The present invention relates to a method and a corresponding device for transforming a first set of write parameters of a write strategy for recording marks in an information layer of a record carrier by irradiating the information layer with a pulsed radiation beam at a first recording speed into a second set of write parameters of said write strategy for recording marks at a second recording speed. The present invention further relates to a recording device for recording marks in an information layer of a record carrier by irradiating the information layer by means of a pulsed radiation beam, each mark being written by a sequence of one or more write pulses according to a write strategy.
The present invention is especially suitable for use with a record carrier comprising an information layer having a phase that is reversibly changeable between a crystal phase and an amorphous phase, generally known as a phase-change layer. Such a phase-change layer is often applied in optical record carriers of the rewritable type such as, for example, CD-RW and DVD-RW discs. A recording operation of optical signals is performed in such a manner that the recording material in the layer is reversibly changed in phase between an amorphous phase and a crystalline phase by changing the irradiation conditions of a radiation beam, so as to record the signals in the phase-change layer as a pattern of marks. A playback operation of the recorded signals is performed by detecting differences in optical properties between the amorphous and crystalline phases of the phase-change layer, so that the signals are reproduced. Such a phase-change layer allows information to be recorded and erased by modulation of the power of the radiation beam between a write power level, an erase power level, and a bias power level.
Recording speed is the main performance factor in optical recording. For CD-RW the basic standard is defined for the speed range 1× to 4× (1× being the standard scanning velocity of a CD Digital Audio disc of approx. 1.2 m/s), while the High-Speed CD-RW standard has a range from 4× to 10×. In September 2002, version 1.0 of the latest Ultra-Speed CD-RW standard was released defining CD-RW discs for speeds up to 24×, including also reservations for 32× and higher speeds (Recordable Compact Disc Systems, Part III: CD-RW, Volume 3: Ultra-Speed, Version 1.0, September 2002). To achieve these higher recording speeds, use has to be made of a so-called 2T write strategy as defined in the Ultra-Speed CD-RW standard. Therein, basically one write pulse is used for every two clock cycles of a reference clock (one clock cycle being indicated as T). This is done to obtain sufficient cooling times between two consecutive write pulses and thereby to avoid recrystallization, which is a problem especially with faster phase-change materials. A consequence of such a 2T write strategy is that consecutive even and odd marks are written with an identical number of write pulses, for example 3 pulses for both a 6T and a 7T mark.
A method and a recording device for recording marks in an information layer of an optical record carrier using a 2T write strategy have been described in European patent application 02 080 394.6 (PHNL021391EPP). The described method and recording device solve the problem of how to record marks in an information layer when no write parameter settings specifically tuned to the record carrier to be recorded are available for use in the 2T write strategy, or when the record carrier cannot be identified. Preferred settings for the write parameters of a 2T write strategy are proposed.
An important aspect of the 2T write strategy is the choice of the write parameters that define the difference between even and odd marks written with an identical number of write pulses. Even marks are generally recorded in a straightforward way by applying a pulse-train with a multi-pulse length Tmp and a cooling gap Tc. To record a corresponding odd mark with a length of (length of even mark+1T), the pulse-train may be modified in three positions; an elongation of the penultimate gap (Δ1g), of the last pulse (Δ1p), and of the last cooling gap (Δ2), wherein Δ1g=Δ1p=Δ1 according to the Ultra-Speed CD-RW standard. Moreover, the shortest mark length I3 is defined by three special parameters, the pulse length T3, the gap length Tc3, and the shift of the leading edge dT3.
When implementing such a 2T write strategy it has been observed that the recording jitter is very sensitive to a large number of the write parameters. Consequently, these parameters have to be tuned very accurately. A problem is that the optimal parameter settings may be different for different recording speeds. Due to the limited rotation speed of the disc in the drive, the maximum recording speed is achieved at the outer radius of the disc; the recording speed on the inner part of the disc is normally lower. In the case of Ultra-Speed CD-RW, the maximum speed can be 24× or 32× (at present) or even higher (in the future), whereas at the inner part of the disc typically 16× (or 20×) recording speed is achieved. Thus, the recording speed is increased in a drive from the inside to the outside of the disc, for example in a constant angular velocity (CAV) mode, in a P-CAV mode (partial CAV mode) in which the first part is written in a CAV mode and the second part is written in a constant linear velocity (CLV) mode at the maximum recording speed of the disc, or in a Z-CLV mode (zoned CLV mode) in which the recording speed is increased in a number of discrete steps. Therefore, when the recording speed changes, new optimal sets of write parameters have to be determined for every recording speed.
