Patent Description:
Another important quantum technology is the quantum computer that operates on quantum bits (qubits) and promises to solve computational problems in a much shorter time than classical computers. Multiple quantum computers may be linked by exchanging entangled qubits between them and thus create a powerful computer cluster. To achieve this quantum communication (QC) over large distances, it has been proposed to use satellites exchanging qubits via a single photon communication system.

A crucial part of any space-based solution for QKD or QC is a laser communication terminal (LCT) that includes an optical bench and a telescope to facilitate the exchange of photons over long distances. In general, LCTs require ultra-high precision control of the pointing of multiple laser beams on the order of few µrad or below. This pointing accuracy needs to be established towards the communication partner located hundreds to thousands of kilometers apart. The communication partner may be a satellite or a ground station that receives and/or transmits the laser beams. For the pointing, LCTs typically use a control loop feeding back an error signal to a fine-steering mechanism (FSM) as an actuator. In a conventional optical bench, one FSM allows for accurate pointing of a single laser beam. Consequently, introducing an extra light beam into the optical bench and overlaying it with the first via free-space beam splitters requires an extra FSM to control the relative pointing between the two light beams. This extra FSM introduces more complexity and costs, as well as an additional single point of failure to such conventional system. LCTs for space-based QKD or QC need to spatially overlap at least two beam paths: the quantum channel and the classical channel. An inadequate beam overlap between the two results in optical losses and, in the case of QKD, it represents a notable security vulnerability for the quantum channel.

From <CIT> a system for use with quantum system is known. The document discloses a transmitter that uses four different polarized attenuated lasers to generate quantum bits through the quantum bit generator. Photons from the quantum bit generator are delivered via a single mode fiber to a telescope.

From <CIT> a free space optical communications terminal. The terminal includes an optical source arranged to provide a first beam of light encoding information to be communicated; an optical source arranged to provide photons encoding bits of a key of a Quantum Key Distribution protocol; and an optics arrangement. The optics arrangement is configured to combine the first beam and the photons via a polarization beam combiner into a single, second, beam to be transmitted to a receiver terminal.

Thus, there is a need for a technical solution for overlapping laser signals/beams with a reduced complexity, especially in communication terminals.

This technical need/object is achieved/solved by a system according to claim <NUM>, a terminal according to claim <NUM>, a satellite or ground-based station or aircraft or spacecraft according to claim <NUM>, and a method according to claim <NUM>.

According to a first aspect, a system for information transmission (quantum key distribution and quantum communication) in a quantum communication network is provided. The system comprises a first laser signal source, a second laser signal source, a coupler unit, an optical waveguide and a directional unit. The first laser signal source is configured to generate a first laser signal. The second laser signal source is configured to generate a second laser signal. Each laser signal source (of the first laser signal source and the second laser signal source) is configured to provide the corresponding laser signal to the coupler unit. The coupler unit is configured to receive and to couple both (the first laser signal and the second laser signal) laser signals. The coupler unit is configured to provide coupled laser signals to the optical waveguide. The optical waveguide is configured to receive the coupled laser signals. The optical waveguide is configured to cause a (passive) concentric (spatial) alignment of the coupled laser signals by allowing the received coupled laser signals a mode propagation to provide concentrically (spatially) aligned laser signals. The waveguide may be configured to (only) transmit (spatial) mode-matched laser signals, wherein said mode-matched laser signals may be achieved in the optical waveguide by forcing the coupled laser signals, in particular each laser signal of the coupled laser signals into a mode propagation, in particular a single-/fundamental-mode propagation to provide concentrically (spatially) aligned laser signals. The optical waveguide is configured to provide the concentrically (spatially) aligned or mode-matched laser signals to the directional unit. The directional unit is configured to receive the concentrically (spatially) aligned or mode-matched laser signals. The directional unit is configured to provide the concentrically (spatially) aligned or mode-matched laser signals to a second terminal of the quantum communication network. The directional unit can be configured to point the concentrically (spatially) aligned or mode-matched laser signals to a receiver or a second terminal of the quantum communication network. The optical waveguide may, in short, sometimes be referred to as waveguide, but still be configured as an optical waveguide.

