Pulse counter circuit and displacement measuring device

Abstract: Disclosed is a pulse counting circuit for counting pulse signals comprising a first pulse signal generating means for generating a first pulse signal corresponding to an input signal, a counting means for counting at least either of said first pulse signal and a second pulse signal which differ from said first pulse signal corresponding to said input signal, said first pulse signal possessing a pitch set smaller than that of said second pulse signal, and a control means for selectively controlling the operation of said count means for counting said first and second pulse signal.

Description: BACKGROUND OF THE INVENTION Field of the Invention This invention relates to a pulse counter circuit and a displacement measuring device employing this pulse counter circuit. The present invention are ideally usable, for example, on incremental-type rotary encoders or linear encoders. Related Background Art Conventionally, on magnetic or optical incremantal-type rotary encoders or linear encoders, displacement amounts of movable scales, shift directions, and others are detected by using two types of sinusoidal wave signals (2-phase sinusoidal wave signals) having mutually different phases and obtainable from two sensors. On linear encoders, for instance, it is known that signal insertion circuits are adopted to improve the resolution of position detection of linear scales. From the above-mentioned 2-phase sinusoidal wave signals, a plural number of sinusoidal wave signals mutually possessing phase differences are generated and based on these sinusoidal wave signals, a plural number of divided pulse signals are formed. Fig. 1 is a block diagram showing an example signal insertion circuit. The components indicat:ed with the numerals of 1 and 2 in this figure are input terminals. For example, input into these terminals are sinusoidal wave signals with mutually differing phases that are output from two sensors of a linear encoder. For instance, while signal "a" is input into input terminal 1, what is input into input terminal 2 is signal "b" possessing 90-degree phase difference from signal "a". Also, by inputting signal "a" into reverse circuit 3, signal "c" possessing 180-degree phase difference from signal "a" can be obtained. Then, by appropriately conducting weight adding to these three types of sinusoidal signals "a", "b", and "c" with resistance and others, sinusoidal wave signals with optional angles (phase angles) are inserted. In this Fig. 1, the same values for resistance R are used to thereby obtain signals "d" and "e" with phase differences of 45 degrees and 135 degrees, respectively. The signals "a", "d", "b" and "e" are converted to rectangular wave signals (binary signals) "f", "g", "h", and "i" by means of respectively corresponding comparator 4,5,6, and 7. The signals are then output in the form of a pulse train by direction discriminator 8. The pulses forming this pulse train are generally termed up-down pulses. Depending on phase relations between signals "a" and "b" (which is leading), these up-down pulses are divided into up pulse "j" or down pulse "k". In this manner, since original signal "a" (or "b") is subjected to multiple division, resolution for angle detection can be upgraded. Shown in Fig. 2 are the waveform examples of signals "f" through "k" mentioned in connection with Fig. 1. In this case, obtained is pulse signal "j" ("k" during reverse rotation) with 8 division of one cycle of rectangular wave signal "f" (or "h") corresponding to input signal "a" (or "b"). By counting of these up-down pulses (divided pulses) "j" and "k", scale positions are detected. However, when the linear scale shift speed is accelerated, frequencies of sinusoidal wave signals input into input terminals 1 and 2 are increased. It was found that as a result of this frequency rise, there occur the cases where accurate measurement of linear scale displacement becomes not possible while the signal insertion circuit fails to follow up those high-frequecny signals and to correctly generate divided pulses. From EP-A-244 385 a displacement detector is known for an encoder which is provided with a phase locked loop connected to a detection head facing a scale of the encoder, wherein the use of a signal switching circuit allows optimum selection of signals used for generation of a system output signal depending on the speed of the relative movement between the detection head and the scale, thereby assuring generation of the system output signal at high degree of dissolution at any speed of the relative movement. Another pulse counting circuit is known from Patent Abstracts of Japan, vol. 8, No. 121 (P-278), June 7, 1984, Publication No.: JP-A-59 027 221. SUMMARY OF THE INVENTION Prime objective of the subject invention lies in providing an improved pulse counter circuit capable of eliminating the above-mentioned problems. Secondary objective of this invention is to provide a displacement measuring device equipped with the improved pulse counter circuit that can solve above-mentioned problems. Other purposes of the present invention will be clarified in the detailed description of the embodiments according to the present invention. BRIEF DESCRIPTION OF THE DRAWINGS Figs. 1 and 2 are the