It is therefore an object of the present invention to provide a method and a corresponding device for transforming a first set of write parameters of a write strategy, which are tuned to a first recording speed, into a second set of write parameters of said write strategy, which are tuned to a second recording speed, without reducing the recording performance or the quality of the recorded marks and while avoiding an increase of unwanted jitter as much as possible.
This object is achieved according to the present invention by providing a method as claimed in claim 1, wherein the duration of the write pulses is kept substantially constant in time, and the duration of a complete sequence of write pulses for recording a mark is kept substantially constant as a fraction of the reference clock.
A corresponding device that is adapted for carrying out the method is defined in claim 9, said device comprising input means for receiving a first set of write parameters and an information about said first and second recording speed, first transforming means for keeping the duration of the write pulses constant in time, second transforming means for keeping the duration of a complete sequence of write pulses for recording a mark constant as a fraction of the reference clock, and output means for outputting a second set of write parameters.
The present invention proposes a scheme for scaling write strategies for different recording speeds. If the parameter settings are known or predetermined at a given recording speed, they can be directly scaled to a different recording speed. The write performance at this target speed yields at least an acceptable recording performance. Adapting, in a further step, the recording power or other write parameters may of course further optimize the recording performance.
The present invention is based on the idea of distinguishing two fundamental classes of write parameters. One class of write parameters is related to the individual write pulses, the other class is related to the duration of the complete pulse train for a certain effect length. The relevant time scale for the first class, that is the write pulses, is an absolute time scale (i.e. in ns). The write parameter settings belonging to this category are kept constant in absolute time for the different recording speeds. In other words, write parameters of this category are changing on a relative time scale (duty cycle) when the recording speed is changed. The relevant time scale for the write parameters not directly related to the write pulses is a relative time scale (i.e. relative to the reference clock). These parameters are kept constant as a fraction of the reference clock when the recording speed is changed.
The absolute time scale is important for the write pulses because it defines the energy dissipated in the information layer of the disc, and thus the temperature profile. It has to be realized that the displacement of the optical spot during a write pulse is much smaller than the optical spot size, even at high speeds. Therefore, a write pulse of a certain absolute duration will typically melt the same area in the information layer of the disc, regardless of the recording speed. Keeping all write pulses constant in time will achieve a similar recording result at all recording speeds, applying typically the same write power.
Embodiments of the invention are defined in the dependent claims. In an embodiment it is proposed that an even mark having a time length of nT, where n represents an integer value equal to 4, 6, 8 or 10 and T represents the length of one period of the reference clock, is written by a sequence of n/2 write pulses, whereas an odd mark having a time length of nT, where n represents an integer value equal to 5, 7, 9 or 11, is written by a sequence of (n−1)/2 write pulses, and that a mark having a time length of 3T is written by a single write pulse.
Thus, a 2T write strategy as defined in the Ultra-Speed CD-RW standard is employed according to the present invention. However, it should be noted that the present invention can generally be applied to other 2T write strategies, 1T write strategies or even mT write strategies (where m is larger than 2) as well. The speed scaling for a 2T write strategy is difficult because there are two series of runlengths, i.e. odd effects and even effects. The problem is that there is always an odd effect that is written with the same number of write pulses as a corresponding even effect; for example, 4T and 5T marks are both written with two write pulses. Now, the 2T write strategy must be tuned to give as a result either a 4T or a 5T mark. However, as soon as some recording parameters change, for example the recording speed, the resulting mark lengths may behave differently for odd and even marks. In the case of a 1T write strategy this problem is less dramatic; the marks are written with (n−1) write pulses, therefore there are never two marks written with an identical number of write pulses.
