Time measurement circuit and optoelectronic distance meter having such a time measurement circuit

10185032 · 2019-01-22

Assignee

Inventors

Cpc classification

International classification

Abstract

Some embodiments of the invention relate to a time measurement circuit for an incoming signal. In some embodiments, the time measurement circuit has a comparator stage, for generating a comparator output signal depending on a fulfillment of a criterion by the incoming signal, wherein exceeding or falling below a threshold value is defined as the criterion. Furthermore, a digitization stage is provided, for sampling, which is performed at a defined sampling rate, of an input signal fed to the digitization stage and converting it into digital data containing sampled values for the input signal, and an evaluation unit for determining a chronological location for the incoming signal by evaluating the digital data.

Claims

1. A time measurement circuit for an incoming signal, the time measurement circuit comprising: a comparator circuit stage for generating a comparator output signal depending on a fulfillment of a criterion by the incoming signal, wherein exceeding or falling below a threshold value is defined as the criterion; a digitization circuit stage for sampling, which is performed at a defined sampling rate, of an input signal fed to the digitization circuit stage and converting it into digital data containing sampled values for the input signal; an evaluation circuit unit for determining a chronological location for the incoming signal by evaluating the digital data; and a signal generating stage interconnected between the comparator circuit stage and the digitization stage, which is configured to generate and output, in a chronologically fixed manner dependent on the content of the comparator output signal, an analog shape signal, which is configured for post-sampling interpolation ability, of known shape, wherein the evaluation circuit unit is configured to determine a time for the incoming signal while using a chronological interpolation of the values contained in the digital data and the known shape of the shape signal.

2. Time measurement circuit according to claim 1, wherein: the signal generating stage is configured such that the shape signal is pulsed with defined pulse width and changes its signal values asynchronously to the sampling rate of the digitization circuit stage multiple times within the pulse width, wherein the shape signal is formed as: bell-shaped, sawtoothed, triangular, trapezoidal, or stepped.

3. Time measurement circuit according to claim 1, wherein: the signal generating stage comprises at least one flip-flop circuit and a low-pass filter.

4. Time measurement circuit according to claim 1, wherein: the signal generating stage comprises at least one D flip-flop and a low-pass filter.

5. An optoelectronic distance meter according to the time-of-flight principle, the distance meter comprising: at least one light source for emitting at least one pulsed light signal, onto a target object, a receiving circuit having a detector for detecting the light signal returning from the target object and signal processing electronics downstream from the detector, and an evaluation circuit unit for determining a distance to the target object, wherein: a time measurement circuit according to claim 1 is provided as part of the signal processing electronics and the evaluation unit.

6. A distance meter according to claim 5, wherein: the comparator circuit stage of the time measurement circuit is configured and provided with criteria such that a comparator output signal is generated and output in each case for a rising flank and for a falling flank of the returning detected light signal, the evaluation circuit unit of the time measurement circuit is configured for determining a first time, that for the rising flank, and a second time, that for the falling flank, and the evaluation circuit unit of the distance meter is configured for deriving a distance to the target object depending on the determined first time and the determined second time.

7. A distance meter according to claim 5, wherein: the comparator circuit stage of the time measurement circuit is configured and provided with criteria such that a comparator output signal is generated and output in each case for a rising flank of the returning detected light signal depending on at least one first and one second set trigger threshold, the evaluation circuit unit of the time measurement circuit is configured for determining a first time, that for exceeding the first trigger threshold, and a second time, that for exceeding the second trigger threshold, and the evaluation circuit unit of the distance meter is configured for deriving a distance to the target object depending on the determined first time and the determined second time, wherein a quality specification about the distance determination is furthermore also derivable depending on the determined first time and the determined second time.

