Optical inspection device and method for inspecting an object to be optically inspected
The optical inspection apparatus efficiently measures lens centering and polarization alignment in a single step, reducing space and time requirements by integrating rotation-based brightness analysis.
Patent Information
- Application Number
- JP2024139490
- Authority / Receiving Office
- JP · JP
- Patent Type
- Patents
- Current Assignee / Owner
- Priority Date
- 2023-08-21
- Filing Date
- 2024-08-21
- Publication Date
- 2025-10-14
- Estimated Expiration
- 2044-08-21
AI Technical Summary
Existing optical inspection devices require multiple work steps and significant space for measuring lens centering and polarization axis alignment, leading to increased costs and long measurement times.
An optical inspection apparatus that simultaneously measures decenter and polarization properties using a single structure, incorporating a light source, filter element, rotation unit, detector unit, and evaluation unit to determine these properties from brightness changes during rotation.
Enables compact design and reduced measurement time by simultaneously determining multiple parameters, eliminating the need for separate measurements and additional equipment.
Smart Images

Figure 0007753471000001 
Figure 0007753471000002 
Figure 0007753471000003
Abstract
Description
[Technical Field]
[0001] The approach presented here provides an apparatus for inspecting an optical inspection object and an apparatus for inspecting an optical inspection object according to the main claims.
[0002] Many lenses have polarization-influencing properties, either because they generate optical power (liquid crystal lenses) or because they are coated accordingly (polarizing layers, lambda / quadrature layers, etc.). When fitting such lenses, both the centering of the lens and the alignment of its polarization axis are crucial. However, multiple work steps are often required to measure the centering on the one hand and the polarization axis alignment on the other. However, performing multiple work steps requires additional costs in terms of the design of the test equipment, since the centering and polarization axis alignment must be measured in various work steps. At the same time, such test equipment requires a large amount of space. Therefore, one continuous measurement of centering and polarization is performed using two different measuring heads. Correspondingly, the measurement technology requires a large amount of space, and the two separate, individual measurements result in long measurement times.
[0003] Against this background, it is an object of the present invention to provide an improved inspection device for optical inspection objects and an improved method for inspecting optical inspection objects.
[0004] The above problem is solved by the subject matter of the main claim.
[0005] The approach presented herein provides an optical test object inspection apparatus for determining the decenter and polarization properties of the test object, the inspection apparatus having the following features: a light source for emitting a bundle of light rays along an optical axis; an optical element in the optical axis designed as a filter element for imparting a specific polarization direction to the light of the ray bundle or to the light reflected or transmitted by the object to be examined or for filtering the light; a rotation unit designed to rotate the test object, which is located at least close to the optical axis, by a rotation angle relative to the measurement system and / or the test unit; a detector unit designed to capture light reflected or transmitted by the object under inspection and to produce an at least approximately sharp image of the light source or reticle; an evaluation unit designed to determine a characteristic value for centering from the measured drawn circle and to determine the polarization axis of the test object from the rotation angle and the change in the brightness signal of the light beam of the light bundle reflected by or transmitted through the test object, which change is related to this rotation angle;
[0006] Furthermore, the approach presented herein provides an inspection device for an optical inspection object, which inspection device has the following features: a light source for emitting a bundle of light rays along an optical axis; an optical element for collimating the emitted ray bundle; an optical element designed as a polarization-influencing element for imparting a specific polarization direction to the light of a bundle of rays; an element for holding an optical inspection object; an optical element for recollimating the bundle of rays focused by the object under examination; an optical element for filtering the light transmitted by the object to be examined, the optical element being designed as a polarizing filter; an optical element for refocusing light transmitted by the test object onto the detection surface; a rotation unit designed to rotate the test object located in the optical axis relative to the test device and / or individual components of the test device about the beam axis and / or the optical axis; a detector unit designed to simultaneously determine the polarization axis of the test object and the decentering of the test object from the rotation angle and from the rays of the ray bundle transmitted by the test object; It is equipped with:
[0007] The term "ray source" can be understood, for example, as a ray source or lamp that outputs corresponding light rays as a ray bundle along an optical axis. Alternatively, it can be an illuminated reticle. The term "filter element" can be understood, for example, as an optical element that imparts a corresponding polarization direction to incident light. The term "rotation unit" can be understood, for example, as a mechanical unit that rotates the test object relative to the measurement device. Such rotation can be performed by actively rotating the test object itself when the filter element is stationary, or by rotating the measurement device when the test object is stationary. For example, the rotation unit can be designed to rotate the measurement device or the test object by a certain rotation angle, for example, around the optical axis or the axis of the ray bundle, using an electric drive. The term "detector unit" can be understood, for example, as an optical sensor or projection surface on which light reflected by or transmitted through the test object is imaged and subsequently evaluated by a corresponding evaluation unit with respect to the position of the polarization axis of the test object.
