METHOD OF RECORDING A BINARY SIGNAL ON AN OPTICALLY READABLE RECORD CARRIER AND APPARATUS FOR CARRYING OUT THE METHOD

Abstract: A method and apparatus are described for recording a binary information signal (Fig. 2a) on a record carrier (1) having an information layer (2) whose optical properties are modified upon heating. An information pattern corresponding to this information signal (Fig. 2a) is obtained in that the record carrier 1 is moved relative to an optical system (3) for focussing a radiation beam (4) on the information layer (2), a subsequent recording mark (5) being written on the information layer (2) in selected time intervals (τ) by locally heating the information layer by means of the radiation beam (4). The amount of radiation energy (E) applied in a selected time interval depends on the position of the selected time interval (τ) in the sequence of consecutive selected time intervals (τ). This provides compensation for the influence of the radiation energy (E) applied in the preceding time interval (τ) on the temperature at the location of the recording mark (5) to be written in the time interval (τ), so that for each recording mark (5) the temperature (T r ) which is reached in the information layer (2) and hence the size of the recording mark (5) is substantially the same.

Description: The invention relates to a method of recording a binary information signal on an optically readable record carrier comprising an information layer whose optical properties experience a change upon heating, in which method an information pattern corresponding to the information signal is formed on the information layer, which information pattern comprises recorded areas with modified optical properties and non-recorded areas with non-modified optical properties, the recorded areas being obtained in that a system for focussing a radiation beam on the information layer and the information layer are moved relative to each other, every subsequent recording mark of a sequence of consecutive and overlapping recording marks being formed by heating a target area with the aid of the radiation beam so as to bring about the change in optical properties in the target area. The invention further relates to an apparatus for carrying out the method comprising a radiation source, an optical system for focussing the radation produced by the radiation source on an information layer of a record carrier, the optical properties of said information layer being subject to a change upon heating, a drive means for moving the record carrier and the optical system relative to one another, and a control device for controlling the radiation source depending on a binary information signal, sequences of consecutive radiation pulses being obtained depending on the binary information signal in order to heat the information layer adequately to produce a recording mark having modified optical properties on the information layer. Such a method and apparatus are known from the Applicants U.S. Patent Specification US 4,473,829. In the known method and apparatus each recording mark is formed by means of one radiation pulse of constant energy content. The application of radiation energy results in a recording mark of substanially constant dimensions being formed on the information layer. This method is eminently suitable for the ablative recording of signals, the information layer at the location of the recording marks being removed as a result of the applied radiation energy. However, when this knwon method is used with information layers where the material at the location of the recording mark is not removed but where the brief temperature rise in the target area caused by the radiation energy gives rise to a change in optical properties of the material at the location of the recording marks, the dimensions of the recording marks are found not to be constant. An example of this is an information layer having an amorphous structure which changes into a cristalline structure upon heating. This variation in the dimensions of the recording marks results in distortion of the read signal obtained by reading the information pattern. From JP-A 60,247,827 an optical recording method and apparatus is known in which recording marks are produced with continuous radiation pulses. In order to improve the distortion in the read sigal, the intensity of the radiation pulse is increased at the beginning of each pulse. US-A-4 475 028 already discloses micromachining by laser in which the number of pulses is doubled at the beginning It is the object of the invention to provide a method and apparatus of the type defined in the opening paragraphs, which enable the record carrier to be provided with an information pattern which produces less distortion in the output signal obtained by reading. As regards the method this object is achieved in that the first recording mark of the sequence is formed by means of at least one preheating radiation pulse which after a predetermined time interval is followed by a writing radiation pulse, the writing radiation pulse producing a recording mark on the information layer and the energy content of the preheating radiation pulse being inadequate to produce the change in optical properties outside the area which is occupied by the recording mark produced by the writing radiation pulse. With respect to the apparatus this object is achieved in