• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    The invention relates to an arrangement (100) for data transmission comprising a transmitter (1) and a receiver (2) connected to the transmitter (1) via an optical channel (3), the transmitter (1) having a transmitter laser (13) and comprises a transmitter-side electroabsorption modulator (10) connected downstream of the transmitter laser (13), the optical output (11) of the transmitter-side electroabsorption modulator (10) forming the output of the transmitter (1) and being coupled to the optical channel (3), and wherein the transmitter (1) has an electrical data input which is connected to the electrical modulation connection (12) of the transmitter-side electroabsorption modulator (10), - wherein the receiver (2) has a receiver laser (23) and a receiver-side electroabsorption modulator (20) connected downstream of the receiver laser (23) comprises, wherein the optical output (21) of the receiver-side electroabsorption modulator (20) forms the input of the receiver (2) and to the optical channel al (3) is coupled, and wherein the receiver (2) has an electrical data output which is connected to the electrical modulation connection (22) of the receiver-side electroabsorption modulator (20), - the transmitter laser (13) and the receiver laser (23) through Specification of a physical variable, in particular by specifying the laser current (IL) or the laser temperature (Temp), can be detuned, - with a transmitter-side control unit (14) and a receiver-side control unit (24) being provided, which use the respective physical variable for detuning the respective Lasers (13, 23), - the transmitter-side control unit (14) and the receiver-side control unit (24) being synchronized with one another, and - the transmitter-side control unit (14) and the receiver-side control unit (24) at their output (15, 25) ) each specify the same signal for defining the physical quantity for defining the laser frequency.
    公开号:AT522381A4
    申请号:T50374/2019
    申请日:2019-04-25
    公开日:2020-10-15
    发明作者:
    申请人:Ait Austrian Institute Tech Gmbh；
    IPC主号:
    专利说明:

    Devices for transmitting data or signals, each comprising a laser and an electro-absorption modulator, are known from the prior art. The light emitted by the laser is weakened by the electroabsorption modulator so that the light is present in modulated form at the output of the electroabsorption modulator and transmitted to a receiver via an optical waveguide
    can.
    In order to enable coherent detection of the transmitted signal in such an arrangement, a precise correspondence between the laser frequency of the transmitter and that of the receiver is required. However, due to, for example, reflection of light at discontinuities in the optical channel, the signal transmitted via the optical channel can be partially superimposed, which leads to a deteriorated detection of the signal at the receiver.
    The object of the invention is therefore to provide a remedy in this regard and to provide an arrangement and a method which prevent crosstalk of the received signal, for example due to discontinuities in the optical channel
    minimize.
    The invention solves this problem with an arrangement for data transmission comprising a transmitter and a receiver connected to the transmitter via an optical channel. According to the invention, it is provided that the transmitter comprises a transmitter laser and a transmitter-side electro-absorption modulator connected downstream of the transmitter laser, wherein the The optical output of the transmitter-side electroabsorption modulator forms the output of the transmitter and is coupled to the optical channel, and the transmitter has an electrical data input that is connected to the electrical modulation connection of the transmitter-side electroabsorption modulator, - the receiver has a receiver laser and a receiver-side electroabsorption modulator connected downstream of the receiver laser includes,
    The invention also relates to a method for data transmission between a transmitter
    and a receiver connected to the transmitter via an optical channel.
    According to the invention it is provided that - the transmitter comprises a transmitter laser and a transmitter-side electroabsorption modulator connected downstream of the transmitter laser, wherein the optical output of the transmitter-side electroabsorption modulator forms the output of the transmitter and is coupled to the optical channel, and wherein the transmitter has an electrical data input that is connected to the electrical modulation connection of the transmitter-side electroabsorption modulator, - wherein the receiver comprises a receiver laser and a receiver-side electroabsorption modulator connected downstream of the receiver laser, wherein the optical output of the receiver-side electroabsorption modulator forms the input of the receiver and is coupled to the optical channel, and wherein the receiver has a has electrical data output which is connected to the electrical modulation connection of the receiver-side electroabsorption modulator,
    - The respective physical variable for detuning the respective laser is specified by a transmitter-side control unit and a receiver-side control unit, and
    - The control unit on the transmitter side and the control unit on the receiver side being synchronized with one another and
    - With the transmitter-side control unit and the receiver-side control unit at their respective output the same signal for determining the physical variable for determining the laser frequency is specified.
