This Application is related to U.S. patent application Ser. No. 11/176,028, filed Jul. 6, 2005 and further related to U.S. patent application Ser. No. 11/074,490, filed Mar. 7, 2005 and further related to U.S. patent application Ser. No. 11/179,117, filed Jul. 12, 2005 all of which are hereby incorporated by reference in their entirely.
Many projection systems and other imaging devices incorporate high intensity arc-light sources that have small point sources that are called “fireballs.” The fireball is usually located within a concave reflector that has a focal point, such as a parabolic, elliptical, or other curved shaped mirror. The light emanating from the fireball in the focal point is reflected off the surface of reflector. Often times the reflector is made of a glass, metal, or other substrate that requires a special coating to be applied to provide a specular surface for reflection. When the reflector is fabricated, the special coating may be deposited, sprayed, dipped, painted, or otherwise applied to the reflector surface. The quality of the special coating may need to be determined to ensure that the special coating was applied properly. For instance, the amount of reflection at various wavelengths may need to be determined. Further, the consistency of the reflective surface may need to be examined over a substantial portion of the special coating.
Prior inspection techniques used a fiber source at the focal point of the reflector. The fiber source was oriented to allow light escaping it to scan across the surface of the reflector while with difficulty maintaining the fiber's spatial position at the focal point. Another problem with using an optical fiber included not being able to control the angular spread of the emerging light beam which causes the spatial extent (area) of the scanned region on the reflector surface to vary based on the relative tilt of the fiber.
Accordingly, a more flexible and efficient method of testing the reflective coating is needed to lower the cost and increase the quality of reflectors used for arc light sources. Having a better method of testing will ensure rapid alignment and accurate testing of reflector surfaces.
The accompanying drawings illustrate various embodiments of the present apparatus and method and are a part of the specification. The illustrated embodiments are merely exemplary embodiments of apparatuses and methods and do not limit the scope of the disclosure. Throughout the drawings, identical reference numbers designate similar, but not necessarily identical, elements.
To better examine reflective coatings, a mirror is positioned at a focal point of a concave mirror used as a lamp reflector to “fold” light from the focal point to an area or portion on the concave mirror surface. This “fold mirror” is allowed to rotate on at least one axis to allow light reflected from it to scan multiple discrete areas of the concave mirror surface. In some instances, the concave mirror has a lamp opening for a replaceable or fixed bulb. In other embodiments, a test unit, sampled from a production lot, has a hole drilled, bored, milled, or otherwise opened within it to allow external electromagnetic (EM) energy (radiation) to become incident on the fold mirror. The fold mirror is preferably a front surface mirror with an all-band metal reflective coating such as an aluminum or silver deposition. Alternatively, the fold mirror may be formed of dielectric or other coatings as required.
The fold mirror may be attached to an opto-mechanical assembly that holds the fold mirror in an external attachment that is brought to the required position from the wide opening of the concave mirror. The fold mirror rotates or tilts in one or more directions about its center which is located at the focal point of the concave mirror. The fold mirror's rotation can be done in discrete or continuous steps to scan the surface of the concave mirror. Alternatively, the fold mirror can be positioned to a known orientation and the concave mirror can be held in a rotating fixture to allow rotation about its optical axis.
To limit the spatial extent (SE, the area of incident EM on the concave mirror surface) of the EM energy reaching the concave mirror from the fold mirror, the EM energy entering the opening to the fold mirror can be adjusted by an iris or other f-stop mechanism to limit the angular spread (solid angle) of the incoming EM radiation. During scanning of the reflective surface of the concave mirror, the f-stop mechanism can be continuously adjusted with respect to the tilt of the fold mirror to maintain a substantially constant spatial extent across the reflective surface of the concave mirror.
There are several methods of ensuring that the concave reflector and fold mirror are aligned properly in a test setup. One is to create a ‘test’ optical axis between the EM source and a center of the detector. The optical axis of the concave reflector is oriented along the test optical axis using some form of mechanical dimensioning. The fold mirror is then positioned such that its rotational center is placed at or near the focal point of the concave mirror. The fold mirror then is used in conjunction with EM sources and the sensor to maximize the output of the sensor while either adjusting the (x, y, z) position of the fold mirror center location and the transverse (x, y) positioning of the concave reflector using the mechanical dimensioning. The rotational center of the fold mirror is disposed at the focal point of the concave mirror when the sensor signal is maximized.