8. A distance meter according to any one of claim 5, wherein: the signal processing electronics have a first and a second channel, wherein the time measurement circuit is provided in the first channel and it is therefore provided for the case of an activation of the detector, which is caused by the returning light signal, in its middle and upper amplitude range, and the second channel is provided for the case of an activation of the detector, which is caused by the returning light signal, in its lower linear amplitude range and for this purpose has a digitization circuit stage for sampling, which is performed at a defined sampling rate, of the detected light signal and converting it into digital WFD data containing sampled values and an evaluation circuit unit for determining a chronological location of the detected light signal in consideration of a pulse shape, which is depicted on the basis of the sampled values, for the detected light signal, wherein the evaluation circuit unit of the distance meter is configured so that the distance to the target objectdepending on the activation of the detector, which is caused by the returning light signal, in its middle and upper amplitude range or in its lower, linear amplitude rangeis determinable on the basis of the digital data generated in the first channel or on the basis of the digital WFD data.

9. A distance meter according to any one of claim 5, wherein: the detector is configured as a receiver photodiode having a downstream amplifier stage, and having a low-noise trans-impedance amplifier element TIA.

10. A distance meter according to any one of claim 5, wherein: the evaluation circuit unit comprises an FPGA.

11. A distance meter according to any one of claim 5, wherein: the evaluation circuit unit comprises a microprocessor.

12. A distance meter according to any one of claim 5, wherein: the evaluation circuit unit comprises a DSP.

13. A distance meter according to any one of claim 5, wherein: an electronically adjustable damping element VGA is directly upstream of the comparator circuit stage of the time measurement circuit, wherein the damping is dynamically adaptable by the evaluation unit, optionally the FPGA.

14. A distance meter according to any one of claim 5, wherein: the distance meter and the evaluation circuit unit of the distance meter are configured for progressive determination, which is performed in real time, of distances, wherein the evaluation circuit unit is configured to output the distance.

15. A distance meter according to any one of claim 5, wherein: the distance meter and the evaluation circuit unit of the distance meter are configured for progressive determination, which is performed in real time, of distances, wherein the evaluation circuit unit is configured to output the distance, together with a derived amplitude for the returning light signal and a derived quality specification about the distance determination, at a rate in the range of 0.1 to 100 MHz.

16. Time measurement method for an incoming signal, the method comprising: progressive checking of a fulfillment of a defined criterion by the incoming signal and outputting a trigger signal upon fulfilling the criterion, wherein exceeding or falling below a threshold value is defined as the criterion, generating and outputting an artificial analog shape signal in a chronologically fixed manner depending on the output of the trigger signal, wherein the shape signal is configured for post-sampling interpolation ability and has known shape and known amplitude, sampling, which is performed at a defined sampling rate, of the shape signal and converting it into digital data containing sampled values for the shape signal, and deriving a point in time for the incoming signal by evaluation of the digital data, depending on a determination of a chronological location of the shape signal, which is performed using a chronological interpolation of the values contained in the digital data and the known shape of the shape signal.

17. Time measurement method according to claim 16, wherein: the shape signal is pulsed having defined pulse width and changes its signal values asynchronously to the sampling rate multiple times within the pulse width, wherein the shape signal is formed as: bell-shaped, sawtoothed, triangular, trapezoidal, or stepped.

18. Time measurement method according to claim 16, wherein: the shape signal is pulsed having defined pulse width and changes its signal values asynchronously to the sampling rate multiple times within the pulse width progressively or continuously.

19. An optoelectronic distance measurement method according to the time-of-flight principle, the distance measurement method comprising emitting at least one pulsed laser light signal toward a target object, detecting the light signal returning from the target object, and determining a distance to the target object depending on a point in time derived for the returning light signal, wherein: deriving the point in time for the returning light signal is performed using a time measurement method according to one of claim 16.

20. A time measurement circuit for an incoming signal, the time measurement circuit comprising: a comparator circuit stage for generating a comparator output signal depending on a fulfillment of a criterion by the incoming signal, wherein exceeding or falling below a threshold value is defined as the criterion; a signal generating stage interconnected between the comparator circuit stage and a digitization circuit stage, which is configured to generate, in a chronologically fixed manner dependent on the content of the comparator output signal, an analog shape signal of known shape, the digitization circuit stage for sampling, which is performed at a defined sampling rate, of an input signal fed to the digitization circuit stage, and converting it into digital data containing sampled values for the input signal; and an evaluation circuit unit for determining a chronological location for the incoming signal by evaluating the digital data; wherein the input signal is provided by the analog shape signal and the analog shape signal is configured that interpolation of the values contained in the digital data is ensured; and wherein the evaluation circuit unit is configured to determine a time for the incoming signal while using a chronological interpolation of the values contained in the digital data and the known shape of the shape signal.