    Such a configuration of an arrangement and a method for data transmission advantageously ensures that by specifying a physical variable, for example the laser current or the laser temperature, the transmitter laser and the receiver laser can be detuned so that an injection locking of the transmitter laser and the receiver laser takes place, and due to the precise one
    coherent homodyne reception is possible with matching laser frequencies.
    The possibility of a synchronous specification of the laser frequencies of the transmitter and receiver laser also advantageously enables that in the event that e.g. There are discontinuities in the optical channel that lead to reflections of light, the laser frequencies can be matched to them and crosstalk of the respective optical received signal is almost completely prevented.
    In the event that discontinuities in the optical channel lead to superimposition or crosstalk of the signal arriving at the receiver, it can be provided
    - that the position of a discontinuity or a source of optical feedback, in particular of reflections, in the optical channel, as well as the light transit time that the signal needs from the receiver laser to the discontinuity and back to the receiver laser, are determined, and
    - That a signal curve and the optical frequency curve of the receiver laser resulting from the signal curve are defined in such a way that those time ranges of crosstalk in which the difference between the frequency curve and the optical frequency curve shifted by the light travel time exceeds the optical bandwidth of the electrical signal to be transmitted
    are minimal.
    A further improvement of the signal arriving at the receiver in the event of discontinuities occurring in the optical channel can be achieved if a sawtooth-shaped signal curve is defined, the period duration Tperoptimaı of which is selected on the basis of the light transit time,
    In particular, it is provided that for a coherent homodyne reception the lowest possible frequency of fopima = C / 2L is used as the sawtooth frequency, where c indicates the speed of light in the optical channel and L is the distance between the receiver laser and the discontinuity, so that the period duration Trper , optimal = 2L / c.
    Such a choice of the signal course ensures particularly effectively that the period in which crosstalk of the optical signal emitted by the transmitter inevitably falls into the spectrum of the optical received signal arriving at the receiver, due to reflections at a discontinuity, is minimal.
    In order to particularly effectively prevent data loss during the data transmission in the event that discontinuities occur in the optical channel, it can be provided that no data is recorded during the time ranges of crosstalk that are defined in this way
    be transmitted.
    A possibility for tap-proof data transmission between the transmitter and the receiver can be provided if for tap-proof data transmission between the transmitter and the receiver
    - a key is exchanged between the transmitter-side control units and the receiver-side control unit,
    - Identical signal curves are derived from the exchanged key in the transmitter-side control units and the receiver-side control unit, and
    One possibility of avoiding data loss in the case of data transmission, in particular tap-proof, between the transmitter and the receiver can be provided if
    - the receiver laser emits light in frequencies from the lower to the upper limit of the operating frequency band range over time in a predetermined operating frequency band range, in particular with a sawtooth-shaped signal curve,
    - it is examined whether light in one or more frequencies within the operating frequency band range is radiated via the optical channel onto the receiver-side electro-absorption modulator and
    - For the data transmission between the transmitter and the receiver, at least one frequency band is selected within the operating frequency band range, within which no light is incident on the electro-absorption modulator on the receiver side.
    Further advantages and configurations of the invention emerge from the description and the accompanying drawings.
    The invention is shown schematically in the following with the aid of particularly advantageous but not restrictive exemplary embodiments in the drawings and is described by way of example with reference to the drawings.
    The following shows schematically:
    1 shows an embodiment of an arrangement according to the invention for data transmission,
    2 shows an example of a sawtooth-shaped signal profile with a period
    Tpersoptimal »FIG. 3 shows a detailed view of the sawtooth-shaped signal curve.
    1 shows an exemplary embodiment of an arrangement 100 according to the invention for data transmission. The arrangement 100 comprises a transmitter 1 and a receiver 2 which are connected to one another via an optical channel 3, for example a fiber optic cable. The transmitter 1 comprises a transmitter laser 13 and a transmitter-side electroabsorption modulator 10 connected downstream of the transmitter laser 13. The transmitter-side electroabsorption modulator 10 has an optical output 11,
    The receiver 2 of the arrangement 100 comprises a receiver laser 23 and a receiver-side electroabsorption modulator 20 connected downstream of the receiver laser 23. The optical output 21 of the receiver-side electroabsorption modulator 20 forms the input of the receiver 2 and is coupled to the optical channel 3. The receiver 2 also has an electrical data output which is connected to the electrical modulation connection 22 of the electroabsorption modulator 20 on the receiver side.
