. While these two approaches attempt to balance the positive and negative contributions to chromatic aberration they still have a number of drawbacks. For example, the residual chromatic aberration is generally larger than desired. Also, both achromatic and apochromatic prisms, because of the different prism components and materials, are generally bulky, complicated and expensive. Thus it would be desirable to provide achromatic prisms and apochromatic prisms with a simplified construction. It would also be desirable to provide achromatic and apochromatic prisms having improved performance with extremely small residual chromatic and anamorphic aberrations. Prism and grating combinations are known from WO-A-93/21548 and US-A-5101458. WO-A-95/21548, which is only cited under Article 54(3) EPC, discloses a grism system comprising: an achromatic prism assembly comprising a first prism that transmits energy over the entirety of a given spectral band, the first prism having first and second faces disposed at a first prism angle Al, and a second prism that transmits energy over the entirety of said spectral band, the second prism having first and second faces disposed at a second prism angle A2; and a grating on one of the faces of the first and second prisms, the grating having a predetermined grating period. With the foregoing in mind, in a grism system according to the present invention distinguishes over this state of the art by the subject matter that the first and second prisms and grating perform apochromatic correction by mutually cooperating to change the angle of at least three colors within a design spectral wavelength band such that the primary and secondary angular spread for the given spectral band is approximately zero. The various advantages of the present invention will become apparent to those skilled in the art after a study of the following specification and by reference to the drawings in which: FIG. 1 is a schematic of a prism illustrating with both primary and secondary angular spreads for its beam deviation; FIG. 2 is a schematic of an all-refractive achromatic prism; FIG. 3 is a schematic of a refractive-diffractive achromatic grism for use in a system according to the present invention; and FIG. 4 is a schematic of an apochromatic refractive-diffractive grism in accordance with the present invention. FIG. 5 is a diagram of a variable power anamorphic grism in accordance with the present invention. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT Referring now to FIG. 1, a typical prism 10 is shown with a prism angle 11 (A) between first and second faces 12, 14 respectively. The beam deviation angle 15 (δ) is defined as the angular difference between the light beam incident on the prism and the light beam emerging from the prism for a middle wavelength 16 (λ d ) of the spectral band of light. The primary angular spread 17 (Δ) is defined as the output angle difference between the short wavelength 18 (λ f ) and the long wavelength 20 (λ c ). The secondary angular spread 22 (ε) is defined as the output refractive angular difference between the long wavelength 20 (λ c ) and the middle wavelength 16 (λ d ). In an achromatic prism, by definition, there is no primary angular spread error. An apochromatic prism is defined as a prism with no primary angular spread and no secondary angular spread errors. Although an apochromatic prism has no primary and secondary angular errors, it still has residual chromatic angular errors for those wavelengths different from the three design wavelengths. These residual chromatic angular errors often are the main chromatic aberration which restricts the use of the prism for certain applications. FIG. 2 shows an achromatic prisms 24 with prism angles 26 and 28 (A 1 and A 2 ), indices of refraction 30 and 32 (n d1 and n d2 ) for the middle wavelength 16 (λ d ), Abbe numbers V 1 and V 2 , and partial dispersion coefficient P 1 and P 2 for the spectral band from the short wavelength 18 (λ f ) to the long wavelength 20 (λ c ). If the beam deviation angle 15 (δ) and the secondary spectrum angular spread 22 (ε) are as indicated in FIG. 2, an achromatic prism satisfies the following relationships: Referring now to FIG. 3, a "grism" 34 for use in a system according to the present invention is shown. In essence, a grism is a combination of a grating and prism. Thus, the grism 34 in FIG. 3 is comprised of a prism 36 and a grating 38. In this embodiment, the grating 38 is attached to the first surface 40 of the prism 36. For further details about grisms and their design reference is made to co-pending U.S. Patent Application Serial No. 07/ 993,344 (EP-A-0 602 992) entitled "A Grism (Grating - Prism Combination)". For a diffraction grating such as the one 38 in FIG. 3, the Abbe number (V g ) and partial dispersion coefficient (P g ) are reduced to the following equations: V g = λ d λ f - λ c < 0 P g = λ d - λ c λ f - λ c > 0 Therefore, for an achromatic grism 34, the first order solution of the prism angle 11 (A), the grating period T and the secondary angular spread 22 (ε) are: Also, the index of refraction (n) as a function of wavelength can be approximated as: n = A 1 + A 2 λ -2 + A 3 λ -4 + A 4 λ 2 + A 5 λ 4 +.... From the above derived equations, Table 1 summarizes the Abbe numbers (V) and partial dispersion coefficient (P) for two well-known refractive materials (BK7 and F2) and for a diffractive grating. ABBE NUMBER AND PARTIAL DISPERSION COEFFICIENT FOR REFRACTIVE AND DIFFRACTIVE OPTICAL ELEMENTS BK7 F2 Diffractive Grating V 64.17 36.37 -3.45 P 0.3075 0.2937 0.4036 The secondary angular spread-to-beam deviation angle ratio, ε/δ, is significant because it reveals the chromatic aberration with respect to the prismatic power. Accordingly, a desirable secondary angular spread-to-beam deviation angle ratio would be one that is close to zero. From equation (3) and Table 1, the secondary angular spread-to-beam deviation angle ratio, ε/δ, for a BK7-F2 achromatic prism is 4.964 X 10 -4 . Similarly, the secondary angular spread-to-beam deviation angle ratio, for a BK7-grating achromatic prism is -1.5826 X 10 -3 . It should be noted that the algebraic sign of the secondary angular spread-to-beam deviation angle ratio, ε/δ, for a conventional achromatic prism is opposite to that of a refractive-diffractive achromatic grism. The opposite algebraic sign in secondary angular spread 22 between an all-refractive prism and a refractive-diffractive grism can make the secondary chromatic aberration