Quantum communication system using photon polarization correction

Abstract

A receiver (20-m) of a multiplexed signal (S10-n) and an optical signal (S10-h) transmitted independently through a transmission channel (50) is proposed, the multiplexed signal comprising a first quantum signal (Qn) and at least one polarization state control signal (Rn1), said optical signal comprising a second quantum signal (Qh), said receiver comprising a processing chain (Cm) and a correlation module (260) associated with a polarization base of at least one polarization state, said chain being adapted to determine the polarization state of the control signal and to modify the polarization of the multiplexed signal to align the determined state with the state of said base, the module being configured to perform a correlation measurement between the first and second quantum signals, and to generate, from the measurement, at least one information signal (Imk) of the entanglement state of the first and second quantum signals.Figure for the abstract: [Fig.6].

Description

[0001] Title of the invention: Quantum communication system using photon polarization correction Technical field

[0002] The present invention relates generally to quantum telecommunications, and in particular to a transmitter for transmitting optical signals comprising entangled quantum signals, a receiver for receiving optical signals comprising quantum signals, and a system comprising such transmitters and receivers, and the associated methods implemented.

[0003] The main application of current quantum telecommunication systems is to use quantum information theory to distribute a cryptographic key (or encryption key) between two telecommunications devices (i.e., two users), via specific quantum protocols, with the aim of subsequently and securely encrypting communications between these two devices. The secret cryptographic keys obtained have a higher degree of security than keys obtained by classical protocols.

[0004] In a quantum telecommunication system, the two users may be too physically distant to simply use the usual steps of QKD (or 'Quantum Key Distribution' according to the corresponding English expression) quantum protocols to share such an encryption key. In this context, quantum state teleportation and entanglement sharing quantum protocols make it possible to link two distant quantum devices together, to share an encryption key.

[0005] Such quantum protocols for quantum state teleportation and entanglement sharing consist of making quantum particles interfere with each other, resulting from two entangled quantum signals, each particle belonging to a pair of entangled quantum particles.

[0006] The information used to generate an encryption key is obtained by measuring a previously encoded encoding variable of quantum particles (also called "qubits"), generally corresponding to photons. This encoding variable has a random value but is identical for the two entangled particles, which makes it possible to share the same information. An encoding variable of a qubit corresponds to a degree of freedom of the quantum particle and can be the polarization of the photon. However, the polarization state of quantum particles during their propagation, between different devices of a system, undergoes random rotations. These can be due to the birefringence of the various media crossed or to the displacement of the transmitting device relative to the receiving device, such as the movement of a satellite (transmitter or receiver) relative to a ground station in the case of communications via a space segment.

[0007] To avoid such random rotations of polarization state, some known quantum systems use propagation only in free space in which the polarization of photons is stable, during their propagation through a transmission channel (or communication channel). However, in some applications, it is necessary to use guided optical transmission, as a transmission channel, for example for propagation on a ground network or on board a satellite to relax the construction constraints of the payload.

[0008] To compensate (or correct) random rotations of polarization state, some known systems use, at the start of quantum protocol implementation, a single polarization reference which makes it possible to initially estimate the polarization rotations induced during propagation and to align the polarization of the transmitted photons with the measurement bases in reception. However, this single reference does not make it possible to correct the new polarization rotations after the initial estimation phase. Alternatively, other existing systems instead use a periodic generation of reference signals of the encoding bases from the source of entangled quantum signals and therefore time-multiplexed with the qubits, which reduces the useful throughput of the system.

[0009] There is thus a need for an improved quantum communication system, capable of correcting in real time the rotations of the polarization states of the qubits. Summary of the invention

[0010] For this purpose, a receiver is provided configured to receive a multiplexed optical signal and an optical signal transmitted independently through a transmission channel, the multiplexed optical signal comprising a first quantum signal, the optical signal comprising a second quantum signal, the multiplexed optical signal further comprising at least one polarization state control signal, the receiver comprising a processing chain associated with a polarization base composed of at least one polarization state and adapted to determine the polarization state of the at least one polarization state control signal and to modify the polarization of the multiplexed optical signal so as to align the determined polarization state with respect to one of the at least one polarization state of the associated base,the receiver further comprising a correlation module adapted to carry out a correlation measurement between the first quantum signal from the multiplexed optical signal with modified polarization and the second quantum signal, the correlation module being associated with the polarization base, the correlation module being further adapted to generate at least one information signal from the correlation measurement, the signal, information including entanglement information of the polarization states of the first and second quantum signals.

[0011] In embodiments, the processing chain may comprise a module control signal detection module and an analysis device, the control signal detection module being configured to demultiplex the at least one control signal and the first quantum signal from the multiplexed optical signal, the detection module being further configured to route the demultiplexed control signal to the polarization analysis device, the analysis device comprising at least one detection unit adapted to detect the control signal according to one of the at least one polarization state of the associated base.

[0012] According to certain aspects, the detection module may further comprise a processor configured to analyze the determined polarization state and to generate a servo signal applied to a polarization correction module of the multiplexed optical signal.

[0013] In some embodiments, the receiver may be formed from polarization maintaining fibers and / or single-mode optical fibers.

[0014] The present invention further provides a transmitter configured to transmit optical signals comprising:

[0015] - a signal generator configured to generate a first quantum signal, a second quantum signal, and a polarization state control signal, the first quantum signal and the second quantum signal being mutually entangled quantum signals,

[0016] - a signal integrator configured to generate a multiplexed optical signal, the multiplexed signal comprising the first control signal and the first quantum signal.

[0017] The transmitter is configured to transmit through a transmission channel, the multiplexed optical signal and an optical signal comprising the second quantum signal.

[0018] Embodiments of the invention thus provide a quantum communication system comprising a plurality of transmitters, and at least one receiver.

[0019] In embodiments, the plurality of transmitters may include at least a first transmitter and a second transmitter, and the system may further include a plurality of auxiliary receivers including a first auxiliary receiver configured to receive an optical signal including a quantum signal transmitted by the first transmitter, and a second auxiliary receiver configured to receive an optical signal including a quantum signal transmitted by the second transmitter, each auxiliary receiver being associated with a polarization base of measurement composed of at least one polarization state and adapted to measure the associated quantum signal according to at least one of the at least one polarization state of the associated measurement polarization base. Each auxiliary receiver can be configured to receive an entanglement information signal comprising entanglement information of polarization states of quantum signals transmitted by the at least one receiver, each auxiliary receiver being configured to determine a shared quantum encryption key from the measurement of the associated quantum signal and the entanglement information of polarization states of quantum signals.

[0020] According to certain aspects, for one or both auxiliary receivers, the optical signal received by the auxiliary receiver may be a multiplexed optical signal further comprising a polarization state control signal, the auxiliary receiver(s) comprising a processing chain associated with the measurement polarization base and adapted to determine the polarization state of the polarization state control signal and to modify the polarization of the multiplexed optical signal so as to align the determined polarization state with respect to one of the at least one polarization state of the associated measurement polarization base.

[0021] In some embodiments, the multiplexed signals may be frequency-multiplexed signals.

[0022] Advantageously, the absolute value of the wavelength difference between the quantum wavelength of a quantum signal and the reference wavelength of a control signal may be greater than or equal to a minimum wavelength difference value.

[0023] There is also provided a method for determining at least one information signal in response to the reception of a multiplexed optical signal and an optical signal transmitted independently through a transmission channel, the multiplexed optical signal comprising a first quantum signal, the optical signal comprising a second quantum signal, the multiplexed optical signal further comprising at least one polarization state control signal, the method comprising a processing phase, associated with a polarization base composed of at least one polarization state, for determining the polarization state of the at least one polarization state control signal and for modifying the polarization of the multiplexed optical signal so as to align the determined polarization state with respect to one of the at least one polarization state of the associated base.The method further comprises a correlation step comprising a correlation measurement between the first quantum signal from the polarization-modified multiplexed optical signal and the second quantum signal, the correlation measurement being associated with the polarization base, the correlation step further comprising the generation of the at least one information signal. from the correlation measurement, the information signal comprising entanglement information of the polarization states of the first and second quantum signals.

[0024] The embodiments of the invention thus make it possible to correct the polarization rotations of the qubits transmitted between transmitters and receivers of entangled quantum signals, in particular in order to establish a quantum key between two distant receivers.

[0025] In particular, the embodiments of the invention provide optical signal transmitters, associated with pairs of entangled quantum particles, making it possible to robustly integrate one or more polarization state reference signals of these quantum particles.