[0008] The approach presented herein is based on the finding that the position of the polarization axis can be very easily evaluated by rotating the test object relative to the filter element. This can be done, for example, by detecting and evaluating changes in brightness during rotation, taking advantage of the fact that, when the test object's polarization axis or the test object's surface is in the same position, the filter element imparts a polarization direction to the light of the ray bundle, thereby maximizing the light intensity that can be received by the detector unit. In this way, an inspection device for optical test objects can be provided using very simple means from a technical standpoint, in which the test object's polarization axis can be detected and, at the same time, a centering measurement, i.e., measurement of the position of the optical center or the test object's optical axis, can be performed using the same measurement structure. The approach proposed herein therefore offers the advantage of simultaneously or simultaneously measuring multiple parameters of the test object using the proposed measurement structure, which makes it possible to dispense with additional measurement structures and thereby save structural space in the inspection device.
[0009] An embodiment of the approach proposed herein is advantageous, in which the detector unit is designed to determine the polarization axis of the test object using the brightness, brightness pattern and / or light intensity pattern of the rays of the ray bundle. Such an embodiment offers the advantage that the brightness and / or brightness or intensity pattern can be detected very simply from a technical point of view, and thus the polarization axis of the test object can be accurately determined.
[0010] Furthermore, an embodiment of the approach proposed herein is advantageous, in which the rotation unit is designed to rotate the test object and / or the sensor unit about a beam axis and / or an optical axis. For example, such a beam axis can be the axis of a light ray in a beam bundle. Such an embodiment offers the advantage of a compact design of the test device.
[0011] According to another embodiment of the approach proposed herein, the filter element can be designed to impart a circular or linear polarization direction to the light and / or the detector unit has an analyzer designed to pass circular or linear polarization light. Such an embodiment offers the advantage that the filter element can easily impart or evaluate a precise polarization direction to the light of the ray bundle, thereby making it very easy to recognize the polarization direction of the examined object from a technical point of view.
[0012] Furthermore, an embodiment of the approach proposed herein is particularly advantageous, in which the polarizer and the analyzer are arranged relative to one another in such a way that a predetermined azimuthal angle is set between the polarization direction defined by the polarizer and the polarization direction of the light passing through the analyzer defined by the analyzer. By setting a predetermined azimuthal angle, if this angle is known, the accuracy of identifying the polarization axis of the test object can be further improved, and in addition the polarization axis of the birefringent optical element can also be determined.
[0013] Particularly advantageous are embodiments of the approach proposed herein, in which the detector unit is designed to perform a centering measurement of the test object. Such a centering measurement of the test object can include, for example, the measurement of the optical axis, the optical center, or another parameter of the test object. Such an embodiment of the approach proposed herein offers the advantage that several parameters, such as the polarization axis and the centering value of the test object, can be determined using one measurement structure, thereby significantly reducing the required construction space of the inspection device, while the measurements can be performed without laboriously transferring the test object to different instruments or without performing different measurements on one instrument.
[0014] Furthermore, according to one embodiment of the approach presented herein, the detector unit can be designed to measure the diameter and / or radius of the detected drawn circle as a measure for the centration measurement. Such diameter or radius detection makes the centration measurement very simple and fast to perform from a technical point of view.
