KR20090031660A - Jitter detecting method and apparatus - Google Patents
Jitter detecting method and apparatus Download PDFInfo
- Publication number
- KR20090031660A KR20090031660A KR1020087018754A KR20087018754A KR20090031660A KR 20090031660 A KR20090031660 A KR 20090031660A KR 1020087018754 A KR1020087018754 A KR 1020087018754A KR 20087018754 A KR20087018754 A KR 20087018754A KR 20090031660 A KR20090031660 A KR 20090031660A
- Authority
- KR
- South Korea
- Prior art keywords
- signal
- circuit
- mask
- binarization
- jitter
- Prior art date
Links
Images
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R29/00—Arrangements for measuring or indicating electric quantities not covered by groups G01R19/00 - G01R27/00
- G01R29/02—Measuring characteristics of individual pulses, e.g. deviation from pulse flatness, rise time or duration
- G01R29/027—Indicating that a pulse characteristic is either above or below a predetermined value or within or beyond a predetermined range of values
- G01R29/0273—Indicating that a pulse characteristic is either above or below a predetermined value or within or beyond a predetermined range of values the pulse characteristic being duration, i.e. width (indicating that frequency of pulses is above or below a certain limit)
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R29/00—Arrangements for measuring or indicating electric quantities not covered by groups G01R19/00 - G01R27/00
- G01R29/26—Measuring noise figure; Measuring signal-to-noise ratio
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B19/00—Driving, starting, stopping record carriers not specifically of filamentary or web form, or of supports therefor; Control thereof; Control of operating function ; Driving both disc and head
- G11B19/20—Driving; Starting; Stopping; Control thereof
- G11B19/28—Speed controlling, regulating, or indicating
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B20/00—Signal processing not specific to the method of recording or reproducing; Circuits therefor
- G11B20/10—Digital recording or reproducing
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B20/00—Signal processing not specific to the method of recording or reproducing; Circuits therefor
- G11B20/10—Digital recording or reproducing
- G11B20/10009—Improvement or modification of read or write signals
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B20/00—Signal processing not specific to the method of recording or reproducing; Circuits therefor
- G11B20/10—Digital recording or reproducing
- G11B20/10009—Improvement or modification of read or write signals
- G11B20/10018—Improvement or modification of read or write signals analog processing for digital recording or reproduction
- G11B20/10027—Improvement or modification of read or write signals analog processing for digital recording or reproduction adjusting the signal strength during recording or reproduction, e.g. variable gain amplifiers
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B20/00—Signal processing not specific to the method of recording or reproducing; Circuits therefor
- G11B20/10—Digital recording or reproducing
- G11B20/10009—Improvement or modification of read or write signals
- G11B20/10037—A/D conversion, D/A conversion, sampling, slicing and digital quantisation or adjusting parameters thereof
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B20/00—Signal processing not specific to the method of recording or reproducing; Circuits therefor
- G11B20/10—Digital recording or reproducing
- G11B20/10009—Improvement or modification of read or write signals
- G11B20/10046—Improvement or modification of read or write signals filtering or equalising, e.g. setting the tap weights of an FIR filter
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B20/00—Signal processing not specific to the method of recording or reproducing; Circuits therefor
- G11B20/10—Digital recording or reproducing
- G11B20/10009—Improvement or modification of read or write signals
- G11B20/10046—Improvement or modification of read or write signals filtering or equalising, e.g. setting the tap weights of an FIR filter
- G11B20/10055—Improvement or modification of read or write signals filtering or equalising, e.g. setting the tap weights of an FIR filter using partial response filtering when writing the signal to the medium or reading it therefrom
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B20/00—Signal processing not specific to the method of recording or reproducing; Circuits therefor
- G11B20/10—Digital recording or reproducing
- G11B20/10009—Improvement or modification of read or write signals
