Abstract:
Provided is a reference mirror converter of a Linnik interferometer in which a first object lens  30  focuses light emitted from a beam splitter  20  on a reference mirror  40 , a plurality of reference mirrors  40  reflects light incident from the first object lens  30 , a plurality of reference mirrors  40  is disposed on a plurality of reference mirror brackets  45 , respectively, the plurality of reference mirror brackets  45  is disposed on a rotary plate  60  at the same angles, and the rotary plate  60  is rotated using a motor  70  to control a rotation of the rotary plate  60  to select the reference mirror  40  having a reflectivity similar to that of a target  200  to be measured from among the plurality of reference mirrors  40 . Accordingly, since a separate state between articles is maintained at all times, adhesiveness between articles packaged with an easily adhesive material may be prevented.

Description:
TECHNICAL FIELD 
     Example embodiments relate to a reference mirror converter of a Linnik interferometer, and more particularly, to a reference mirror converter of a Linnik interferometer that enables a two-dimensional (2D) measurement by shielding light reflected from a reference mirror and thereby preventing an occurrence of interference using a Linnik-typed interference lens stereoscope, and may enhance the visibility and intensity of a three-dimensional (3D) image by selecting a reference mirror having a reflectivity similar to that of a target to be measured from among a plurality of reference mirrors. 
     RELATED ART 
     An interference microscope refers to a microscope using an interference phenomenon of light. If light emitted from the same point is split into two at a time and put together again, a phase difference between two wavy surfaces is constant. Thus, a degree of illumination of an observing place shows the uniform distribution in terms of a place. 
     As a microscope capable of observing an unevenness             of a subject or a difference in an optical thickness of the subject using such interference of light based on a difference in contrast or color, a refractive differentiation interference microscope has been distributed for the purposes of a biological microscope.
     Types of an interference lens may include a Michelson type, a Mirau type, and a Linnik type. Here, the Michelson type is provided in a structure in which Work Distance (W.D) of five times or less is secured compared to that of a low magnification interference lens. The Mirau type is provided in a structure in which the W.D of ten times or more is secured. The Linnik type may cause interference in all of magnifications. 
     Measurement principles thereof will be described with reference to  FIG. 1 .  FIG. 1  illustrates a light source  1 , a translucent glass  2 , a reference mirror  3 , an object lens  4 , and a target  5  to be measured. The measurement principles have been conceived into consideration of a phenomenon that, since a portion in which a difference between lengths of two optical paths of light corresponds to even folds of λ/2 (λ: wavelength of light) appears bright and a portion in which the difference corresponds to odd folds of λ/2 appears dark due to interference between light reflected from the surface of the target  5  and light reflected from the reference mirror  3 , a contour pattern  6  of λ/2 pitch appears on the target surface. Here, the difference between the lengths of optical paths has an effect at a point at which the difference reaches twice of unevenness amounts of the target surface. 
     While the interference microscope is advantageous in observing the overall shape of a target to be measured at a high location generally or intuitively, the interference microscope is disadvantageous in quantitatively verifying the shape of the target. In this regard, the interference microscope was not readily applied to a shape measurement. 
     However, as illustrated in  FIG. 1 , due to an interference pattern that is generated as a phenomenon that two waves encounter and perform reinforcing and extinctive interference, an interference lens cannot easily two-dimensionally measure a diameter of a circle. That is, the interference lens may not readily perform binarization processing. 
     When the interference pattern is removed, a two-dimensional (2D) measurement may be performed. Thus, as for currently commercialized technology, a principle of performing a three-dimensional (3D) measurement includes an AFM method, an optical interference (interferometry) method, a laser confocal method, an optical triangulation method, and the like. 
     Initially, the AFM method has a relatively excellent height resolving power, however, cannot measure a relatively large scale and a relatively high step. Further, the optical triangulation method is advantageous in measuring a relatively large scale and a relatively high step, however, has a relatively poor height resolving power and thus, cannot measure a nano unit. 
     Currently, the laser confocal method using an object lens may perform a 2D measurement and a 3D measurement. However, the laser confocal method has a varying height resolving power based on a depth of focus of the object lens and has a degraded height resolving power compared to the principle of optical interference. 
     To outperform the issues found in the interference microscope that is advantageous in observing the overall shape of a target to be measured at a high location generally or intuitively, however, is disadvantageous in quantitatively verifying the shape of the target, the art titled “ shape measuring method and system of  3 D curved surface ” using interference of light to quantitatively and quickly perform a measurement is disclosed in Korean Patent Publication No. 10-1992-0010550. 