[0015] Embodiments of the approach proposed herein, in which the detector unit is designed to perform the determination of the polarization axis and the centration measurement in parallel and / or simultaneously, and in which brightness variations are detected in addition to the radius and / or diameter in the circular image, work particularly efficiently, making it possible to provide an inspection device that requires less construction space and is easy to handle during operation.
[0016] According to another embodiment of the approach proposed herein, the radiation source and detector unit can also be integrated into an autocollimator together with a polarizing filter element in the optical axis, and a beam splitter is provided for extracting the light reflected by the inspection object from an optical path parallel to the light emitted by the radiation source. Such an embodiment offers the advantage of a very compact construction of the inspection device.
[0017] According to another embodiment, an additional rotation of the polarizing element in the measurement system can be performed relative to the measurement system. This can be done mechanically or optically. The optical rotation of the polarizing element can be realized, for example, via a liquid crystal or LCD element. In that case, the polarization axis is rotated by applying a voltage.
[0018] This is particularly advantageous in embodiments where the polarization element is rotated by a factor of 1.25. Thus, a 360-degree physical rotation rotates the polarization element by another 90°. A subsequent second rotation increases the polarization element's rotation by an additional 180°, which optically corresponds to the initial configuration. Thus, two intensity values are obtained for each point of the double circle, associated with mutually perpendicular polarization directions, resulting in correspondingly different or inverted intensity profiles. This results in additionally high signal intensities in areas of the circle where otherwise only very low signal intensities exist. This complementary intensity profile allows the "complete" circle to be used to measure eccentricity by adding the images. Alternatively, this advantageous signal reception can be achieved by mechanically moving the measurement system and the polarization element relative to each other and rotating them at different speeds.
[0019] According to another embodiment of the approach proposed herein, a collimator preceded by a polarizer can be used as a filter element, and a telescope with an analyzer can be provided in the optical path between the auxiliary optics and / or the decollimating lens.
[0020] An embodiment of the approach proposed herein is further advantageous as a method for inspecting an optical inspection object, which method is carried out using a variant of the inspection device introduced herein and comprises the following steps: - outputting light of the bundle of rays from the radiation source through a filter element towards the test object, and receiving the light of the bundle of rays emitted and reflected or transmitted by the test object in a detector unit; - performing a relative rotational movement between the test object and the measuring device; - determining the polarization axis of the test object from light reflected or transmitted by the test object; Includes.
[0021] The above-mentioned advantages can also be achieved quickly and efficiently with such an embodiment.
[0022] In another embodiment of the method, the rotational movement of the centration measuring unit is performed at a different rotational speed than the rotational movement of the polarizing element or deflecting elements.
[0023] The approach presented herein further provides a control device designed to execute, control or implement the steps of the method variants presented herein in a corresponding device. This embodiment variant of the invention in the form of a control device also allows for a rapid and efficient solution of the problem underlying the invention.
[0024] For this purpose, the evaluation device can have at least one computing unit for processing signals or data, at least one memory unit for storing signals or data, at least one interface to a sensor or actuator for reading sensor signals from the sensor or outputting control signals to the actuator, and / or at least one communication interface for reading or outputting data embedded in a communication protocol. The computing unit can be, for example, a signal processor, a microcontroller, etc., and the memory unit can be a flash memory or a magnetic storage unit. The communication interface can be configured to read or output data wirelessly and / or via a wired connection, where a communication interface capable of reading or outputting data via a wired connection can read or output the data, for example, electrically or optically, from or to a corresponding data transmission line.
[0025] A control device unit can be understood here as an electrical device that processes sensor signals and outputs control and / or data signals accordingly. The control device can have an interface that can be implemented by hardware and / or software. If implemented by hardware, the interface can be, for example, part of a so-called system ASIC that includes many of the functions of the control device. However, the interface can also be a dedicated integrated circuit or can be at least partially composed of discrete components. If implemented by software, the interface can be, for example, a software module that resides in a microcontroller together with other software modules.