that the apparatus is adapted to generate as the first pulse of the sequence of radiaton pulses (p) a preheating radiation pulse being inadequate to produce the change in optical properties outside the area which is occupied by the recording marks produced by other radiation pulses of the said sequence. The invention is based on the recognition of the fact that when a recording mark is recorded the target area has already been preheated as a result of the preheating radiation pulse. As a result of this, the dimensions of the recording marks, which dimensions depend on the temperature which is reached in the target area, remain substantially constant. Consequently, the distortion of the read signal is minimal. This method in accordance with the invention has the advantage that the amount of radiation energy to be applied by means of the writing radiation-pulse can be limited. The dimensions of a recording mark in a method as defined in the opening paragraph, in which the recording marks are formed by changes in the optical properties of the material of the information layer are generally smaller than the dimensions of the recording marks formed by similar ablative recording methods. As a result of this, the resulting information pattern formed by recording marks with modified optical properties does not comply with the standards already established, for ablative recording. It is another object of the invention to provide an embodiment of the method in accordance with the invention which mitigates this drawback. This object is achieved by means of a method of recording a binary information signal on an optically readable record carrier comprising an information layer whose optical properties experience a change upon heating, in which method an information pattern corresponding to the information signal is formed on the information layer, which information pattern comprises recorded areas with modified optical properties and non-recorded areas with non-modifed optical properties, the recorded areas being obtainedin that a system for focussing a radiation beam on the information layer and the information layer are moved relative to each other, every subsequent recording mark of a sequence of consecutive and overlapping recording marks being formed by heating a target area with the aid of the radiation beam so as to bring about the change in optical properties in the target area, the information signal comprising bit cells, the number of consecutive bit cells of a first logic value being at least equal to n , n being an integer greater than or equal to 2, and an inscribed area corresponding to m bit cells, m being an integer greater than or equal to 2, being obtained by forming the sequence of overlapping recording marks by means of a radiation pulse at every instant of a series m-n+1 substantially equidistant instants, characterized in that the first recording mark of the sequence of overlapping recording marks is produced by means of at least two radiation pulses generated with time interval(s) smaller than the time intervals between the substantially equidistant instants at which the radiation pulses are generated for the productions of the subsequent recording marks of the overlapping recording marks. An apparatus for carrying out the method, comprises a radiation source, an optical system for focussing the radation produced by the radiation source on an information layer of a record carrier, the optical properties ofsaid information layer being subject to a change upon heating, a drive means for moving the record carrier and the optical system relative to one another, and a control device for controlling the radiation source depending on a binary information signal (Vi), sequences of consecutive radiation pulses (p) being obtained depending on the binary information signal comprising bit cells, the number of consecutive bit cells of a first logic value being at least equal to n , n being a integer greater than or equal to 2, for the production of an incribed area corresponding to a sequence of m bit cells the sequence of radiation pulses comprising m-n+1 radiation pulses at substantially equidistant time intervals, and is characterized in that the apparatus is arranged to generate at least one additional radiation pulse preceding the sequence m-n+1 radiation pulses, the time intervals between the additional pulse and the first radiation pulse of the sequence of m-n+1 radiation pulses being smaller than the time intervals between the m-n+1 radiation pulses Embodiments of the invention will now be described in more detail, by way of example with reference to Figures 1 to 16, in which Figure 1 illustrates the principle of recording binary signals on materials whose optical properties are modifiable by heating, Figure 2 and 6 illustrate prior-art methods of recording binary signals, Figures 4, 5, 7, 8 and 15 illustrate methods in accordance with the invention, Figures 9 and 16 show embodiments of an apparatus for carrying out the inventive method, Figure 10 shows an example of a radiation source suitable for use in the apparatus shown in Figure 9, Figure 11 shows a suitable example of the control device of Figure 9 for controlling the radiation source, Figure 12 shows a number of signals generated in the control device shown in Figure 11, Figures 13 and 14 show parts of the control device shown in Figure 11. Figure 1a shows