     However, even in this art, still remains the issue that the interference microscope cannot perform a 2D measurement due to an interference phenomenon. 
     DETAILED DESCRIPTION 
     Objects 
     The present disclosure is conceived to outperform the aforementioned issues and an aspect provides a reference mirror converter of a Linnik interferometer that may perform a two-dimensional (2D) measurement by shielding light reflected from a reference mirror and thereby removing an interference pattern. 
     Another aspect provides a reference mirror converter of a Linnik interferometer that may enhance the visibility and intensity of an image by selecting a reference mirror having a reflectivity similar to that of a target to be measured. 
     Solutions 
     To achieve the aforementioned objects, a reference mirror converter of a Linnik interferometer according to example embodiments includes a second object lens configured to enable a camera to take a picture of an image magnified from a target to be measured; a beam splitter configured to transmit or reflect a portion of light irradiated from a light source or a portion of light emitted from the second object lens to be directed toward the camera, and to direct the remaining light toward a reference mirror; a first object lens configured to focus light emitted from the beam splitter on the reference mirror; a plurality of reference mirrors configured to reflect light incident from the first object lens; a plurality of reference mirror brackets configured to support the plurality of reference mirrors, respectively; a rotary plate on which the plurality of reference mirror brackets is disposed at the same angles; a motor configured to generate a rotational force for rotating the rotary plate; an initial rotation angle sensor configured to sense an initial rotation angle of the rotary plate; and a control device configured to rotate the rotary plate by controlling a driving of the motor in response to a command of a user, to sense an initial rotation angle using the initial rotation angle sensor, and to control a rotation of the rotary plate to select a desired reference mirror from among the plurality of reference mirrors. 
     A plurality of bracket holes may be formed on the rotary plate to dispose the plurality of reference mirror brackets, respectively, and a portion on which the bracket hole is absent may serve as a shielding plate configured to shield the light incident from the first object lens instead of reflecting the light, thereby enabling a two-dimensional (2D) measurement. 
     A focus adjust groove may be formed on a front surface of the reference mirror bracket to traverse a center of the reference mirror bracket, and the reference mirror bracket may move forward or backward to adjust an optical path of the first object lens and an optical path of the second object lens to match by inserting a rotating device into the focus adjust groove and thereby rotating the reference mirror bracket clockwise (in a right-handed screw direction) or counterclockwise. 
     A plurality of tilting adjust screws may be disposed at preset angles along the circumference of each of the plurality of reference mirror brackets to adjust an optical path of the first object lens and an optical path of the second object lens to match with respect to the light incident from the first object lens, and thereby adjust a central optical axis of the first object lens and a reference mirror plane to constitute a normal. 
     A reference mirror bracket fastening device may be disposed at a location corresponding to each of the plurality of reference mirror brackets on the side of the rotary plate to fasten the reference mirror bracket in a tilting-adjusted state and in a state in which the optical path of the first object lens and the optical path of the second object lens are adjusted to match. 
     The reference mirror bracket fastening device may fasten a bracket set screw by forming a set screw hole along the side of the rotary plate and by disposing a fastening member made using synthetic resin. 
     Effect 
     According to example embodiments, it is possible to enable a two-dimensional (2D) measurement by disposing a plurality of reference mirrors on a rotary plate, by configuring a reference mirror-free portion, and by preventing interference from occurring when the reference mirror-free portion comes into a focus of an object lens. Further, it is possible to enhance the visibility and intensity of a three-dimensional (3D) image by selecting a reference mirror having a reflectivity similar to that of a target to be measured from the plurality of reference mirrors. 
    
    
     
       BRIEF DESCRIPTION OF DRAWINGS 
         FIG. 1  illustrates a principle of an interference microscope according to the related art; 
         FIG. 2  is a perspective view and  FIG. 3  is a cross-sectional view illustrating a configuration of a reference mirror converter of a Linnik interferometer according to example embodiments; 
         FIG. 4  is a side view observed at the side of the reference mirror converter to view a rotary plate from the front according to example embodiments; 
         FIG. 5 , parts (a) and (b), are perspective views illustrating a front and a rear of the rotary plate according to example embodiments; 
         FIG. 6  is a front view of the rotary plate according to example embodiments; and 
         FIG. 7  is a cross-sectional view cut along line A-A of  FIG. 6 . 
     
    
    
     BEST MODE 
     Hereinafter, example embodiments will be described with reference to the accompanying drawings. 