21. Time measurement circuit according to claim 20, wherein: the signal generating stage is configured such that the shape signal is pulsed with defined pulse width and changes its signal values asynchronously to the sampling rate of the digitization circuit stage multiple times within the pulse width, wherein the shape signal is formed as: bell-shaped, sawtoothed, triangular, trapezoidal, or stepped.

22. Time measurement circuit according to claim 20, wherein: the signal generating stage comprises at least one flip-flop circuit and a low-pass filter.

23. Time measurement circuit according to claim 20, wherein: the signal generating stage comprises at least one D flip-flop and a low-pass filter.

24. An optoelectronic distance meter according to the time-of-flight principle, the distance meter comprising: at least one light source for emitting at least one pulsed light signal, onto a target object, a receiving circuit having a detector for detecting the light signal returning from the target object and signal processing electronics downstream from the detector, and an evaluation circuit unit for determining a distance to the target object, wherein: a time measurement circuit according to claim 20 is provided as part of the signal processing electronics and the evaluation unit.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) The method according to the invention and the device according to the invention will be described in greater detail hereafter, solely for exemplary purposes, on the basis of specific exemplary embodiments, which are schematically illustrated in the drawings, wherein further advantages of the invention will also be described. In the figures:

(2) FIG. 1a shows a schematic illustration of an optoelectronic distance meter according to the prior art,

(3) FIG. 1b shows a schematic illustration of a runtime measurement method according to the prior art,

(4) FIG. 2a shows a schematic illustration of a threshold value method for backscattered light signals according to the prior art,

(5) FIG. 2b shows a schematic illustration of the threshold problem of the threshold value method,

(6) FIG. 3a shows a schematic illustration of a sampling method for backscattered light signals according to the prior art,

(7) FIG. 3b shows a schematic illustration of the saturation problem of the sampling method,

(8) FIG. 4 shows a time curve of an incoming signal (for example, a detected light signal returning from the target), for which at least one point in time is to be determined as an example,

(9) FIG. 5 shows time determination using a conventional TDC method known according to the prior art,

(10) FIGS. 6a-d show graphs of signal curves and sampled data over time in relation to the individual stages and units of the time measurement circuit according to the invention,

(11) FIGS. 7a-d show different variants for the design of the shape signal according to the principle according to the invention,

(12) FIG. 8 shows a block diagram of an embodiment according to the invention for the time measurement circuit, wherein this forms a part of a distance meter according to the invention having additional WFD channel,

(13) FIGS. 9a,b show the amplitude dependence of the measured runtime and a possible correction curve, and

(14) FIG. 10 shows distance noise of an embodiment according to the invention having TDC and WFD channel.

DETAILED DESCRIPTION

(15) FIG. 1a shows a schematic illustration of an optoelectronic distance meter 1 of the prior art according to the pulse runtime principle. A transmitter 2 and a receiver 3 are arranged in the distance meter 1. The transmitter 2 emits a light pulse 4a, which is detected again by the receiver 3 after the reflection or backscattering on a target, for example a retroreflector 5, as the backscattered light pulse 4b. Instead of a single light pulse, according to the invention, an analog or digital coded pulse sequence or a continuously modulated transmitted signal can also be used.

(16) As explained in FIG. 1b in a schematic illustration, the distance is ascertained from the runtime T as the chronological difference between the starting point in time of the emission of a light pulse 4 and the receiving point in time of the backscattered light pulse 4. The ascertainment of the receiving point in time is performed in this case by the evaluation of a feature of the signal pulse s(t), for example, by exceeding a signal threshold or by focal point determination of the integrated pulse curve. In the threshold value method, other methods are also usable for measuring the runtime T, for example, the conversion of the received signal into a bipolar signal and subsequent determination of the zero crossing.