explanatory diagrams with regard to the prior art. Fig. 3 is a block diagram of signal insertion circuit of a first embodiment according to the present invention. Fig. 4 is a time chart showing waveform for the same embodiment. Fig. 5 is a conceptional diagram of operation of the same embodiment. Fig. 6A is a overall schematic diagram of a displacement measuring device of the same embodiment. Fig. 6B is a schematic diagram of reflection elements used in the same displacement measuring device. Fig. 7 is a block diagram showing a signal insertion circuit of a second embodiment according to the present invention. Figs. 8 and 9 are time charts showing waveform examples for explanation of operation in the same embodiment. DESCRIPTION OF THE PREFERRED EMBODIMENTS Fig. 3 is a block diagram showing a signal insertion circuit used for the first embodiment of this invention. Similarly to Fig. 1, this signal insertion circuit is mounted on a linear encoder. On those components in this Fig. 3 which are identical with those shown in Fig. 1, the same identification symbols are affixed and the explanations of these components are omitted. The reference numeral 9 is a counter which counts up-down pulses "j" and "k" sent from a direction discriminator 8 and outputs count data "m". The numeral 10 is a temporary data retention circuit for a latch circuit and others. This circuit latches count data "m" obtained from counter 9 and outputs the latched value as data "n". Data latching is conducted by a pulse signal "u" described later. The reference numeral 11 is a direction discriminator configured in the same way as the direction discriminator 8. This discriminator generates up-down pulses "p" and "q" which are equivalent to signals "a" and "b" and are corresponding to signals "f" and "h" before splitting. Another counter 12 counts up-down pulses "p" and "q" and outputs count data "r" similarly to the counter 9. The reference numeral 13 is a multiplication circuit or a multiplier and this multiplier outputs data "s". In this case, data "s" represents the value obtained by multiplying count data "r" with value "N" which is equivalent to the ratios between resolutions (frequencies) of up-down pulses "p" and "q" and up-down pulses "j" and "k". In the example shown in Fig. 3, the value of "N" becomes 2 because pulses "p" and "q" are obtained by dividing input signals in four while "j" and "k" are obtained by dividing input signals in eight. The reference numeral 14 is an adder that perform addition of data "n" and data "s" and issues the resultant (n + s) value as data "w". This circuit also inputs data "w" into the reset data input terminal of counter 9. The numeral 15 is a speed detecting circuit. As for the example in Fig. 3, this speed detector detects pulse intervals or frequencies of up-down pulses "p" and "q" and issues detection output "t" corresponding to linear scale speed in the form of logical signals. The numeral 16 is a latch circuit and this circuit latches signal "t" at the rise edge of signal "f" to output as logical signal "u". This signal "u" is used as a latch signal for temporary data retention circuit 10 and also as a reset signal (negative logic) for counter 12. The numeral 17 is a pulse generator for generating pulse signal "v" when logical signal "u" is reversed. This pulse signal "v" is used for loading of preset data of counter 9. All such component circuits mentioned above constitute signal insertion circuit 200. With reference to the signal waveform examples shown in Fig. 4, the operation of the circuits in Fig. 3 will be explained. Fig. 4 shows an example case where a moving object, namely, the linear scale, is first gradually accelerated on its speed and then gradually decelerated. Therefore, it is observable that frequencies of signals "f", "j", and "p" are lowered after once raised. Division means (1-8) cannot follow signal "j" subjected to 8 division at the high-frequency portion resulting in creating unreliable status in the area between (3) and (4) of Fig. 4 (range G). On the other hand, on a speed detection circuit 15, such configurations are adopted as to enable to judge that scale shift is at high speed considerably before signal "j" becomes unable to make follow-up. Output signal "t" as shown in Fig. 4 can be obtained because circuit 15 judges existence of low speed before (1) as well as after (5) (range A) and of high speed between (1) and (5) (range B). Fig. 4 also shows the types of waveforms for pulse signal "v" and signal "u" obtained by latching signal "t" at the rise of signal "f". The reference numeral (2) represents a position where signal "f" rises for the first time after signal "t" hecomes "high" and this is also the point where signal "u" is converted to "high". The numeral (6) is a point where signal "f" rises for the first time after signal "t" becomes "low" and signal "u" is changed to "low". In a range C in Fig, 4, a counter 9 continues counting of pulse "j" in normal manner and keeps outputting the counting results as signal "m". A temporary data retention circuit 10 remains in the state of letting count data "m" as output data "n" because signal "u" is at "low". During this time, on the other hand, a counter 12 is under reset state and output "r" is maintained at zero level, consequently causing data "s" to