[0026] Such references can be generated at any power, independently of the generation of the qubits, to form an efficient and affordable solution in terms of hardware complexity. A guided optics transmitter, according to the embodiments of the invention, advantageously has reduced volume and mass compactness, as well as optimized size and robustness. Furthermore, frequency multiplexing of such references to the qubits makes it possible to maintain a high transmission rate of useful information (i.e. the qubits).

[0027] The receiver(s) according to the embodiments of the invention make it possible to correct in real time the polarization rotations undergone by the qubits before detection. Such receivers make it possible in particular to analyze the qubits and the reference signals independently, in order to best align the polarization of the qubits with measurement bases of the receiver. Description of the figures

[0028] Other characteristics, details and advantages of the invention will emerge on reading the description given with reference to the appended drawings given by way of example.

[0029] [Fig.l] [Fig.l] is a diagram representing a quantum communication system, according to embodiments of the invention.

[0030] [Fig.2] [Fig.2] is a diagram representing a quantum communication system, according to embodiments of the invention.

[0031] [Fig.3] [Fig.3] is a diagram representing a transmitter of a quantum communication system, according to embodiments of the invention.

[0032] [Fig.4] [Fig.4] is a diagram representing a transmitter of a quantum communication system, according to embodiments of the invention.

[0033] [Fig.5] [Fig.5] is a diagram showing a signal generator of a transmitter of a quantum communication system, according to embodiments of the invention.

[0034] [Fig.6] [Fig.6] is a diagram representing an intermediate receiver of a quantum communication system, according to embodiments of the invention.

[0035] [Fig.7] [Fig.7] is a diagram showing an intermediate receiver of a quantum communication system, according to embodiments of the invention

[0036] [Fig.8] [Fig.8] is a diagram representing a processing chain of an intermediate receiver of a quantum communication system, according to embodiments of the invention

[0037] [Fig.9] [Fig.9] is a diagram showing a module for detecting a signal from control of an intermediate receiver of a quantum communication system, according to embodiments of the invention

[0038] [Fig. 10] [Fig. 10] is a diagram representing a module for detecting a control signal of an intermediate receiver of a quantum communication system, according to embodiments of the invention

[0039] [Fig. 11] [Fig. 11] is a diagram showing an end receiver of a quantum communication system, according to embodiments of the invention

[0040] [Fig. 12] [Fig. 12] is a diagram showing a quantum photon analysis module of an end receiver of a quantum communication system, according to embodiments of the invention.

[0041] [Fig. 13] [Fig. 13] is a flowchart representing a method of transmitting optical signals implemented by a transmitter of a quantum communication system, according to embodiments of the invention.

[0042] [Fig. 14] [Fig. 14] is a flowchart representing a method for intermediate reception of optical signals implemented by a receiver of a quantum communication system, according to embodiments of the invention.

[0043] [Fig. 15] [Fig. 15] is a flowchart representing a final reception method of optical signals implemented by a receiver of a quantum communication system, according to embodiments of the invention.

[0044] Identical references are used in the figures to designate identical or similar elements. For reasons of clarity, the elements shown are not to scale. Detailed description

[0045] Figures 1 and 2 schematically represent a quantum communication system 1 comprising a first set of devices 10, a second set of devices 20 and a third set of devices 30, capable of communicating with each other, according to embodiments of the invention.

[0046] The first set of devices 10 of the system 1 comprises a plurality of 10-n transmitter devices. The index 'n' is associated with the n-th transmitter device of the system 1 and is an integer between 1 and N, the value of N being greater than or equal to 2.

[0047] The second set of devices 20 of the system 1 comprises one or more receiver devices 20-m, also called 'intermediate receivers'. The index 'm' is associated with the m-th receiver device of the system 1 and is an integer between 1 and M, the value of M being greater than or equal to 1.

[0048] The third set of devices 30 of the system 1 comprises two receiving devices, also called 'final receivers', denoted 30-1 and 30-2 (or more generally 30-k, the index 'k' being an integer equal to 1 or 2).

[0049] The quantum communication system 1 can be used in various applications. For example and without limitations, the quantum communication system 1 can be used in the space domain and comprise a 10-n transmitter and / or a receiver (20-m and / or 30-k) mounted on board a satellite. In such an example of application of the invention to the space domain, the system 1 can also comprise a 10-n transmitter and / or a receiver (20-m and / or 30-k) on the ground, which can be embedded in one or more terrestrial devices. The system 1 can also be used in avionics applications, at least one of the 10-n transmitter devices and / or receivers (20-m and / or 30-k) then being an avionics device. The system 1 may also be used in fiber optic network applications, wherein at least one of the 10-n transmitter devices and / or one receiver (20-m and / or 30-k) is a fiber optic device integrated into a ground network.

[0050] A device of the system 1 may be fixed or in motion relative to another device with which it communicates.

[0051] By way of non-limiting example, devices of the quantum communication system 1 may be quantum computers or quantum sensor networks.

[0052] A transmitter 10-n comprises a signal generator 120 (also called a 'signal generation module') and at least one signal integrator (also called a 'signal integration module'), as shown in Figures 3 and 4 which illustrate embodiments of the invention.

[0053] As used herein, an 'optical signal' (also simply called a 'signal') results from one or more pulses of coherent light originating from an optical source, such as, for example, a laser beam. A laser beam may in particular be characterized by its pulse rate f and by a laser pulse (i.e., the signal) defined by its frequency te, its intensity T, its polarization P and its phase. The 'frequency œ' of the laser beam designates the 'optical frequency of the laser pulse multiplied by 2tt' defined as a function of the wavelength of the beam A, such that XX denotes the speed of light.

[0054] A transmitter 10-n of the first set of devices 10 of the system 1 is configured to generate and transmit, through a transmission channel 50, two distinct optical transmission signals, denoted Si 0 ni and Si 0 n2 (also called respectively 'first optical transmission signal' and 'second optical transmission signal').

[0055] The transmission channel 50 may be, for example, a free space or a fiber (or guided optics) device for transporting information using, for example, fiber optic elements for communication, according to the field of application of the invention.

[0056] Each optical emission signal delivered by a 10-n transmitter comprises a quantum signal, denoted Qni and Qn2 respectively. The two quantum signals Qni and Qn2 are entangled with each other, each photon of a quantum signal coming respectively from an entangled pair of photons generated by the signal generator 120. The first quantum signal Qni is associated with a polarization state, denoted PQ nb and the second quantum signal Qn2 is associated with a polarization state, denoted PQ n2.

[0057] As used herein, the term 'quantum signal' refers to an optical signal comprising at least one photon that is entangled with another photon of another 'quantum signal'. These two quantum signals are then called 'entangled quantum signals'. An 'entangled photon pair' refers to two photons forming a linked system, and exhibiting quantum states dependent on each other regardless of the distance separating them. There are correlations between the physical properties (in particular between their polarization state), which can be measured, of these distinct particles. The entanglement of a photon pair arises from the fact that these photons, respectively included in a specific quantum signal, are both generated from the same pump photon. Entangled quantum signals can be pulsed or continuous optical signals.Measuring a quantum signal provides a measure of detection of a photon (or 'particle') depending on a 'detection probability' of that photon.

[0058] In embodiments, the polarization states PQ ni and PQ n2, of the first and second quantum signals Qni and Qn2 respectively may be identical (i.e. correlated) and / or orthogonal to each other (i.e. anticorrelated). Advantageously, the polarization states PQ ni and PQ n2 of the entangled quantum signals are not individual polarization states well defined at the generation of the signals, and may only be defined during an entanglement measurement.

[0059] The first optical emission signal SiO ni delivered by the transmitter 10-n is a multiplexed optical signal (also called 'multiplexed optical signal' or 'signal of multiplexed communication') comprising the first quantum signal Qni and a first integrated optical polarization control signal, denoted Rni. Such a signal is also called 'first control signal' or 'first reference signal'.

[0060] In embodiments, the polarization state of the first control signal Rni may be defined in a polarization basis BQ ni (also called 'first control polarization basis'). For example and without limitation, the polarization basis BQ ni may be the polarization basis H / V comprising a linear polarization state of type H, i.e. "horizontal", and a linear polarization state of type V, i.e. "vertical". In other embodiments, the polarization basis BQ ni may be the polarization basis D / A comprising a linear polarization state of type D, i.e. "diagonal", and a linear polarization state of type A, i.e. "anti-diagonal".

[0061] In certain embodiments, the first multiplexed optical signal SiO ni delivered by the transmitter 10-n may further comprise a second integrated optical polarization control signal, denoted Rn2. Such a signal is also called 'second control signal' or 'second reference signal'. Advantageously, the polarization state of the second control signal Rn2 may be defined in a polarization base BQ n2 (also called 'second control polarization base'). In particular, the polarization base BQ n2 may be a polarization base non-orthogonal to the polarization base BQ ni of the first control signal Rnb

[0062] In certain embodiments, the second optical emission signal Si0. n2 delivered by the transmitter 10-n may also be a multiplexed optical signal comprising, in addition to the second quantum signal Qn2, the first control signal Rni and / or the second control signal Rn2.