Regarding the waveguide: The waveguide comprises one or more certain waveguide properties (e.g. dimension, material(s), numerical aperture etc.) which allow a certain received laser signal with certain laser signal properties a mode propagation, e. a single mode propagation, within/along the waveguide. In other words, if the laser signal properties are within one or more certain mode propagation criteria, the received laser signal propagates within/along the waveguide at a certain mode, in particular a/the same mode. In case of two laser signals with different wavelengths but within the mode propagation criteria, both laser signals propagate through the same mode but at different wavelengths. When the mode propagating laser signals leave the waveguide through one end, a nearly perfect concentric (spatial) alignment or mode-matching of the said laser signals may be passively caused. The laser signals that leave the waveguide through one end may be (nearly or almost perfectly) concentrically (spatially) aligned or mode-matched as they propagated previously at the (same) mode, in particular the (same) single or fundamental-mode within/along the waveguide. Hence, the waveguide may cause a (nearly perfect) concentric (spatial) alignment or mode-matching.

The first laser signal source is configured to provide classic information via an optical modulations scheme. The second laser signal source is configured to provide quantum information via single photon pulses.

This has the advantage that accurate steering (pointing towards a receiver of another LCT) of a low power quantum channel can be done indirectly via a steering of the classical channel, which operates at much higher optical powers and thus results in a better signal for the pointing feedback and thus a better pointing performance. Apart from this, the system may simplify the efforts in alignment, integration and test (AIT), due to the reduced number of parts. Any thermo-mechanical effects on the optical bench of the LCT affects both channels in a very same way and can be compensated by the one (and only) fine steering mechanism in the directional unit. Moreover, the algorithm running the single pointing in the directional unit is less complex than the algorithm running two pointing systems simultaneously, like in conventional LCTs for QKD and QC. This contributes favorably to the stability, performance and security of the system in operation.

Further, the laser beam with single photon signals may be controlled/guided between the laser terminals without monitoring any of the single photons.

The mode propagation may be configured as a single, in particular as a same single, mode propagation. The single mode may be or comprise or be understood as the lowest (order) propagation mode of the waveguide. In case of an optical single-mode fiber, this may be the LP<NUM> Mode. In one specific implementation, the waveguide can be configured as a single-mode fiber.

The first laser signal may comprise a first laser signal power. The second laser signal may comprise a second laser signal power. The coupler unit can be further configured to couple both laser signals, i. the first laser signal and the second laser signal, according to a predefined power division ratio. The power division ratio might be in favor of the first laser signal. The power division ratio might be <NUM>:<NUM> or <NUM>:<NUM>. This can allow that most power of the first laser signal, in particular the classical channel, is combined with a fraction of the second laser signal, in particular the quantum channel.

The coupler unit can further comprise a first entrance, configured to receive the first laser signal. The coupler unit can further comprise a second entrance, configured to receive the second laser signal. Each entrance, i. the first entrance and the second entrance, may be configured to provide their received laser signal (first entrance, first signal; second entrance, second signal) to a couple area. The couple area can be configured to receive both laser signals. The couple area can be configured to couple both laser signals. The couple area can be configured to couple both laser signals according to the predefined power division ratio into a first portion of coupled laser signals and a second portion of coupled laser signals.

The couple area can be configured to provide the first portion of coupled laser signals to a first output. The couple area can be configured to provide the second portion of coupled laser signals to a second output. The first output can be configured to provide the first portion of coupled laser signals to the waveguide. The second output can be configured to provide the second portion of the coupled laser signals to an absorber or an absorber unit/material. Alternatively, the second output can be configured to provide the second portion of the coupled laser signals to a fiber terminator or a detection unit, in particular a photodetector. The detection unit, in particular the photodetector, can be configured to monitor the power of the second portion and/or monitor the power division ratio.

The coupler unit can be configured as a beam coupler, in particular a free space beam coupler, or an (optical) fiber coupler, in particular a single-mode fiber coupler.

