Patent Application
20190310133
The present invention relates to the field of semiconductor equipment and, in particular, to a device and method for measuring amplitude of a scanning mirror.
A projection photolithography tool is a piece of equipment that projects an image of a mask pattern onto a wafer by means of an objective lens. The projection photolithography tool must be provided with a control system for automatic focusing, which is capable of accurately placing a wafer surface to a specified position for exposure. Such a system can be accomplished in several ways. For example, a scanning mirror and a detection slit may be arranged in a detection optical path. When the scanning mirror vibrates at a fast frequency in a simple harmonic fashion, a projected light spot will reciprocate around the detection slit at a corresponding high speed. Periodically shaded by the slit, a photodetector will eventually detect a signal of a dynamic nature. The dynamic signal can be analyzed to derive a position for the light spot where a high signal-to-noise ratio (SNR) can be obtained. Based on this position, a level of the wafer surface can be determined and service as a basis for a wafer support mechanism to tune the wafer surface until it is located at an optimal focal plane. Reference can be made to Chinese Patent Application Publication No. CN100535763C for more details in this regard.
An existing scanning mirror-based photoelectric vertical measurement system typically consists of a projection branch with a projection slit and a detection branch with a detection slit. The projection and detection slit are of equal size, and a vertical level of an object being measured can be derived from a characteristic of a signal modulated by the scanning mirror.
As a signal modulator in the photoelectric vertical measurement system, the scanning mirror is considered as a critical component for the whole photoelectric vertical measurement system. However, as its performance can only be assessed in combination with the performance of other system components, whether it is functionally satisfactory will be known as late as in the system testing phase, and if is problematic, waste of labor, resources and time will be incurred. Up to now, there has not been any established measuring device capable of independently and accurately assessing the performance of a scanning mirror.
It is an objective of the present invention to provide a device and method for measuring amplitude of a scanning mirror, which can easily characterize the scanning mirror and determine whether it can perform in a desired way before it is put into use.
To this end, the present invention provides a device for measuring amplitude of a scanning mirror, including:
a light source for outputting an optical signal;
a diaphragm for modifying a size and a shape of a light spot of the optical signal output by the light source;
a scanning mirror retainer for placing a scanning mirror to be measured, the scanning mirror, after being retained, being able to periodically reflect the optical signal;
a photoelectric sensor disposed lateral to the scanning mirror, the photoelectric sensor including three or more sensing elements and configured to detect and collect the optical signal reflected by the scanning mirror; and
a signal acquisition and processing unit for processing a signal collected by the photoelectric sensor to derive an amplitude of the scanning mirror.
Optionally, the optical signal output by the light source may be an optical signal with a spatial Gaussian distribution.
Optionally, a number of the sensing elements may be odd.
Optionally, the sensing elements may be densely disposed.
Optionally, the light spot may be round and have a diameter of equal to an effective area of the sensing element.
Optionally, the device may further include a position adjusting unit for adjusting a horizontal position of the photoelectric sensor, allowing the photoelectric sensor to locate at a first horizontal position or a second horizontal position.
Optionally, a distance from the first horizontal position to the second horizontal position ranges from 0.2 m to 1 m.
Optionally, the distance from the first horizontal position to the second horizontal position is 0.5 m.
The present invention also provides a method for measuring amplitude of a scanning mirror using the device for measuring amplitude of a scanning mirror as defined above, including:
recording vertical positions of the sensing elements y1, yz, . . . yN;
placing the scanning mirror on a scanning mirror retainer, causing the scanning mirror to vibrate at a frequency of so as to project a light spot onto a photoelectric sensor;
collecting, by a signal acquisition and processing unit, light intensities Iji detected by the sensing elements at time instants tji:
sensing element 1: (t11, I11), (t12, I12), . . . , (t1i, I1i) . . . ,
sensing element 2: (t21, I21), (t22, 122), . . . , (t2i, I2i) . . . ,
sensing element j: (tj1, Ij1), (tj2, Ij2), . . . , (tji, Iji) . . . ,
sensing element N: (tN1, IN1), (tN2, IN2) , . . . , (tNi, INi);
fitting the collected light intensities Ij1 to determine, for each of the sensing elements, time instants Tjk when maximum light intensities are recorded:
sensing element 1: T11, T12, . . . , T1k, . . . , where T11<T12< . . . <T1k< . . . ,
sensing element 2: T21, T22, . . . , T2k, . . . , where T21<T22< . . . <T2k< . . . ,
sensing element j: Tj1, Tj2, . . . , Tjk, . . . , where Tj1<Tj2< . . . <Tjk< . . . ,
sensing element N: TTN1, TN2, . . . . TNk, . . ., where TN1<TN2< . . .<TNk< . . . ;
calculating, for each of the sensing elements, two successive time instant differences Tj(k+1)−Tjk and Tjk−Tj(k−1); identifying the Tj(k+1)−Tjk for the sensing element having the two successive time instant differences both being greater than 1/(2f), and obtaining a vibration frequency fc of the light spot as 1/(Tj(k+1)−Tjk); and
for the sensing elements with the two successive time instant differences not both being greater than 1/(2f), obtaining the amplitude of the scanning mirror based on the vibration frequency fc of the light spot and vertical positions and time instants corresponding to maximum light intensities of said sensing elements with the two successive time instant differences not both being greater than 1/(2f), according to a vibration function, wherein N, i, j and k are positive integers, N≥3, and 1≤j≤N.