(17) In FIG. 2a, a threshold value method for backscattered light signals 6c according to the prior art is explained. To suppress noise, background components, or systematic interfering signals, for example, due to the optical and electrical crosstalk between transmitter signal path and receiver signal path, and exclude them from a detection, a detection threshold 9 (for example, in the form of a comparator component) is used. Signal intensities s(t) located below this detection threshold 9 do not result in a response of the comparator, which generates a stop signal, as the discriminator and therefore do not result in a detection. If the signal 6c exceeds the detection threshold 9 in its intensity, the detection occurs and therefore the generation of the stop signal and the registration of the receiving point in time. The output signal provided by the threshold value method is therefore dependent on the received or input signal reaching or exceeding the detection threshold 9. However, if the signal intensity s(t) always remains below a detection threshold 9, as shown in the example of FIG. 2b, no response of the discriminator (comparator) thus occurs and the signal 6d is not detected. This threshold problem of the threshold value method occurs, for example, in the case of large measurement distances or corresponding background influences, which can drive the required threshold level of the threshold signal upward. This is also the case with a proportional discriminator (constant fraction discriminator), in which the trigger threshold is varied proportionally to the maximum amplitude. In the event of small signals, the trigger threshold cannot be sufficiently reduced, since otherwise random noise would trigger receiving time marks.

(18) The simple threshold value method typically allows lower distance determination accuracies than the sampling method (WFD principle) mentioned hereafter, at least if the received pulse is not located in the saturation of the detector.

(19) FIG. 3a illustrates the principle of a sampling method (WFD) for backscattered light signals according to the prior art. A received signal 6a or the signal curve thereof is sampled at various points in time 7 and/or assigned time intervals, so that the signal shape may be derived. To also be able to detect large variations of the signal pulse s(t), a high dynamic response is required on the receiver side, which enables the complete acquisition or sampling of the signal 6a. Otherwise, the situation shown in FIG. 3b can occur, if parts of the signal 6b are outside the dynamic range and saturation problems of the sampling method occur. Above a saturation limit, a saturated range 8 of the receiver exists, in which no meaningfully usable sampling values of the pulse are available. The use of the sampled values for the determination of the chronological location of the pulse is then restricted to the range located below the saturation limit. A determination of the signal shape and location is then difficult, in particular in the case of a high flank steepness.

(20) FIG. 4 shows a time curve of an incoming electrical signal, for which at least one point in time is to be determined as an example. The moderately-sized pulse in the front part of the time signal generates a first trigger event, and the second, saturated pulse in the rear part of the time signal generates a further trigger event. The comparator stage and the signal generating stage of the time measurement circuit according to the invention now generate, for each pulse, a picosecond-accurate shape signal having constant amplitude, which is supplied to a gigahertz-speed A/D converter and digitized therein. Subpicosecond-accurate time interpolations may be implemented using known algorithmic methods from the data sequence. Since this shape signal, which is fed to the A/D converter, is independent of the amplitude of the received pulses, no dynamic errors occur. The optional emphasis of the amplitude-dependent time shifts or distance offsets occurring at the comparator stage is explained for exemplary purposes in FIGS. 9a and 9b.

(21) FIG. 5 shows the time determination using a conventional TDC method. In a first step, the time is determined in a coarse measurement, this is implemented using a quartz-accurate counter. The remaining uncertainty of the trigger point in time t is determined in a second step by means of a time interpolator, i.e., an additional circuit assembly. This can be a capacitor, for example, which is charged by a triggered constant current source and subsequently read out. These conventional circuit assemblies for time interpolation have generally reached an accuracy of at best 10 ps up to this point.

(22) FIGS. 6a-6d show graphs of signal curves and sampled data over time in relation to the individual stages and units of the time measurement circuit according to the invention.

(23) FIG. 6a shows the output signal of the comparator stage of the device according to the invention. The step in the signal is generated when, for example, the rising flank of the incoming signal to be analyzed (for example: the signal which is generated by a light detector and then amplified) exceeds the defined threshold value. The output signal of the comparator stage then has, for example, the shape of a picosecond-speed digital step function, as shown.