[0063] An intermediate receiver 20-m of the second set of devices 20 of the system 1 is configured to receive, from the transmission channel 50, on the one hand a multiplexed optical signal, SiO n (i.e. a signal Si0. ni or Si0. n 2), transmitted by a first transmitter 10-n of the first set of devices 10, and on the other hand an optical transmission signal, Sio h (corresponding to a signal Si0. h 1 or Si0. h 2) transmitted by a second transmitter, denoted 10-h, of the first set of devices 10 and different from the first transmitter 10-n, the index 'h' being an integer between 1 and N and different from the index 'n'. Thus, as illustrated in Figures 1 and 2, the intermediate receiver 20-1 for example is configured to receive on the one hand the first optical transmission signal transmitted by the first transmitter 10-1, and on the other hand an optical transmission signal transmitted by the second transmitter 10-2.The first optical transmission signal received by the intermediate receiver 20-1 is the first optical transmission signal Sio-n transmitted by the first transmitter 10-1 corresponding to a multiplexed optical signal. comprising a quantum signal Qn (or Qni) and at least a first control signal Rni. Furthermore, the optical transmission signal transmitted by the second transmitter 10-2 may be either the first optical transmission signal S10-21 corresponding to a multiplexed optical signal, or the second optical transmission signal S10-22 also corresponding to a multiplexed optical signal, or comprising only a quantum signal Qh (or Q22, as in the example illustrated in Figures 1 and 2).

[0064] The intermediate receiver 20-m is then configured to perform an estimation of the first control signal Rn[ received, via the optical transmission signal transmitted by the first transmitter 10-n, which provides a first estimated control signal, noted Rm nb

[0065] In embodiments where the multiplexed optical signal Sio-n received by the intermediate receiver 20-m, transmitted by the first transmitter 10-n, comprises a second control signal Rn2, the intermediate receiver 20-m can further be configured to perform an estimation of the second control signal Rn2 received, transmitted by the first transmitter 10-n, which provides a second estimated control signal, denoted Rm n2.

[0066] In certain embodiments where the optical transmission signal Sio_h transmitted by the second transmitter 10-h and received by the intermediate receiver 20-m is a multiplexed optical signal comprising a first control signal Rh[ and / or a second control signal Rh2, the intermediate receiver 20-m can further be configured to perform an estimation of the first and / or second control signal Ru and / or Rh2 received, transmitted by the second transmitter 10-h, which provides a third and / or a fourth estimated control signal, denoted respectively Rmh[ and Rmh2.

[0067] Furthermore, the intermediate receiver 20-m is configured to perform a correlated measurement of quantum signals, relating to the quantum signal Qn of the multiplexed optical signal Si0.n received, transmitted by the first transmitter 10-n, and to the quantum signal Qh (ie Qh 1 or Qh 2) of the optical emission signal Sio h (ie Si0. h 1 or Sio_ h 2 respectively) received, transmitted by the second transmitter 10-h. The correlated measurement of quantum signals is further performed from the first estimated control signal Rmni by the intermediate receiver 20-m.

[0068] In embodiments, the correlated measurement of quantum signals can further be performed from the second estimated control signal Rmn2, the third estimated control signal Rmhi and / or the fourth estimated control signal Rmh2.

[0069] Each of the quantum particles from the two quantum signals, i.e. Qn and Qh, received separately by the intermediate receiver 20-m is associated with an independently generated entangled pair of photons. Furthermore, the particles of the first quantum signal Qn 1 of the multiplexed optical signal Si0-ni transmitted by the first transmitter 10-n to the receiver 20-m, belong to an entangled pair associated to the particles of the second quantum signal Qn2 of the optical emission signal Si0. n2 emitted by the first emitter 10-n. In the same way, the particles of the quantum signal Qh, for example and without limitation of the first quantum signal Qu, of the optical emission signal Sio hi transmitted by the second emitter 10-h to the receiver 20-m, belong to an entangled pair associated with the particles of the second quantum signal Qh2 of the optical emission signal Sio h2 emitted by the second emitter 10-h.

[0070] Advantageously, the correlated measurement of quantum signals carried out by the intermediate receiver 20-m can be a Bell measurement, projecting these received quantum particles, Qn and Qh, into a polarization-entangled Bell state. Such a projection induces an entanglement called 'resultant entanglement', between these received particles.This resulting entanglement consequently induces an entanglement called 'teleported entanglement' (or 'induced entanglement' or 'consequent entanglement'), between the quantum particles entangled with the particles Qn and Qh received by the 20-m receiver, that is to say respectively between: .

[0071] - the particles of the second quantum signal Qn2 of the optical emission signal Sion2 emitted by the first transmitter 10-n (ie not received by the receiver 20-m), and the particles of the second quantum signal Qh2 of the optical emission signal Sio h2 emitted by the second transmitter 10-h (ie not received by the receiver 20-m), if the intermediate receiver 20-m is configured to receive the multiplexed optical signal Sio-hi, or

[0072] - the particles of the second quantum signal Qn2 of the optical emission signal Sio n2 emitted by the first transmitter 10-n (i.e. not received by the receiver 20-m), and the particles of the first quantum signal Qhi of the multiplexed optical signal Sio-hi emitted by the second transmitter 10-h (i.e. not received by the receiver 20-m), if the intermediate receiver 20-m is configured to receive the optical transmission signal Si0_h2-

[0073] In embodiments, the two final receivers 30-1 and 30-2 (also called “additional receivers” or “auxiliary receivers”) of the third set of devices 30 of the system 1 can be configured to each receive a distinct optical transmission signal, originating from the transmission channel 50. The two optical transmission signals, each received by a final receiver 30-k, are transmitted independently by two distinct transmitters originating from the first set of devices 10. These optical transmission signals are thus not previously received by an intermediate receiver 20-m, any, of the second set of devices 20..

[0074] In embodiments, the first final receiver 30-1 can then be configured to receive an optical emission signal SiO n (and specifically Sio. n2) transmitted by a transmitter 10-n, while the second final receiver 30-2 can be configured to receive an optical emission signal Sio h (and specifically Sio h 2 or Sio-hi) transmitted by another transmitter 10-h of the first set of devices 10. Each final receiver 30-k can thus be configured to perform an estimation of the quantum signal from the received optical transmission signal, which provides an estimated received quantum signal, noted SQk respectively (i.e. SQi for the first final receiver 30-1 or Sq2 for the second final receiver 30-2).

[0075] For example and without limitation, as illustrated in Figures 1 and 2, the first final receiver 30-1 can be configured to receive the optical transmission signal Sim 2 (optionally being a multiplexed optical signal) transmitted by the first transmitter 10-1, and thus be configured to determine the estimated received quantum signal SQ i (i.e. estimation of the second quantum signal Qn from the signal Sim2).

[0076] In the example illustrated in [Fig. 1], the second final receiver 30-2 may be configured to receive the optical transmission signal S10-22 (optionally being a multiplexed optical signal) transmitted by the second transmitter 10-2, while in the example illustrated in [Fig. 2], the second final receiver 30-2 may be configured to receive the optical transmission signal S10-32 (optionally being a multiplexed optical signal) transmitted by a third transmitter 10-3 of the first set of devices 10. The second final receiver 30-2 may also be configured to determine the estimated received quantum signal SQ2 (i.e. estimation of the second quantum signal Q22 from the signal Si0.22, or Q32 from the signal Si0_32 for example).

[0077] Furthermore, in embodiments where the second set of devices 20 of the system 1 comprises a single intermediate receiver, then denoted 20-1, as shown in [Fig.l], the single receiver 20-1 can be further configured to generate two information signals each comprising the result of the correlated measurement of quantum signals carried out by the single receiver 20-1 (i.e. comprising the result of the projection of the quantum particles received independently into a Bell polarization state). Each information signal, denoted In or I22, comprising resulting entanglement information from the correlated measurement carried out, can be transmitted respectively to one of the two final receivers 30-1 or 30-2.