[0026] Also advantageous is a computer program product or computer program which can be stored on a machine-readable carrier or storage medium, such as a semiconductor memory, a hard disk memory or an optical memory, and which comprises a program code used to execute, perform and / or control the steps of the method according to one of the aforementioned embodiments, in particular when the program product or program is run on a computer or device. [Brief explanation of the drawings]
[0027] Advantageous exemplary embodiments of the approach introduced herein are described in detail below with reference to the accompanying figures.
[0028] [Figure 1] 1 shows a schematic diagram of an exemplary embodiment of an inspection apparatus for inspecting an optical inspection object; [Figure 2] 2 shows a schematic view of an image of light reflected by a test object towards a sensor in a corresponding arrangement according to FIG. 1; [Figure 3] 10 shows a schematic diagram of the signal profile of the detected light intensity without and with an additional rotation of the polarizing element. [Figure 4] 1 shows a schematic diagram of an exemplary embodiment of an inspection apparatus for inspecting an optical inspection object in transmission; [Figure 5] 1 shows a flowchart of an exemplary embodiment of a method.
[0029] In the following figures, identical or similar elements are given identical or similar reference numerals, and repeated description of these elements will be omitted for clarity.
[0030] FIG. 1 shows a schematic diagram of an exemplary embodiment of an inspection apparatus 100 for inspecting an optical inspection object 105. In this case, a light beam 115 is deflected by a beam splitter 120 along an optical axis 117 from a light beam source 145 in the form of a bundle of rays, after which the light beam 115 is incident on a filter element 125. The light beam source can be advantageously combined with a crosshair (reticle). In this case, the filter element 125 can be designed as a polarizer or analyzer, which can impart a specific polarization direction to the light beam 115 or transmit light reflected by the inspection object 105 only with a specific polarization direction. Furthermore, a collimating and focusing unit 130 can be provided, for example, arranged on the optical axis 117 and capable of focusing the light 115 onto the optical inspection object 105. In that case, the collimating and focusing unit 130 can be arranged, for example, in two subunits 130a and 130b, respectively, before or after the filter element 125 in the light beam direction. In that case, the optical element 130a is called a collimating lens, and the optical element 130b is called a focusing lens or a front lens. Furthermore, a rotation unit 135 is provided, which is designed, for example, as an electric drive for rotating the test object 105 through a rotation angle 140. In FIG. 1, this rotation is shown as the rotation unit 135 rotating the test object 105 or a holder for the test object 105, which is not shown in FIG. 1. Alternatively or additionally, the rotation unit 135 can also be designed to rotate the entire measurement system 100 through the rotation angle 140. The rotation unit is controlled via a control unit 165.
[0031] The light of the light beam 115 is then reflected by the test object 105, or more precisely by its surface, resulting in a polarization effect in which high-intensity light incident with the same polarization direction as that most strongly reflected by the surface of the test object 105 is reflected. This reflected light then passes through the beam splitter 120 and is received by the sensor 110 of the detector unit 147. The detector unit 147 can be integrated with the sensor 110 or can be part of the control device 150 and connected to the sensor via a suitable wired or wireless interface. In order to obtain an image of the center of curvature of the surface of the optical test object 105 from the reflected light, the sensor 110 can be designed, for example, as a CMOS or CCD camera or as a projection screen towards which a camera is pointed.
[0032] In that case, the control device 150 can be used to operate the device 100. In that case, the output of light by the light source 145 can be controlled by the output unit 155. Then, with the controlled output of light, the reflected light or a corresponding signal obtained at the sensor 110 correspondingly can be read by the reading interface 160. Then, for example, if the rotation of the test object 105 is controlled by a corresponding rotation angle 140, from this, the position of the polarization axis of the test object 105 can be determined using the determination unit 170 from the light reflected by the test object 105 together with the image obtained by the sensor 110.
[0033] At the same time, it is also possible to perform centering measurements using the structure shown in Figure 1, which is possible simply by further evaluating the image of light reflected by the test object 105 detected by the sensor 110.