    Electroabsorption modulators, such as the electroabsorption modulator 10, 20 shown in FIG. 1, are known from the prior art and are described, for example, in 7. / do et al., IEEE Phot. Tech. Lett., Vol. 6, no.10, pp. 1207-1209 (1994). Such electro-absorption modulators 10, 20 can together with laser elements such as the transmitter laser 13 or the receiver laser 23 on a chip
    co-integrated.
    The electroabsorption modulators 10, 20 have the property that with them light S ,, entering from the respective laser 13, 23 is weakened depending on the voltage applied to the respective electrical modulation connection 12, 22 of the transmitter or receiver-side electroabsorption modulator 10, 20 and as outgoing or incoming optical signal S, rt, Som emitted or received via an optical connection 11, 21 and fed into the optical channel 3, e.g. B. an optical fiber such as a fiber optic cable, is coupled in or out. Alternatively, the optical channel 3 can also be designed as a free section.
    The electrical current Ip, I + flowing through the electrical modulation connection 12, 22 of the electroabsorption modulator 10, 20 is approximately proportional to the amount of light that is taken from the light Si emitted by the respective laser 13, 23 and not into the transmitted optical signal Sort, Soap is forwarded.
    In the present exemplary embodiment, the frequency f_ of the light S, _ is within an optical frequency range F of typically +0.1 ... 1 GHz around the optical frequency fr
    The fact that the received signal S ,, a radiates onto the receiver laser 23, which has approximately the same frequency as the light Sı emitted by the receiver laser 23, results in an injection locking in which the frequency of the ("slave" -) Laser emitted light S_ to the optical ("master") frequency of the received optical signal S ,, a. The coherent-optical detection of the optical received signal Som thus takes place with an exact adaptation of these frequencies, which corresponds to the case of homodyne detection in the electro-absorption modulator 20.
    If the frequencies of the light S_ of the transmitter laser 13 and the received optical received signal S, pa are matched to one another by injection locking, a superposition takes place in which the signals contained in the received optical received signal Soap come to lie exactly in the baseband ("homodyne detection "). These signals are therefore particularly easy to read out and in electrical form without additional digital signal processing for the purpose of frequency offset correction
    Received signal Ir particularly easy to identify.
    In the exemplary embodiment shown, the transmitter laser 13 and the receiver laser 23 can be detuned by specifying a physical variable. This can be, for example, the laser current I_ or the laser temperature Temp. The dependence of the light S_ emitted by the laser 13, 23 on the temperature Temp of the laser 13, 23 can be used to roughly determine the frequency of the light Si. The fine control of the frequency of the light Si can be done by varying the
    Laser current I_ı are made.
    In the exemplary embodiment in FIG. 1, a transmitter-side control unit 14 and a receiver-side control unit 24 of the arrangement 100 are connected to the electrical input 130, 230 of the transmitter laser 13 or the receiver laser 23 and specify the respective physical variable for detuning the respective laser 13, 23 . The laser current I_ used to create the light S_ can be regulated via the electrical input 130, 230. By specifying the laser current I_ can
    Furthermore, the transmitter laser 13 and the receiver laser 23 each have an optical laser output 131, 231, from which the light Si generated by the laser 13, 23 is emitted.
    The arrangement 100 further comprises a synchronization unit 30 which is connected to the control unit 14 on the transmitter side and the control unit 24 on the receiver side and which synchronizes them with one another. As a result of this synchronization, the transmitter-side control unit 14 and the receiver-side control unit 24 each specify the same signal adapted to the transmission distance at their output 15, 25 for specifying the physical variable for determining the laser frequency. This means that the start of the frequency profile on the transmitter laser 13 is synchronized with the start of the frequency profile on the receiver laser 23. However, the signal is previously transmitted over the distance between the transmitter 1 and the receiver 2, so that the frequency profile on the transmitter 1 starts slightly earlier, for example offset by the light travel time between the transmitter 1 and the receiver 2, so that synchronization with the frequency profile on the Receiver 2 is ensured.
    By superimposing the light Si of the receiver laser 23 and the received optical received signal S ,, a, a current signal Ip is created which is approximately proportional to the product of the field strengths of the light Si and the received signal S ,, a. Due to the adjustment of the frequency f_ of the receiver laser 23 to the central frequency fr of the received signal S, .a, the frequency band created by the received signal S ,, a is mapped into a frequency range around 0 Hz and therefore ends up in the electrical baseband.
    The optical frequencies are advantageously in the range of 150-800 THz. The bandwidth of the signal modulated in the optical signal S, 7 can - depending on the number of optical carrier frequencies f_ selected in parallel - be selected in the range of a few GHz, but in connection with broadband information signals it can typically range up to 100 GHz.