- G11B20/10305—Improvement or modification of read or write signals signal quality assessment
- G11B20/10314—Improvement or modification of read or write signals signal quality assessment amplitude of the recorded or reproduced signal
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B20/00—Signal processing not specific to the method of recording or reproducing; Circuits therefor
- G11B20/22—Signal processing not specific to the method of recording or reproducing; Circuits therefor for reducing distortions
- G11B20/225—Signal processing not specific to the method of recording or reproducing; Circuits therefor for reducing distortions for reducing wow or flutter
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
- G11B7/004—Recording, reproducing or erasing methods; Read, write or erase circuits therefor
- G11B7/005—Reproducing
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R31/00—Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
- G01R31/28—Testing of electronic circuits, e.g. by signal tracer
- G01R31/317—Testing of digital circuits
- G01R31/31708—Analysis of signal quality
- G01R31/31709—Jitter measurements; Jitter generators
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B20/00—Signal processing not specific to the method of recording or reproducing; Circuits therefor
- G11B20/10—Digital recording or reproducing
- G11B20/14—Digital recording or reproducing using self-clocking codes
- G11B20/1403—Digital recording or reproducing using self-clocking codes characterised by the use of two levels
- G11B20/1423—Code representation depending on subsequent bits, e.g. delay modulation, double density code, Miller code
- G11B20/1426—Code representation depending on subsequent bits, e.g. delay modulation, double density code, Miller code conversion to or from block codes or representations thereof
- G11B2020/1442—8 to 12 modulation
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B20/00—Signal processing not specific to the method of recording or reproducing; Circuits therefor
- G11B20/10—Digital recording or reproducing
- G11B20/14—Digital recording or reproducing using self-clocking codes
- G11B20/1403—Digital recording or reproducing using self-clocking codes characterised by the use of two levels
- G11B20/1423—Code representation depending on subsequent bits, e.g. delay modulation, double density code, Miller code
- G11B20/1426—Code representation depending on subsequent bits, e.g. delay modulation, double density code, Miller code conversion to or from block codes or representations thereof
- G11B2020/1461—8 to 14 modulation, e.g. the EFM code used on CDs or mini-discs
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B2220/00—Record carriers by type
- G11B2220/20—Disc-shaped record carriers
- G11B2220/25—Disc-shaped record carriers characterised in that the disc is based on a specific recording technology
- G11B2220/2537—Optical discs
- G11B2220/2562—DVDs [digital versatile discs]; Digital video discs; MMCDs; HDCDs
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B2220/00—Record carriers by type
- G11B2220/20—Disc-shaped record carriers
- G11B2220/25—Disc-shaped record carriers characterised in that the disc is based on a specific recording technology
- G11B2220/2537—Optical discs
- G11B2220/2579—HD-DVDs [high definition DVDs]; AODs [advanced optical discs]
Abstract
The present invention provides an improved jitter detection device capable of performing jitter detection.
The jitter detecting device for this purpose includes a receiving circuit 1 for receiving a signal, a determining circuit 3 for determining a signal portion used for jitter detection in the received signal based on the signal amplitude, and the determined signal portion. And jitter detection circuit 5 for detecting jitter related to the signal. The determination circuit 3 uses a first threshold setting circuit for generating a first threshold value, a second threshold setting circuit for generating a second threshold value, and the first and second threshold values for a period of time. A period signal generation circuit for generating a signal may be included, and the jitter detection circuit 5 may include a signal portion detection circuit for detecting a signal portion by responding to a received signal according to the period signal.
Description
This application claims the priority based on Japanese Patent Application No. 2006-180702 of a "method and apparatus for detecting jitter" of the application on June 30, 2006, The specification, drawings, claims The entire beginning disclosure is incorporated into the text.
The disclosed embodiment relates to a method and apparatus for detecting jitter in a signal.
