MIRROR

Inventors: Todd Scott Rutherford

William Earl Phillips III Brandon Antonio Sosa

CROSS-REFERENCE TO RELATED APPLICATION(S)

[0001] This application claims priority to U.S. Provisional Patent Application Serial No. 62/903,687, “High Image Quality During Off-Axis Projection Using A Free-Form Mirror,” filed Sept 20, 2019. The subject matter of all of the foregoing is incorporated herein by reference in its entirety.

BACKGROUND

1. Technical Field

[0002] This disclosure relates generally to off-axis image projection systems.

2. Description of Related Art

[0003] Off-axis image projection systems suffer from non-uniform relative illumination (RI), non-uniform modulus of the optical transfer function (MTF), non-uniform magnification (distortion) and non-uniform shape (keystoning), to name a few issues. These non-uniformities are exasperated when the off-axis projection angles increase and/or when the distance from the projector’s final optical surface is forced to come close to the output projection plane.

BRIEF DESCRIPTION OF THE DRAWINGS

[0004] The patent or application file contains at least one drawing executed in color. Copies of this patent or patent application publication with color drawing(s) will be provided by the Office upon request and payment of the necessary fee.

[0005] Embodiments of the disclosure have other advantages and features which will be more readily apparent from the following detailed description and the appended claims, when taken in conjunction with the examples in the accompanying drawings, in which:

[0006] Figure 1 is a cross-sectional view of an example embodiment of an off-axis image projection system.

[0007] Figure 2 is a diagram of the image source for the projection system of Figure 1. [0008] Figure 3 is a ray trace through the MLA and Fourier Transforming lens of Figure 2.

[0009] Figures 4A and 4B show the irradiance profile striking the DMD after beam homogenization.

[0010] Figures 5A and 5B are a diagram and ray trace for the imaging path through the off-axis image projection system of Figure 1.

[0011] Figures 6A and 6B show the irradiance profile striking the final projection surface of Figure 1.

[0012] Figure 7 plots the MTF for the system of Figure 1.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS [0013] The figures and the following description relate to preferred embodiments by way of illustration only. It should be noted that from the following discussion, alternative embodiments of the structures and methods disclosed herein will be readily recognized as viable alternatives that may be employed without departing from the principles of what is claimed.

[0014] In some embodiments, an extreme off-axis image projection system substantially compensates for image-quality-degrading aberrations typical to off-axis imaging systems. This is accomplished through the use of a free-form mirror (or other type of non- spherical mirror) in conjunction with both spherical and aspherical refractive elements and an off-axis placement of the input image source.

[0015] Figure 1 is a cross-sectional view of an example embodiment of such an off-axis image projection system. The off-axis image projection system 100 contains a projection lens system 110 with multiple lenses and also contains a free-form mirror 120. Figure 5 A (discussed in more detail below) is a magnified view of the lens system 110. In this example, the lens system 110 contains spherical and aspherical lenses. The projection system 110 projects light from an image source 150 onto a surface 160 (aka, projection surface). The projection surface 160 is both close to the projector (in z) and extends away from the projector (in x and y).

[0016] The coordinate system is defined as follows. The optical axis of the lens system 110 defines the z-axis. The projection surface 160 may be non-planar (e.g., a car door), but it extends primarily perpendicularly to the z-axis. The long direction of the projection surface 160 defines the x-axis and the other direction defines the y-axis. For example, if the projection surface is approximately rectangular, then the long edge of the rectangle defines the x-axis and the short edge defines the y-axis.

[0017] The image source 150 is offset in one direction along the x-axis (along the -x direction in Figure 1), and the mirror 120 and the projection surface 160 are offset in an opposite direction along the x-axis (+x direction in Figure 1). In some designs, all of the image-forming rays from the image source 150 originate from one side of the y-z plane (i.e., from the -x side). They cross the y-z plane and then reflect off the mirror 120 to the projection surface 160, so that the footprint of the image-forming rays on the mirror 120 is entirely on the +x side of the y-z plane, as is the image on the projection surface 160. The image source 150 and projection surface 160 may also be offset in opposite directions with respect to the y-axis.

[0018] In these designs, the overall system (image source 150, projection system 100 projection surface 160) is compact along the z dimension, but the projection surface 160 may extend significantly in the x- and y-directions. In some embodiments, the length of the system along the z-axis is not more than 220mm, or even 200mm or less; while the projection surface is at least 1000mm x 600mm (x-dimension x y-dimension) or even 1200mm x 680mm or larger. In some embodiments, the x-extent of the projection surface is in the range 850mm to 1600mm, or even larger. The y-extent of the projection surface may be in the range 500mm to 800mm or even larger. The ratio of the x-extent to the z-extent is preferably at least 6:1, and may be in the range of 4: 1 to 10:1.

[0019] Image quality issues, such as low relative illumination (RI), low modulus of the optical transfer function (MTF), high distortion, high keystoning, and other image quality degradations, are substantially mitigated by using a free-form mirror 120 in conjunction with off-axis refractive optics 110, as described in more detail below.