[0078] Alternatively, in embodiments where the second set of devices 20 of the system 1 comprises several intermediate receivers, as shown in [Fig. 2], a predetermined receiver 20-m among the second set 20 may be configured to generate a first information signal comprising the result of the correlated measurement of quantum signals, carried out by the predetermined receiver 20-m, while another receiver, denoted 20-p, also predetermined among the second set 20 may be configured to generate a second information signal comprising the result of the correlated measurement of quantum signals carried out by the other predetermined receiver 20-p. In this case, the index 'p' is an integer between 1 and M and different from the index 'm'. The first information signal, noted for example Imk, comprises resulting entanglement information from the correlated measurement, carried out by the predetermined 20-m receiver, and can be transmitted to a 30-k receiver of the two final receivers, while the second information signal, noted for example Ipq, comprises resulting entanglement information from the correlated measurement, carried out by the predetermined 20-p receiver, and can be transmitted to the other 30-q receiver of the two final receivers of the system 1. In this embodiment, the index 'q' is an integer equal to 1 or 2, and different from the index 'k'.

[0079] The information signals, generally denoted 1^, can be transmitted by an intermediate receiver to a final receiver of the system 1, through the transmission channel 50. Furthermore, a resulting entanglement information value, to be included in an information signal to be transmitted, can correspond, for example and without limitation, to an entanglement value equal to 1, associated with photons of quantum signals Qn and Qh received having identical polarization states between them (i.e. correlated), or alternatively to an entanglement value equal to 0 associated with received photons having different polarization states between them (i.e. anticorrelated).

[0080] Thus, each final receiver 30-k (30-1 and 30-2) of the third set of devices 30 of the system 1 can be configured to receive a single entanglement information signal Imk transmitted by an intermediate receiver 20-m of the second set of devices 20, and to determine (i.e. deduce therefrom) the associated resulting entanglement information(s).

[0081] According to one aspect of the invention, the first final receiver 30-1 and the second final receiver 30-2 of the third set of devices 30 of the system 1 can be configured to determine (i.e. establish) a quantum encryption key, using the received quantum signal SQi estimated by the first final receiver 30-1 and the received quantum signal SQ2 estimated by the second final receiver 30-2. In particular, such a quantum distribution of key(s) is also carried out from the entanglement information signals Imi and Im2 (or for example Imi and Iq2) received by the final receivers 30-k, and therefore from the associated resulting entanglement information, the two estimated received quantum signals SQk being associated respectively with a teleported entanglement generated by one or more resulting entanglements from one or more intermediate receivers 20-m.System 1 can thus be a quantum distribution system for encryption keys by quantum “teleportation”. That is to say, system 1 can be configured to carry out a quantum distribution of key(s) using one or more quantum repeaters, corresponding respectively to one or more intermediate receivers configured to “repeat” resulting entanglement information initially coming from several transmitters. of independently generated pairs of entangled photons. Quantum key distribution can be implemented in particular within a space or terrestrial communication service in order to ensure the security of some or all of the communications exchanged between the final receivers, for example.

[0082] Figures 3 and 4 schematically represent a transmitter 10-n of the first set of devices 10 configured to form at least one multiplexed optical signal, according to embodiments of the invention.

[0083] The multiplexed optical signal transmitted by the 10-n transmitter is generated via a signal integrator of the 10-n transmitter, from a quantum signal and at least one control signal, delivered by a signal generator 120.

[0084] In embodiments, the transmitter 10-n may comprise a single signal integrator, denoted 140-1 (or 140), configured to generate the multiplexed optical signal SiOni.

[0085] Advantageously, the transmitter 10-n can comprise two signal integration modules, denoted 140-1 and 140-2, each configured to generate a multiplexed optical signal. The first integrator 140-1 can be configured to generate the first multiplexed optical signal Sio-ni and the second integrator 140-2 can be configured to generate the second multiplexed optical signal Sio_n2-

[0086] The single (or first) signal integrator 140-1 is configured to generate the (first) multiplexed optical signal SiO ni, from the first quantum signal Qni and (at least) the control signal Rnb as shown in Figures 3 and 4.

[0087] In some embodiments where a transmitter 10-n is configured to produce both control signals Rni and Rn2, as shown in [Fig.4], the first (or single) signal integrator 140-1 may be configured to generate the (first) multiplexed optical signal Sio-ni, further from the second control signal Rn2.

[0088] In embodiments, the second signal integrator 140-2, shown in [Fig.4], may be configured to generate the second multiplexed optical signal Sio-n 2, from the second quantum signal Qn 2 and the first control signal Rnl and / or the second control signal Rn2.

[0089] Thus, in other words, an integration module of a 10-n transmitter, configured to generate a multiplexed optical signal, is adapted to optically multiplex (or optically combine), on the same optical path, a quantum signal with one or more control signals.

[0090] In embodiments where a 10-n transmitter is a guided optical (or all-optical) device, i.e. comprising optical signal transmission paths made up of optical fibers and / or so-called integrated waveguides, typically used in integrated photonics, one or more means of transmitting The transmitter can be made of polarization maintaining fibers, or PMF (acronym for Polarization Maintaining Fiber) and / or single-mode optical fibers, or SMF (acronym for Single Mode Fiber).

[0091] In embodiments, a multiplexed optical signal generated by a transmitter 10-n of the first set of devices 10 may be frequency multiplexed. In this case, the signal generator 120 of the transmitter may be configured to generate the entangled quantum signals, Qni and Qn2, of wavelength denoted XQ (or of respective wavelengths ni and XQ n 2, and also called 'quantum wavelength(s)'), and at least the first control signal Rni of control wavelength (or 'reference wavelength' denoted ^Rni), the quantum wavelength(s) being distinct from the control wavelength.

[0092] In embodiments, the signal generator 120 may further be configured to generate the second control signal Rn 2 of control wavelength denoted ^Rn 2, the wavelengths XQ, ^Rn[ and ÀRn 2 all three being distinct from each other. [Fig. 5] schematically represents such a signal generator 120, according to embodiments of the invention.

[0093] Advantageously, the signal generator 120 may comprise a first laser source 122-0 emitting a laser beam (or 'pump laser') of wavelength \pump. The pump wavelength of laser emission may be in the visible or infrared range. For example and in a non-limiting manner, the first laser source 122-0 may be a DFB laser diode (acronym for the corresponding English expression "Distributed Feedback") using a Bragg grating making it possible to choose the emission wavelength. The chosen emission wavelength of the laser diode may be equal to, for example, 780 nm. Such a laser diode emits in particular a continuous laser beam. Alternatively, the first laser source 122-0 may be a pulsed laser unit, i.e. with switched gain (or gain-switched according to the English expression).

[0094] The signal generator 120 may also comprise one or two other additional laser sources, denoted 122-1 and 122-2, as shown in FIG. 5, configured to respectively emit a laser beam of wavelength XR1 and a laser beam of wavelength XR2. The laser emission wavelengths XR1 and ^R2 may be in the visible or infrared range. For example and in a non-limiting manner, the additional laser source(s) 122-1 and 122-2 may be DFB laser diodes or pulsed laser units.

[0095] According to some embodiments, the signal generation module 120 may further comprise one or more intensity modulation units 124 configured to modulate the intensity of the laser pulses generated at the output of the first laser source 122-0 and form quantum pulses.

[0096] An intensity modulation unit 124 may also be configured to modulate the rate of the laser pulses, from the order of a few kilohertz up to a few tens of gigahertz for example, and / or the time width of the laser pulses, for example up to a few nanoseconds.

[0097] As shown in [Fig.5], the signal generation module 120 may further comprise an entanglement unit 126, configured to receive a single initial optical signal, denoted Sn0, and to deliver the two entangled quantum signals, corresponding to the first and second quantum signals Qn i and Qn2, comprising pairs of entangled photons. Such an entanglement unit 126 may advantageously be arranged at the output of an intensity modulation unit 124.

[0098] For example and without limitation, the entanglement unit 126 can be implemented in the form of a Sagnac loop, in which the passage of the initial optical signal Sn0 through a non-linear crystal (or a microresonator), in particular in two distinct directions, generates a pair of polarization-entangled photons. Such a non-linear crystal can be a PPLN crystal (or Periodically poled lithium niobate according to the corresponding English expression).

[0099] Advantageously, the quantum wavelengths kQ nl and kQ n 2 (or XQ) of the entangled quantum signals can be determined as a function of the pump wavelength \ompe of the initial optical signal Sn0. In particular, since the conservation of energy during the generation of a pair of entangled photons is respected, the sum of the frequencies of the entangled photons is equal to the frequency of the initial pump photon. By way of illustration, for a wavelength \ompe equal to 780nm, the quantum wavelengths can be approximately equal to 1560nm, to respect the conservation of energy.