    In FIG. 1, the electrical received signal Ip is applied to the electrical modulation connection 22 of the receiver 2 in the form of a current signal. This current signal Ip is proportional to the light power or light intensity prevailing in the electro-absorption modulator 2. Since the frequency of the light emitted by the receiving laser 23 Sı
    To send optical signals S, - by means of an electroabsorption modulator 10 shown in FIG. 1, a transmission signal St is specified, which is forwarded as an electrical voltage signal I + to the relevant electrical modulation connection 12 of the electroabsorption modulator 10.
    As is indicated schematically in FIG. 1, the optical channel 3 has a discontinuity 4 or a source of optical feedback. As a result of such discontinuities 4 in the optical channel 3, the light Sı emitted by the receiver laser 23 is partially reflected in the direction of the receiver 2 or the receiver laser 23 and there is a partial superimposition or crosstalk on the optical transmission signal S, coming from the transmitter 1: . That is, this crosstalk of the optical transmission signal S, +, i. the crosstalk caused by a signal emitted at the same time by the receiver laser 23 falls within the bandwidth of the optical reception signal Soa arriving at the receiver 2, so that the data encoded therein are only transmitted to the receiver 2
    can be received and read with reduced quality.
    To avoid this, in a method according to the invention, the frequency of the light S_ emanating from the receiver laser 23 is advantageously shifted in such a way that the spectral distance between the optical signal Sort emanating from the transmitter-side electroabsorption modulator 10 and the crosstalk occurring with a time delay is maximum at the receiver 2. For this purpose, the position of the discontinuity 4 or the source of optical feedback in the optical channel 3 as well as the time of flight that the light S emitted by the receiver laser 23 needs to reach the discontinuity 4 and back to the receiver laser 23 is determined.
    The signal curve or the optical frequency curve of the receiver laser 23 resulting from this signal curve are then adapted to the distance L between the discontinuity 4 and the receiver laser 23. By defining the signal curve or the optical frequency curve, those time ranges of crosstalk in which the difference between the frequency curve
    and the optical frequency profile which is shifted by the light travel time and falls below the optical bandwidth to be transmitted of the electrical signal Ir to be transmitted (see FIG. 2).
    Such an optical frequency profile is shown in FIG. As can be seen in FIG. 2, by adapting the signal profile or the frequency profile to the distance between the receiver laser 23 and the discontinuity 4, the detuning is maximized at the point in time at which the light S_ reflected by the discontinuity 4 returns to the receiver laser 23 occurs, so that the crosstalk is shifted from the bandwidth of the optical received signal S ,, a arriving at the receiver 2, as can be seen in the reception spectrum in FIG.
    As can be seen in FIG. 2, a sawtooth-shaped signal curve is established in the exemplary embodiment, the period T of which is selected optimally on the basis of the light transit time. For example, the lowest possible frequency of foptimaı = C € / 2L can be used as the sawtooth frequency. Here, c is the speed of light in the optical channel 3 and L is the distance between the receiver 2 and the discontinuity 4, so that the period duration of T per, optimaı = 2L / c results.
    If, for example, the frequency curve or the wavelength curve of the receiver laser 23 follows a sawtooth-shaped curve, with an optical emission frequency of vs (t) = tAF / Tper, optimaa where AF is the maximum deviation of the optical emission frequency and Tperoptima is the period of the curve, this shows Crosstalk caused by the reflection at the discontinuity 4 in the optical channel 3 delays the same course with an optical frequency vpe (t) = vs (t + At). The delay At is determined by the distance L between the electro-absorption modulator 20 and the discontinuity 4, which is associated with a round-trip time of At = 2L / c.
    The spectral offset or the deviation AV of the crosstalk is determined by the difference in the optical frequencies that arrive at the receiver 2 or the electro-absorption modulator 20: AV (t) = vR (t) - vs (t) = 2LÄAF / CT per, optimal
    The optimum frequency profile is therefore obtained when the offset is constant and at maximum for AF. This is the case for fopimaı = 1 / Tper, optimaı = C / 2L, which, as already mentioned above, is the lowest possible frequency that ensures optimal reception of the optical transmission signal S, + at the receiver 2 even in the case of crosstalk.
    In the exemplary embodiment, a sawtooth function is advantageously selected as the signal profile, the edge of which has an infinitely steep drop. In the area of the flank of the frequency profile, an overlapping of the optical transmission signal S, + with the light reflected by the discontinuity 4 cannot be avoided. By choosing such an asymmetrical triangle function, however, this overlap is minimized.