stay at zero output condition. As a result, the addition result "w" at an adder 14 is equal to the count data "m". In other words, it is evident that counting results of signal "j" (up-down pulse) obtained by division are output as they are. At a point (2) in Fig. 4, concurrently with rise of signal "u" and counting start by counter 12, a temporary data retention circuit 10 is latched. This temporary data retention circuit 10 retains the value of count data "m" available immediately before latching (retention value M) and outputs this value as data "n". Since signal "v" is simultaneously generated at this time, preset data "w = n + s"(value M) is loaded on counter 9. In range D starting from this point, the value of data "n" remains as that of M. Instead, count data "r" as well as count data "s" obtained by N-time multiplication of "r" are changed and output "w" from adder 14 is also changed according to changes of "r" and "s". Therefore, from point (2) in Fig. 4 and thereafter, obtained as output signal "w" are the values obtained by adding the retention value M to the data "s" collected from counting signal "p". At the portion between (3) and (4) in Fig. 4, signal "j" obtained by division becomes unreliable. During this period, however, by counting signal "p" corresponding to signal "f" (namely, signal "a") generated from output "w" is the value with data "s" added to retention value M. In this case, at the time when signal "p" is input, accurate values with high-level resolution are obtainable. At point (5) in Fig. 4, signal "t" becomes "low". However, at this point, the above-mentioned operation is continued and signal "j" is not utilized. When it comes to point (6) in Fig. 4, the output signal "w" available at this point is preset on the counter 9 by pulse signal "v". ("w" becomes accurate value at this point). At the same time, since signal "u" becomes "low", the temporary data retention circuit 10 discontinues the retention and starts output of input signals as such. Also, the counter 12 is reset and data "r" and "s" become zero. Namely, from this point on, counting is resumed by using signal "j" obtained through division from preset correct values. Fig. 5 illustrates the conceptional summary of the above-mentioned circuit operation. Pertaining to this Fig. 5, high-frequency narrow pitch signals corresponding to up-down pulses "j" and "k" after the above-mentioned division are termed high resolution pulses. On the other hand, low-frequency (wide-pitch) signals corresponding to up-down pulses "p" and "q" before the said division are termed low resolution pulses. In this example too, assumed is the case where shift of a moving object is first changed from low speed to high speed and then returned to low speed again. During low-speed shift, low resolution pulses remain reset and count results Jl of high resolution pulses are output. When speed becomes high, counting of high resolution pulses is stopped and count value M during change-over time is held. Simultaneously, counting of low resolution pulses is started and output is made of the value with hold value M added to the value with resolution ratio N multiplied to count value P. When speed drops to the level judged to be low speed, counting of low resolution pulses is reset. At the same time, addition results S (M + P x N immediately before resetting) are preset on the counter of high resolution pulses (counter 12 shown in Fig. 1). From this point on, counting of high resolution pulses is resumed. As explained above, by counting up-down pulses before division during low speed and by counting up-down pulses after division during high speed, the encoders with high-level resolution and high-speed response can be realized. The above explanation relates to the case of shifting the moving object in a predetermined direction. However, same operating principles are applicable to a movement in reverse direction. On the above embodiment, more stable operation is achievable by providing certain delays on signal "u" or "v" and addition of such adjustment will not cause deviation from the present invention. In the said embodiment, explained is the case of 8 division of one cycle of sinusoidal wave signals entered into input terminals 1 and 2. However, by division in higher rates, similar configurations can be satisfied. Rather, it can be said that into the greater numbers the division is made, the more conspicuously the effects of this invention can be realized. It may also be possible to use the signals which divide signals "p" and "q" as signals "j" and "k" and conduct switching between these two types of signals. Further, as signals "p" and "q", but usable signal types are not limited to these examples with 4 division of input signals a, b. In other words, other signals can be equally used as long as those signals possess the resolution (1/4 cycle) multiplied by integers obtainable from signals "f" and "h". As signals "p" and "q", use is also possible of the signals that do not divide input signals "a" and "b" (signals with same cycles with input signals "a" and "b"). Detection means of shift speed of moving objects are not limited to the above-mentioned method. However, it is desirable to adopt the configurations which allow switching with sufficient leeway to counting of signals before