It is clear that in case of a fiber coupler, in particular a single mode fiber coupler, the concentric (spatial) alignment or mode-matching may be achieved at that moment, when both laser signals are coupled in the couple area. Hence, both outputs of the fiber coupler may provide concentrically (spatially) aligned coupled laser signals or mode-matched coupled laser signals.

The waveguide can further comprise a first and a second end. The first end can be configured to receive the first portion of coupled laser signals. The second end can be configured to provide the concentrically (spatially) aligned or mode-matched laser signals to the directional unit.

The second laser signal source, the coupler unit and the waveguide may be arranged within a security unit to prevent eavesdropping, in particular photon-number splitting attacks. The absorption unit/material can be within a security unit to prevent eavesdropping, in particular photon-number splitting attacks. The security unit can be configured to prevent compromising radiation.

The first laser signal source can be further configured to be an entrance interface to the security unit. A second end of the waveguide that provides the concentrically (spatially) aligned or mode-matched laser signals may be further configured to be an output interface out of the security unit.

According to a second aspect, a communication terminal, in particular a laser communication terminal, comprising the system according to the first aspect is proposed.

According to a third aspect, a satellite or ground-based station or aircraft or spacecraft comprising the system according to the first aspect is proposed.

According to a fourth aspect, an apparatus for providing concentrically (spatially) aligned or mode-matched laser beams maybe provided. The apparatus may comprises at least two laser beam sources, a coupler and an optical waveguide. Each of the at least two laser beam sources may be configured to generate a laser beam and provide the laser beam to the coupler. The coupler may be configured to receive the at least two laser beams. The coupler may be configured to couple the at least two laser beams. The coupler may be configured to provide at least two coupled laser beams to the optical waveguide. The optical waveguide may be configured to receive the at least two coupled laser beams. The optical waveguide may be configured to cause a concentric (spatial) alignment or mode-matching of the coupled laser beams by allowing/enforcing the received at least two laser beams a mode propagation, e. a single mode propagation. In this way, the optical waveguide may be configured to provide concentrically (spatially) aligned or mode-matched laser beams.

The mode propagation may be configured as a single, in particular as a same single, mode propagation (of the waveguide of the apparatus). The single mode may be or comprise or be understood as the lowest (order) propagation mode physically possible. In case of an optical single-mode fiber, this may be the LP<NUM> Mode. In one specific implementation, the waveguide can be configured as a single-mode fiber.

The first laser beam can comprise a first laser beam power. The second laser beam can comprise a second laser beam power. The coupler may be further configured to couple both laser beams according to a predefined power division ratio.

The coupler can further comprise a first entrance, configured to receive the first laser beam. The coupler can further comprise a second entrance, configured to receive the second laser beam. Each entrance of the coupler can be configured to provide their received laser beam to a couple area of the coupler. The couple area can be configured to receive both laser beams. The couple area of the coupler can be configured to couple both laser beams according to the predefined power division ratio into a first portion of coupled laser beams and a second portion of coupled laser beams. The couple area can be further configured to provide the first portion of coupled laser beams to a first output. The couple area can be further configured to provide the second portion of coupled laser beams to a second output. The first output of the coupler can be configured to provide the first portion of coupled laser beams to the waveguide of the apparatus. The second output of the coupler of the apparatus can be configured to provide the second portion of coupled laser beams to an absorber or an absorber unit/material.

The coupler can be configured as beam coupler, in particular a free space beam coupler, or an optical fiber coupler, in particular a single-mode fiber coupler.

It is clear that in case of a fiber coupler, in particular a single mode fiber coupler, the concentric (spatial) alignment or mode-matching may be achieved at that moment, when both laser beams are coupled in the couple area. Hence, both outputs of the single mode fiber coupler may provide concentrically (spatially) aligned coupled laser beams or mode-matched coupled laser beams.