a transparent record carrier 1 provided with an information layer 2 of a type whose optical properties can be modified by heating and subsequently cooling the information layer 2. Such an information layer 2 may consist of, for example, a material having an amorphous structure which can be converted into a crystalline structure by locally melting the information layer by applying heat and subsequently rapidly cooling the layer. Such a material may be, for example, an alloy of Te, Se and Sb. For a survey of such materials reference is made to G. Bouwhuis, J. Braat, A. Huyser, J. Pasman, G. van Rosmalen and K. Schouhamer Immink "Principles of Optical Disc Systems", Adam Hilger Ltd., Bristol 1985, pages 219-225. Further, Figure 1a shows an optical system 3 by means of which a radiation beam 4 produced by a radiation source, for example a laser beam, can be focussed to form a minute radiation spot (of the order of magnitude of 0.9 µ) on the information layer 2. The radiation source can generate a radiation pulse P whose energy content is adequate to heat the information layer to such an extent that changes in optical properties are brought about. Figure 1b is a plan view of the information layer 2 on which a recording mark 5 is formed by means of the radiation pulse P using the method described above. Figure 1c illustrates the distribution T of the temperature T r along the line 1 of the information 2 immediately after heating by the radiation pulse P. The line 6 represents the recording level T s above which the change in optical properties is obtained. The heat applied by means of the radiation pulse P spreads to the area surrounding the recording mark 5, causing the temperature at the location of the recording mark 5 to decrease and the temperature in the area surrounding the recording mark to increase. By way of illustration the temperature distribution within the information layer at two consecutive instants after application of the radiation pulse is indicated by T a and T b in Figure 1c. Figure 2a illustrates a bit sequence of a digital information signal comprising consecutive bit cells having a logic value "0" or "1". The signal shown here is encoded in such a way that the number of bit cells having a logic value "1" is at least equal to three. An example of such a coding is the EFM (Eight-to-Fourteen Modulation) described in Netherlands Patent Application 8004028 and which is used as a modulation for recording digital audio information on an optically readable disc in the Compact Disc Digital Audio System. As is described in said U.S. Patent Specification US 4,473,829 such an EFM encoded information signal can be recorded by forming an information pattern of recording marks 5 in the information layer 2, a sequence of three consecutive bit cells of the logic value "1" being represented by one recording mark 5 (see Figure 2c). A longer sequence of bit cells of the logic value "1" is represented by an area comprising a plurality of overlapping recording marks 5. Such a pattern of recording marks can be obtained by moving the record carrier 1 relative to the optical system 3 in the direction indicated by the arrow 7 (see Figure 1a) and by forming in each of the selected time intervals of a sequence of consecutive time intervals a recording mark 5 in the information layer by locally heating the information layer to a temperature above the recording level T s by means of a sequence of radiation pulses P with constant energy. In Figure 2e the radiation pulses P are designated P₁, ..., P₆, the index representing the sequence number of each radiation pulse in a sequence of consecutive radiation pulses P. For the second and subsequent radiation pulses P₂, ..., P₆ of the sequence of radiation pulses the temperature in the area where the next recording mark 5 is to be formed will already exceed the ambient value T o as a result of previous radiation pulses. These temperature rises are indicated by the levels T o1 , T o2 , T o3 , T o5 in Figure 2g. These levels increase asymptotically. The temperature distributions in the information layer are represented by T₁, ..., T₆ in Figure 2g, the index again representing the sequence number of the corresponding radiation pulse. The recording marks 5 thus obtained are shown in Figure 2f. Figures 2e-g illustrate the temperature variation T₁, T₂, ..., T₅ in the record carrier and the dimensions of the recording marks in the case that the energy content of each radiation pulse P is the same. In that case the temperature during the formation of the recording marks is not the same for all the recording marks 5, as a result of which the diameters of the recording marks 5 are not constant. When the information pattern comprising such recording marks of varying dimensions is read the read signal will be distorted. The amount of radiation reflected by a recording mark 5 is then not the same for each recording mark. Figure 3 and 4 illustrates the manner in which the amount of radiation energy applied in the selected time intervals τ can be varied using a method in accordance with the invention. In accordance with this method the radiation energy is administrered by applying unitary radiation pulses of constant energy content. Figure 3 illustrates the application of the radiation energy in the first selected time interval τ of a sequence of consecutive selected time intervals τ. In such a selected