division at least against the ranges where divided signals become unreliable. As explained up to this point, the circuit according to the present embodiment comprises a speed detection means for detecting changes of linear scale shift speed by using signals before or after division, and two counting means for counting of signal numbers before division and of signal numbers after division, respectively. When the scale shift speed is judged to be high speed by above-mentioned speed detection method, count results of signal after division are not used and instead, the results before division are employed. By adopting such circuit configurations, signal insertion circuits with high-speed response can be realized. Fig. 6A and 6B are the overall schematic diagrams of a displacement measuring device incorporating the above-mentioned signal insertion circuit. In this embodiment, cited is an example use of optical displacement measuring device for the purpose of wafer stage position measurement on an exposure device for semiconductor manufacturing. On the subsequently explained other embodiments, the signal insertion circuits are provided in the interior of displacement measuring devices. Referring to Fig. 6A and 6B, the reference numeral 100 is a scale reader, 101 a semiconductor laser, 102 a collimator lens, and 30 an optical scale. This optical scale 30 is mounted on wafer stage 300 and is provided with a diffraction grating with grating pitch "d", capable of moving in arrow "x" direction shown in the figure by speed "v". Wafer stage 300 is driven by a driving device 500. The reference numeral 109 is a deflection beam splitter, 151 and 152 are 1/4 wavelength plate and 111 and 112 denote reflection mirrors. Further, 106 is a beam splitter while 171 and 172 are deflector plates with respectively orthogonal axes. These deflector plates 171 and 172 are arranged so that their deflection axes form 45-degree angles with the deflection axes of 1/4 wavelength plates 151 and 152. 181 and 182 are light-receiving elements which perform photoelectric conversion of interferences. The reference numeral 110 is a stick-shaped lens of refractive index distribution type possessing two-end flat surfaces for forming the light entering from one end surface into images on the other end surface. On one end of this lens, a reflection film 121 is coated. The lens 110 and reflection film 121 constitute a reflection element 120. As will be explained later, the sinusoidal wave signals from light-receiving elements 181 and 182 mutually possess 90-degree phase difference. Signals with phase angle of 0° from light receiving element 181 are entered into the input terminal 1 of the signal insertion circuit 200 while signals with phase angle of 90° go from light-receiving element 182 into input terminal 2 of the signals insertion circuit 200. Signal insertion circuit 200, composed of the circuits shown in Fig. 3, counts the first up-down pulses formed by dividing (by inserting) the signals from light-receiving elements 181 and 182. Further, this circuit counts not only the first up-down pulses but also the second up-down pulses corresponding to the signals before division. By such counting of two types of up-down pulses, relative displacement of a wafer stage 300 against the device mainframe is measured. The measurement results are transmitted to a controller 400 and this controller 400 performs position control of the wafer stage 300 by way of a driving device 500. At this point, the shift speed of wafer stage 300 is increased and when frequencies of the signals from the light-receiving elements 181 and 182 rise above certain levels, input signals from the signal insertion circuit 200 to the controller 400 are switched from count results of the first up-down pulses to count results of the second up-down pulses. Further, when the shift speed of the wafer stage 300 is lowered to the contrary, input signal from the signal insertion circuit 200 to the controller 400 are switched from count results of the second up-down pulses to count results of the first up-down pulses. In the present embodiment, interferable beams from the semiconductor laser 101 are made approximately parallel beams by the collimator lens 102 and these parallel beams are entered into the deflection beam splitter 109 for splitting into two types of beams, namely transmission beams of linear deflection (P deflection) and reflection beams of linear deflection (S deflection). In this case, installation position of the semiconductor laser 101 is properly adjusted so that linear deflection direction of emission beams from the semiconductor laser 101 forms 45-degree angle against deflection direction of the deflection beam splitter 109. By conducting such adjustment, the relation of approximately 1:1 is established on the intensity ratio between transmission beams and reflection beams from the deflection beam splitter 109. The reflection beams and transmission beams from the deflection beam splitter 109 are subjected to circular deflection via the wavelength plates 151 and 152 and reflected with reflection mirrors 111 and 112. Then, diagonal incidence of reflected beams is made into optical scale 30. Further, respective beams are entered into optical scale 30 so that "m"-order diffraction light from target optical