Conventionally, reading of data recorded on an optical disc such as a CD or a DVD is performed by digitalizing a reproduction signal from the optical disc and binarizing the reproduction signal from the optical disc, for example, as disclosed in Japanese Patent Laid-Open No. 2004-295965. This is done by detecting the length of each mark or space. In the binarization for data reading, for example, the median value of the peak peak of the reproduction signal is usually used as the slice level for the reproduction signal from the conventional DVD shown in Fig. 1 (b). The detection of jitter in the digital signal from the optical disk thus detected is also performed using the same slice level as the data detection. That is, using the slice level which is the intermediate value of the peak peak of the reproduction signal, the reproduction signal from the DVD is binarized, for example, the length of each mark / space in the digital signal after binarization is detected, and the variation in this length is varied. Jitter is measured by examining. For example, in the case of a DVD, there is a mark / space having a period of 3T to 11T and 14T. Here, T is equal to one period of the clock used for the DVD. In this way, by measuring the jitter in the signal from the optical disk, the quality of the optical disk itself was checked or the optical axis of the optical beam in the optical pickup was adjusted.
Recently, as an optical disc, a new optical disc standard such as HD (High-Definition) DVD has emerged. In such an optical disc, the recording density is further increased as compared with the conventional DVD. For example, in HD DVD, an ETM code (Eight to Twelve Modulation Code) is used, and the reproduction signal therefrom is a waveform as shown in Fig. 1A. As can be seen when comparing with the reproduction signal from the DVD using the conventional EFM code of Fig. 1 (b), there are some smaller components of the signal amplitude, and the components with the smallest amplitude peak near the slice level. Have This is because the higher the recording density, the lower the signal amplitude due to inter-signal interference, and the higher the linear density, the lower the signal amplitude. For example, at the shortest 2T mark or the length of the space, the peak p of the signal amplitude is near the slice level. In the case of reading data from an optical disc causing such a reproduction signal, in the binarization method using a slice level as in the prior art, many identification errors occur even in the vicinity of the slice level, so that stable data detection is difficult. Therefore, in the HD DVD standard, it is decided to use a PRML (Partial Response and Maximum Likelihood) signal processing method as a data reading method. Accordingly, the reproduction signal evaluation method is also evaluated not by jitter but by SbER (Simulated Bit Error Rate) and PRSNR (Partial Response Signal to Noise).
However, in the method of evaluating such SbER and PRSNR, since a large number of samples is required in comparison with the jitter measurement, the real time is low as compared with the method using a conventional slice level. For this reason, in the production site of the optical disc related products, an adjustment operation such as an optical axis adjustment step of the optical pickup is required, but in such an adjustment operation, a constant number of samples preset for evaluation by SbER or PRSNR is required for each fine adjustment. There is a problem that the adjustment takes time. This also causes a problem that the production efficiency as a whole product is lowered.
Various aspects and embodiments described below will be described and described with respect to devices, circuits, and methods, but these are merely illustrative and are not meant to limit the scope. In various embodiments, one or more of the above problems are alleviated or eliminated, but there are other embodiments for use for other improvements.
In one embodiment, the jitter detection method includes a step of receiving a signal, a determination step of determining a signal portion used for jitter detection in the received signal based on a signal amplitude, and based on the determined signal portion And detecting jitter in the signal.
In another embodiment, the jitter detection device includes a reception circuit for receiving a signal, a decision circuit for determining a signal portion used for jitter detection in the received signal based on a signal amplitude, and the above determination. And a jitter detection circuit for detecting jitter related to the signal based on the signal portion.
In addition to the exemplary embodiments and aspects described above, other embodiments and aspects will become apparent to those skilled in the art upon reviewing the following description with reference to the drawings.
1 (a) is a diagram showing a waveform example of a reproduction signal from an HD DVD;
1B is a diagram showing an example waveform of a reproduction signal from a DVD;
2 is a block diagram showing the configuration of a jitter detection device according to one embodiment;
FIG. 3 is a diagram showing a relationship between various signal components included in an HD DVD playback signal, and slice levels, upper threshold values, and lower threshold values thereof.
FIG. 4 is a diagram for explaining, in principle, a method of determining a signal portion used for jitter detection in an HD DVD playback signal, in which (a) shows the case of clear crossing; FIGS. 4 (b-1) and (b). -2) is a figure showing a case of a return type non-clear crossing, 4 (c-1) and (c-2) is a figure showing a case of a non-return type non-clear crossing,
FIG. 5 is the same view as FIG. 4, wherein (d) shows a case where non-return non-clear crossing is continuous.