correction perfect. In addition, the magnitude of the secondary angular spread-to-beam deviation angle ratio, ε/δ, for a refractive-diffractive achromatic grism is much larger than that of an all-refractive achromatic prism. Combining one classical achromatic prism and one grism (where the secondary angular spread 22 of both the prism and grism have opposite algebraic signs) yields a total prism assembly which is apochromatic. Therefore, for a fixed beam deviation angle, the required prismatic power for a refractive-diffractive apochromatic prism is much smaller than that of an all-refractive apochromatic prism (The prismatic power indicates a prism's ability to alter the deviation angle). Consequently, the aberrations introduced by refractive-diffractive apochromatic grisms are much smaller than that of the all-refractive prism. Referring again to FIG. 3 in a preferred embodiment, the refractive-diffractive achromatic grism 34 has a prism angle 11 of ten degrees and a grating 38 frequency of 212.401 lines per inch (1 inch = 25.4 mm). The beam deviation angle 15 is 15.558 degrees with a secondary angular spread 22 is 0.008 degrees. With reference to FIG. 4, a refractive-diffractive apochromatic grism 42 according to the invention includes a diffractive grating 44 with a spatial frequency of 29.5858 lines per inch etched on the front surface 46 of a first prism 48. A second prism 50 has its front surface attached to the rear surface 54 of the first prism 48. The prism angles At and A 2 are 11.1407 degrees and 4.561 degrees for the first and second prisms (48, 50) respectively. First prism 48 is made of BK7 material and second prism 50 is made of F2 material. The beam deviation angle 15 is 8.4157 degrees with almost perfect correction for the secondary spectrum. The advantages of the refractive-diffractive apochromatic grism 42 over an all-refractive apochromatic prism include: (1) excellent secondary color correction with very little residual angular spread for any wavelength within the design spectral band, (2) only two different refractive materials are required, without the need of any special glass material, and (3) the grism assembly is very simple and the prism angle is small; therefore, the prismatic power induced aberrations are very small. Referring now to FIG. 5 another embodiment of the present invention is shown. Here, a variable power anamorphic grism apparatus 56 is shown. The term "Anamorphic" means that different optical magnification is produced along mutually perpendicular direction. It will be appreciated that the magnification of an afocal optical system is given by the ratio of the diameters of its entrance and exit pupils. A refracting prism, used at other than minimum deviation has different sized exit and entrance beams, and thus produces a magnification in the meridian in which it produces a deviation. Thus a single prism may be used as an anamorphic system. To eliminate the angular deviation, two prisms arranged so that their deviations cancel and their magnifications combined are usually used. FIG. 5 illustrates a compound anamorphic grism system 56 made up of a grism 58, and a prism 60. The grism 58 comprises a prism 62 and a diffraction grating 64 attached to its front surface. Since the "magnification" of a prism is a function of the angle at which the beam enters the prism, a variable power anamorphic can be made by rotating the prisms in such a way that their deviations always cancel. Prism anamorphic systems are "in focus" and free of axial stigmatism only when used in parallel light. The advantage of using a grism in the anamorphic system 56 is that the primary and secondary chromatic aberrations can be well corrected with a very small residual chromatic aberration for those wavelengths different from those three design wavelengths. Additionally, the anamorphic prism assembly is very compact. It should be noted that the construction of a grism is not limited to the particular configuration shown above. For example, the diffraction grating may be attached to the rear rather than the front surface of the prism. Also, the grating may be etched onto the prism surface, attached or bonded in some manner, or merely placed adjacent to the prism. Those skilled in the art can appreciate that other advantages can be obtained from the use of this invention and that modification may be made without departing from the scope of the invention as defined in the claims.

Claims: A grism system (42) comprising: an achromatic prism assembly comprising a first prism (48) that transmits energy over the entirety of a given spectral band, the first prism (48) having first (46) and second (54) faces disposed at a first prism angle A1, and a second prism (50) that transmits energy over the entirety of said spectral band, the second prism (50) having first (52) and second faces disposed at a second prism angle A2; and a grating (44) on one of the faces (46,52,54) of the first and second prisms (48,50), the grating (44) having a predetermined grating period, wherein the first and second prisms (48,50) and grating (44) perform apochromatic correction by mutually cooperating to change the angle of at least three colors within a design spectral wavelength band such that the primary and secondary angular spread (ε) for the given spectral band is approximately zero. A system according to claim 1, wherein one prism is made of infrared transmitting optical material. A system according to claim 2, wherein one prism (48) is made of BK7 material and the other prism (50) is made of F2 material. A system according to claim 1, wherein the first and second prisms (48,50) are made of glass material. A system according to any preceding claim, wherein the prisms (48,50) have high positive Abbe numbers and the grating (44) has a low negative Abbe number; whereby residual chromatic angular spread of the grism (42) is minimized. A system according to any preceding claim, wherein the grating (44) is etched onto the first prism (48). A system according to any preceding claim, wherein the second face (54) of the first prism (48) is adjacent the first face (52) of the second prism (50) and the grating (44) is disposed adjacent to the first face (46) of the first prism (48). A system according to claim 1, wherein the system is a variable power anamorphic grism apparatus (56).

Inventors: CHEN CHUNGTE W, CHEN, CHUNGTE W.
Applicants: RAYTHEON CO, RAYTHEON COMPANY
Application year: 1993
Main classification: G02B27
IPC codes: G02B27, G02B5