scale 30 can be emitted approximately perpendicularly from the diffraction grating surface of optical scale 30. In other words, beam incidence is achieved in the manner to satisfy the following equation. m ≃ sin -1 (mλ/p) Where, P: Grating pitch of diffraction grating of optical scale 30 λ : Wavelength of interferable beam from semiconductor laser 101 m : Integer m: Angle of incidence to diffraction grating surface of interferable beams (angle from perpendicular line to diffraction grating surface) Reflection beams from deflection beams splitter 109 achieve diagonal incidence into optical scale 30 by angle of incidence of m and then reflection diffraction is performed by the diffraction grating of optical scale 30, followed by perpendicular emission of primary diffraction light from this scale. On the other hand, diagonal incidence of transmission beams from deflection beam splitter 109 into optical scale 30 is achieved by the angle of incidence of - m and reflection diffraction is performed by the diffraction grating of optical scale 30, resulting perpendicular emission of negative primary diffraction light. In this application example, incidence positions of refrection beams and transmission beams into optical scale 30 are made identical and therefore, a pair of diffraction lights (± primary) vertically ejecting from scale 30 are overlapped each other. Consequently, such reflected diffraction lights form mutually common optical paths. In this case, the optical paths for transmission beams and reflection beams from deflection beam splitter 109 as well as for reflected diffraction lights are included into the same incidence surface (surface parallel with paper). ± primary diffraction lights perpendicularly omitted from optical scale 30 are directed toward reflection element 120 and enter into the end surface of lens 110. This lens 110, a stick-shaped one, is provided with the predetermined length to permit the parallel lights entering into one end surface of the lens to form images on the other end surface. In other words, the focal point surface of element 120 is located on its end surface. On the other end surface, formed is reflection film 121. Therefore, ± primary diffraction lights entering into lens 110 are reflected by reflection film 121 as shown in Fig. 6B, return to original optical paths, are emitted from lens 110, and then go into optional scale 30 again. Then, ± primary reflected diffraction lights, rediffracted by the diffraction grating of optical scale 30, return to the original optical paths, under reflection by reflection mirrors 111 and 112, and enter again into deflection beam splitter 109 after passing through 1/4 wavelength plates 151 and 152. At this time, the rediffracted lights have again passed through 1/4 wavelength plated 151 and 152. Therefore, at the time of reincidence, the beams first reflected by deflection beam splittor 109 (S deflection) are in the status of P deflection with 90-degree different deflection direction against the splitter. Therefore, these first reflected beams now pass through deflection beam splitter 109. Reversely, the beam which first have passed through the splitter becomes S deflection and become reflected when the beams make reincidence into deflection beam splitter 109. As explained above, two types of rediffracted lights are overlapped by deflection beam splitter 109 and such lights are converted to circular deflection lights with mutually reverse rotations by way of 1/4 wavelength plate 153. The beam splitter 106 splits the lights into two types of beams and converts into linearly deflected lights via deflection plates 171 and 172. These linearly deflected lights finally enter into light-receiving elements 181 and 182 as interference light. Angle of incidence m on Equation (1) mentioned above can be any values within the range which permits incidence of diffraction light into reflection element 120 and reincidence into optical scale 30. In this application example, the phase of "m"- order diffraction light is changed by 2mπ per each 1-pitch shift of diffraction grating. Therefore, light-receiving elements 181 and 182 perform photoelectric conversion by receiving the interference light subjected to interference by beams which undergo two times each of positive and negative "m"-order diffraction. Because of this reason, when the grating of diffraction grating is shifted by 1 pitch, 4m pieces of sinusoidal wave signals can be obtained. Accordingly, 3.2 µm is used as the pitch of diffraction grating of optical scale 30 primary ("M"= 1) is adopted as the diffraction light. As a result, when optical scale 30 is shifted by 3.2 µm, 4 pieces of sinusoidal wave signals can be obtained from light-receiving elements 181 and 182. That is, as the resolution per each sinusoidal wave, obtainable is 1/4 of the pitch of diffraction grating 30, namely 3.2/4 = 0.8 µm. By combining 1/4 wavelength plates 151 and 152 as well as deflection plates 171 and 172, 90-degree phase is provided between output signals from light-receiving elements 181 and 182 so that discrimination of shift direction of diffraction grating 30 and signal insertion become possible. In this embodiment, by using common optical paths for ±primary diffraction lights emitted from optional scale 30, the lights are directed again