According to a fifth aspect, a method for information transmission / quantum key distribution and quantum communication in a quantum communication network is proposed. The method comprises providing a first laser signal source configured to provide a first laser signal. The method comprises providing a second laser signal source configured to provide a second laser signal. The method comprises providing both laser signals to a coupler unit. The method comprises receiving by and coupling in/into the coupler unit both laser signals. The method comprises providing coupled laser signals to an optical waveguide. The method comprises receiving the coupled laser signals at the optical waveguide and causing a (passive) concentric (spatial) alignment or mode-matching of the coupled laser signals by allowing the received laser signals a mode, in particular a single-mode, propagation in the waveguide. The method for information transmission/quantum key distribution and quantum communication in a quantum communication network further comprises providing a concentrically (spatially) aligned or mode-matched laser signal to a directional unit. The method comprises receiving the concentrically (spatially) aligned or mode-matched laser signals at the directional unit. The method comprises providing the concentrically (spatially) aligned or mode-matched laser signals to a second terminal of the quantum communication network.

According to a sixth aspect, a method for providing concentrically (spatially) aligned or mode-matched laser beams may be provided. The method may comprises providing at least two laser beam sources, each of the at least two laser beam sources being configured to generate a laser beam. The method may comprises providing the laser beam to a coupler, wherein the coupler is configured to receive the at least two laser beams. The method for providing the concentrically (spatially) aligned or mode-matched laser beams may further comprises providing the at least two coupled laser beams to an optical waveguide. The method further may comprises, at or by the optical waveguide, receiving the at least two coupled laser beams and causing a (passive) concentric (spatial) alignment or mode-matching of the coupled laser beams by allowing the received at least two laser beams a mode, in particular single-mode, propagation to provide concentrically (spatially) aligned or mode-matched laser beams. The method for providing the concentrically (spatially) aligned or mode-matched laser beams may further comprises providing the concentrically (spatially) aligned or mode-matched laser beams.

These and other aspects of the invention will now be further described, by way of example only, with reference to the accompanying figures, wherein like reference numerals refer to like parts, and in which:.

<FIG> illustrates a system <NUM> for information transmission/quantum key distribution and quantum communication in a quantum communication network. The system <NUM> comprises two laser signals sources <NUM>, <NUM>. The first laser signal source <NUM> emits a first laser signal <NUM>, which carries classic information via an optical modulations scheme. The second laser signals source <NUM> emits a second laser signal <NUM>, which carries quantum information via single photon pulses, for example quantum bits for quantum key distribution. Both laser signals <NUM>, <NUM> are sent towards the coupler unit <NUM> which couples both signals <NUM>, <NUM>. As a result, both laser signals <NUM>, <NUM> are spatially aligned reasonably well. In other words, both laser signal centers (spatial domain), are slightly misaligned to each other. To achieve mode-matching (i.e., a nearly perfect concentric and unidirectional alignment) of both laser signals <NUM>, <NUM>, both signals are sent from the coupler unit <NUM> to an optical waveguide <NUM>, in the present case illustrated by way of example, a single-mode fiber <NUM>. The first end <NUM> of the single-mode fiber <NUM> is directly connected to the first output of the coupler unit <NUM>. The laser signals <NUM>, <NUM> received by the single-mode fiber <NUM> propagate in the fundamental mode along the single-mode fiber <NUM>, for example LP<NUM>. The second end of the single-mode fiber comprises a lens <NUM>, that receives both laser signals, propagating in single-mode, from the single-mode fiber <NUM> and provides those signals as concentrically spatially aligned or mode-matched laser signals <NUM> to the directional unit <NUM>.

The concentric spatial and unidirectional alignment of the laser signals is passively achieved by the properties of the single-mode fiber <NUM>. The single-mode fiber <NUM> allows the received laser signals a single-mode propagation (only) through the said single-mode fiber <NUM>. Any alignment imperfection of any of the beams at the input of the fiber <NUM> are converted to amplitude modulation. Both signals are nearly perfectly aligned when leaving the single-mode fiber via the second end.

An additional (passive or active) alignment of the laser signals <NUM>, <NUM> via an alignment mechanism is not necessary. The only mechanical control mechanism is a pointing or steering mechanism (not shown) in the directional unit <NUM>, that steers the spatial concentrically aligned or mode-matched signals towards a second terminal/receiver of the quantum communication network.

To prevent photon-number splitting attacks, the vulnerable second laser signal source <NUM> for the quantum channel, the coupler unit <NUM> and the single-mode fiber <NUM> are within a security unit <NUM> to prevent unwanted light signals reaching a potential attacker. The only entrance interface is given by the first laser signal source <NUM> that carries classical information.

