Dynamic information storage or retrieval – Condition indicating – monitoring – or testing – Including radiation storage or retrieval
Reexamination Certificate
2003-06-11
2004-02-17
Huber, Paul W. (Department: 2653)
Dynamic information storage or retrieval
Condition indicating, monitoring, or testing
Including radiation storage or retrieval
C369S059110
Reexamination Certificate
active
06693864
ABSTRACT:
The invention relates to a method of recording at a recording speed an information signal on an information layer of a recording medium by irradiating the information layer by means of a radiation beam, said information layer having a phase reversibly changeable between a first state and a second state, which method comprises a write step for applying the radiation beam, in response to the information signal, to a first area of the information layer to cause the first area of the information layer to assume the first state, thereby forming a mark, and an erase step for applying a pulsed radiation beam to a second area of the information layer, before and after the mark, to cause the second area of the information layer to assume a state substantially identical to the second state, the pulsed radiation beam comprising erase pulses having an erase power level (P
e
) and a bias power level (P
b
) between the erase pulses.
The invention also relates to a recording device for recording at a recording speed an information signal on an information layer of a recording medium by irradiating the information layer by means of a radiation beam, said information layer having a phase reversibly changeable between a first state and a second state, the device comprising a radiation source for providing the radiation beam and control means for controlling the power of the radiation beam such that in response to the information signal the radiation beam is applied to a first area of the information layer to cause the first area of the information layer to assume the first state, thereby forming a mark, and such that a pulsed radiation beam comprising erase pulses having an erase power level (P
e
) and a bias power level (P
b
) between the erase pulses is applied to a second area of the information layer, before and after the mark, to cause the second area of the information layer to assume a state substantially identical to the second state.
A recording method of the kind set forth in the preamble is known from U.S. Pat. No. 5,291,470. A mark is written by a sequence of write pulses and the previously written marks between the marks being written are erased by applying a sequence of erase pulses. The write pluses are at a write power level (P
w
) and the erase pulse are at an erase power level (P
e
), the erase power level (P
e
) being lower than the write power level (P
w
). The power level between the write pulses as well as the erase pulses is a bias power level (P
b
). In general, this bias power level (P
b
) is set equal to the reading power level (P
0
).
The above method is known as a “pulsed erase” recording method as opposed to a recording method where the previously written marks between the marks being written are erased by applying a radiation beam having a constant erase power level. Because of this constant erase power level, the temperature of the information layer rises gradually. This temperature rise leads to erasure of not only marks in the actual track, but also of marks in adjacent tracks. This so-called “thermal cross-write” effect is reduced by applying the pulsed erase method.
It is a drawback of the “pulsed erase” recording method that it does not achieve sufficiently low jitter in the read signal obtained from reading marks recorded by using the “pulsed erase” method, especially when the marks are recorded at a variable recording speed. The jitter is the standard deviation of the time differences between level transitions in a digitized read signal and the corresponding transitions in a clock signal, the time difference being normalized by the duration of one period of said clock.
The recording speed may vary, for example, when recording at a Constant Angular Velocity (CAV). In this case the recording speed, i.e. the speed at which the recording medium moves relative to the spot of the radiation beam on the recording medium, increases when going from the center towards the periphery of a disc shaped recording medium. The recording speed is also known as the Linear Velocity.
It is an object of the invention to provide a method according to the opening paragraph for recording marks with reduced jitter while preventing “thermal cross-write” during erase.
This object is achieved by a method of the kind set forth which is characterized in that the bias power level (P
b
) depends on the recording speed.
When the bias power level (P
b
) is set at a fixed level no thermal cross write occurs while a minimal jitter of the recorded marks is obtained at a specific recording speed only. However, when the bias power level (P
b
) is set in dependence on the recording speed, minimal jitter of the recorded marks may be obtained for each recording speed while still preventing the occurrence of thermal cross write to occur.
A more optimum setting can be obtained by introducing additional degree of freedom in the settings for the sequence of erase pulses (i.e., a variable bias power level instead of a fixed one), resulting in a reduced jitter of the recorded marks.
A version of the method according to the invention is characterized in that the bias power level (P
b
) increases in a range between zero and the erase power level (P
e
) as the recording speed (V) increases.
During recording at a low recording speed the spot of the radiation beam on the recording medium will remain comparatively long in one specific area of the recording medium compared to recording taking place at a high recording speed. Therefore, during recording at a low recording speed the area on the recording medium will experience a significant temperature rise resulting in a significant thermal cross-write. This temperature rise, and hence the thermal cross write, is reduced when a low bias power level (P
b
) is used. However, during recording at a high recording speed the spot of the radiation beam on the recording medium will remain in one specific area of the recording medium for a comparatively short time only. Therefore, a higher bias power level (P
b
), even up to the erase power level (P
e
), may be used without introducing thermal cross write. Application of a high bias power level (P
b
) results in low jitter of the recorded marks.
A preferred version of the method according to the invention is characterized in that the bias power level (P
b
) increases in a range between zero and the erase power level (P
e
) as the recording speed (V) increases when the recording speed is below a chosen recording speed, and that the bias power level (P
b
) is substantially identical to the erase power level (P
e
) when the recording speed exceeds the chosen recording speed.
Beyond a certain recording speed no thermal cross write occurs, because the spot of the radiation beam on the recording medium remains only very briefly in one specific area of the recording medium. Beyond this recording speed the bias power level (P
e
) is set substantially equal to the erase power level (P
e
), resulting in a radiation beam having a constant erase power level. Because of this constant erase power level a. Jitter of the recorded marks is minimized.
A version of the method according to the invention is characterized in that the duty cycle of the erase pulses depends on the recording speed.
In addition to changing the bias power level (P
b
), the amount of energy transferred from the radiation beam to the recording medium, and hence the local temperature rise of the recording medium, can also be influenced by changing the duty cycle of the erase pulses. Both jitter of the recorded marks and thermal cross can both be minimized by setting the duty cycle of the erase pulses in dependency of the recording speed.
A version of the method according to the invention is characterized in that the duty cycle increases in a range between nearly zero and unity as the recording speed (V) increases.
During recording at a low recording speed, the spot of the radiation beam on the recording medium will remain comparatively long in one specific area of the recording medium compared to when recording takes place at a high recording speed. Therefore, during
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