time interval τ the radiation energy is applied by means of radiation pulses P' and P, each having an intensity I s and a duration Δτ. Figure 4 illustrates the application of radiation energy in a time interval τ for the second and subsequent selected time intervals τ of a sequence of consecutive selected time intervals τ. The radiation energy is now applied by means of one unitary radiation pulse P. Figure 5 illustrates the temperature distribution T₁', T₁, ..., T₉ in the information layer immediately after application of the unitary radiation pulses P', P₁, ... P₉ in the situation that the radiation energy is applied by the above method using unitary radiation pulses in a sequence of nine consecutive selected time intervals τ₁, ..., τ₉. As is apparent from Figure 5, the preheating pulse P₁' is dimensioned in such a way that the temperature rise produced by this pulse is inadequate to bring the temperature of the information layer above the recording level T s . Therefore, this first unitary radiation pulse does not produce a change in the optical properties of the information layer 2. This is an advantage because the first recording mark 5 in a sequence of consecutive recording marks then does not become undesirably large. By way of comparison figures 6a and 6b give the temperature distributions T₁, ..., T₉ in the case that the radiation energy is applied in accordance with the prior-art method, which does not employ preheating pulses. It is apparent from Figure 6 that the variations in temperature in the information layer and hence the variations in the dimensions of the recording marks are large if no preheating pulse P₁′ is applied. In the ablative recording of EFM signals it is customary to use a 0.9µ diameter ratiation beam for recording the recording marks. For this diameter the dimension of the recording mark is found to be 1.1 µ. The dimension of this recording mark corresponds to a sequence of three bit cells of the logic vlaue "1". Sequences of 4 or more bit cells of the logic value "1" are obtained by extending the information pattern by 0.3 µ by each time forming a subsequent recording mark which overlaps the preceding recording mark. Such a ratio between the dimensions of the recording mark and the extensions yields an optimum duty cycle of the read signal obtained by reading the information pattern. When EFM signals are recorded on record carriers having information layers whose optical properties change the optimum diameter of the recording mark is frequently found to be smaller than in ablative recording with a radiation beam of the same diameter. If the diameter of the radiation beam used for recording on such record carriers is selected to be the same as in ablative recording, which may be desirable for reasons of standardisation, the diameters of the recording marks for the two recording methods are not the same, which means that the dimensions of the information patterns for the two recording methods will not be the same either. Hereinafter, a method in accordance with the invention will be described which by means of a radiation beam of the same diameter as in ablative recording enables an information pattern to be obtained which with respect to its dimensions complies with the above-described standard for the ablative recording of EFM signals. In accordance with this method two recording marks which overlap one another almost completely are formed in the first time interval τ of a sequence of consecutive selected time intervals τ, in such a way that the overall length of the two overlapping recording marks corresponds to the diameter of the optimum recording mark in ablative recording. Figure 7a illustrates a method of applying radiation energy, in which two overlapping recording marks are obtained in the first selected time intervals τ. In accordance with this method the radiation energy is applied by means of three radiation pulses P, P′, P″ of equal energy content, of which P′ serves as a preheating pulse and of which P and P″ serve as writing pulses. Figure 7b illustrates the application of the radiation energy for the second and subsequent selected time intervals τ of a sequence of consecutive selected time intervals τ. The radiation energy is now applied to the information layer 2 by means of only one unitary radiation pulse. Figure 8a shows the unitary radiation pulses P₁′, P₁″ and P₁, ..., P₉ which are generated in a sequence of nine consecutive selected time intervals τ ₁, ... τ ₉, the raidation energy being applied in the manner illustrated in Figure 7. Figure 8b illustrates the temperature distribution T₁′, T₁″, T₁, ..., T₉ in the information layer 2 immediately after application of the radiation pulses P′, P″, P₁, ..., P₉. In Figure 8c the area with modified optical properties formed in the first selected time interval of the sequence bears the reference numeral 10. The area 10 comprises two overlapping recording marks 5 produced by radiation pulses P₁″ and P₁. Another method in accordance with the invention will be described with reference to Figure 15, which method enables the afore-mentioned heat-sensitive information layers to be provided with an information pattern whose dimensions comply with the said standard for the ablative recording of EFM signals by means of a radiation beam of the same diameter as is customary in ablative recording. Figure 15a shows an EFM coded