(24) The comparator stage can then be designed so that the output signal remains on top until a separate reset signal (for example, from an FPGA or DSP) is fed.

(25) The output signal of the comparator stage is fed to the signal generating stage.

(26) FIG. 6b shows the chronologically fixed shape signal, which is generated and output depending on the content of the comparator output signal by the signal generating stage. The shape signal is in this case a signal of known shape and in particular known amplitude, which is designed for post-sampling interpolation ability.

(27) In the embodiment shown, the shape signal has a pulse shape, having known shape, amplitude, and width.

(28) In a special embodiment, such a signal can be generated, for example, by a flip-flop circuit or by a logic gate.

(29) A short rectangular pulse of defined amplitude can thus firstly be generated, for example, having a width of less than 1 ns.

(30) This rectangular pulse can then be filtered by a corresponding low-pass filter, whereby a bell-shaped pulse (having known shape, and also having known amplitude and width, which are essentially unchanged from the rectangular pulse) arises, as shown as an example in FIG. 6b.

(31) The generated shape signal can then be supplied to the digitization stage (i.e., for example, an ADC). This samples the signal supplied thereto at a defined sampling rate and converts it into digital data containing sampled values.

(32) FIG. 6c shows an example of the procedure of the quantification and digitization of the shape signal. The amplitude of this artificial shape signal can in particular be selected in this case so that it covers a majority of the signal range of the ADC between the lowest-value and the highest-value bit (LSB (least significant bit) and MSB (most significant bit)).

(33) FIG. 6d illustrates the digital data generated by the digitization stage (such as an ADC), which then contain the sampled values for the input signal of the ADC (i.e., for the shape signal). In other words, the digital data thus contain a digital signal sequence having the relevant pulse information, which is then used as an input data set for the time interpolation algorithm.

(34) The sampling rate of the digitization stage (the ADC) can be between approximately 200 MHz and 10 GHz, for example, in this case.

(35) The sampled shape signal (i.e., the values sampled for this purpose, which are now contained in the digital data) can finally be evaluated with respect to its chronological location by way of time interpolation algorithms known per se. For example, such a time interpolation method is described in publication document WO 2011/076907, wherein time interpolation accuracies in the subpicosecond range are then achievable using such a method.

(36) In a distance meter, in which a so-called starting pulse (optionally given by an optical starting reference pulse, which is detected) is also chronologically determined for the measurement of the runtime of the light (i.e., a first starting point in time is determined for the so-called starting pulse), it can be ensured in particular by a resampling (i.e., by a sampling rate conversion) that the identical sampling pattern is applied for the sampling of the starting pulse and the sampling of the shape signalwhich then is generally used as a stop pulse here. The accuracy of the runtime determination can therefore be further increased.

(37) The evaluation unit (optionally providedat least partiallyby an FPGA) can then determine the runtime of the light, especially in real time (i.e., for example, at a rate of greater than 1 MHz), using a corresponding waveform algorithm as the time interpolation, as the time passed between the first point in time determined for the reference pulse used as the starting pulse and the second point in time determined for the shape signal. The desired distance to the target can then be derived via this runtime.

(38) Similarly thereto, this principle of sampling rate conversion (resampling) can also be applied for two shape signals, which are generated successively, once for the rising flank of the pulse of the actual incoming signal and once for the falling flank of the signal (whichsee also the description of FIGS. 9b and 9bcan also be applied to correct a so-called range walk, which possibly occurs in the threshold value method). With reference to the embodiment of the circuit as shown in FIG. 8, wherein the pulse generator component 14 can be constructed from two flip-flops, for example, the two rectangular pulses generated by the flip-flops (for the rising flank and the falling flank) can be combined with an OR gate after the flip-flops and then fed to the low-pass filter. The second pulse is then fed to the same ADC.

(39) FIGS. 7a to 7d show various variants for the design of the shape signal according to the principle according to the invention, wherein these are each designed for optimum post-sampling interpolation ability.

(40) FIG. 7a shows a bell-shaped shape pulse as the shape signal, FIG. 7b shows a sawtoothed one, FIG. 7c shows a trapezoidal one, and FIG. 7d shows a stepped one.