       FIG. 2  is a perspective view and  FIG. 3  is a cross-sectional view illustrating a configuration of a reference mirror converter of a Linnik interferometer according to example embodiments. 
     A reference mirror converter  100  according to example embodiments includes a second object lens  10  configured to focus an image magnified from a target  200  to be measured on a zoom lens  110  and a focusing lens  120 , to magnify again the focused image at the zoom lens  110  and the focusing lens  120 , and to enable a camera  130  to take a picture of the image; a beam splitter  20  configured to reflect a portion of light irradiated from a light source  25  or a portion of light emitted from the second object lens  10  to be directed toward the camera  130  through the zoom lens  110  and the focusing lens  120  and to direct the remaining light toward a reference mirror  40 ; a first object lens  30  configured to focus light emitted from the beam splitter  20  on the reference mirror  40 ; a plurality of reference mirrors  40  configured to reflect light incident from the first object lens  30 ; a plurality of reference mirror brackets  50  configured to support the plurality of reference mirrors  40 , respectively; a rotary plate  60  on which the plurality of reference mirror brackets  45  is disposed at the same angles; a motor  70  configured to generate a rotational force for rotating the rotary plate  60 ; an initial rotation angle sensor  80  configured to sense an initial rotation angle of the rotary plate  60 ; and a control device configured to rotate the rotary plate  60  by controlling a driving of the motor  70  in response to a command for selecting the specific reference mirror  40  input from a user, to sensing an initial rotation angle using the initial rotation angle sensor  80 , and to control a rotation of the rotary plate  60  to select the desired reference mirror  40  from among the plurality of reference mirrors  40 . 
     Reference numerals not described herein, “ 75 ” denotes a coupling configured to transfer the rotational force of the motor  70  to the rotary plate  60 , “ 65 ” denotes a bearing configured to decrease a friction on a rotating shaft of the rotary plate  60 , “ 85 ” denotes a rotary plate support configured to support the rotary plate  60 , and “ 76 ” denotes a motor bracket configured to support the motor  70  against the rotary plate support  85 . 
     The reference mirror converter  100  of the Linnik interferometer according to example embodiments enables a three-dimensional (3D) measurement of the target  200  by causing interference between light reflected from the target  200  and light reflected from the reference mirror  40  and thereby generating an interference pattern on the magnified image of the target  200 . 
     When a reflectivity of the target  200  and a reflectivity of the reference mirror  40  differ from each other, the visibility and intensity of the image may be decreased. Accordingly, the interferometer enables a first reference mirror  40   a  having a reflectivity similar to that of the target  200  to be selected from among the plurality of reference mirrors  40  by rotating the rotary plate  60  on which the plurality of reference mirror brackets  45  is disposed with the motor  70 . 
     In response to the command for selecting the specific reference mirror  40 , for example, the first reference mirror  40   a , input from the user into the control device, the control device applies the rotational force generated from the motor  70  to the rotary plate  60  through the coupling  75 , for example, a flexible coupling and the like, and rotates the rotary plate  60  with the applied rotational force by controlling the motor  70 , senses the initial rotation angle using the initial rotation angle sensor  80  in response to the rotation of the rotary plate  60 , and controls a rotation of the rotary plate  60  to select the desired reference mirror  40 , for example, the first reference mirror  40   a , having the reflectivity similar to that of the target  200  from among the plurality of reference mirrors  40 . Here, a description related to the control device will be omitted. 
       FIG. 4  is a side view observed at the side of the reference mirror converter to view a rotary plate from the front according to example embodiments, and  FIG. 5 , parts (a) and (b), are perspective views illustrating a front and a rear of the rotary plate according to example embodiments.  FIG. 6 a    is a front view of the rotary plate according to example embodiments, and  FIG. 6 b    is a cross-sectional view cut along line A-A of  FIG. 6 . 
     The rotary plate  60  according to example embodiments is provided in a form of a circular plate, five bracket holes  61  are formed at the angle of 60° on the rotary plate  60  to dispose five reference mirror brackets  50   a ,  50   b ,  50   c ,  50   d , and  50   e , respectively, and a portion on which the bracket hole  61  is absent serves as a shielding plate configured to shield the light incident from the first object lens  30  instead of reflecting the light, thereby enabling a two-dimensional (2D) measurement. Here, the shielding plate refers to a rotary plate itself on which the reference mirror bracket  50  is not disposed. 