6 is a block diagram showing a jitter detection device of one embodiment incorporating the determination principle described in FIGS. 4 and 5;
7 is a timing diagram showing signal waveforms of respective units in the apparatus of FIG. 6;
FIG. 8 is a timing diagram showing signal waveforms of respective parts in the apparatus of FIG. 6 in the case where the non-return type non-clear crossing shown in FIG. 5 occurs continuously; FIG.
9 is a flowchart of a program for realizing the same function as that performed by the
FIG. 10 is a block diagram showing another embodiment of the jitter detection circuit in the jitter detection device shown in FIG. 2;
FIG. 11 is a block diagram showing another embodiment of the jitter detection circuit in the jitter detection device shown in FIG. 2;
12 is a diagram showing a jitter measuring device having a jitter detecting device of one embodiment;
FIG. 13 is a diagram illustrating an electronic device including the jitter detection device of one embodiment. FIG.
Next, various embodiments will be described in detail with reference to the drawings.
2 is a block diagram showing the configuration of a jitter detection device according to one embodiment. As shown in the drawing, the jitter detecting device includes a
More specifically, the signal
Here, with reference to FIG. 3, those upper threshold value THU and lower threshold value THL are demonstrated. For example, assuming that the received signal is a reproduction signal from an HD DVD, the reproduction signal becomes a waveform as shown in FIG. 3, for example. At this time, when the intermediate value of the peak peak of the reproduction signal is set to zero level, the reproduction signal includes signal components c1 to c13 having positive (+) or negative (-) peaks. Here, in the waveform example shown, the component having the largest positive or negative peak is c1, c2, c5, c13, and the component having the next lowest peak is c8, and the component having the lower peak is c4, c11, and the minimum peak components are c3, c6, c7, c9, c10, c12.
In this case, assuming that the illustrated zero level is binarized as the slice level, the component having the smallest peak has a very high probability of generating an identification error in c3, c6, c7, c9, c10, and c12. Moreover, the probability of the identification error of the component adjacent to these minimum peak components also increases. For example, considering the component c3, the identification error of the mark / space length occurring in the component c3 directly affects the data length in the adjacent components C2 and C4, so that the probability of the identification error is also reduced. Increases. Therefore, in the jitter detection device of one embodiment, the jitter detection of the signal is performed based on the signal portion where the occurrence probability of the identification error of the mark / space length is not high. For this reason, identification of the part with a high probability of occurrence of an identification error and the part which is not, based on signal amplitude is performed. As an example, the upper threshold value THU and the lower threshold value THL are determined for the zero level to determine a signal portion where the probability of identification error is not high, and the slice level is zero level as in the conventional jitter detection method. As a result, a method of binarizing and detecting jitter is employed. Thereby, high speed similar to the conventional jitter detection method can be realized.
Here, the setting method of the upper threshold value THU and the lower threshold value THL will be described in more detail. For example, if these thresholds are set at the positions of the dotted lines, the components (c3, c6, c7, c9, cl0, c12) of the minimum peak and components other than this can be identified in this case. Further, for example, if the upper threshold value THU is set at the positions THU 'and THL' indicated by a dashed-dotted line, the signal portion including the minimum peak component and the components having the next lowest peak (c4, c1l) and the same Other parts can be identified. In the example of the reproduction signal from the HD DVD, when the component of the shortest mark / space length of 2T is excluded from the determination object, those thresholds are larger than the peak of the 2T component but smaller than the peak of the next long 3T component. Level, for example, THU and THL. When not only 2T but also 3T or longer periods, for example, 5T components are to be excluded, the threshold is larger than the peak of 5T, but smaller than the peak of the 6T component, for example, THU 'and THL'. You can set it at the same level. Thus, the magnitude | size of an upper threshold value and a lower threshold value can be set to predetermined value, or it can continuously change according to the periodic component to be excluded from a determination object.