Optionally, the method may further include: arranging the photoelectric sensor at a first horizontal position to conduct measuring so as to obtain, by fitting, a first amplitude A1 of the scanning mirror at the first horizontal position; arranging the photoelectric sensor at a second horizontal position to conduct measuring so as to obtain, by fitting, a second amplitude A2 of the scanning mirror at the second horizontal position, where a distance from the second horizontal position to the first horizontal position is ΔL; and obtaining a maximum swing angle θm of a light beam reflected by the scanning mirror based on the first amplitude A1, the second amplitude A2 and the distance ΔL.
The device and method of the present invention entail a brand new solution in the art, which can easily characterize a scanning mirror and determine whether it can perform in a desired way before it is put into use.
The present invention will be described below in greater detail with reference to the accompanying schematics, which present preferred embodiments of the invention. It is to be appreciated that those skilled in the art can make changes to the invention disclosed herein while still obtaining the beneficial results thereof. Therefore, the following description shall be construed as being intended to be widely known by those skilled in the art rather than as limiting the invention.
For simplicity and clarity of illustration, not all features of the disclosed specific embodiment are described. Additionally, description and details of well-known functions and structures are omitted to avoid unnecessarily obscuring the invention. The development of any specific embodiment of the present invention includes specific decisions made to achieve the developer's specific goals, such as compliance with system-related and business-related constraints, which will vary from one implementation to another. Moreover, such a development effort might be complex and time consuming but would nevertheless be a routine undertaking for those of ordinary skill in the art.
The present invention will be further described in the following paragraphs by way of examples with reference to the accompanying drawings. Features and advantages of the invention will be more apparent from the following detailed description, and from the appended claims. Note that the accompanying drawings are provided in a very simplified form not necessarily presented to scale, with the only intention of facilitating convenience and clarity in explaining the embodiments.
Preferred embodiments of the present invention will be enumerated below in order for the invention to be better understood. It is to be noted that the invention is not limited to the embodiments disclosed below but intended to embrace all modifications made by those of ordinary skill in the art based on common general knowledge within its spirit and scope.
Reference is now made to
a light source 20, for outputting an optical signal;
a diaphragm 21 for modifying the size and shape of a light spot resulting from the optical signal output by the light source 20;
a scanning mirror retainer for holding the scanning mirror 22 to be measured while allowing the scanning mirror 22, after being held, to periodically vibrate and to periodically reflect the optical signal;
a photoelectric sensor 23 including three or more sensing elements and configured to detect and collect the optical signal reflected from the scanning mirror 22, the photoelectric sensor 23 optional disposed either at a first position 231 or a second position 232 (see
a signal acquisition and processing unit 24 for deriving the amplitude of the scanning mirror by processing readings of the photoelectric sensor 23.
As also shown in
Specifically, in this embodiment, the optical signal output from the light source 20 is light with a spatial Gaussian distribution. The diaphragm 21 can ensure that the light spot on the photoelectric sensor 23 is sized equal to an effective area of each of the sensing elements in the photoelectric sensor 23 so as to be matched with the photoelectric sensor 23 to permit high measurement accuracy.
As can be seen from
In order for the amplitude of the scanning mirror 22 to be measurable, the light from the light source 20 is required to be fully incident on the reflecting surface of the scanning mirror 22. Hereinafter, the direction of an optical axis of the reflected light beam when it is at the initial orientation is defined as a horizontal direction, and a direction perpendicular to the horizontal direction is defined as a vertical direction. In this embodiment, the light exits the light source 20 in the vertical direction, and the photoelectric sensor 23 is oriented also in the vertical direction.
In
With additional reference to
A method for measuring amplitude of a scanning mirror using the device as defined above will be described below with reference to
In step S11, vertical positions y1, y2, . . . , yN of the sensing elements are recorded. Specifically, vertical positions of their centers may be recorded relative to a single reference point. Of course, this is just for easier implementation, and those skilled in the art can also record vertical positions of some edge points of the sensing elements, if appropriate, to represent the vertical directions of the whole sensing elements.
In step S12, the scanning mirror 22 is placed on the scanning mirror retainer and caused to vibrate at a fixed frequency f to project the light beam onto the photoelectric sensor 23.