information signal comprising four consecutive bit cells of the logic value "1". An information pattern corresponding to this information signal can be written by means of the radiation pulses P**₁, P*₁, P*₂ and P*₃ shown in Figure 15b. The corresponding temperature differences T**₁, T*₁, T*₂ and T*₃ are given in Figure 15c. By means of the radiation pulses P*₁ and P*₁ and P*₂ two overlapping recording marks 5a and 5b are produced, the dimensions of the two overlapping recording marks corresponding to the optimum dimension for ablative recording. The radiation pulse P**₁ functions as a preheating pulse. It is to be noted that the preheating pulse P**₁ causes the temperature T**₁ of the information layer to rise to a level above the recording level T S . As a result of this, the optical properties of the information layer are modified within an area 50. However, this is not a problem if this area, as is shown, is so small that it is overlapped completely by the recording mark 5a. In that case the change in optical properties in the area∼ 50 does not influence the dimensions of the information pattern. By means of the radiation pulse P*₃ the recording mark 5c is recorded, the recording mark 5c overlapping the recording mark 5b to such an extent that the area with modified optical properties formed by the recording marks 5a, 5b and 5c corresponds to four bit cells of the logic value "1". The sequence of consecutive radiation pulses P**₁, P*₁, P*₂ and P*₃ can be obtained in that the first selected time interval T₁ of a sequence of consecutive selected time intervals two radiation pulses which are shifted relative to each other are generated at fixed instants t₁ and t₂ within the time interval τ₁ and in that subsequently in the second and subsequent selected time intervals τ₂, τ₃, ... each time a radiation pulse is generated at a fixed instant t₃ within each of these time intervals. Figure 9 shows an embodiment of an apparatus 20 for carrying out the inventive method. The apparatus 20 comprises a drive system 21 for rotating the disc-shaped information carrier 1. The optical system 3 is arranged opposite the information layer 2 of the rotating record carrier 1 to focus the radiation beam 4 originating from a light source 22 on the information layer 2. The radiation source 22 is of a type in which the intensity of the emitted radiation can be modulated by means of a control signal R s generated by a control device 23. The radiation source 22 may be, for example, a solid-state laser which can be turned on or off depending on the logic level of the control signal R s . Another suitable radiation source 22 is shown in Figure 10. The radiation source 22 comprises a laser 25 for continuously generating the radiation beam 4. The beam 4 is passed through an acousto-optic modulator 26 which is controlled by the control signal R S . The acousto-optic modulator 26 deflects or does not deflect the beam 4 depending on the logic level of the control signal, so that the beam 4 is transmitted to the optical system 3 depending on the control signal R S . Figure 11 by way of example shows a control device 23 for generating the control signal R S for the radiation source 22. The information signal V i (see Figure 12) is a binary signal in which the number of consecutive bit cells of the logic value "1" is at least equal to three, for example an EFM coded signal. The control device 23 comprises a memory 30 for the storage of the information signal V i to be recorded. The memory 30 is of a type which delivers the information signal V i on an output in synchronism with a clock signal c1′. Such a memory may be, for example, a shift register. The consecutive periods of the clock signal c1′ correspond to the said consecutive time intervals τ. The clock signal c1′ is derived from a clock signal c1 whose frequency is eight times as high by means of a 3-bit counter 31. Fig. 12 shows the signals c1, c1′ and V i as a function of time. The clock signal c1 is in synchronism with the speed of recording 1 in the area where the information signal V i is to be recorded. The manner in which the clock signal is derived falls beyond the scope of the present invention and is therefore not described. For this reference is made to the Applicant's Netherlands Patent Application no. 8000121, which comprehensively describes a method of deriving a speed-synchronous clock signal for the purpose of recording on an optically readable record carrier. The information signal V i supplied by the memory 30 is delayed by two periods of the clock signal c1′ by means of delay circuits 32 and 33, for example 1-bit shift registers controlled by the clock signal c1′. The delayed information signal V i ′ is shown in Figure 12. An AND gate 34 drives from the information signal V i and the delayed informatiion signal V i ′ a signal V s which indicates the selected time intervals in which a recording mark is to be formed. By means of a memory 35 in the form of a flip-flop which is clocked by a clock signal c1′ the signal V s is stored for one time interval τ. By means of an AND gate 36 a signal V g1 is derived from the signals V s and V s ′, to indicate that the selected time interval τ indicated by V s is preceded by selected time interval τ. By means of an inverter circuit 37 and AND gate 38 a signal V g2 is derived from the signals V s and V s ′ to indicate that the selected time interval