    Optionally, data loss can be completely avoided if no data is transmitted from the transmitter 1 to the receiver 2 during the crosstalk time ranges established in this way.
    Since the laser frequency f_ of the transmitter laser 13 and of the receiver laser 23 are each predetermined in the same way, a coherent homodyne detection can also take place in this case. In the exemplary embodiment shown, stable injection locking of the lasers 13, 23 is ensured by the fact that the maximum spectral offset of the reflected signal is much greater than the frequency range of typically around 100 MHz used for injection locking. The spectral offset is typically> 2 GHz according to the modulation parameters and can go far beyond this.
    The data transmission between the transmitter 1 and the receiver 2 can optionally be designed to be tap-proof if a key is exchanged between the transmitter-side control unit 14 and the receiver-side control unit 24. Using the exchanged key, identical signal curves or frequency curves are derived in the transmitter-side control unit 14 and the receiver-side control unit 24 and transmitted to the transmitter laser 13 or the receiving laser 23 during the data transmission. In this case too, the control units 14, 24 are synchronized.
    Advantageously, the detunability of the receiver 2 can be used beforehand in order to first scan the signal spectrum so that when the above-described "hopping" of the frequency curve occurs, jumping onto existing channels is avoided. To this end, the entire frequency range is first continuously scanned, for example by means of a sawtooth-shaped signal curve over the entire control range of the transmitter laser 13 or of the receiver laser 23, in order to identify existing channels
    and mask out in the created identical signal curves.
    In the exemplary embodiment, a distinction is made between a transmitter 1 and a receiver 2 and an optical signal S, yt is emitted from the transmitter 1 to the receiver 2. If it is such a unidirectional connection shown in FIG. 1, the crosstalk arises from the laser signal Si of the local oscillator or the receiver laser 23, which is also emitted by the receiver 2. The transmitter 1 and the receiver 2 are, however, designed to be identical, so that an optical signal S ,, t can also be transmitted from the receiver 2 to the transmitter 1.
    The electro-absorption modulators 10, 20 can, however, also be operated bidirectionally, i.e. the receiver 2 can also transmit at the same time or the transmitter 1 can also receive at the same time. This is for example in B. Schrenk et al., “A Coherent Homodyne TO-Can Transceiver as Simple as an EML”, IEEE / OSA J. Lightwave Technol., Vol. 37, no. 2, pp. 555-561, Jan. 2019. In this case, the crosstalk arises from the transmission signal that is transmitted by the receiver 2 at the same time. The transmitter 1 or receiver 2 shown in FIG. 1 can therefore function simultaneously as a transmitter and receiver.
    For each discontinuity 4 in the optical channel 3 there is not only one possible frequency for the detuning sequence, but several. In practice, the smallest frequency fopima is preferably chosen. For different distances between the electro-absorption modulator 10, 20 and discontinuity 4, different optimal frequencies fopima result. Since there are now several possible frequencies for the detuning sequence, they also coincide at some point, with this "common" frequency being selected. So there are several possible frequency bands for a respective detuning sequence, from which one can
    Overlap, i.e. chooses a common frequency.
    If the stroke AV of the detuning is selected to be large, there is also a greater distance between the lines of foptimaı UNd fopt, aelay-um an optimal frequency foptimaı around the dashed lines in Fig. 2 and Fig. 3, the frequency actually used can vary Stroke AV of detuning varies. In the case of, for example, very broad frequency bands for a possible frequency, there are also several possible common frequencies for different distances to a discontinuity 4. This means that the detuning AV can be selected to be greater in the case of several discontinuities 4 in the optical channel 3 in order to ensure the existence of common frequencies
    force.