[0034] FIG. 2 shows a schematic diagram of an image 200 of light reflected by the test object 105 toward the sensor 110. The illustration in FIG. 2 shows light reflected or incident toward the sensor 110, forming a corresponding light pattern 210 or intensity pattern. It can be seen that the reflected light generates an image of an object (a cross in the example) that forms a circle 220 due to the rotation of the test object or autocollimator. From the radius R of the circle, the eccentricity of the test object 105 can be inferred. Depending on the rotational position of the test object relative to the filter element 125 and the polarization-affecting properties of the test object, the (light) signal intensity varies during the rotational movement. If the filter element 125 or the test object 105 is rotated 360° and all camera images are combined, instead of a circle with constant intensity, a sinusoidal intensity distribution that varies with the azimuth angle is obtained. In FIG. 2, this variation is illustrated by an intensity profile. The rotation angle at which the intensity is maximized can be understood as the angle at which the polarization axis of the test object 105 is aligned. Thus, the intensity variation over the rotation angle contains information about the alignment of the polarization axis of the test object 105, whereas the diameter or radius R of the drawn circle 220 is a measure of the centration of the test object 105. Thus, the rotational movement of the test object 105 is utilized to sense both measurands, which are advantageously measured in parallel.
[0035] Figure 3 shows a schematic diagram of the signal profile of the detected light intensity with and without additional rotation of the polarizing element. In this case, normalized intensity is plotted on the ordinate against angle on the abscissa. The solid sinusoidal curve shows the signal profile detected when the test object is rotated at a constant rotation speed relative to the measurement system without additional rotation of the polarizer / analyzer. For reflection measurements, this can be achieved by rotating the ACM or the test object. The dashed or dotted sinusoidal curves are produced when the polarizer / analyzer is rotated mechanically or optically at high speed relative to the measurement system. This results in a first signal (dashed line) and a second, inverted signal (dotted line) being detected for each azimuthal position. Adding the signal profiles results in a fully illuminated circle.
[0036] Therefore, if the dashed and dotted intensity profiles are added together, a "complete" drawn circle can be obtained, as shown in the bottom part of FIG.
[0037] Therefore, advantageously, the centering measurement and the polarization measurement can be associated in one measurement process, thereby keeping the construction space compact and minimizing the measurement time. To achieve this, according to one exemplary embodiment, the centering measurement, in which a rotation of the test object is performed, is associated with the polarization light path. The approach presented herein therefore enables an advantageous association of the centering measurement and the polarization measurement, which allows for a compact measurement construction and short measurement times.
[0038] Depending on the characteristics of the object to be inspected, the filter element 125 or the polarizer and / or analyzer can be designed for circular polarization instead of linear polarization, or an azimuthal angle can be set between the polarizer and the (separate) analyzer.
[0039] Another technical embodiment of the variant of the inspection device introduced herein is e.g. A telescope with a collimator and analyzer preceded by a polarizer in the optical path between the pre-optical system and the "decollimating lens". Centration is measured in transmission.
[0040] FIG. 4 shows a schematic diagram of an exemplary embodiment of an inspection apparatus 100 for inspecting an optical inspection object 105 in transmission, in which simultaneous measurements of the decentering and polarization-changing characteristics of an optical element are performed in transmission. Again, decentering is detected based on the radius or diameter of the drawn circle created by rotating the inspection object relative to the measurement system. To determine the polarization-changing characteristics of the inspection object 105, a collimator 400 is provided with a polarizing element, e.g., a polarizer 125, and a telescope 420 is provided with a polarizing filter element, e.g., an analyzer 410, which includes a prelens 430 and a focusing or "decollimating" lens, not explicitly shown in FIG. 4 . The polarizer 125 in the collimator 400 is illuminated, for example, through an illuminated reticle 435. As shown in FIG. 3 and described above, the polarizing element itself can be optically or mechanically rotated relative to the measurement system, for example, to obtain a complementary signal profile. The polarizer 125 and the analyzer 410 can be rotated independently of each other, or an additional quarter-wave plate can be rotated instead, which is advantageous, for example, when determining the Mueller matrix of the test object. Furthermore, the polarizer 125 and the analyzer 410 can have different optical properties. For example, the polarizer 125 can be designed as a retardation plate or can be combined with or connected to a retardation plate, so that the light beam after the collimator 400 has circular polarization. The light beam is then focused to the test object focal point 440 before the pre-lens 430 or the analyzer 410. Such a variant is advantageous, for example, when the test object 105 changes the polarization of the light beam, for example, from circular to linear, as is the case for pancake optics for AR / VR. Therefore, for such test objects 105, performing measurements in transmission is particularly advantageous.