(41) The artificial pulses from FIGS. 7a and 7b change their signal values continuously over the entire pulse width.

(42) The artificial pulse from FIG. 7c changes its signal values at least partiallyover multiple sampling periodscontinuously within the pulse width.

(43) The artificial pulse from FIG. 7d changes its signal values multiple times within the pulse width, wherein the change takes place asynchronously in relation to the sampling rate.

(44) FIG. 8 shows a block diagram of a time measurement circuit 10 according to the invention according to the threshold value principle (at least in a first channel of the receiving circuit) having a digital time converter (time-to-digital converter, TDC) according to the invention. The detection signal of a photodetector (for example, APD), which is converted by a current-voltage converter (TIA, trans-impedance amplifier) 11, is fed, in the first channel (threshold value channel), to a comparator stage (discriminator) 12, which is indicated by a rising rectangular pulse. Optionally, the signal fed to the comparator 12 can be damped upstream in this case by a VGA, which is designed in particular as a VGA having controllable damping. If the signal applied to the comparator exceeds a predefined threshold value, a comparator output signal 13 is generated, which is fed to a signal generating stage having a pulse generator component 14, which can comprise, for example, two electronic flip-flop circuits (i.e., bistable trigger elements, high-speed logic gates, not shown). Using the signal generating stage, which can optionally also contain a low-pass filter 15 downstream from the pulse generator component, according to one embodiment, an analog, defined pulsed signal having a defined time curve and defined amplitude (optionally optimized to the signal range of the ADC) is generated. This synthetically generated signal is then fed to a rapid, signal-resolving analog-to-digital converter circuit (ADC) 16 having adapted time and amplitude resolution. The sampled data are processed in real-time or pipelined in correspondingly designed electronics hardware 17 (FPGA). A field programmable gate array is an integrated circuit (IC) of digital technology, in which a logic circuit can be programmed. The English designation can be translated as (application) field programmable (logic) gate array. Manifold embodiments of FPGAs are known in the prior art. Various terminals of the FPGA 17 are indicated in FIG. 8, specifically A for the input of artificially generated, flank-triggered shape signals, which are independent of the amplitude of the original incoming signal, B for setting the pulse length, C for a reset at the beginning of a start/stop time window, and D for setting the sensitivity of the VGA. A shape signal triggered by the actual incoming signal (for example, detected light pulse, and in this case by exceeding a threshold) is thus applied to the input A. A time measurement circuit TDC is implemented using these functionalities, together with the components 14, 15, and 16 upstream from the FPGA, wherein, however, the electronic components used and the evaluation of the chronological location of the shape signal correspond in principle to those of a known WFD circuit having ultrahigh time resolution.

(45) In a further embodiment (not shown), the time measurement circuit 10 can have an additional second signal channel 12, 13, 14, 15, 16 according to the threshold value principle.

(46) It can differ from the above-described channel by way of a comparator 12, which triggers on the falling flank of the input signal. The FPGA 17 ascertains, together with the result from the first channel, the width of the input signal. This width is used to remedy a distance offset caused by the unknown amplitude of the actual incoming signal (i.e., a distance offset therefore caused by the discriminator 12).

(47) In still a further specially constructed embodiment, the time measurement circuit 10 can contain a third channel 12, 13, 14, 15, 16 according to the threshold value principle. It differs from the two previous TDC channels by way of a comparator 12, which triggers on the rising flank of the input signal in the event of a signal threshold value differing from the first channel. Two measurement points are thus acquired on the rising flank, the downstream FPGA determines the slope of the flank therefrom. If the slope is not in the expected ratio to the pulse width, interference of the received signal due to a particular arrangement of the laser measurement beam in relation to the target object thus exists. For example, if the laser beam is partially incident at an object edge on the first object and an object located behind it, a double reflection thus arises. If the two objects are spaced apart closely (<1 m), the two associated electronic received pulses thus overlap and the relation between steepness of the rising flank and pulse width deviates from a previously determined reference value. Double targets, which result in overlap of received pulses, may thus be recognized, corrected or at least partially eliminated.