Next, referring to Figs. 4 and 5, the principle of the determination method of the signal portion used for jitter detection will be described using an HD DVD playback signal as an example. In this example, the threshold value is set for the purpose of eliminating the shortest signal component of 2T. In these figures, the waveform of a signal related to a coded signal (data recorded on an optical disc), a waveform of a reproduction signal from the optical disc below it, and a threshold used for determination is shown at the top. First, Fig. 4 (a) shows an example of "clear crossing" in which the reproduction signal crosses the slice level to clear on both sides, and (b-1) and (c-1) show the slice level on both sides. An example of "non-clear cross" intersecting with non-clear is shown. The example of crossing the slice level on the negative side is shown in Figs. 4B-2 and 4-2 for the case of non-clear crossing. Incidentally, "cross to clear" or "clear cross" means that the occurrence of the identification error is not high, and "cross to non-clear" or "non-clear cross" is the probability of occurrence of identification error. It is used as showing the intersection in this high state.
Referring first to Fig. 4A, when components of a period longer than 2T are continuous, for example, the slice level crosses the clear at the time t2 from both sides to the negative side, and a clear crossing point cr1 occurs. In this case, the probability of occurrence of identification error at the position crossing the slice level is low. Here, the "upper threshold crossing" signal rises when the reproduction signal crosses the upper threshold THU when the reproduction signal changes from zero level to both sides, and changes from both sides to the zero level side to cross the threshold value. It is said to descend. On the other hand, the "lower threshold crossing" signal rises when the reproduction signal crosses the lower threshold THL when the reproduction signal changes from the zero level to the more negative side, and changes from the negative side to the zero level side to cross the threshold value. It is said to descend. The "upper mask" signal is a signal for excluding a signal portion having a high probability of identifying error, and is mainly a signal generated based on an upper threshold value, while the "lower mask" signal has a similar probability of identifying error. As a signal for excluding this high signal portion, the signal is mainly generated based on the lower threshold. In the case of the clear crossing of Fig. 4A, the reproduction signal crosses the lower threshold on the opposite side at a predetermined time, for example, at time t3 within a time of 2T, at the time t1 when the upper threshold crosses the upper threshold. In this case, since the probability of identification error occurrence is not high, it stops low because neither the upper nor the lower mask needs to be generated.
On the other hand, as shown in Fig. 4B-1, when one 2T component continues after a periodic component longer than 2T, the reproduction signal passes the upper threshold on both sides, but crosses the slice level, A non-clear crossover occurs, returning from the vicinity and returning to both sides without reaching the lower threshold. That is, the non-clear crossing points cr2 and cr3 are continuous. In this case, it is called a "return type" non-clear crossing because it enters both sides and exits the slice level. At this time, when the upper threshold crossing signal becomes low, the lower threshold crossing signal does not become high within the time of 2T. In this case, since a portion having a high probability of identifying error occurs and enters from the upper side with respect to the slice level, the upper mask signal rises high to start the mask signal. In this way, it is possible to distinguish between the clear crossing of (a) and the non-clear crossing of (b-1) by whether the lower threshold crossing signal becomes high within the time of 2T. In addition, although FIG.4 (b-1) showed about the case of one 2T component, it is suitable also in the other cases where an odd number of 2T components are continued.
On the other hand, as shown in Fig. 4 (c-1), when two 2T components are continued after a periodic component longer than 2T, the reproduction signal passes the upper threshold on both sides and near the slice level. A non-clear crossing occurs that changes and passes through the lower threshold after repeating the slice level crossing. That is, the non-clear crossing points cr4, cr5, cr6 and cr7 are continuous. In this case, since it enters into the slice level from both sides and goes out to the negative side, it is called "non-returning" non-clear crossing. At this time, the lower threshold crossing signal does not become a high level within the time of 2T from the time when the upper threshold crossing signal becomes low, but becomes high after the passage of the 2T time. Also in this case, since a portion having a high probability of identifying error occurs and enters from the upper side with respect to the slice level, the upper mask signal rises high to start the mask signal. In this way, it is possible to distinguish between the clear crossing of (a) and the non-clear crossing of (c-1) by whether the lower threshold crossing signal becomes high within the time of 2T.
