Method and arrangement for controlling modulated lasers

Coherent light generators – Particular component circuitry – Having feedback circuitry

Reexamination Certificate

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C372S029015, C372S032000, C372S038020, C372S038070

Reexamination Certificate

active

06647040

ABSTRACT:

BACKGROUND OF THE INVENTION
1. Field of the Invention
The invention relates to a method for controlling modulated lasers,
in which an input signal of a laser is modulated by a pilot signal and this combined signal is emitted by the laser,
in which the light emitted by the laser is received by a receiver element, and
in which this received signal is evaluated and utilized to control the laser.
The invention also relates to an arrangement for carrying out this method.
2. Description of the Related Art
Modulated lasers are used, for example, for optical data transmission—both for free-space data transmission and for data transmission using optical fibers. The data is in this case sent, for example, using the time division multiplex method. In this method, a plurality of individual channels are transmitted in different time slots on the same transmission channel.
In all data transmission methods, it is important for the emitted light intensity, which is allocated to a digital value, to be within a predetermined tolerance range. Due to various effects (for example, the operating temperature or the ageing of the components used for the laser), a constant relationship between the input power and the output power cannot be presumed. It is therefore necessary to apply a control method, which changes the operating current of the laser so that the intensity of the output light stays within a defined range.
International patent document WO 98/43330 “Laser Modulation Control Method and Apparatus” dated Mar. 17, 1998 discloses that, for this purpose, a pilot tone is superimposed on the drive signal. In this case, the amplitude of the pilot tone is substantially less than the amplitude of the drive signal. Furthermore, the frequency of the pilot tone is also substantially less than the frequency of the drive signal. The light emitted by the laser is received by a monitor diode, and the signal component caused by the pilot tone is utilized to control the laser power. In this way, the average optical output power of the laser and the amplitude of the output power can be kept constant. Consequently, the intensity of the emitted light, which is allocated to a digital value, is constant.
Since the pilot tone has a comparatively small amplitude in relation to the drive signal, the evaluation can be significantly perturbed if the frequency of the pilot tone coincides with a main spectral line of the frequency spectrum of the drive signal. This problem can be avoided by suitable choice of the frequency of the pilot tone. Such a frequency can generally be determined if the frequency spectrum of the drive signal is known.
However, modern transmission systems are used under a wide variety of constraints. For example, the transmission rate is not predefined, but rather is matched to the current requirements. Furthermore, different data formats are also utilized for optical data transmission. This situation makes it difficult to determine a suitable frequency for the pilot tone, or even make pilot tone determination impossible if information about the drive signal is absent or lacking.
SUMMARY OF THE INVENTION
It is therefore an object of the invention to provide a method and an arrangement which simplify the control of modulated lasers.
This is achieved according to the invention by a method of the type mentioned in the introduction, in which the pilot signal has a frequency spectrum that is spread substantially uniformly at least over a section in the spectral operating range of the laser, especially in the spectral range of the input signal.
By applying such a pilot signal, the problem of effects due to individual spectral lines of the input signal can be substantially avoided in a particularly straightforward way. Only those signal components of the combined signal received by the receiver element which are attributable to the pilot signal then make a substantial contribution to the signal that is utilized to control the laser. To that end, for example, an equivalent measure of the pilot tone amplitude is determined from this signal component. Separation of the input signal and the pilot signal can then be achieved, for example, using correlation techniques. By choosing a suitable pilot signal, the cross correlation between the input signal and the pilot signal should then, in any event, be kept as small as possible. Such a signal sequence could be a pseudonoise sequence.
Such methods, which reduce any mutual influence of the signals by spreading the allocated frequency spectra, are also known by the term “spread spectrum systems”.
The amplitude of the pilot signal is ideally substantially less than the amplitude of the input signal. In this way, the optical transmission of the input signal is affected comparatively little by the superimposed pilot signal.
A particularly advantageous configuration of the invention provides a method in which a digital signal sequence is provided for the pilot signal. Such a signal sequence is, for example, a pseudonoise sequence that is chosen so that it has a small cross correlation with the input signal. By using a correlator for demodulation, the problem of effects due to individual spectral lines of the data signal can be substantially avoided. The evaluation in the correlator then involves, in principle, multiplying the signal received by the receiver element and the modulation signal. Only those signal components which are attributable to the pilot signal make a substantial contribution to the signal that is utilized to control the laser.
It is also advantageous if a pulse sequence is provided for the pilot signal. Pulses have a wide frequency spectrum that is spread substantially uniformly, so that they are very suitable for generating a pilot signal.
An advantageous variant of the invention is obtained if the time intervals between the individual pulses are spread pseudorandomly. This virtually precludes any correlation with the input signal. This method is also known by the term “time hopping”. In order to obtain the pilot signal from the combined signal received by the receiver element, the time intervals must also be taken into account in the receiver element.
It is particularly advantageous if the pilot signal is generated using feedback shift registers. These represent an established means for producing various digital signal sequences, for example for generating pseudonoise sequences. These sequences are then utilized both to modulate the input signal by the pilot signal and to demodulate the signal received by the receiver element. Apart from this embodiment variant, other methods from spread spectrum technology are also known in principle.
A favorable variant of the invention is obtained if an analog signal, especially an at least piecewise sinusoidal signal, is provided for the pilot signal. In this way, for example, existing circuits can be advantageously reused to generate a pilot tone. According to the prior art, analog signals can also be generated by digital circuits. Thus, a definitive distinction between pure digital technology and analog technology cannot be drawn in this context.
It is also favorable if the frequency of the pilot signal is progressively varied, especially by discontinuous frequency change. Discontinuous frequency changes are also known, for example, by the term “frequency hopping”. This frequency variation can be used to obtain a frequency spectrum with arbitrary width. An example of this is a wobble signal, which is a substantially sinusoidal signal whose frequency is varied progressively and constantly. In order to obtain the pilot signal from the combined signal received by the receiver element, the relevant instantaneous frequency of the pilot signal must also be taken into account in the receiver element.
A favorable configuration of the invention is obtained
if the average output power of the laser is determined from the signal received by the receiver element,
if the slope of the laser characteristic curve is determined from the signal received by the receiver element, and
if the laser output power allocated to a digi

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