In step S13, the signal acquisition and processing unit 24 collects light intensities Iji detected by the sensing elements at various time instants tji:
Sensing element 1: (t11, (t12, I12) . . . , (t1i, I1i) . . . ,
Sensing element 2: (t21, I21), (t22, I22), . . . , (t2i, I2i) . . . ,
Sensing element j: (tuj1, Ij1), (tj2, Ij2), . . . , (tji, Iji) . . . ,
Sensing element N: (tN1, IN1), (tN2, IN2), . . . , (tNi, IN1) . . . , where j represents the j-th sensing element, i denotes the i-th time instant, and 1≤j≤N.
In step S14, the light intensities detected by the sensing elements at the various time instants tji and collected by the signal acquisition and processing unit 24 are fitted to find, for each of the sensing elements, the time instants Tjk when the maximum light intensities are recorded:
Sensing element 1: T11, T12, . . . , T1k, . . . , where T11<T12< . . . <T1k< . . . ,
Sensing element 2: T21, T22, . . . T2k, . . . , where T21<T22< . . . <T2k< . . . ,
Sensing element j: Tj1, Tj2, . . . , Tjk, . . . , where Tj1<Tj2< . . . <Tjk< . . . ,
Sensing element N: TN1, TN2, . . . TNk, . . . , where TN1<TN2< . . . <TNk< . . . .
In step S15, for each of the sensing elements, two successive time instant differences Tj(k+1)−Tjk and Tjk−Tj(k−1) are calculated and serve as basis for identifying edge sensing elements and non-edge sensing elements. Specifically, Tj(k+1)−Tjk and Tjk−Tj(k−1) for each edge sensing element are both greater than 1/(2f), and Tj(k+1)−Tjk and Tjk−Tj(k−1) for each non-edge sensing element are not both greater than 1/(2f). The edge sensing elements are involved in calculating a vibration frequency fc of the light spot but not in calculating the amplitude A of the scanning mirror. The non-edge sensing elements are involved in calculating the amplitude A of the scanning mirror but not in calculating the vibration frequency fc.
Here, the edge sensing elements refer to the two outermost sensing elements in the photoelectric sensor 23, while the non-edge sensing elements refer to all the other sensing elements than the two outermost sensing elements in the photoelectric sensor 23. Theoretically, as the edge sensing elements are disposed at opposing edges of the photoelectric sensor 23, the light intensities they receive peak once in each scanning cycle. Therefore, the time instant difference between two successively maximum light intensities is substantially equal to 1/f, and two successive such time instant differences are both greater than 1/2f. Each of the non-edge sensing elements experiences two light intensity peaks in each scanning cycle, so their two successive such time instant differences are not both greater than 1/2f. Here, reference can be made to
In step S161, based on the calculation performed in step S15, the vibration frequency fc of the light spot is obtained as the reciprocal of (Tj(k+1)−Tjk) of the edge sensing elements, i.e., 1/Tj(k+1)−Tjk.
In step S162, based on the calculation performed in step S15, vertical positions ym and time instants Tmk corresponding to maximum light intensities are obtained for each of the non-edge sensing elements:
Non-edge sensing element m (m1, ym), (Tm2, ym), (Tmk, ym), where 1≤m<N−1.
In step S17, the amplitude A of the scanning mirror is calculated based on the vibration frequency fc of the light spot and the vertical positions ym and time instants Tmk corresponding to maximum light intensities of the non-edge sensing elements according to the vibration function ym=A*sin(2πfctm+ϕ) , where ym represents the positions of the light spot; tm, the time instants; and φ, an initial phase.
In the above steps, it is to be understood that N, i, j, k, and m are all positive integers, and N≥3.
If desirable, the maximum swing angle θm of the light beam reflected by the scanning mirror 22 may also be determined.
Specifically, the photoelectric sensor 23 may be disposed at the first position 231, and amplitude A1 of the scanning mirror 22 at the first position may be obtained by performing the above steps S11-S17. The photoelectric sensor 23 may then be displaced horizontally by ΔL so that it is located at the second position 232, and amplitude A2 of the scanning mirror 22 at the second position may be obtained in a similar way.
The amplitudes A1, A2 and ΔL may be substituted into A≠2θmL to result in the following equations, where L represents the horizontal distance from the photoelectric sensor 23 to the scanning mirror, and A represents the amplitudes of the scanning mirror 22 at the above positions:
These equations may be solved to obtain the maximum swing angle θm of the light beam reflected by the scanning mirror as well as the horizontal distance L1 between the photoelectric sensor and the scanning mirror when the photoelectric sensor 23 is at the first position 231 and the horizontal distance L2 between the photoelectric sensor and the scanning mirror when the photoelectric sensor 23 is at the second position 232.
The device and method of the present invention entail a brand new solution in the art, which can easily characterize a scanning mirror and determine whether it can perform in a desired way before it is put into use.
It is apparent that those skilled in the art can make various modifications and variations to the present invention without departing from the spirit and scope thereof. Accordingly, the invention is intended to embrace all such modifications and variations if they fall within the scope of the appended claims and equivalents thereof.
| Number | Date | Country | Kind |
|---|---|---|---|
| 201610614644.9 | Jul 2016 | CN | national |
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/CN2017/094614 | 7/27/2017 | WO | 00 |