[0100] In embodiments, the frequency difference between a quantum wavelength kQ and a reference wavelength (kR1 and / or XR2) may be greater than or equal to a first minimum wavelength difference value Sk, according to the following inequality (01):

[0101] |Xq-Xr1 / R2| >ôà (01)

[0102] Furthermore, in embodiments where the generator 120 comprises two distinct laser sources 122-1 and 122-2, the frequency difference between the reference wavelengths (XR1 and / or XR2) of each of the control signals Rn[ and Rn 2 may be greater than or equal to a second minimum value 5X' of wavelength difference, according to the following inequality (02):

[0103] |^R1'^R2| >SK (02)

[0104] Advantageously, the first minimum value dÀ and the second minimum value <5X' of wavelength difference may be predefined and equal, for example and without limitation, to 1.6nm and 0.8nm respectively.

[0105] In embodiments where the transmitter 10-n is a device comprising means for transmitting a signal in free space, an entanglement unit 126 of the signal generator 120 may comprise one or more dichroic filters making it possible in particular to direct the initial optical signal Sn0 towards the Sagnac loop and / or to separate (i.e. filter), on two distinct optical paths, the two photons of each entangled pair of photons formed to deliver the two entangled quantum signals Qn i and Qn2.

[0106] In the embodiments where a multiplexed signal generated by the transmitter 10-n is frequency multiplexed (i.e. the quantum wavelengths XQ and reference wavelengths XR1 and / or XR2 are distinct from each other), a signal integrator (140-1 and / or 140-2) of the transmitter 10-n may comprise one or two wavelength division multiplexing or WDM units (meaning Wavelength Division Multiplexing), each unit being adapted to combine a quantum signal considered and one of the control signals (Rn i or Rn 2) on the same optical path into a resulting signal.

[0107] In embodiments, such a signal integrator may alternatively comprise one or two dichroic filters, each filter being adapted to combine a quantum signal considered and one of the control signals (Rn[ or Rn2) on the same optical path into a resulting signal.

[0108] In embodiments, a multiplexed optical signal generated by a 10-n transmitter of the first set of devices 10 may be time-multiplexed. In this case, such a multiplexed signal may be a signal comprising a set of two or three temporally distinct pulses, the set being repeated according to a period T, the distinct pulses corresponding respectively to an entangled quantum signal, Qni or Qn2, a first control signal Rn i and / or a second control signal Rn 2.

[0109] Advantageously, the entangled quantum signals and the control signals generated by the signal generator 120 can be pulse signals characterized by a period T identical to the period of the multiplexed signal delivered by the transmitter 10-n.

[0110] In embodiments, the signal generator 120 may be configured to generate the pair of entangled particles (Qni and Qn2) and the control signals Rn i and Rn 2 according to a predefined time offset between each pulse. Alternatively (or additionally), a signal integrator (140-1 and / or 140-2) may be configured to apply a predefined time shift between a quantum signal and a control signal so as to obtain time-multiplexed signal pulses.

[0111] It should be noted that in the embodiments involving time multiplexing, the entangled particles (Qni and Qn2) of the same pair are not time shifted.

[0112] The resulting time difference between each of the successive distinct pulses in a multiplexed signal can thus be strictly less than the repetition period T of the resulting signal (or of the quantum signal), according to the following inequalities (03) and (04):

[0113] |tQ-tR1 / R2| <T(03)

[0114] |tR1-tR2| <T(04)

[0115] In these embodiments where the multiplexed signal generated by a 10-n transmitter is time-multiplexed, the quantum wavelengths XQ and reference (XR1 and / or XR2) may be equal to each other.

[0116] In this case, the first laser source 122-0 and the additional laser source(s) 122-1 and 122-2 may for example correspond to a single laser source 122-0, and the signal generator 120 may further comprise a beam splitting unit (not shown in the figures) configured to provide one or two signal components associated with the control signals Rn i and Rn 2, as well as another signal component associated with the initial optical signal Sn0. Such a beam splitting unit may comprise one or more optical couplers, symmetrical or asymmetrical, for example polarization-maintaining. The beam splitting unit may further be an optical selector generating a predefined time shift between each delivered signal component.

[0117] In embodiments, the beam splitting unit of the signal generator 120 may be arranged at the output of the first laser source 122-0, the resulting control signals Rn i and Rn 2 then corresponding to conventional (i.e. non-quantum) light pulse signals. Alternatively, this beam splitting unit may be arranged at the output of an intensity modulation unit 124, the resulting control signals Rn i and Rn 2 then corresponding to low light intensity signals.

[0118] Figures 6 and 7 schematically represent a 20-m intermediate receiver comprising at least one received multiplexed optical signal processing chain, and a correlation module 260, according to embodiments.

[0119] The correlation module 260 of a 20-m intermediate receiver is configured to perform a correlated measurement of a first received quantum signal Qmi from from a first 10-n transmitter, with a second received quantum signal Qm 2 from a second 10-h transmitter.

[0120] In particular, the correlation module 260 may be implemented in the form of an optical instrument, such as an optical interferometer for example, to perform a Bell measurement (corresponding to a Bell measurement module). Such a correlation module 260 comprises in particular a plurality of detection units. Each detection unit may be adapted to measure one or more quantum signals according to a predefined measurement polarization state, for example, in a B26D polarization basis (also called 'measurement polarization basis' and corresponding for example and without limitations to an H / V basis or a D / A basis).

[0121] A processing chain of an intermediate receiver 20-m, denoted Cm, is configured to receive a multiplexed optical signal and deliver a received quantum signal Qm. For example, as shown in FIGS. 6 and 7, a processing chain Cm can be configured to receive the multiplexed optical signal SiO n or SiO ni) transmitted by a first transmitter 10-n and deliver the first received quantum signal Qmi associated with the signal Qn (or Qni) transmitted by the first transmitter 10-n via the signal SiO n.

[0122] A processing chain Cm is further adapted to determine the polarization state of the control signal(s) originating from the received multiplexed optical signal. For example, the processing chain Cm may be associated with the first control polarization base BQ ni and be adapted to measure in this base the polarization state of the first control signal Rni transmitted by the first transmitter 10-n via the multiplexed optical signal Sio-n- The processing chain Cm may further be associated with the second control polarization base BQ n 2 and be adapted to measure in this second base the polarization state of the second control signal Rn 2 transmitted by the first transmitter 10-n via the multiplexed optical signal SiO n.

[0123] A processing chain Cm is further adapted to align a determined polarization state with one of the predefined measurement polarization states of the correlation module 260. In embodiments, the measurement polarization basis B260 may correspond to the first control polarization basis BQ ni. Alternatively, the measurement polarization basis B260 may correspond to the second control polarization basis Bq n 2. As used herein, the expression 'alignment of a polarization state with a polarization basis' refers to a rotation of the polarization state of the signal so that it corresponds to a proper detection axis of the basis determined by a quantum signal detection equipment.

[0124] Thus, a Cm processing chain of a 20-m intermediate receiver can be adapted to perform a rotation of the polarization state of all the signals from the multiplexed optical signal received, at the input of the processing chain Cm, to ensure that the particles of the quantum signal Qm at the output of the processing chain Cm are aligned with the measurement polarization base B26o •

[0125] In embodiments, as shown in [Fig.7], an intermediate receiver 20-m may comprise two processing chains Cm configured to each process either the multiplexed optical signal SiO n transmitted by the first transmitter 10-n, or the multiplexed optical signal Sio h transmitted by the second transmitter 10-h.

[0126] In other embodiments, an intermediate receiver 20-m may comprise a single processing chain Cm configured to process the multiplexed optical signal Si0.n transmitted by the first transmitter 10-n, as shown in [Fig.6]. In this case, the optical transmission signal Sio h transmitted by the second transmitter 10-h is not a multiplexed signal and only comprises a quantum signal Qh, corresponding directly to the second received quantum signal Qm2 from a second transmitter 10-h.

[0127] Advantageously, a processing chain Cm may comprise a control loop between a polarization state correction module 220 and a control signal detection module 240. As shown in [Fig.8], the correction module 220 may be arranged upstream of the detection module 240.

[0128] A correction module 220 of a 20-m intermediate receiver can be configured to modify the polarization of a signal passing through it, in response to a setpoint signal. The correction module 220 can therefore be configured to receive a multiplexed optical signal (for example Si0.n, or more precisely SiO ni, transmitted by a first 10-n transmitter) and deliver a multiplexed optical signal with modified polarization, denoted Sm.

[0129] The setpoint signal of the correction module 220 may be an electrical or radiofrequency signal for example. Advantageously, a correction module 220 may be a fiber polarization controller comprising in particular one or more polarization rotation fibers whose constraint axis(es) (adapted for rotating the polarization of the signal) are controlled (or adjusted) from the setpoint signal. For example and without limitation, such a controllable constraint axis may be implemented in the form of a wound fiber component of adjustable geometry, or using a piezoelectric element inducing mechanical stresses on a fiber. Alternatively, a correction module 220 may comprise one or more so-called active delay plates, i.e. whose blade rotation (i.e. its optical axis) is controlled (or adjusted) from the setpoint signal.The correction module 220 may be, for example and without limitation, a triplet of delay blades. active successively comprising a quarter-wave plate, a half-wave plate and a quarter-wave plate.