In the case of Fig. 4 (b-1) and (c-1), the mask signal once started is continued until a clear crossover as shown in Fig. 4 (a) occurs, and immediately before the slice level is crossed. For example, it terminates at the time which crosses an upper threshold (t1 of FIG. 4 (a)). Thereby, all the periodic components affected by the identification error which arise in the shortest periodic component can be excluded from a jitter determination object. Specifically, in the case of Fig. 4 (c-1), since two 2T periodic components are followed by a periodic component cx longer than 2T, the clear intersection point cr8 at t5 in this periodic component cx is continued. This is happening. However, the clear crossover here is from the negative side to the both side, which is opposite to the polarity of the regeneration signal immediately before the mask is started. Therefore, when the upper mask is terminated at the time t4 immediately before t5, the regeneration signal of the masked result is obtained. Since? Causes a state change immediately after the time t4, the slice level crossing due to the mask occurs. The slice level crossing due to such a mask does not have to occur in jitter detection. Therefore, in Fig. 4C-1, the mask is terminated at the same polarity side, that is, at the threshold crossing time of both sides, for example, at t6 or t7. However, the condition is that clear crossover as shown in Fig. 4A occurs immediately after t7. In addition, in FIG.4 (c-1), although the case where two 2T components are continued is shown, the case where even number other than two is continued is similarly suitable.
Next, Fig. 5 (d) shows that when a non-return type non-clear crossing is continuous, that is, two components having a length longer than 2T are continued after two consecutive 2T components, and then two 2T components are continued again. The case is shown. In this case, unlike in the case of Fig. 4 (c-1), the clear intersection is between the four consecutive non-clear crossing points cr10 to cr13 and the next four non-clear crossing points cr14 to cr17. It does not occur and the clear crossing point cr18 occurs at t10 following the latter clear crossing point. Also in this case, after the upper mask signal becomes high at t8, the same clear crossover as in FIG. 4 (a) occurs at t10, and therefore remains high until immediately before t9.
In addition, although not shown in the figure, in the case where the return-type non-clear crossing is continuous, it can be dealt with by processing in the same manner as in FIG. 4 (b-1).
Next, with reference to FIG. 6, the jitter detection apparatus of one Embodiment which actualized the determination principle demonstrated in FIG. 4 and FIG. 5 is demonstrated. As shown, this jitter detecting apparatus corresponds to the receiving
In detail, the
Next, the details of the
Next, the upper mask generator 304 includes a
The OR gate 3044 then receives the lower threshold crossing signal CTHL on one input, receives the lower mask signal MSL from the F /
Next, the F /
The next mask generator 308 includes an
Next, with reference to FIG. 7, the operation | movement of the
Next, in the case of the non-return type non-clear crossing, since this case starts from both sides, it is necessary to generate an upper mask. That is, when the delay upper threshold crossing signal CTHUD falls at t14, the upper mask prohibition signal INHU is low (the lower threshold crossing signal CTHL is low at its fall at t14) and the mask is masked. Since the generation is not prohibited, the upper mask MSU is started high. Thereafter, the next drop of the delay upper threshold crossing signal CTHUD occurs at time t16, but at this time, the upper mask prohibition signal INHU is high [the lower threshold crossing signal CTHL is high at t16] and the mask is Since the generation is prohibited, the upper mask MSU is turned low to terminate the upper mask. The last return non-clear crossing 2 has the same polarity as the return non-clear crossing 1 described earlier, but generates the upper mask in the same operation. At the time t15, the delay lower threshold crossing signal CTHLD falls. At this time, the lower mask prohibition signal INHL becomes high. This is because the upper threshold crossing signal CTHU is high at time t15.