[0041] 5 shows a flowchart of an exemplary embodiment of a method 500 for inspecting an optical inspection object, the method 500 being performed using an inspection apparatus according to the variant introduced herein and including step 510 of outputting a light beam from a light source through a filter element to the inspection object, and receiving the light beam reflected or transmitted by the inspection object at a detector unit. The method 500 further includes step 520 of rotating the inspection object relative to the filter element and step 530 of determining a polarization axis of the inspection object from the light reflected or transmitted by the inspection object.
Claims
1. An inspection device (100) for an optical inspection object (105), said inspection device (100) having the following features: a light source (145) for emitting a light beam (115) along an optical axis (117); a filter element (125) designed as a polarizer (125) and an analyzer (125) on said optical axis (117), said polarizer (125) giving a specific polarization direction to the light of said bundle of rays (115) and said analyzer (125) filtering the light reflected by said test object (105); a rotation unit (135) designed to rotate the inspection object (105) located on the optical axis (117) relative to the inspection device and / or individual components of the inspection device about the beam axis and / or the optical axis (117); a detector unit (147) designed to simultaneously determine the polarization axis of the test object (105) and the decentering of the test object (105) from the rotation angle (140) and from the imaging of the bundle of rays (115) reflected by the test object (105); An inspection device (100) comprising:
2. 2. The inspection device (100) of claim 1, wherein the polarizer (125) is mechanically and / or optically rotatable in the optical path.
3. 2. The inspection device (100) of claim 1, wherein the detector unit (147) is designed to determine the polarization axis of the object to be inspected (105) using the brightness, brightness pattern and / or light intensity pattern (210) of the reflected light rays of the light bundle (115).
4. 2. The inspection device (100) according to claim 1, characterized in that the detector unit (147) is designed to detect the degree of decentering from the traced circle (220) of the detected brightness variation.
5. 2. The inspection device (100) of claim 1, characterized in that the light source (145) and the sensor (110) are integrated in an autocollimator on the optical axis (117) together with the polarizer (125) and the analyzer (125), and a beam splitter (120) is provided to extract light reflected by the object to be inspected (105) from an optical path parallel to the light irradiated by the light source (145).
6. A method (500) for inspecting an optical inspection object (105), said method (500) being carried out using an inspection device (100) according to claim 1, comprising the following steps: - a step (510) of emitting a bundle of rays (115) of light from a light source (145) towards the test object (105), wherein the bundle of rays is first polarized, and receiving an image of the bundle of rays (115) reflected and filtered by the test object (105) in a detection unit (147); - rotating (520) the test object (105) relative to the test device (100) and / or individual components of the test device; - determining (530) simultaneously the polarization axis of the test object (105) and the decentering of the test object (105) from the imaging of the light reflected by the test object (105); A method comprising:
7. A method (500) as described in claim 6, characterized in that the polarizer (125) is rotated relative to the inspection device, and a first intensity signal and a second intensity signal different from the first intensity signal are detected for each azimuthal position of the object to be inspected over the course of at least two rotations.
8. 8. The method (500) of claim 7, wherein the first intensity signal and the second intensity signal are added to obtain a drawn circle having an intensity variation within an acceptable range for measuring the eccentricity.
9. A control device (150), configured to perform and / or control the steps (510, 520, 530) of the method (500) of claim 6 in corresponding units (155, 160, 170).
10. A computer program configured to perform and / or control the steps (510, 520, 530) of the method (500) according to claim 8.
11. A machine-readable storage medium having the computer program of claim 10 stored thereon.
Citation Information
Patent Citations
Eccentricity amount measuring method
JP2007017431A
Examination Kit for Polarized Lens
US20120300193A1