According to a further embodiment it is proposed that a last write pulse in the sequence of write pulses for writing an odd mark is a period Δ1 longer than a last write pulse in the sequence of write pulses for writing an even mark, and a gap preceding the last write pulse in the sequence of write pulses for writing an odd mark is a period Δ1 longer than a gap preceding the last write pulse in the sequence of write pulses for writing an even mark.
It is thus preferred that the period Δ1 is kept constant in time when the second set of write parameters for a second recording speed is determined. Preferably, said period Δ1 is within a range from 1 to 5 ns, in particular within a range from 2 to 4 ns. An exemplary value for Δ1 is 3.6 ns. If too small a value for Δ1 is used, the cooling gaps of the odd marks have to be made much longer than the cooling gaps of the even marks because the 1T difference has to be put somewhere in the pulse train of the write pulses. As a result the effect shapes are really different, which increases jitters. If too high a value for Δ1 is used, the last odd mark will be relatively long, which causes recrystallization since the cooling is not good enough to deal with the increased energy, resulting again in higher jitters.
Preferred ranges for the write parameters to be kept constant in time, and preferred substantial values for these parameters are defined in claim 5.
According to a further embodiment of the invention, a mark having a time length of 3T is written by a single write pulse having a time length T3′−dT3, the start of which is delayed by a period of dT3 relative to the start of write pulses for writing an even or odd mark, and which is a period of Δ3−dT3 longer than the write pulses for writing an even mark. When the write pulse for writing a 3T mark is prolonged by a time period Δ3 having a fixed time duration with respect to the duration of a single write pulse, a good sequence for writing a 3T mark is obtained. It should be noted that dT3, as defined in the above-mentioned Ultra-Speed CD-RW standard, may have a positive or a negative value. It is defined as a delay in the Ultra-Speed CD-RW standard.
Parameters defining the length of the complete write pulse train for a certain mark length are defined as a fraction of the reference clock. The preferred choice is to define the parameters Θeven, Θodd and Θ3 as the beginning of the erase pulse at the end of a write pulse sequence relative to the nominal write pulse; that is, for a mark of length nT the erase power level starts (n−Θ)T after the beginning of the mark.
According to another embodiment of the invention it is thus proposed that the duration of a complete sequence of write pulses for writing a mark having a time length of nT, where n represents an integer value equal to 4, 6, 8 or 10, is equal to (n−Θeven)T, the duration of a complete sequence of write pulses for recording a mark having a time length of nT, where n represents an integer value equal to 5, 7, 9 or 11, is equal to (n−Θodd)T, and the duration of the single write pulse and the subsequent cooling gap for recording a mark having a time length of 3T is equal to (3−Θ3)T, wherein said values of Θeven, Θodd, and Θ3 are kept constant as a fraction of the reference clock T.
The reason for introducing this new set of Θ-parameters is that a certain mark length will always be written with a certain pulse train length, such as an I6 mark which will always be written with a pulse train of about 6T length. This basic rule holds in fact at any recording speed. Therefore, it can be expected that the related Θ-parameters are not changed substantially when the recording speed is changed. It should be noted that the Θ-parameters are strongly coupled. In general the differences between the Θ-parameters should be very small, preferably smaller than 2/8T.
Preferred ranges and preferred substantial values for the Θ-parameters are defined in claim 8. It should be noted that these parameters are dependent on other parameters, such as the time length of a normal write pulse and the period Δ1.
The present invention is preferably applied in a recording device comprising a radiation source for providing the radiation beam, a control unit operative in controlling the power of the radiation beam and in providing the sequences of pulses for recording the marks, a selection unit operative in selecting and/or controlling the recording speed, and a transformation device for transforming a first set of write parameters of a 2T write strategy for recording marks at a first recording speed into a second set of write parameters of said 2T write strategy for recording marks at a second recording speed according to the method as claimed in claim 1.