[0020] Figure 2 is a diagram of the image source 150 for the projection system of Figure 1, including light source collimators, spectral beam combiners, and beam homogenizer. In this example, the light sources are arrays of red, green and blue light emitting diodes (LEDs) 251R,G,B. Extractor lenses 252, condenser lenses 253 and dichroic plates 254 are used to condition and combine the light from the different LED arrays 251. A Micro-Lens Array (MLA) 255 is used in conjunction with a Fourier Transforming lens 256 to convert the Gaussian-like beam intensity profiles from the collimated light sources to a substantially-flat irradiance profile at the spatial light modulator 257, which in this example is a deformable micromirror device (DMD). A Total Internal Reflection (TIR) prism pair 258 is used to couple the light into and out of the DMD. [0021] Figure 3 is a ray trace through the MLA 255 and Fourier Transforming lens 256, to the DMD 257, indicating how light from all portions of the input collimated Gaussian beam (from the LEDs and entering the MLA 255 on the left) become shared across the plane of light that irradiates the DMD 257. The Fourier Transforming lens 256 converts angles of light rays exiting the MLA 255 into light ray positions at the DMD 257 and converts light ray positions exiting the MLA 255 into light ray angles irradiating the DMD 257. In this manner, each location on the DMD 257 receives light rays from many different portions of the Gaussian beam profile irradiating the MLA 255. This substantially homogenizes the beam irradiance onto the DMD 257.

[0022] Figures 4A and 4B show the irradiance profile striking the DMD 257 after beam homogenization. Figure 4A is a two-dimensional plot across the surface of the DMD 257, where the color indicates the irradiance. Figure 4B shows one-dimensional traces A-A and B-B through the two-dimensional profile of Figure 4A. Except for some anomalous irradiance at extreme comers, the RI at the DMD is substantially homogenized. In addition, this approach (MLA plus Fourier Transforming lens) is inexpensive and compact.

[0023] Tables 1 and 2 show the optical prescription data for the system’s light source collimation optics and beam homogenizer.

Table 1 : Optical prescription for LED collimator Table 2: Optical prescription for beam homogenizer

[0024] Figures 5A and 5B are a diagram and ray trace for the imaging path through the off-axis image projection system of Figure 1. Table 3 shows the optical prescription data for the projection lens system 110 and free-form mirror 120. Table 3: Optical prescription for projection lens system and free-form mirror

[0025] Once the light reflects off the DMD, it enters the projection optical system, as diagrammed in Figure 5. Off-axis imaging compensation begins by placing the DMD off- axis at the front-end of the imaging path. Along the imaging path, both spherical and aspherical refractive optical elements 110 are used in conjunction with a free-form mirror 120 at the output plane of the projection optics. The alignment of the DMD, the projection lens system 110 and the free-form mirror 120 all work together to pre-aberrate the output image forming rays such that when they propagate to the projection surface, all rays are substantially mapped into their appropriate location with an appropriate brightness such that the observed image on the extreme-off-axis projection surface has high RI, high MTF, low distortion and low keystoning (i.e., high image quality). For example, embodiments may achieve RI of at least 50% at 90% of the field height, at least 3 pixel resolution across the entire field, and/or distortion of not more than 30% across the entire field.

[0026] The first lens group 511 near the DMD work to make the lens near telecentric and improve the RI of the system. The aspheres in this group correct for aberrations and some distortion. The second lens group 512 and the free form mirror 120 create the wide angle field of view (WFOV). The free form mirror 120 is correcting for the distortion associated with WFOV systems. In one application, the projection surface is the side of a car. Keystone or other distortion in the final image may originate from the shape of the car.

It can be corrected with a pre-distorted image. That is, a controller coupled to the spatial light modulator predistorts the image displayed by the spatial light modulator. There is a large depth of field due to the large image space F/#. Therefore, the system may project images onto a wide range of surface contours.

[0027] Figures 6A and 6B show the irradiance profile striking the final projection surface of Figure 1. Figure 6A is a two-dimensional plot across the projection surface, where the color indicates the irradiance. Figure 6B shows one-dimensional traces A-A and B-B through the two-dimensional profile of Figure 6A. With the exception of anomalous RI at the two opposing comers of the image, the overall RI is held substantially flat using this optical design.

[0028] Figure 7 plots the MTF for this system (i.e., the final output plane MTF versus spatial frequency). The solid lines are tangential, and the dotted lines are sagittal. The Nyquist frequency of the DMD spatial light modulator (mapped on the output plane’s projection surface) is 0.6 cycles per millimeter when the DMD’s pixel pitch is 5.4 microns (0.833 mm pixel pitch when projected onto the output surface). The DMD has full HD resolution (1920 pixels by 1080 pixels) and the output projection plane is 1.6 meters long in the x-direction.

[0029] The projection system described above may be used in many applications. Short projection distance situations where the projection system cannot be in the projection area could use this design architecture. The system may be modified to cover a range of projection areas and display sizes. In the example design described above, the image source (DMD spatial light modulator) is offset in both x and y. In a typical short throw projector, the image source is offset along the short axis (y axis) of the source. This design is also offset along the long axis (x axis) of the source so the light can be projected both down and along the side of the vehicle.

[0030] Although the detailed description contains many specifics, these should not be construed as limiting the scope of the invention but merely as illustrating different examples and aspects of the invention. It should be appreciated that the scope of the invention includes other embodiments not discussed in detail above. Various other modifications, changes and variations which will be apparent to those skilled in the art may be made in the arrangement, operation and details of the method and apparatus of the present invention disclosed herein without departing from the spirit and scope of the invention as defined in the appended claims. Therefore, the scope of the invention should be determined by the appended claims and their legal equivalents.