A full ellipse has two foci that are conjugates. In the partial elliptical reflector shown, a arc-lamp is disposed in the elliptical reflector 10 such that its fireball in operation is positioned at a first focus F116. EM energy 30 that is emitted from the fireball at F1 is reflected off of the optical coating 14 and collected at the conjugate second focus F218.
The reflectors 10, 10′ may be formed in a glass, metal (e.g. aluminum or copper) or other solid substrate (e.g. ceramic or quartz) to form an elliptical body 22 or a parabolic body 24. The reflector bodies 22, 24 may contain an opening 26 to receive a bulb such as a mercury-arc bulb. Alternatively, the reflector body may have only a small hole or be solid and thus a reflector may be sampled (selected from a set produced in the same process lot) and a hole 28 created to allow EM energy 30 from a test apparatus to enter the reflector cavity.
A controller 60 includes a central processing unit (CPU) 62, memory 64 and input/output logic 66 and 68. The controller 60 can be used to implement the methods described below to implement the testing of the optical coating. The method may be embodied at least in part in any computer readable media for use by or in connection with an instruction execution system on CPU 62 or in logic circuits. “Computer readable media” can be any media that can contain, store, or maintain programs and data for by or in connection with the instruction execution system. Computer readable media such as memory 64 can include any one of many physical media such as, electronic, magnetic, optical, electromagnetic, infrared, or semiconductor media. Specific but not exclusive suitable computer readable media include a portable computer diskette, hard drives, compact discs, or DVD discs. Semiconductor memory includes, but is not limited to, DRAM, SRAM, EEPROM, FLASH, one time programmable, read only memory, and the like.
The CPU 62 can control the wide band EM source 12 such as through signal 81. The iris 44 can be controlled by a peripheral interface 84 and likewise the roller mechanism 85 by control bus 84. The CPU can select the angle of the fold mirror 40 by use of a fold mirror link 90. The sensors 50A-50C can be controlled with computer interface I/O links 88-89 to read analog or digital data depending on the sensors used and to control the selection of the desired sensor during the test. The various I/O, peripheral, sensor, and controller interfaces used in embodiments may include but are not limited to LVDS (low voltage differential signaling), Ethernet, SDI (serial digital interface), SDV (serial digital video), various IEEE 1149 test solutions, USB (universal serial bus), Bluetooth, and standard or custom UART interfaces, just to name a few.
The interferogram is generated at sensor 50 because of the recombination of the EM from the fixed mirror 74 and movable mirror 78 at the beam splitter 76. To create the interferogram, the movable mirror 78 is moved at a constant speed while the sensor 50 is sampled at a uniform rate. As the intensity of the EM received at the sensor 50 is detected and recorded, the movable mirror 78 is directed towards or away from the beam splitter 76. The recorded sensor data is the interferogram that is Fourier transformed into the respective frequency data. Because the combined EM from the beam splitter 76 is passed through condenser lens 80 and iris 44 to the reflective surface of reflector 10, the filtering aspects of the reflector surface on reflector 10 can be characterized and compared to an ideal or known representative data set.
To allow the characterization to be implemented over a large portion of the reflective surface of reflector 10, a controller 60 is used in conjunction with the fold mirror 40, iris 44, sensor 50 and FTS 70 to scan the EM beam over a set of first angles A2 (longitude) and a set of second angles A1 (latitude) from the proximal end 46 to the distal end 48 of reflector 10. The controller 60 includes a central processing unit (CPU) 62 which may be a personal computer, microprocessor, digital signal processor, workstation, flow controller, discrete logic, or other programmable controller. The CPU 62 receives computer executable instructions form a computer readable memory 64. The computer readable memory may be any type of memory including magnetic or optical disc storage, dynamic refreshable memory, static memory, flash memory, or other electronic memory storage. The CPU 62 also interfaces to various input/output (I/O) logic to allow it to control the different components of the test system. For example, the CPU 62 may have a computer interface bus 86 to control the operation of the FTS 70. CPU 62 may also be able to control the focus of condenser lens 80 through an optic bus 82 and the iris 44 opening D1 through a peripheral interface 84. If the sensor 50 is part of FTS 70, the CPU may access it from the computer interface bus 86. If the sensor 50 is separate from the FTS 70 or in addition to it, the CPU 62 may access the sensor 50 on a separate sensor link 88. The fold mirror 40 may have at least one angle such as angle A1 or A2 controlled through fold mirror link 90. Fold mirror link 90 may control an additional axis of rotation of fold mirror 40 or it may control also a motor or other mover to rotate the reflector 10 about its optical axis such as with A3 which may be equivalent to A2.