<FIG> illustrates a variant of the embodiment of <FIG>. In this illustrated case, the coupler unit <NUM> is configured as a free space beam coupler <NUM> / short beam coupler <NUM>. This beam coupler <NUM> comprises a first entrance <NUM> and a second entrance <NUM>. Each entrance receives the corresponding laser signals <NUM> or <NUM>. The beam coupler <NUM> comprises an area, in which the two received signals <NUM>, <NUM> are coupled. In case of the specific beam coupler <NUM> exemplarily provided in the variant of <FIG>, the coupler area corresponds to a semi-transparent mirror. At this semi-transparent mirror, both signals <NUM>, <NUM> are coupled according to a power division ratio of, for example, <NUM>:<NUM>. In other words, a small part of the second laser signal <NUM> (quantum channel) is coupled with a major part of the first laser signal <NUM> (classic channel) to represent the first portion of coupled laser signals <NUM>. The remaining laser signal parts represent the second portion of coupled laser signals and are sent towards an absorption unit <NUM>.

The first portion of laser signals <NUM> is sent to the first end <NUM> of the waveguide <NUM>, which, in the illustrated case, is configured as a single-mode fiber <NUM>. The first end <NUM> is, by way of example, configured as a first lens <NUM> to receive the first portion of coupled laser signals <NUM> as they propagate in free space. The first end <NUM> provides the said portion of coupled laser signals <NUM> to the single-mode fiber <NUM>.

The first portion of coupled laser signals <NUM> received by the single-mode fiber <NUM> propagates in single-mode or fundamental-mode along the single-mode fiber <NUM>, for example LP<NUM>. The second end of the single-mode fiber <NUM> comprises a second lens <NUM>, that receives the first portion of coupled laser signals <NUM> from the single-mode fiber <NUM> and provides those signals <NUM> as concentrically spatially aligned or mode-matched laser signals <NUM> to the directional unit <NUM>.

The concentric spatial alignment or mode-matching of the first portion of coupled laser signals <NUM> is passively achieved by the properties of the single-mode fiber <NUM>. The single-mode fiber <NUM> allows the received first portion of coupled laser signals <NUM> a single-mode propagation through the said single-mode fiber <NUM>. Hence, the first portion of coupled laser signals <NUM> are nearly perfectly aligned when leaving the single-mode fiber <NUM> via the second lens <NUM>.

An additional alignment of the laser signal <NUM>, <NUM> via an alignment mechanism is not necessary. The only mechanical control mechanism is a pointing or steering mechanism in the directional unit <NUM> that steers the concentrically spatially aligned laser signals <NUM> towards a second terminal/receiver of the quantum communication network.

To prevent photon-number splitting attacks, the vulnerable second laser signal source <NUM> for the quantum channel, the beam coupler <NUM>, the absorption unit <NUM>, and the single-mode fiber <NUM> are within a security unit <NUM> to prevent unwanted electromagnetic signals reaching a potential attacker. The only entrance interface is given by the first laser signal source <NUM> that carries classical information. The output is given by the second lens <NUM>.

<FIG> illustrates a variant of the embodiment of <FIG>. In this illustrated case, the coupler unit <NUM> is configured as a fiber coupler <NUM>. Both laser signal sources <NUM>, <NUM> provide their laser signal via an optical fiber to the fiber coupler <NUM>.

This fiber coupler <NUM> comprises a first <NUM> and a second entrance <NUM>. Each entrance receives the corresponding laser signal <NUM> or <NUM> via a fiber. The fiber coupler <NUM> comprises an area in which the two received laser signals <NUM>, <NUM> are coupled. At this coupler area, both signals <NUM>, <NUM> are coupled according to a power division ratio of, for example, <NUM>:<NUM>. In other words, a small part of the second laser signal (quantum channel) is coupled with a major part of the first laser signal (classic channel) to represent the first portion of coupled laser signals. The remaining laser signal parts represent the second portion of coupled laser signals and are sent towards an absorption unit <NUM>.