toward this optical scale 30 by way of common reflection element 20. This means that because installation of individual reflection mirrors is not required for individual diffraction light, the device can be compact in its size and simple in its configurations. Also, by utilizing such benefits, ratios of stray light generation to reach to the light-receiving elements are reduced, thus contributing to improvement of detection accuracy of interference fringes. Additionally, as shown in Fig. 6A, providing of the device composing components all at the upper side of optical scale 30 (one side) can be facilitated, thereby enabling offer of optical encoders extremely rich with general applicability. Reflection element 120 mentioned in this embodiment is provided with the reflection surface in the neighborhood of focal point surface. Therefore, for instance, even feeble change of diffraction angle occurs due to oscillation wavelength variations of laser beam accompanying alteration of the angle of incidence into lens 110, diffraction light can be returned to optical scale 30 by way of approximately same optical paths. This capability permits securate overlapping of two type of, namely, positive and negative, diffraction lights consequently preventing degradation of S/N ratio of the output signals from light-receiving elements 181 and 182. Further, size reduction of entire device is attempted by presetting the angle of incidence 8m of laser beams into optical scale 30 as mentioned above concurrently by using reflection element 120. If the grating pitch of diffraction grating of optical scale 30 is 3.2 µm and the wavelength of laser 101 is 0.78 µm the diffraction angle of ± primary diffraction lights is 14.2° as previously mentioned. Hence, when refraction-rate distribution-type lens with diameter of about 2mm is used as lens 110 to reflect only ± primary diffraction lights, the distance from optical scale 30 to lens 110 becomes 2/tan 14.2° = 7.9mm. In other words, separation of only about 8mm is all that is mended and this advantage makes configurations of entire device highly compact. Under the subject embodiment, the optical path lengths are identical for a pair of rediffracted lights which form interference fringes (single color) on light-receiving element 181 and 182. Therefore even if the wavelength of semiconductor laser 101 are changed, it is possible to generate the interference fringes that react only against displacement of optical scale 30. Also, what becomes possible is mounting of low-priced multimode semiconductor laser as a light-emitting element. In this embodiment, as is comprehensible from Fig. 6, symmetry exists on the optical paths of optical system composed of deflection beam splitter 109, reflection mirrors 111 and 112, and reflection element 120. This fact makes the system configurations resistant against external disturbance of optical scale 30 by vertical movement and others. The signal insertion circuit in the first embodiment explained up to this point comprises a division means for dividing original signals and generating preliminarily determined plural numbers of pulses, a first count means for counting said plural numbers of pulses, a second count means for counting designated pulses corresponding to the original signal, and a control means for controlling counting operation of said the first and the second counting means in compliance with frequencies of said original signals. By adopting this configurations of this type, even when original-signal frequencies are elevated and the division means fails to achieve accurate generation of divided pulses, the control means enables the use of count results by the second count means in lieu of the results by the first count means. Consequently, for instance, by applying the circuit linear encoders or other devices, scale displacement can be constantly measured regardless of the speed variation of linear scales. The displacement measuring device according to the present embodiment comprising a scale reading means that outputs signals in compliance with scale displacement levels by reading the scale graduations provided on the movable scale, a division means that divides signals from said first scale reading means and generates plural pulses of predetermined numbers, and a first count means that counts the numbers of these plural pulses, further comprises a second count means that counts pulses corresponding to signals from said scale reading means, and a control means that controls the counting operation of said first and second count means in line with variations of frequencies of signals from said scale reading means, thereby enabling the measurement of scale displacement from the results of said second count means even when scale shift speed (parallel shift or rotation) varies and frequencies of signals from the scale reading means are increassed. Also provided is a displacement measuring device according to the present embodiment which comprises a scale reading means that reads the graduations on the movable scale and issures signals pursuant to the scale displacement, a pulse generating means that creates first pulses of predetermined frequencies and second pulses of frequencies lower (greater pitches) than said first pulses based on signals from the scale reading