[0130] In embodiments, the transmission means of an intermediate receiver 20-m, and in particular of a processing chain Cm, may be single-mode optical fibers SMF, and / or advantageously, polarization-maintaining fibers PMF.

[0131] Figures 9 and 10 schematically represent a detection module 240 of a processing chain Cm comprising a signal demultiplexing unit 242 and a device DA for analyzing polarization of the control signal, according to embodiments of the invention.

[0132] The signal demultiplexing unit 242 can receive as input the polarization-modified multiplexed optical signal Sm and can be configured to separate from this signal a received quantum signal component Qm relating to the quantum signal from the received multiplexed signal, and respectively one or two received control signal components Rm relating to the control signal or signals from the received multiplexed signal. For example, for a received multiplexed optical signal Si0.n transmitted by a first transmitter 10-n and comprising the quantum signal Qn (or Qni) and the control signal Rn[, the demultiplexing unit 242 can be configured to determine the signal quantum component Qm relating to the quantum signal Qn i and the signal control component Rm relating to the control signal Rn[.

[0133] The demultiplexed quantum component Qm of the signal Sm at the output of the unit 242 can then be routed to the correlation module 260 of the intermediate receiver 20-m, while the control component Rm can be routed to an analysis device DA.

[0134] In embodiments where the received multiplexed optical signal Si0.n comprises the quantum signal Qni and the two control signals Rn[ and Rn2, the demultiplexing unit 242 may be configured to separate the quantum component Qm relating to the quantum signal Qnb, a first signal control component Rmi relating to the first control signal Rn[ and a second signal control component Rm2 relating to the second control signal Rn2. In this case, the first control component Rm[ may be routed to a first analysis device, while the second control component Rm2 may be routed to a second analysis device (not shown in the figures).The two analysis devices are configured in a similar manner, each being adapted to the characteristics of the control component to be processed, i.e. to the control polarization base (BQ ni and BQ n 2) to be used and optionally to the reference wavelength considered. The use of two separate analysis devices. allows to obtain a better estimate of the polarization rotations (or distortions) undergone by the multiplexed optical signal SiO n between transmission and reception on the transmission channel. For example and without limitation, the second analysis device can be used to confirm the polarization analysis of the control signal determined by the first analysis device.

[0135] In embodiments involving time division multiplexing where the received multiplexed optical signal Si0.n comprises the quantum signal Q„i and the two control signals Rni and Rn2, the demultiplexed first and second signal control components Rm[ and Rm2 may be routed to a single analysis device, configured to alternately analyze these components as a function of the time difference between successive distinct pulses associated with the control signals.

[0136] The demultiplexing unit 242 of a detection module 240 may in particular comprise one or more demultiplexing elements determined as a function of the type of multiplexing of the signal by the transmitter considered, i.e. frequency and / or time.

[0137] In embodiments where the received multiplexed signal is frequency multiplexed, the demultiplexing unit 242 may comprise at least one filter configured to separate the quantum component Qm from a control component Rm. For example and without limitation, such a filter may be a band rejection filter such as an FBG filter (acronym for Fiber Bragg Grating) or a filter called “Add / Drop WDM”. The filter may be chosen from the predetermined frequency difference between the quantum wavelength \> and a reference wavelength (XR1 and / or / vR2), defined for example by equation (01).

[0138] In embodiments, the demultiplexing unit 242 may further comprise a filter configured to separate control components from each other. Such a filter may be chosen from the predetermined frequency difference between the reference wavelengths XR1 and ^R2 of each of the control signals, and defined for example by equation (02).

[0139] The transmission means 240-i and 242-i at the output of the demultiplexing unit 242 to the correlation module 280 and the analysis device DA respectively, as well as transmission means included in the unit 242 (not shown in the figures), may be single-mode optical fibers SMF. Advantageously, these transmission means may be polarization-maintaining fibers PMF.

[0140] A DA analysis device for polarizing the control signal of a processing chain Cm can be configured to detect the control component Rm to be processed, according to a predefined polarization base, so as to provide an estimated control signal.

[0141] It should be noted that at the output of a 10-n transmitter, a control signal (Rn i and / or Rn 2 ) is characterized by its well-defined polarization state. During the propagation of a multiplexed signal between the 10-n transmitter and an intermediate 20-m receiver, the polarization state of the control signal considered may have undergone random rotations so that the polarization state of the control component Rm received and detected, relative to the control signal considered, may be different from the initially defined polarization state.

[0142] Thus, the control signal polarization analysis device DA may comprise at least one detection unit configured to detect the control signal considered, in particular according to a predefined polarization, so as to provide the estimate of the control signal received (for example Rmni, or Rmn 2 respectively).

[0143] In embodiments, a detection unit of the DA analysis device may be adapted to detect conventional light pulse signals. For example and without limitation, such a unit may be a photodiode configured to deliver a photocurrent, depending on the measurement of the received control signal component associated with the processing chain Cm.

[0144] Alternatively, a detection unit of the DA analysis device may be a single photon detection unit. Such a unit may be composed of a detection surface configured to detect the “presence” of single photons at its detection surface (i.e. by photon / surface interaction). This detection of the presence of single photons is defined according to a given detection quantum efficiency. For example and without limitation, the single photon detection unit may be an avalanche photodiode or APD (acronym for the corresponding English expression Avalanche Photodiode Detectof) or a superconducting nanowire single photon detector or SNSPD (acronym for the corresponding English expression Superconducting Nanowire Single Photon Detectof).In particular, the single photon detection unit may include an internal amplification mechanism configured to output a voltage when a photon is detected.

[0145] In certain embodiments, as shown in [Fig.9], the analysis device DA may comprise a polarizer 244-A and a single detection unit 246 of the control component Rm associated with the control signal considered, for example Rn[ (or Rn 2). The polarizer 244-A (also called 'polarizing filter') may be arranged to transmit to the detection unit 246 only the optical signals defined in a predefined polarization state. The detection unit 246 is thus configured to detect the light energy relating to the control component Rm defined only according to the considered polarization state (i.e. of the predefined polarization base processed by the analysis device DA), and to provide the estimate of the received control signal, for example Rmni (or Rmn2 respectively). According to this configuration, the value of the control signal detected (or measured) by the detection unit 246 is maximum if the polarization state of the received control signal component is equal to the predefined polarization state. Conversely, the value of the detected control signal may be minimum if the polarization state of the received control signal component is orthogonal to the predefined polarization state.

[0146] Advantageously, the DA analysis device can comprise a polarizing detection unit directly grouping (i.e. combining) the functionalities of the polarizer 244-A and the detection unit 246.

[0147] In embodiments, as shown in [Fig. 10], the analysis device DA may comprise a polarized beam separation unit 244-B, preceded by two separate detection units 246-1 and 246-2. The polarized beam separation unit 244-B (also called a 'polarizing separator') may be adapted to provide two polarized signal sub-components relating to the control component Rm considered. Each sub-component may propagate on a transmission means (244-il or 244-i2) at the output of the separation unit 244-B to one of the two detection units (246-1 or 246-2) then defined only in one of the two polarization states of the predefined polarization base processed by the analysis device DA).Each detection unit (246-1 and 246-2) is thus configured to detect the light energy relating to one of the two polarized sub-components of the control component Rm to provide the estimate of the received control signal. For example and without limitation, according to this configuration, the value relating to the estimated control signal, measured by the first detection unit 246-1, may be maximum, and the value measured by the second detection unit 246-2 may be minimum, if the polarization state of the control component Rm is equal to the initial polarization state of the control signal considered emitted by the transmitter.Conversely, the value relative to the estimated control signal, measured by the first detection unit 246-1, may be minimal and the value measured by the second detection unit 246-2 may be maximal, if the polarization state of the control component Rm is orthogonal to the initial polarization state of the control signal considered emitted by the transmitter.

[0148] For example and without limitation, a DA device for analyzing the polarization of a received Rm control component associated with the H / V diagonal base may comprise a separation unit 244-B configured to provide a first sub-component having a linear polarization of type H propagating on the transmission means 244-il, and a second sub-component having a V-type linear polarization propagating on the transmission means 244-i2. In this example, the two corresponding detection units 246-1 and 246-2 are therefore configured to respectively detect the sub-component relating to the H-type linear polarization of the control component Rm and the sub-component relating to the V-type linear polarization of the control component Rm.