The first portion of laser signals is sent to the waveguide <NUM>, which, in the illustrated case, is configured as a single-mode fiber <NUM>. The first end (no reference sign) of the single-mode fiber <NUM> is directly connected to fiber coupler <NUM> at the first entrance <NUM>.

The first portion of coupled laser signals (inside <NUM>) received by the single-mode fiber <NUM> propagates in fundamental-mode along the single-mode fiber <NUM>, for example LP<NUM>. The second end of the single-mode fiber <NUM> comprises a second lens <NUM>, that receives both in single-mode propagating laser signals from the single-mode fiber <NUM> and provides those signals as concentrically spatially aligned or mode-matched laser signals <NUM> to the directional unit <NUM>.

The concentric spatial alignment or mode-matching is passively achieved by the properties of the single-mode fiber <NUM>. The single-mode fiber <NUM> allows the received first portion of laser signals (only) a single mode propagation through the said single-mode fiber <NUM>. Hence, the first portion of coupled laser signals is nearly perfectly aligned when leaving the single-mode fiber <NUM> via the second end <NUM>.

An additional alignment of the laser signal <NUM>, <NUM> via an alignment mechanism is not necessary. The only mechanical control mechanism is a pointing or steering mechanism in the directional unit <NUM>, that redirects and steers the concentrically spatially aligned laser signal <NUM> towards a second terminal/receiver of the quantum communication network.

To prevent photon-number splitting attacks, the vulnerable second laser signal source <NUM> for the quantum channel, the fiber coupler <NUM>, the absorption unit <NUM>, and the single-mode fiber <NUM> are with a security unit <NUM> to prevent unwanted electromagnetic signals reaching a potential attacker. The only entrance interface is given by the first laser signal source <NUM> that carries classic information. The output is given by the second lens <NUM>.

<FIG> illustrates the steps of a method for information transmission (quantum key distribution and quantum communication) in a quantum communication network.

<FIG> illustrates an embodiment of the apparatus <NUM> for providing concentrically unidirectionally aligned or mode-matched laser beams.

The apparatus <NUM> comprises a first and second laser beam source <NUM>, <NUM>. Each laser beam source <NUM>, <NUM> emits a corresponding laser beam <NUM>, <NUM> towards a beam coupler <NUM>. The beam coupler <NUM> couples both laser beams <NUM>, <NUM> and provides the coupled laser signal to a single-mode fiber <NUM>. The single-mode fiber <NUM> provides concentrically spatially and unidirectionally aligned laser beams to a lens <NUM> at the second end of the said single-mode fiber <NUM>.

The concentric spatial unidirectional alignment or mode matching of the laser beams <NUM>, <NUM> is passively achieved by the properties of the single-mode fiber <NUM>. The single-mode fiber <NUM> allows the received coupled laser beams (only) a single-mode propagation through the said single-mode fiber <NUM>. Hence, the coupled laser beams are nearly perfectly spatially aligned when leaving the single-mode fiber <NUM> via the second end <NUM> into the free space.

<FIG> illustrates the steps of a method S2 for providing concentrically (and unidirectionally) aligned laser beams. The method S2 comprises the steps:.

wherein the coupler is configured to receive the at least two laser beams;.

The present concept as described herein may be considered to simplify the LCT for space-based QKD and QC by coupling the transmission channels TxQ and TxC into a single mode fiber (SMF) in comparison to state of the art approaches as illustrated in <FIG>. The two channels are spatially overlapped in the single-mode fiber and, thus, only a single set of fine steering mechanism (FSM), photodetector, and feedback loop is used - instead of two FSM in case of conventional LCTs as exemplified by <FIG> - to achieve accurate pointing of both laser beams simultaneously towards the communication partner. The two channels may be coupled into the same fiber either by means of a fiber-based beam splitter (variant in <FIG>) or by a free-space beam splitter in front of a single mode fiber (variant in <FIG>).