means, measurement means that counts said first and second pulses and measures displacement of the scale, and control means that controls said measurement means based on the shift speed variations of the scale. By adopting the configurations of this type, similarly to the above-mentioned device, scale displacement can be measured by the measurement means irrespective of the scale shift speed. Moreover, the measurement method can be selected depending on the scale shift speed. For instance, in case of high speed, measurement is made by counting the second pulses and in case of low speed, measurement is achieved by counting the first pulses. This measurement method selection can be made either per each target scale or according to shift speed changes during measurement of one of the scales. Fig. 7 is a block diagram showing the signal insertion circuit used in the second embodiment of this invention. On those components identical with those shown in Fig. 3, the same symbols and numbers are affixed. Therefore, explanations on the identical components are omitted or explanations will be limited to those which require clarifications. In this second embodiment, the speed detection circuit 15' is indicated in place of the speed detection circuit 15 shown in the first embodiment. The reference numerals 73 and 74 are pulse generating circuits of single stable multivibrator or others that can be retriggered, capable of generating up-down pulses "ua" and "va" with widths wider than divided pulses "j" and "k". Reference numeral 90 is a counter which counts up-down pulses "ua" and "va" with wide widths from pulse generating circuits 73 and 74 and outputs count data "qa". The numeral 70 is a delay circuit which assigns certain delay D to signal "f" corresponding to original signal before division. The numeral 71 is a pulse generator made of single stable multivibrator or others and this circuit generates pulse "ra" with predetermined time width in response to rise edge of signal "f" with delay D from delay circuit 70. This pulse "ra" is used as the reset signal of counter 90. Numeral 75 is a discriminator circuit designed for judging whether or not count data "qa" from counter 90 coincides with division number N preliminarily determined by this circuit. Configurations of this circuit allow its output "sa" to become H (high level/logic 1) only when the said coincidence exists. Numeral 76 is a detection signal circuit which outputs the signals (detection output "t" that become H (high level) during one cycle period of signal "f" when H signal is not received from discriminator circuit 75. All these circuits explained above constitute signal detection circuit 15". By referring to the signal waveform examples shown in Fig. 8, explanations will be made on the circuit operation of Fig. 7. The circuits in Fig. 7 perform, similarly to the circuits in Fig. 3, eight division of one cycle of input signals (original signals). Count data "qa" is reset at point (1') (at rise of signal "f") and counter 90 counts up at each rise edge of signal "ua". Therefore, unless erroneous operation occurs on the circuits up to direction discriminator 8, count data "qa" becomes 8 (binary and 1.0.0.0 from upper bit) at next rise point (2') of signal "f". At this time, discriminator circuit 75 judges that data "qa" is coincided with division number N (N ≦ 8) and from that point on, output "sa" becomes H. At point (3') with lapse of short time D from point (2'), counter 90 is reset by signal "ra" and simultaneously output "sa" from discriminator circuit 75 becomes L (low level/logic 0) In the present embodiment, correct performance of 8 division is confirmed by the fact that signal "sa" becomes H immediately after rise edge of signal "f". By using this discriminator circuit 75, various processing can be performed. Output from discriminator circuit 75 is sent to detection signal circuit 76 which issues L output because signal "sa" is H at rise of signal "f". This way, while correct performance of 8 division is being confirmed, detection signal circuit 76 continues L output. Next, by referring to the example shown in Fig. 9, explanations will be made regarding the case where (slightly before) separation of division pulses from direction discriminator 8 becomes not possible due to rise of frequencies of sinusoidal wave signals (phase angles 0°, 90°) entered into input terminals 1 and 2. Count data "qa" is reset at point (1') of Fig. 9 (during rise of signal "f") and continues count-up at each rise edge of signal "ua". On the example shown in Fig. 9, pulse array cycles are varied from 3rd through 6th pulse and separation is not possible between 3rd and 4th pulses as well as 5th and 6th pulses (marked with Δ). As a result, at the next rise of signal "f", namely, point (2'), count data "ua" becomes 6 (0.1.1.0 from upper bit). At this time, since data "qa" does not correspond with division number N (N ≦ 8) at discriminator circuit 75, output "sa" remains L. Because signal "sa" is L during rise of signal "f", detection signal circuits 76 issues H output for one cycle period of signal "f". If signal "sa" still remains at L at the next rise edge of signal "f", the circuit continues output H for another one cycle period of signal "f". Detection signal circuit 76 keeps issuance of output H in this