This means that during operation a new set of write parameters can be determined (almost) in real-time when the recording speed is changed, for example when at first data is recorded at the inner side of a disc and subsequently data is recorded at the outer side of a disc. This may be used to advantage, for example, when data is recorded in a constant angular velocity mode or in a partial constant angular velocity mode, where the inner part of the disc is recorded in a constant angular velocity mode and the outer part of the disc is recorded in a constant linear velocity mode, as is most often used by present day drives.
According to another embodiment the recording device further comprises a storage means for storing at least two sets of write parameter settings for recording marks at different recording speeds, wherein said transformation device is further operative in selecting the corresponding set of write parameters from said storage means according to the selected recording speed. It is thus possible that two or more sets of write parameters for different recording speeds are determined in advance, for example the recording speeds typically used by the recording device during recording, and that during operation the appropriate write parameters settings are selected in accordance with the applied recording speed.
The transformation of the write parameters can thus be done in the drive itself during or before the recording of data, for example when a new disc for recording of data is inserted, or alternatively by the manufacturer of the drive, who then stores the different sets of write parameters in the recording device, for example in a look-up table. Thus, the invention can be used for (almost) real-time scaling in the device itself, or for scaling during drive development.
The invention will now be explained in more detail with reference to the accompanying drawings in which
The control signals are used to control the power of the radiation beam, where it is assumed that the power of the radiation beam is proportional to the corresponding level of the control signal. A mark is recorded by a sequence of pulses having a write power level Pw and having a bias power level Pb in between the pulses. Previously recorded marks between the marks being recorded are erased by applying an erase power level Pe.
Since a 2T write strategy is used, the even marks having a time length of nT are recorded by a sequence of n/2 pulses, and the odd marks having a time length of nT are recorded by a sequence of (n−1)/2 pulses. This results in a 4T even mark and a 5T odd mark being recorded by a sequence of 2 pulses, a 6T even mark and a 7T odd mark being recorded by a sequence of 3 pulses, a 5T even mark and a 9T odd mark being recorded by a sequence of 4 pulses, and a 10T even mark and a 11T odd mark being recorded by a sequence of 5 pulses, as is indicated by the dashed lines in
Furthermore, parameters defining the length of the complete pulse train for a certain mark length are defined. A parameter Θeven is defined for control signal 200 for writing even marks, and a parameter Θodd is defined for control signal 201 for recording odd marks, both being defined as the beginning of the erase power level following the pulse train relative to the nominal mark length, that is, for a mark of length nT, the erase power level Pe starts (n−Θ)T after the beginning of the mark.
The power of the radiation beam 32 is controlled by a control signal SC provided by a control unit 62, where it is assumed that the power of the radiation beam 32 is proportional to the corresponding level of the control signal SC. Examples of such a control signal SC have been shown in
The patterns of the pulses and the gaps between the pulses in the control signal SC are based on a set of write parameters W1′, W2′ related to the applied 2T write strategy. These write parameters W1′, W2′ are provided to the control unit 62 by an output unit 614 of a transformation device 61. In this set of write parameters, the first subset W1′ indicates write parameters which are kept constant in time when they are determined by a first transformation unit 612 from the corresponding subset of write parameters W1 (adapted to a first, e.g. default, recording speed R) according to a new recording speed R′. The second subset W2′ indicates write parameters which are constant as a fraction of the reference clock T when they are determined from the corresponding previous subset of write parameters W2 (adapted to said first, e.g. default, recording speed R) by a second transformation unit 613 according to the new recording speed R′.
The information regarding the initial (first) recording speed R and the new (second) recording speed R′ is received by input means 611 of the transformation device from a selection unit 60 which is adapted for selection and/or control of the recording speed of the motor 34. The selection and/or control of the recording speed is based, for example, on an identification of the record carrier 31, which identification may be based, for example, on a media identifier stored on the record carrier 30. The selection unit 60 may be further adapted for control of the recording speed according to a constant angular velocity mode, a partial constant angular velocity mode, or a zoned constant linear velocity mode, the recording speed being adapted to the position on the information layer 301 where data is to be recorded. Thus, the recording speed can be continuously modified during recording or can be modified in steps if particular recording speeds are assigned to particular areas on the medium 30.