In <FIG>, one output guides a fraction of the power of both TxC and TxQ, which are specific examples of the first laser signal and the second laser signal in <FIG>, to the optical bench, where the combined light is collimated and subsequently sent to FSM1 and the telescope. The other BS output is terminated either by using a fiber terminator or a photodetector. The latter may be used for power monitoring. The power fraction of the two channels is given by the coupling ratio of the SMF BS and it can be chosen depending on the input power levels of TxC and TxQ and the desired output levels. A coupling ratio in which the majority of light from TxQ is terminated, while most of the TxC light is transmitted to the optical bench is beneficial (e.g., a coupling ratio of <NUM>:<NUM>). This is because the TxQ power must be reduced to a mean photon occupancy of <<NUM> photons per pulse before arriving at the optical bench, while the TxC channel benefits from fewer losses to improve the overall power efficiency of the system. The above-mentioned coupling ratio is also favored for security reasons, as described below.

In <FIG> the two channels TxC and TxQ are coupled into the same SMF only after combining the two beams with a free-space BS. This has the same desired effect as the variant in <FIG>, namely that the two beams paths are spatially overlapped in the LCT. In <FIG> one of the BS outputs is terminated in the same fashion as in <FIG>. The considerations about the coupling ratio described above apply for <FIG> as well.

<FIG>, and <FIG> also show security boundaries (SB) that indicate sections of the setups in which the TxQ mean photon occupancy is expected to be > <NUM> photons. As a result, photon-number splitting attacks are possible here in general. Herein, the SMF and beam combiner may be included within the SB.

Finally, it should be mentioned that the concept and its variants described herein may be implemented in an LCT on a satellite or in a ground station. Furthermore, the concept and its variants are beneficial for various kinds of QKD protocols, such as "prepare-and-measure" (e.g. BB84) and entanglement-based protocols. The quantum information may be physically encoded in the light via different degrees-of-freedom, for example polarisation, time-bin or phase.

As stated above, the concept and its variants significantly reduce cost and complexity of the LCT by avoiding the extra FSM2 (see <FIG>) of conventional LCTs. The accurate steering of the low power quantum channel is done via the classical channel, which operates at much higher optical powers and thus results in an accessible signal for the pointing feedback and thus a better pointing performance compared to state-of-the-art solutions. Apart from this, the approach simplifies the efforts in alignment, integration and test (AIT), thanks to the reduced number of parts. Any thermo-mechanical effects on the optical bench of the LCT affects both channels in the very same way and can be compensated by the one (and only) FSM. Moreover, the algorithm running the single pointing system in the present concept and its variants are expected to be less complex than the one running two pointing systems simultaneously in conventional LCTs for QKD and QC. This contributes favourably to the stability of the system in operation.

In entanglement-based QKD protocols, where an optical link is simultaneously established with two users on ground, two photons leaving the source at the same time have to be coupled into two individual optical benches from where they are directed to the individual users on ground. Such setup potentiates the need for optical stability and efficient pointing control between the photon source and optical benches. In such entanglement-based scenario, the presented concepts and its variants would present even higher benefit than in the case of a prepare-and-measure QKD protocol.

Claim 1:
A system (<NUM>) for information transmission in a quantum communication network comprising:
- a first laser signal source (<NUM>) configured to generate a first laser signal (<NUM>), and
- a second laser signal source (<NUM>) configured to generate a second laser signal (<NUM>),
wherein each laser signal source (<NUM>, <NUM>) is configured to provide the corresponding laser signal (<NUM>, <NUM>);
- a coupler unit (<NUM>), wherein said coupler unit is configured to receive and to couple both laser signals (<NUM>, <NUM>);
- an optical waveguide (<NUM>), wherein said optical waveguide is configured to
- receive the coupled laser signals and
- cause a concentric alignment of the coupled laser signals by allowing the received coupled laser signals a mode propagation to provide concentrically aligned laser signals (<NUM>);
- a directional unit (<NUM>), wherein said directional unit (<NUM>) is configured to receive the concentrically aligned laser signals (<NUM>) and to provide the concentrically aligned laser signals to a second terminal of the quantum communication network over a free-space optical link;
wherein the first laser signal source (<NUM>) is further configured to provide classic information via an optical modulations scheme and the second laser signal source (<NUM>) is further configured to provide quantum information via single photon pulses.