[0149] In certain embodiments, the detection unit(s) (246, or 246-1 and 246-2) of a DA analysis device may be adapted to the reference wavelength XRx (i.e. ΔR1 or ΔR2) of the control component Rm to be detected.

[0150] The 20-m intermediate receiver may further comprise one or more processors (also called 'central computing units') or CPU (acronym for the English expression Central Processing Unit).

[0151] In embodiments, each DA analysis device of the 20-m receiver may comprise a specific processor, generally denoted 248, configured to analyze the electrical signal(s) from the detection unit(s) (246, or 246-1 and 246-2) corresponding to the estimated control signal, associated with the DA analysis device. A processor 248 may be configured to generate a servo signal, denoted Sc, corresponding to a polarization correction setpoint signal to be delivered to the correction module 220 associated with the processing chain Cm.

[0152] In certain embodiments, the intermediate receiver 20-m may comprise a single processor 248, configured to analyze all of the electrical signals from the detection units of the analysis devices of the receiver 20-m. In this case, the processor 248 may be configured to generate a servo signal Sc specific to each correction module 220 of a processing chain Cm.

[0153] A control loop of a processing chain Cm (i.e. polarization correction loop generating a control signal) can be implemented continuously or intermittently. A processor 248 can thus be configured to control the control loop(s) of the intermediate receiver 20-m. In particular, a control loop can be activated periodically and / or after evaluation of the polarization state of one or both estimated control signals with respect to one or more associated polarization base(s) polarization states. Furthermore, a control loop can be implemented until alignment of the polarization state of one or both estimated control signals with an associated chosen (or reference) polarization state and / or in a chosen polarization base.

[0154] In embodiments, a processor 248 of the intermediate receiver 20-m can be configured to determine for a specific correction device D a polarization state difference value <5p between the polarization state of the estimated control signal considered and the polarization state of the polarization base associated with the correction device D. The processor 248 can further be configured to evaluate whether this polarization state difference value <5p is strictly greater than (or greater than or equal to) a predefined reference difference value <5pref.

[0155] In particular, a control loop can be activated if a determined polarization state difference value dp is greater than or equal to the reference difference value <5pref.

[0156] Advantageously, a control loop can be implemented so as to optimize (i.e. maximize or minimize) the detection of the component of the control signal(s) according to the associated polarization state(s).

[0157] For example and without limitation, a servo signal of a servo loop can be generated from a differentiable optimization algorithm, such as a gradient descent algorithm, so as to search (by incrementation or iteration) for an optimal point of an objective function associated in particular with the determined polarization state difference value of a correction device D of the 20-m receiver. If an optimal point is found, the servo loop can be stopped.

[0158] The control loop can also be stopped, for example and without limitation, if a determined polarization state difference value ôp is evaluated to be strictly less than (or less than or equal to) the reference difference value dp ref*

[0159] Thus, in embodiments, a control signal Sc relating to the setpoint signal of a correction module 220 can be generated to control this module 220 and in particular to rotate the polarization of the received multiplexed signal until the value of the estimated control signal, measured by the detection unit 240 (for example via the first detection unit 246-1), is optimal, that is to say that the polarization state of the control component Rm is then equal to the initial polarization state of the control signal considered emitted by the transmitter, or alternatively orthogonal to it. The modification of the polarization of the multiplexed signal received via the control signal Sc thus induces a modification of the polarization state of the quantum signal Qm demultiplexed from the signal Sm, at the output of the unit 242, and routed to the correlation module 260 of the receiver 20-m.

[0160] Furthermore, the detection units of the correlation module 260 of a 20-m intermediate receiver may be single photon detection units. detection of the quantum components, Qmi and Qm2, makes it possible to provide at least one entanglement information signal Imk to be provided respectively to a final receiver 30-k of the third set of devices 30 of the system 1.

[0161] In embodiments, a correlation module 260 of a 20-m intermediate receiver may comprise at input one or two additional demultiplexing units (not shown in the figures). Each additional demultiplexing unit of the correlation module 260 is associated with one of the quantum components, Qmi or Qm2, and may be equivalent to the signal demultiplexing unit 242 of the detection module 240 of a processing chain Cm, and configured to transmit the quantum component considered to the Bell measurement module for example. The residual component(s) of the control signals from the demultiplexing unit are then directed towards a beam absorber.

[0162] The additional demultiplexing unit of the correlation module 260 may in particular comprise a demultiplexing element determined as a function of the type of multiplexing of the signal Sm. For example, for frequency multiplexing, the additional demultiplexing unit may be a spectral filter configured to separate a quantum signal Qm from the two residual components of the integrated signals, such as an FBG filter or an “Add / Drop WDM” filter, and chosen from the predetermined frequency difference between the quantum wavelength λQ and the reference wavelengths (kR1 and / or λR2).

[0163] Such an additional demultiplexing unit in the correlation module 260 makes it possible in particular to increase the filtering capacity of the control signal(s) of the multiplexed signal(s) received at the input of the intermediate receiver 20-m, in order to improve the quantum correlation measurement carried out by the module 260.

[0164] [Fig. 11] schematically represents a final receiver 30-k comprising a received multiplexed optical signal processing chain, and a quantum photon analysis module 360, according to embodiments. In this case, the final receiver 30-k can be configured to receive an optical transmission signal being a multiplexed signal SiO n transmitted by a transmitter 10-n of the first set of devices 10. Such a signal can for example be the multiplexed signal Si0_n2 comprising a quantum signal Qn 2 and a first control signal Rni and / or a second control signal Rn2.

[0165] A processing chain of a 30-k final receiver, denoted Ck, can be configured to receive a multiplexed optical signal and deliver a received quantum signal Qk relating to the quantum signal from the multiplexed signal Si0_n. The 360 ​​quantum photon analysis module of a 30-k final receiver can be adapted to measure the received quantum signal, according to at least one polarization state defined in a polarization basis.

[0166] The processing chain Ck may be adapted to determine the polarization state of the control signal(s) originating from the multiplexed optical signal received by the final receiver 30-k. The processing chain Ck may further be adapted so as to align this determined polarization state with one of the predefined measurement polarization states of the analysis module 360. Thus, the processing chain Ck may be adapted to perform a rotation of the polarization state of all the signals originating from the multiplexed optical signal received, at the input of the processing chain Ck, to ensure that the particles of the quantum signal received Ck at the output of the processing chain Ck are well aligned in the polarization base associated with the analysis module 360. The processing chain Ck may thus be equivalent (comprising similar units) to a processing chain Cm of a 20-m intermediate receiver, as illustrated in [Fig.8].

[0167] In particular, the Ck processing chain of a 30-k final receiver may comprise a control loop between a polarization state correction module arranged upstream of a control signal detection module.

[0168] The correction module of the processing chain Ck (equivalent to the correction module 220 of a processing chain Cm of a 20-m receiver) can be configured to modify the polarization of a signal passing through it, in response to a setpoint signal. The correction module is therefore configured to receive a multiplexed optical signal SiO n received by the final receiver 30-k (for example Si0.n 2 transmitted by a first transmitter 10-n) and deliver a multiplexed optical signal with modified polarization, noted Sk for example.

[0169] The detection module of the processing chain Ck (equivalent to the correction module 240 of a processing chain Cm of a 20-m receiver and (thus illustrated in FIGS. 9 and 10) may comprise a signal demultiplexing unit and at least one device for analyzing the polarization of the control signal. The demultiplexing unit may be configured to separate the multiplexed optical signal with modified polarization, into at least one component of the received quantum signal Qk then routed to the quantum photon analysis module 360. A device for analyzing the polarization of the control signal, in the processing chain Ck, may be configured to process a component of the received control signal from the multiplexed optical signal with modified polarization, in particular to generate a control signal corresponding to the polarization correction setpoint signal to be delivered to the correction module of the processing chain Ck.

[0170] In embodiments where a 30-k end receiver is configured to receive a transmit optical signal comprising only a quantum signal (i.e., no multiplexed), the optical emission signal Si0.n then corresponds directly to the received quantum signal Qk to be processed by the analysis module 360.

[0171] The analysis module 360 ​​of a 30-k final receiver may comprise at least one single photon detection unit. The detection of the received quantum signal Qk makes it possible to provide the estimated received quantum signal SQk and thus an estimation of the polarization state of the signal with respect to one or more polarization states defined in a polarization base.

[0172] In some embodiments, the analysis module 360 ​​may comprise a single single photon detection unit 366 configured to detect the received quantum signal Qk defined according to a predetermined polarization state.