A first, or default, set of write parameters W comprising the subsets W1, W2 is further obtained by the input unit 611 from a storage unit 63. This storage unit 63 stores at least one set of write parameters adapted for a particular recording speed in a default storage unit 632. All other sets of write parameters for different recording speeds are determined by the transformation device 61 from this default set of write parameters. This determination preferably takes place online and in real-time when the recording speed is changed by the selection unit 60. This means that these sets of write parameters are determined by the recording device just before actual recording is performed, based on the recording mode to be applied or based on an identification of the recording speeds which will be applied for recording data on this particular record carrier 30.
However, it is alternatively possible that different sets of write parameters for different recording speeds are stored in a look-up table 631, so that in response to a change in recording speed the appropriate set of write parameters W′ is selected from this look-up table 631 and immediately provided to the control unit 62 by the output means 614 of the transformation device 61 without the need for any transformation. The different sets of write parameters stored in the look-up table 631 can thus be provided by the manufacturer of the recording device, who preferably determines these sets of write parameters using a similar or same transformation device 61.
To scale write strategies to different recording speeds, a basic set of write parameters is required to start from. A good starting point is, for example, the default set of write parameters at 16× recording speed such as, for example, the set of write parameters described in European patent application 02080394.6 (PHNL021391EPP). This set of write parameters may also serve as a starting point in an actual drive because the maximum speed at the inner radius is typically 16× for CD-RW. These write parameters can be scaled to 24× and 8×, respectively.
Using this starting point it has been found that at 16× the mark and space lengths are well distributed and within the specified range and that all space and all mark data-to-data jitters (standard deviation of a certain mark length measured in time domain/length of one clock period T) are low, typically 9%. The write power used is 36 mW, as an example. This relates to all effect lengths, i.e. to the recording of 3T to 11T marks.
To obtain the set of write parameters for 24× in a first step, the 16× write parameters are directly scaled as described above, that is, the pulse type parameters (Tmp, T3′, dT3, Δ1) are kept constant in time and the theta parameters (Θodd, Θeven, Θ3) are kept constant as a fraction of the clock. Furthermore, the same writing power as at 16× is used. The mark jitters remain low (typically 9%) and also the mark length distribution is acceptable. The space jitter is slightly increased to 11-12%, which is still within the specified range of 15%. Thus, the write performance after direct scaling to 24× without any parameter changes yields a good writing performance. Optionally, in a second step, the performance can be further improved by adjusting the write power or the write parameters in a fine tuning operation which will not be described in more detail here.
A typical scaling application is to scale to a higher speed as described above. In some cases a scaling to lower speed may also be useful, for example when the write performance at a certain speed is not acceptable and recording at lower speed might yield acceptable results. As an example, the 16× write parameters may be scaled to 8× write parameters. Without any parameter and write power changes, the resulting recording performance was found to be excellent.
Typical write parameters used for 8×, 16× and 24× are listed in the following Table:
In this Table, the write parameters for 24× and 8× are obtained from the write parameters at 16×. Values indicated by bold numbers are kept constant on an absolute or relative time scale, respectively. This experiment was done from 16×, 24×, and 8×, because 16× is exactly between 8× and 24×. Scaling to either lower or higher recording speeds can be useful in practice, especially in a drive development environment. Furthermore, 8× is also a practically important speed since drives in laptops usually start at 8× at the inner radius of the disc.
The parameters described above are a suitable set for understanding the physics of the recording process. For a practical application, write parameters as defined in the Ultra-Speed CD-RW standard are often preferred. The relations between the write parameters described above and the write parameters as defined in the standard are:
In general, write parameters are implemented in a drive as subdivisions of the write clock T. This is the natural choice for the relative time scale, thus the scaling of these parameters is straightforward. However, the write parameters scaled on the basis of the absolute time scale may need to be matched to the subdivision available in a specific device.
Number | Date | Country | Kind |
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03102278.3 | Jul 2003 | EP | regional |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/IB04/51245 | 7/16/2004 | WO | 1/23/2006 |