Next, with reference to FIG. 8, the operation | movement in the case where a non-return type non-clear crossing occurs continuously is demonstrated. In this case, the same operation as the time point t14 of the non-return type non-clear crossing in FIG. 7 occurs at the time point t20, and the upper mask MSU becomes high. Also in the case of the example of FIG. 8, at a time point t21 corresponding to the time point t15 of FIG. 7, the delay lower threshold crossing signal CTHLD falls. At this time, the lower mask prohibition signal INHL becomes high. The reason is that at t21, the upper threshold crossing signal CTHU is low, but unlike the example of Fig. 7, the upper mask signal MSU is high. For this reason, generation | occurrence | production of the lower mask is prohibited, and the lower mask MSL is as it is. Subsequent operations are the same as those in FIG. As described above, while one of the upper mask and the lower mask is generated, the other mask is unnecessary, and thus the occurrence of the mask is prevented.
The mask signal generated as described above generates the mask signal MST in timing with the binarization signal SB by the
Next, with reference to the flowchart of FIG. 9, the method of realizing the
Next, in
Next, the lower threshold crossing variable CTHL is generated from the lower threshold variable THL in
Next, in
Next, in
Similarly, the lower mask is set in
By repeating the operation described above for each sample of the HD DVD playback signal, the operation described in Figs. 6, 7 and 8 can be realized.
Next, another embodiment of the jitter detection circuit shown in FIG. 2 will be described with reference to FIG. 10. In FIG. 6, the
Next, another embodiment of the jitter detection circuit shown in FIG. 2 will be described with reference to FIG. 11. This embodiment differs from the jitter detection circuit in the embodiment of FIG. 6 in that it receives the mask signal, not the latch, but the
Next, with reference to FIG. 12, the jitter measuring apparatus provided with the jitter detection apparatus of one Embodiment mentioned above is demonstrated. The jitter measuring device includes a display / output section that receives a jitter determination output from the jitter detecting device. The output from the jitter detection device can take a form in accordance with the display form or output form in the display / output section. For example, the jitter determination output may be in the form of performing statistical processing on the width of each mark / space length, or in the form of performing statistical processing on the difference between the edge of the mark / space and the edge of the clock as described above. . The display / output unit outputs the received jitter determination output to an output device such as a display or a printer according to a user's selection. According to this embodiment, the jitter-related adjustment work required at the production site of the optical disc related products such as HD DVD can be further speeded up.
Finally, referring to FIG. 13, an electronic device including the jitter detection device of the above-described embodiment will be described. As the electronic device, optical disc related devices such as an optical pickup, an optical disc driver, an optical disc player, and the like are included. If the device uses the PRML signal processing technology, other devices such as a communication device are also included. By providing the jitter detection device of the above-described embodiment in such an electronic device, jitter processing for removing the influence of jitter in the electronic device can be realized at a higher speed or with a simpler circuit configuration.
As mentioned above, some embodiment was described in detail. However, the jitter detection device of the above embodiment can be similarly applied not only to recording media such as HD DVD, but also to jitter detection of signals from other information recording media using the same signal format as HD DVD, for example, magnetic disks. . As described above, the jitter detection device of the above embodiment can be applied to signals from other fields in which the PRML method is used, for example, communication media such as communication lines and networks.
While various exemplary aspects and embodiments have been described in detail above, various changes, substitutions, additions, and subcombinations are recognized by those skilled in the art. Accordingly, the interpretation of the claims set forth in the appended claims and the claims that may be included in future claims are intended to cover all such modifications, substitutions, additions, subcombinations, etc., as fall within the true spirit and scope. Intended to be done.