    权利要求:
    Claims (1)
    [1]
    1. Arrangement (100) for data transmission comprising a transmitter (1) and a receiver (2) connected to the transmitter (1) via an optical channel (3), - wherein the transmitter (1) has a transmitter laser (13) and one of the Transmitter laser (13) comprises downstream transmitter-side electroabsorption modulator (10), wherein the optical output (11) of the transmitter-side electroabsorption modulator (10) forms the output of the transmitter (1) and is coupled to the optical channel (3), and wherein the transmitter (1 ) has an electrical data input which is connected to the electrical modulation connection (12) of the transmitter-side electroabsorption modulator (10), - wherein the receiver (2) comprises a receiver laser (23) and a receiver-side electroabsorption modulator (20) connected downstream of the receiver laser (23), wherein the optical output (21) of the receiver-side electroabsorption modulator (20) forms the input of the receiver (2) and is coupled to the optical channel (3), u nd wherein the receiver (2) has an electrical data output which is connected to the electrical modulation connection (22) of the receiver-side electroabsorption modulator (20), - the transmitter laser (13) and the receiver laser (23) by specifying a physical variable, in particular by Presetting of the laser current (I) or the laser temperature (Temp) are detuned, - with a transmitter-side control unit (14) and a receiver-side control unit (24) being provided, which specify the respective physical variable for detuning the respective laser (13, 23) - the transmitter-side control unit (14) and the receiver-side control unit (24) being synchronized with each other, and - the transmitter-side control unit (14) and the receiver-side control unit (24) each having the same signal at their output (15, 25) for determining the Specify the physical size to define the laser frequency.
    2, method for data transmission between a transmitter (1) and a receiver (2) connected to the transmitter (1) via an optical channel (3), - the transmitter (1) having a transmitter laser (13) and a transmitter laser (13 ) comprises downstream electro-absorption modulator (10) on the transmitter side, the optical output (11) of the transmitter-side electroabsorption modulator (10)
    - The transmitter laser (13) and the receiver laser (23) by specifying a
    physical quantity, in particular by specifying the laser current (I) or the
    Laser temperature (Temp), can be detuned,
    - The respective physical variable for detuning the respective laser (13, 23)
    from a transmitter-side control unit (14) and a receiver-side control unit (24)
    is given, and
    - wherein the transmitter-side control unit (14) and the receiver-side control unit (24)
    are synchronized with each other and
    - With the transmitter-side control unit (14) and the receiver-side
    Control unit (24) at its respective output (15, 25) in each case the same signal for
    Determination of the physical size for determining the laser frequency is specified.
    3. The method according to claim 2, characterized in that
    - That the position of a discontinuity (4) or a source of optical feedback, in particular of reflections, in the optical channel, as well as the light travel time that the signal from the receiver laser (23) to the discontinuity (4) and back to the receiver laser (23) needs , be noted, and
    - That a signal course as well as the optical frequency course of the receiver laser (23) resulting from the signal course are determined in such a way that those time ranges of crosstalk in which the difference between the frequency course and the optical frequency course shifted by the time of flight the optical bandwidth to be transmitted to be transmitted electrical signal
    are minimal.
    it is provided in particular that the lowest possible frequency of fopima = C / 2L is used as the sawtooth frequency for coherent homodyne reception, where c indicates the speed of light in the optical channel (3) and L the distance between the receiver laser (23) and the discontinuity (4) so that the period T per, optimaı = 2L / c.
    5. The method according to any one of claims 3 or 4, characterized in that no data is transmitted during the time ranges of crosstalk determined in this way.
    6. The method according to any one of claims 2 to 5, characterized in that for tap-proof data transmission between the transmitter (1) and the receiver (2)
    - A key is exchanged between the transmitter-side control units (14) and the receiver-side control unit (24),
    - Identical signal curves are derived from the exchanged key in the transmitter-side control units (14) and the receiver-side control unit (24), and - the signal curves are fed to the transmitter laser (13) and the receiver laser (23) during the data transmission.
    7. The method according to any one of claims 2 to 6, characterized in that
    - that the receiver laser (23) in a predetermined operating frequency band range in a predetermined manner, in particular with a sawtooth-shaped signal curve, emits light over time at frequencies from the lower to the upper limit of the operating frequency band range,
    - That it is examined whether light in one or more frequencies within the operating frequency band range is radiated via the optical channel (3) onto the electro-absorption modulator (20) on the receiver side, and
    - That for the data transmission between the transmitter (1) and the receiver (2) at least one frequency band is selected within the operating frequency band range within which no light is incident on the receiver-side electroabsorption modulator (20).
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    CN107658694B|2017-11-16|2020-01-03|太原理工大学|InP-based monolithic integration chaotic semiconductor laser chip with random scattered light feedback|
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    申请号 | 申请日 | 专利标题
    ATA50374/2019A|AT522381B1|2019-04-25|2019-04-25|Arrangement for data transmission|ATA50374/2019A| AT522381B1|2019-04-25|2019-04-25|Arrangement for data transmission|
    EP20160857.7A| EP3734863A1|2019-04-25|2020-03-04|Data transmission assembly|
    US16/848,300| US10911147B2|2019-04-25|2020-04-14|System and method for data transmission|
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