τ indicated by V s is preceded by a non-selected time interval τ. By means of a circuit 39 two control signals R₁ and R₂ are derived from the count of the 3-bit counter 31. The signal R₁ represents the control signal for the radiation source 22 in each first selected time interval τ of a sequence of consecutve selected time intervals τ. The signal R₂ repre sents the control signal for the radiation source 22 in each second and subsequent selected time interval of each sequence of consecutive selected time intervals τ. If the signal V g2 indicates that a recording mark is to be written in a first one of a sequence of selected time intervals the control signal R₁ is transferred to the radiation source 22 by means of an AND-gate 40 and an OR-gate 42. If the signal V g₂ indicates that a recording mark is to be written in a second or subsequent time interval of a sequence of selected time intervals τ the control signal R₂ is transferred to the radiation source 22 by means of an AND-gate 41 and the OR-gate 42. The control signals R₁ and R₂ shown in Figure 12 comprise pulses of constant duration, in such a way that for R₁ three unitary pulses are generated in each time interval τ and for R₂ only one unitary pulse is generated in each time interval τ. The control signals R₁ and R₂ may be derived from, for example, the counts of the counter 31 by means of the circuit 39 shown in Figure 13, which circuit comprises a gate circuit 50 for generating three signals S₁, S₂ and R₂ depending on the count of the counter 31. The relationship between the consecutive counts A₀, ..., A₇, the output signals Q₁, Q₂ and Q₃ of the counter 31 and the output signals S₁, S₂ and R₂ is given in the following Table 1. count Q₁ Q₂ Q₃ S₁ S₂ R₂ A₀ 0 0 0 1 0 0 A₁ 0 0 1 0 0 0 A₂ 0 1 0 0 1 0 A₃ 0 1 1 0 0 0 A₄ 1 0 0 0 0 1 A₅ 1 0 1 0 0 0 A₆ 1 1 0 0 0 0 A₇ 1 1 1 0 0 0 The signals S₁, S₂ and R₂ are applied to an OR-gate 51 on whose output the signal R₁ is generated. Figure 14 shows another example of the circuit 39 for generating control signals R₁ and R₂, a control pulse of a first width being generated for the signal R₁ in each time interval τ and a control pulse of a second width smaller than the first width being generated for the signal R₂ in each time interval. For this purpose the circuit comprises two monostable multivibrators 52 and 53 which each generate pulses of different widths in response to a 0-1 transition of the output signal Q₁ of the counter 31. Figure 16 shows an embodiment of an apparatus for carrying out the method illustrated in Figure 15, the elements of the apparatus corresponding to those in Figure 14 bearing the same reference numerals. In Figure 16, instead of the signal V i and the signals V i ′ delayed by two clock periods of c1′, the signal V i and the signal V ia , which has been delayed by one clock period of c1′ are applied to the AND-gate 34. In the embodiment shown in Figure 16 the output signal V sa , which indicates the selected time intervals τ, becomes "1" during (s-1) time intervals for each sequence of s (s being an integer) consecutive bit-cells of the logic value "1". During the first selected time interval of the sequence represented by the signal V sa the output signal R 1a is transferred to the radiation source 22 by the circuit 39a. During the second and subsequent selected time intervals of each sequence of selected time intervals the signal R 2a is supplied. The signals R 1a and R₂₁ can be derived from the count of the counter 31 in the same way as is illustrated, for example, in Figure 13. The relationship between R 1a , R 2a and the output signals Q₁, Q₂ and Q₃ of the counter 31 is given in the following Table 2. count Q₁ Q₂ Q₃ R 1a R 2a A₀ 0 0 0 0 0 A₁ 0 0 1 1 0 A₂ 0 1 0 0 0 A₃ 0 1 1 0 1 A₄ 1 0 0 1 0 A₅ 1 0 1 0 0 A₆ 1 1 0 0 0 A₇ 1 1 1 0 0 The control device described in the foregoing generates only control signals of two different types for the radiation source 22. It is obvious that in a similar way control signals of a larger number of different types can be generated. In the foregoing the invention has been described, by way of example, for an EFM-coded information signal. For such an information signal the dimensions of the recording mark in a selected time interval correspond to a sequence of 3 bits of the same type. Longer bit sequences of the same type are then obtained by forming overlapping recording marks. The inventive method provides compensation for temperature effects caused by the radiation energy applied in preceding time intervals. Such temperature effects also occur when recording information signals in which the length of the recording mark corresponds to a length other than three bits, for example one bit. It is obvious that the invention can readily be applied to such cases. The invention is described for an information layer of a material whose structure can be modified from amorphous to crystalline by heating. It will also be obvious to those skilled in the art that the invention can also be utilized with other materials whose optical properties can be modified by heating, for example materials in which the application of heat initiates a chemical reaction which results in a change in optical properties, or with materials used in thermomagnetic recording. For a survey of these materials reference is made to pages 219-225 of the afore-mentioned book "Principles of Optical Disc Systems".