     As illustrated in part (b) of  FIG. 5 , the reference mirror  40  is attached on the other surface of each of the five reference mirror brackets  50   a ,  50   b ,  50   c ,  50   d , and  50   e . In detail, five reference mirrors  40   a ,  40   b ,  40   c ,  40   d , and  40   e , each having a different reflectivity, are attached on the other surface of the five reference mirror brackets  50   a ,  50   b ,  50   c ,  50   d , and  50   e , respectively. 
     Here, when referring to five first through fifth reference mirror brackets  50   a ,  50   b ,  50   c ,  50   d , and  50   e  individually, an alphabet small letter such as “a” and the like is added to “ 50 ”, such as indicating a first reference mirror bracket with “ 50   a ”, for example. However, when representatively indicating the same, the representative reference numeral “ 50 ” is used. The same principle is applied to other constituent elements such as the reference mirror  40  and the like. 
     Although five reference mirrors  40  are attached to five reference mirror brackets  50 , respectively, in the present example embodiments, it is only an example. If necessary, six, eight, or more reference mirror brackets  50  may be disposed and the number of reference mirrors  40  corresponding thereto may be attached thereto. 
     Also, an optical path adjust groove  52  is formed on the front surface of the reference mirror bracket  50  to traverse a center of the reference mirror bracket  50 . A plurality of, for example, three tilting adjust screws  51   a ,  51   b , and  51   c  are disposed at preset angles, for example, 120° and the like, along the circumference of the reference mirror bracket  50 . 
     When the desired third reference mirror  40   c  is selected to come into, that is, be located at a focus of the first object lens  30  through rotation using the motor  70  in order to select the reference mirror  40  having a reflectivity similar to that of the target  200 , the reference mirror bracket  50  moves forward or backward to adjust an optical path of the first object lens  30  and an optical path of the second object lens  10  to match by inserting a rotating device, for example, a driver and the like, into the optical path adjust groove  52  and thereby rotating the reference mirror bracket  50  clockwise (in a right-handed screw direction) or counterclockwise, while viewing an image being taken at the camera  130 . 
     Although the selected third reference mirror  40  is adjusted to match the optical path of the first object lens  30  and the optical path of the second object lens  10 , interference patterns may not be disposed at constant intervals on the image being taken at the camera  130 . In this case, the selected reference mirror  40  may be tilted toward one side and thus, the selected third reference mirror  40   c  is adjusted to be vertical (normal) with respect to the light incident from the first object lens  30  by adjusting the first through third tilting adjust screws  51   a ,  51   b , and  51   c.    
     For example, when rotating the first tilting adjust screw  51   a  clockwise or counterclockwise with a driver to move forward or backward, a tilting of a portion, for example, a second upper limit when the image taken at the camera  30  is divided into four upper limits, corresponding to the first tilting adjust screw  51   a  is adjusted. Accordingly, three tilting adjust screws  51  may adjust tiltings of three portions of the reference mirror  40 , respectively, so that light reflected from the selected third reference mirror  40   c  may proceed along the same path as a path of incident light. 
     Although tiltings of three portions of the reference mirror  40  are adjusted by disposing three tilting adjust screws  51 , respectively, in the present example embodiments, it is only an example. If necessary, a tilting may be adjusted in three or more portions of the selected reference mirror  40  by disposing three or more tilting adjust screws  51  on the selected reference mirror  40 . 
     When the adjustment is completed, the reference mirror bracket  50  is fastened in a tilting-adjusted state and in a state in which the optical path of the first object lens  30  and the optical path of the second object lens  10  are adjusted to match by forming a set screw hole  63  at a location corresponding to each of the five reference mirror brackets  50   a ,  50   b ,  50   c ,  50   d , and  50   e  along the side of the rotary plate  60  and by disposing a fastening member  64  made using synthetic resin, for example, acetyl and by fastening the bracket set screw  62  into the fastening member  64 . 
     According to example embodiments, a 2D measurement is enabled by forming, on the rotary plate  60 , a portion on which the reference mirror  40  is not disposed, by enabling light incident from the first object lens  30  to become extinct without being reflected, and thereby preventing interference from occurring in the beam splitter  20  and enabling light emitted from the second object lens  10  to proceed upward through the zoom lens  110  and the focusing lens  120  so that a picture of an image may be taken at the camera  130 . 
     Although the Applicant(s) have described various example embodiments, the example embodiments are only an example to achieve the technical spirit of the present disclosure and thus, it would be appreciated by those skilled in the art that changes or modifications may be made to the example embodiments without departing from the principles and spirit of the present disclosure, the scope of which is defined by the claims and their equivalents.