way as long as there exists probability of failure in correct performance of 8 division. As mentioned above, by checking whether signal "sa" immediately after rise edge of signal "f" is at H or L, it is possible to know if correct division is made on pulses "ua" and "va" generated in response to pulses "j" and "k" shown in Fig. 9, even when separation of pulse "ua" (or "va") starts to become difficult, separation is still possible although pulse cycle variation occurs because widths of split pulses "j" and "k" are narrower. Therefore, correct count values are obtainable at output "m" of counter 9. Thus, further accurate, error-free counting becomes possible by conducting prompt switching through estimating operating trouble before division failure actually occurs. The above-mentioned detection output "t" is sent to latch circuit 16 and pulse generating circuit 17 shown in Fig. 3. By conducting the processes also shown in Fig. 3, cases of division failure (for instance, high speed, namely high frequency) can be properly prevented. In other words, by switching to low-resolution counting of larger-pitch pulses, counting can be smoothly continued. In the above embodiment, indicated is an example case of relatively short-time delay D of signal "f" created by delay circuit 70. Basically, however, setting of this delay will suffice as long as reset operation of counter 90 can be completed before rise of pulse signal subsequent to up-down pulse "ua" (or "va"). In the above embodiment, to detect erroneous operation of the division steps (1 - 8), counter 9 counts the number of split pulse ("ua", "va") within the period corresponding to one cycle of signal "f". This counting period does not need to be limited to one cycle period of signal. The counting period may be any other lengths as long as the period is integer multiplication of resolution (1/4 cycle) obtained from signals "f" and "h". Further, methods other than those explained above can also be applied to judgment on coincidence between count value "qa" and division number N or to styles of signals for indicating judgment results. On the embodiment explained up to this point, the displacement measuring device for position measurement of wafer stage is indicated. This displacement measuring device can be effectively used, for example, for position measurement of magnetic heads or optical heads for formation of tracking tracks on magnetic disks or optical disks. Also, the device is applicable to encoders of magnetic, optical linear, rotary, and various other types. As mentioned above, the means are provided for counting the first pulses and the second pulses with mutually differing frequencies and the employed configurations allow controls of counting operation of these pulses. Therefore, even when frequencies become high and, for instance, the first pulses generated by dividing original signals become inaccurate due to high frequencies of original signals, it is possible to conduct accurate signal processing by using the second pulses corresponding to original signals with lower frequencies (larger pitches). Consequently, regardless of the scale shift speed, the displacement measuring device to perform displacement measurement can be offered. Further, pulse signals with two types of pitches can be formed from the same input signals and complete synchronization can be achieved between these two types of pulses. Then by conducting switching between these types of pulses, and advantage can be created for eliminating counting errors arising from synchronizing errors of both pulse signals during switching.

Claims: A pulse counting circuit (200) for counting pulse signals (a, b), comprising: a first pulse signal generating means (8) for generating first pulse signals (j, k) by dividing an input periodic signal (a, b) into first multiple pulse divisions with a first predetermined division number, and second pulse signal generating means (11) for generating second pulse signals (p, q) by dividing an input periodic signal (a, b) into second multiple pulse divisions with a second predetermined division number, said first division number being greater than said second division number; a first counting means (9) for counting said first pulse signals (j, k); a second counting means (12) for counting said second pulse signals (p, q); a third signal generating means (73, 74) for generating third pulse signals (ua, va) by widening the pulse-width of said first pulse signals (j, k); a third counting means (90) for counting said third pulse signals (ua, va); a comparing means (75) for comparing the result of said third counting means (90) after each period of the input signal (a, b) with the first division number; and a control means (76, 16, 17) which switches to the second counting means (12) when the result of said third counting means (90) does not correspond with the first division number. A circuit according to claim 1, wherein said input periodic signal (a, b) comprises 2-phase sinusoidal wave signals. A displacement measuring device comprising a circuit according to claim 1 or 2. A stage control device comprising a circuit according to claim 1 or 2.

Inventors: ISHII SATOSHI, ISHII, SATOSHI
Applicants: CANON KK, CANON KABUSHIKI KAISHA
Application year: 1990
Main classification: G01D5
IPC codes: G01D5