Claims: A method of recording a binary information signal on an optically readable record carrier (1) comprising an information layer (2) whose optical properties experience a change upon heating, in which method an information pattern corresponding to the information signal is formed on the information layer (2), which information pattern comprises recorded areas with modified optical properties and non-recorded areas (5) the recored areas being obtained in that a system for focussing a radiation beam (4) on the information layer (2) and the information layer (2) are moved relative to each other, every subsequent recording mark (5) of a sequence of consecutive and overlapping recording marks being formed by heating a target area with the aid of the radiation beam (4) so as to bring about the change in optical properties in the target area, characterized in that the first recording mark of the sequence is formed by means of at least one preheating radiation pulse (p₁** in Fig 15) which after a predetermined time inverval is followed by a writing radiation pulse (p₁*), the writing radiation pulse producing a recording mark (5a) on the information layer and the energy content of the preheating radiation pulse being inadequate to produce the change (50) in optical properties outside the area which is occupied by the recording mark (5a) produced by the writing radiation pulse (p₁*). A method of recording a binary information signal on an optically readable record carrier (1) comprising an information layer (2) whose optical properties experience a change upon heating, in which method an information pattern corresponding to the information signal is formed on the information layer (2), which information pattern comprises recorded areas with modified optical properties and non-recorded areas with non-modifed optical properties, the recorded areas being obtained in that a system for focussing a radiation beam on the information layer and the information layer are moved relative to each other, every subsequent recording mark (5) of a sequence of consecutive and overlapping recording marks (5) being formed by heating a target area with the aid of the radiation beam so as to bring about the change in optical properties in the target area, the information signal comprising bit cells, the number m of consecutive bit cells of a first logic value being at least equal to n , n being an integer greater than or equal to 2, a first inscribed area being obtained by forming a first sequence of overlapping recording marks (5) by means of a radiation pulse at every instant of a series m-n+1 substantially equidistant (τ) instants, characterized in that a second inscribed area consisting of a single recording mark preceding and overlapping the first area is produced by means of at least two radiation pulses (p**, p₁* in Fig 15; P', P", P in Fig 8) generated with time interval(s) smaller than the time intervals between the substantially equidistant instants at which the radiation pulses are generated for the productions of the subsequent recording marks (5b, 5c) of the overlapping recording marks, the first and second areas corresponding to m bit cells. An apparatus for carrying out the method as claimed in Claim 1, comprising a radiation source (22), an optical system (3) for focussing the radation produced by the radiation source (22) on an information layer (2) of a record carrier (1), the optical properties of said information layer (2) being subject to a change upon heating, a drive means (21) for moving the record carrier (1) and the optical system relative to one another, and a control device (23) for controlling the radiation source depending on a binary information signal (Vi), sequences of consecutive radiation pulses (p*) being obtained depending on the binary information signal in order to heat the information layer adequately to produce a recording mark having modified optical properties on the information layer, characterized in that the apparatus is adapted to generate as the first pulse of the sequence of radiaton pulses (p) a preheating radiation pulse (p₁**) being inadequate to produce the change in optical properties outside the area which is occupied by the recording marks (5) produced by other radiation pulses (p*) of the said sequence. An apparatus for carrying out the method as claimed in Claim 1, comprising a radiation source (22), an optical system (3) for focussing the radation produced by the radiation source (22) on an information layer (2) of a record carrier (1), the optical properties of said information layer (2) being subject to a change upon heating, a drive means (21) for moving the record carrier (1) and the optical system relative to one another, and a control device (23) for controlling the radiation source depending on a binary information signal (Vi), sequences of consecutive radiation pulses (p) being obtained depending on the binary information signal comprising bit cells, the number m of consecutive bit cells of a first logic value being at least equal to n , n being an integer greater than or equal to 2, for the production of a first incribed area the sequence of radiation pulses comprising m-n+1 radiation pulses at substantially equidistant time intervals, characterized in that the apparatus is arranged to generate at least one additional radiation pulse (p₁**) preceding the sequence m-n+1 radiation pulses (p₁), the time intervals between the additional pulse and the first radiation pulse of the sequence of m-n+1 radiation pulses being smaller than the time intervals between the m-n+1 radiation pulses (p₁*, p₂*) in order to inscribe a second area preceding and overlapping the first area, the first and second areas corresponding to m bit cells.

Inventors: FARLA, MARTIN ANDREW JACQUES PATRICK, VAN TONGEREN, HENDRICUS FRANCISCUS JOANNES JACOBUS
Applicants: N.V. PHILIPS' GLOEILAMPENFABRIEKEN
Application year: 1987
Main classification: G11B7
IPC codes: G11B7, G11B11