In block 104, one or more beams (wavelength bands) of electromagnetic energy is directed onto the fold mirror and reflected there from to illuminate the desired area on the reflector 10. The one or more beams of electromagnetic energy (EM) can be performed at the same time (such as by using a broadband light source, e.g. white light) or it can perform in a sequential manner (such as by selecting increasingly higher or lower frequencies of electromagnetic energy ranging from the IR to the UV spectrum). If desired, an iris 44 can be used to limit the spatial extent of the EM. If the reflector 10 is designed with an opening to allow for insertion of a light source, the opening can be used to direct the EM beams to the fold mirror 40. If not or required, an opening can be made or widened such as by drilling, boring, or milling as required.
In block 106, the intensity of the one or more beams of EM energy that is received from the area on a sensor or set of sensors is detected. From the detected data, the performance of the reflective coating over a range of frequencies can be determined and compared to a reference data set to ensure that the coating was applied properly in that area. If a single band of EM energy is used, a single detector for that band can be used to record an intensity reading. If a wide-band light source is used, the one or more sensors can be used to detect various bands of frequencies within the wide-band source range. Alternatively, various filters can be placed in front of a wide-band sensor to limit the band of wavelengths detected for a particular reading.
In block 108, the folding mirror 40 or the reflector 10 is adjusted to orient with a different area on the reflector 10. The folding mirror 40 can be adjusted in one or two angles as capable. Alternatively, the reflector 10 can be rotated about its optical axis to perform part of the adjustment. After the adjustment is made to orient the folding mirror 40 to a different area, the steps in blocks 104 to block 108 can be repeated as necessary.
In block 102, the folding mirror 40 is placed at the focal point of the reflector 10 as described for
In block 112, a Fourier transform spectrometer or equivalent is used to create an interferogram for the desired area of the reflector 10. The Fourier transform spectrometer as shown in
At step 108, as in
Although the flow diagrams of
The preceding description has been presented only to illustrate and describe exemplary methods and apparatuses. It is not intended to be exhaustive or to limit the disclosure to any precise form disclosed. Many modifications and variations are possible in light of the above teaching. It is intended that the scope of the disclosure be defined by the following claims.
Number | Name | Date | Kind |
---|---|---|---|
3217170 | Ho | Nov 1965 | A |
3506361 | Erickson | Apr 1970 | A |
4692024 | Bloss | Sep 1987 | A |
4699447 | Howard | Oct 1987 | A |
5056917 | Nowacki et al. | Oct 1991 | A |
5131747 | Cerutti-Maori et al. | Jul 1992 | A |
5227861 | Nishizawa et al. | Jul 1993 | A |
5307210 | MacFarlane et al. | Apr 1994 | A |
5398113 | de Groot | Mar 1995 | A |
5467192 | Manning | Nov 1995 | A |
5706086 | Lafleur | Jan 1998 | A |
5737074 | Haga et al. | Apr 1998 | A |
5929992 | Stenton et al. | Jul 1999 | A |
6687007 | Meigs | Feb 2004 | B1 |
20020012124 | Nakayama et al. | Jan 2002 | A1 |
20040223162 | Wax | Nov 2004 | A1 |
20040257584 | Nishida | Dec 2004 | A1 |
20050083521 | Kamerman | Apr 2005 | A1 |
20060033932 | Sezginer | Feb 2006 | A1 |
20060077395 | Chan et al. | Apr 2006 | A1 |
20060132799 | Dubois et al. | Jun 2006 | A1 |
20060238771 | Drabarek et al. | Oct 2006 | A1 |
20060244973 | Yun et al. | Nov 2006 | A1 |
Number | Date | Country |
---|---|---|
40 04 807 | Sep 1990 | DE |
0 617 092 | Sep 1994 | EP |
Number | Date | Country | |
---|---|---|---|
20070091314 A1 | Apr 2007 | US |