Claims (19)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2006180702A JP2008008811A (en) | 2006-06-30 | 2006-06-30 | Method and device for detecting jitter |
JPJP-P-2006-00180702 | 2006-06-30 |
Publications (1)
Publication Number | Publication Date |
---|---|
KR20090031660A true KR20090031660A (en) | 2009-03-27 |
Family
ID=38845341
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
KR1020087018754A KR20090031660A (en) | 2006-06-30 | 2007-05-28 | Jitter detecting method and apparatus |
Country Status (5)
Country | Link |
---|---|
JP (1) | JP2008008811A (en) |
KR (1) | KR20090031660A (en) |
CN (1) | CN101375170A (en) |
TW (1) | TW200809790A (en) |
WO (1) | WO2008001570A1 (en) |
Families Citing this family (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN108318809B (en) * | 2017-01-16 | 2020-09-01 | 奇景光电股份有限公司 | Built-in self-test circuit for frequency jitter |
JP2022174652A (en) * | 2021-05-11 | 2022-11-24 | 株式会社アドバンテスト | Measuring device and measuring method |
CN113434097A (en) * | 2021-05-17 | 2021-09-24 | 厦门汉印电子技术有限公司 | Printer, detection control method and device thereof, and computer-readable storage medium |
Family Cites Families (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0783979A (en) * | 1993-09-16 | 1995-03-31 | Advantest Corp | Jitter analyzer with time window trigger function |
JPWO2003088221A1 (en) * | 2002-04-03 | 2005-08-25 | 松下電器産業株式会社 | Optical information apparatus, optical storage medium, optical storage medium inspection apparatus, and optical storage medium inspection method |
-
2006
- 2006-06-30 JP JP2006180702A patent/JP2008008811A/en not_active Abandoned
-
2007
- 2007-05-28 CN CNA2007800037080A patent/CN101375170A/en active Pending
- 2007-05-28 KR KR1020087018754A patent/KR20090031660A/en not_active Application Discontinuation
- 2007-05-28 WO PCT/JP2007/060821 patent/WO2008001570A1/en active Application Filing
- 2007-06-11 TW TW96121024A patent/TW200809790A/en unknown
Also Published As
Publication number | Publication date |
---|---|
CN101375170A (en) | 2009-02-25 |
TW200809790A (en) | 2008-02-16 |
JP2008008811A (en) | 2008-01-17 |
WO2008001570A1 (en) | 2008-01-03 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US7092462B2 (en) | Asynchronous servo RRO detection employing interpolation | |
KR100694125B1 (en) | Frequency detector in Phase Locked Loop circuit and frequency error detecting method | |
US5625632A (en) | Magnetic disk drive including a data discrimination apparatus capable of correcting signal waveform distortion due to intersymbol interference | |
JP3711140B2 (en) | Information recording / reproducing apparatus and signal evaluation method thereof | |
KR20090031660A (en) | Jitter detecting method and apparatus | |
US7321531B2 (en) | Apparatus for reproducing data from optical storage medium using multiple detector | |
KR20070007927A (en) | Dc-controlled encoding for optical storage system | |
JP2005011506A (en) | Binary data detecting device and method | |
JP3395734B2 (en) | Playback device | |
US7791991B2 (en) | Information reproducing apparatus, information reproducing method, information reproducing program, and information recording medium | |
JP2006338781A (en) | Code discriminating circuit | |
JP3395716B2 (en) | Digital signal reproduction device | |
JP2009527069A (en) | Signal quality evaluation apparatus and method, and optical disk driver | |
JP5612657B2 (en) | Signal quality measuring apparatus and method | |
JP2002260346A (en) | Reproducing device | |
JP4131213B2 (en) | Playback apparatus and program | |
JP2817899B2 (en) | Information playback device | |
JP4106703B2 (en) | Disc signal analyzer | |
KR100739792B1 (en) | Viterbi decoder and viterbi decoding method | |
JP2001006287A (en) | Digital signal reproducing device | |
JP2009015906A (en) | Synchronous pattern detecting device and method of frequency error detecting device, and information processor | |
US8699160B2 (en) | Methods and apparatus for validating detection of RRO address marks | |
JP2002352512A (en) | Digital signal reproducing apparatus | |
JP2008262611A (en) | Decoding method, decoding device and information reproduction device | |
JP2008135139A (en) | Method and device for detecting frequency error, and optical disk drive |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
WITN | Withdrawal due to no request for examination |