(48) Alternatively, the number of the TDC channels can be increased, without the complexity of the overall distance measurement circuit substantially increasing. With a fourth channel 12, 13, 14, 15, 16 according to the threshold value principle, the individual distances assigned to the double targets can even be measured accurately in any case and without a priori assumptions.

(49) Optionallyas indicated in FIG. 8a conventional WFD time measurement circuit 18 can be equipped in a parallel arrangement to the above-described TDC time measurement circuit. This channel essentially consists of an amplifier stage, a low-pass filter or bandpass filter, and an A/D converter channel. The digital data generated by the ADC can be supplied in particular to the same FPGA 17 as the data of the TDC channel (or optionally the multiple TDC channels).

(50) FIG. 9a illustrates a potentially occurring signal-strength-dependent distance error (time walk or range walk).

(51) Depending on the level of the amplitude of the actual incoming signal, a set or oscillating threshold value (Vth) of the comparator stage of the TDC is exceeded either comparatively early or late in comparison to one another. This exceeding point in time also determines the moment relevant for the generation of the stop signal. This exceeding point in time thus now varies depending on the amplitude of the actual incoming signal, which is referred to as a range walk error and can be compensated for by knowing about the width of the actual incoming signal pulse. This width of the signal pulse can be determined by determining a point in time for falling below the threshold value on the side of the falling flank of the signal pulse, which can in turn be performed with the aid of a second comparator designed for this purpose.

(52) FIG. 9b shows the generally, but not necessarily, monotonous relationship between distance offset (i.e., time walk or range walk) and signal strength, which can be performed on the basis of a pulse width measurement by means of the TDC device. The signal strength is used to compensate for the influence of the time walk or range walk (calibration).

(53) The curve also shows in principle the systematic distance deviation, if a fixed distance is measured and the received signal is varied from very small amplitudes up to, for example, 20-fold overload. This systematic distance deviation can consistently be very reproducible.

(54) It is apparent that the TDC is more suitable for the upper signal range up to multiple signal overload and supplies a high distance measurement accuracy there because of the nearly constant distance offset.

(55) In the lower signal range, the TDC displays a stronger signal dependence of the distance offset. The time determination according to the WFD principle (i.e., waveform digitization directly of the actual incoming signal and determination of the chronological location by time interpolation on the basis of the values obtained directly for the signal), in contrast, has advantages in the lower signal range, since this has rather lower noise and additionally practically no signal-dependent distance offset. A conventional WFD can also retrieve accurate distance measurement from very noisy signals by way of signal accumulation.

(56) A 2-channel distance meter according to the invention consisting of a WFD channel and a TDC channel is distinguished by a very high distance measurement accuracy, over an expanded signal dynamic range, in the submillimeter or micrometer range, and independently of the amplitude of the received signal. In the lower signal range, which typically occurs when measuring on black or wet targets, the WFD determines the distance to the object, in the event of inadequate signal-to-noise ratio (SNR), with adaptive accumulation of the digital signal vector, the SNR is additionally raised prior to the distance evaluation and the scattering of the measurement result is thus improved. When measuring on light, glossy, or reflective objects, the TDC channel is the selection which provides advantages, where the signal strengths are in the upper to saturated modulation range of the receiver. The TDC arrangement already enables submillimeter accuracy from moderate signal strengths.

(57) FIG. 10 shows the distance jitter (noise) of the TDC channel with the time measurement circuit according to the invention (top right curve) and the linear WFD channel (bottom left curve) in the case of single shot evaluation.

(58) At small signal amplitudes, the WFD displays better behavior than the TDC channel. In contrast, in the event of overload, the WFD channel no longer supplies usable results and the TDC channel is used here, the distance noise is consistently less than 0.4 mm at all degrees of the signal overload. Optionally, the distance measurement can be executed multiple times (accumulation, moving average, etc.), accuracies in the micrometer range can thus be achieved.

(59) It is obvious that these illustrated figures only schematically illustrate possible exemplary embodiments. The various approaches can also be combined with one another and with methods of the prior art.