[0173] In other embodiments, as shown in [Fig. 12], the analysis module 360 ​​may comprise a switching unit 364, preceded by two single photon detection units 366-1 and 366-2. The switching unit 364 may be equivalent to the polarized beam separation unit 244-B of an analysis device DA included in an intermediate receiver 20-m. The switching unit 364 may therefore be adapted to direct (i.e. route or switch) the demultiplexed quantum signal Qk of the multiplexed signal SiO n received at the input of the final receiver 30-k to one of the two single photon detection units (366-1 or 366-2) depending on the polarization state of the quantum signal. Each single photon detection unit (366-1 and 366-2) is thus configured to detect the presence of single photons defined according to one of the polarization states of the polarization base, processed by the analysis module 360 ​​(i.e. the final 30-k receiver considered)

[0174] By way of illustration, for an analysis module 360 ​​associated, for example and without limitation, with the H / V base, may comprise the switching unit 364 configured to direct the received quantum signal Qk having a horizontal type linear polarization H, towards the first single photon detection unit 366-1 via the transmission means 364-il, or to direct the received quantum signal Qk having a vertical type polarization V, towards the second single photon detection unit 366-2 via the transmission means 364-i2.

[0175] In embodiments where the optical emission signal SiO n received by the final receiver 30-k is a multiplexed signal, the analysis module 360 ​​may comprise at input an additional demultiplexing unit 362, equivalent to a signal demultiplexing unit 242 of a processing chain Cm, or to an additional demultiplexing unit of the correlation module 260, included in an intermediate receiver 20-m. The additional demultiplexing unit 362 may thus be configured to transmit the received quantum signal Qk to the single photon detection unit 366, or to the switching unit 364, as shown in the [Fig. 12]. The residual components of the control signals are then directed to a beam absorber 362-0 as shown in [Fig. 12].

[0176] Furthermore, the analysis module 360 ​​of a final receiver 30-k may comprise a processor 368 configured to analyze the electrical signal(s) from the detection unit(s) (366, or 366-1 and 366-2) corresponding to the estimated received quantum signal SQk. The processor 368 of a final receiver 30-k may be configured to determine a quantum encryption key, i.e. a key shared with the other by the final receiver 30-q, from the estimated received quantum signal SQk and the entanglement information signal Imk received by the final receiver 30-k.

[0177] The determination of a quantum encryption key can be carried out from a quantum key distribution protocol, such as for example a protocol comparable to the protocol named BBM92 (as described in the article “Quantum cryptography without Bell's theorem” by C. Bennett, G. Brassard and D. Mermin, 1992, Physical Review Letters 68 (5), p. 557-559).

[0178] In embodiments, such as for example when the control signals are quantum signals and the multiplexed signal received by the final receiver 30-k is a time-multiplexed signal, the processing chain Ck may consist of a polarization state correction module and at least part of the analysis module 360. In this case, the module 360 ​​configured to detect the received quantum signal Qk, may further be configured to detect one or more of the control signals from the multiplexed optical signal received by the final receiver 30-k. In this case, the processor 368 may also be configured to generate a servo signal corresponding to a polarization correction setpoint signal to be delivered to the correction module of the processing chain Ck.

[0179] [Fig. 13] represents the method of transmitting optical signals implemented by a 10-n transmitter, according to embodiments of the invention.

[0180] The method for emitting optical signals comprises a preliminary step 1020 of generating two entangled quantum signals Qn[ and Qn2, as well as at least one optical polarization control signal Rni.

[0181] In step 1040, the polarization control optical signal Rn[ is inserted on the optical path carrying the first entangled quantum signal Qn[ so as to generate a multiplexed optical signal Sio_ni-

[0182] In step 1060, the multiplexed optical signal SiO ni and an optical emission signal comprising the second quantum signal Qn2 are transmitted through a transmission channel 50.

[0183] [Fig. 14] shows the method of intermediate reception of optical signals implemented by a 20-n intermediate receiver, according to embodiments of the invention.

[0184] The reception method comprises a preliminary step 2020 of receiving a multiplexed optical signal SiO n (or SiO ni) and an optical transmission signal, each comprising an entangled quantum signal transmitted independently, respectively by two distinct transmitters, and transmitted through a transmission channel 50.

[0185] In step 2040, the multiplexed optical signal SiO ni is directed to a processing chain Cm, associated with a predefined polarization base.

[0186] The method for intermediate reception of optical signals further comprises, for the processing chain Cm, a control loop between steps 2042 and 2044. Step 2044 corresponds to the determination of the polarization state of a component of the received multiplexed optical signal traveling through the chain and relating to a control signal Rni emitted by the transmitter 10-n, and step 2042 corresponds to the modification of the polarization of the received multiplexed optical signal as a function of the determined polarization state. The control loop between steps 2042 and 2044 is stopped when the polarization state determined in step 2044 is aligned with respect to one of the polarization states of the predefined base for the processing chain Cm.

[0187] In step 2060, an interferometric measurement is carried out to project onto an entangled polarization state (relative to a measurement polarization basis) the particles associated respectively with the quantum component of the received multiplexed optical signal relative to the entangled quantum signal Qni, and to the entangled quantum signal originating from the received optical emission signal.

[0188] In step 2080, at least one information signal 1^ is generated from entanglement information of the determined polarization states of the received quantum signals, then transmitted through a transmission channel 50.

[0189] [Fig. 14] represents the final reception process of optical signals implemented implemented by a 30-n final receiver, according to embodiments of the invention.

[0190] In embodiments, the final method for receiving optical signals may comprise a preliminary step 3020 of receiving a multiplexed optical signal Sio-n (or Sio-n 2) comprising an entangled quantum signal emitted by a transmitter, as well as an information signal Imk of polarization state entanglement of quantum signals, transmitted through a transmission channel 50.

[0191] In step 3040, the multiplexed optical signal Si0 n2 can be directed to a processing chain Ck, associated with a predefined polarization base.

[0192] The final method for receiving optical signals may further comprise, for the processing chain Ck, a control loop between steps 3042 and 3044. Step 3044 corresponds to the determination of the polarization state of a component of the received multiplexed optical signal traveling through the chain and relating to a control signal Rni emitted by the transmitter 10-n, and step 3042 corresponds to the modification of the polarization of the received multiplexed optical signal as a function of the determined polarization state. The control loop between steps 3042 and 3044 is stopped when the polarization state determined in step 3044 is aligned with respect to one of the polarization states of the predefined base for the processing chain Ck.

[0193] In step 3060, the polarization state of the quantum component of the received multiplexed optical signal relative to the entangled quantum signal Qn 2 can be determined.

[0194] In step 3080, a quantum encryption key, shared with another final receiver 30-q, can be determined from the polarization state of the quantum component of the received multiplexed optical signal relating to the entangled quantum signal Qn2 and the entanglement information of the polarization states of the quantum signals from the information signal 1^.

[0195] Those skilled in the art will easily understand that certain steps of the transmission and reception methods can be carried out respectively simultaneously, sequentially, independently or not, and / or in a different order, for example in an order defined by a transmitter and a receiver considered.

[0196] The quantum system or subsystems of the system (transmitters and receivers), as well as the methods described above, according to the embodiments of the invention, can be implemented in various ways by hardware, or a combination of hardware and software, in particular in the form of program code that can be distributed as a program product, in various forms. The program code can be distributed using computer-readable media, which can include computer-readable storage media and communication media. The methods described in the present description can be implemented in particular in the form of computer program instructions executable by one or more processors in a computer computing system. These computer program instructions can also be stored in a computer-readable medium.

[0197] The invention is not limited to the embodiments described above as a non-limiting example. It encompasses all the variant embodiments that may be envisaged by those skilled in the art. In particular, those skilled in the art will understand that the invention is not limited to the different modules of the transmitters and receivers of the quantum system described as a non-limiting example.

Claims

1.

2. Claims Receiver (20-m) configured to receive a multiplexed optical signal (SiO n) and an optical signal (Sio-h) transmitted independently through a transmission channel (50), said multiplexed optical signal (Si0-n) comprising a first quantum signal (Qn), said optical signal (Sio h) comprising a second quantum signal (Qh), said multiplexed optical signal (Si0.n) further comprising at least one polarization state control signal (Rni), said receiver (20-m) comprising a processing chain (Cm) associated with a polarization base composed of at least one polarization state and adapted to determine the polarization state of said at least one polarization state control signal (Rnl) and to modify the polarization of said multiplexed optical signal (S io-n) so as to align said determined polarization state with respect to one of said at least one polarization state of said associated base,said receiver (20-m) further comprising a correlation module (260) adapted to carry out a correlation measurement between said first quantum signal (Q„i) from said multiplexed optical signal (SiO n) with modified polarization and said second quantum signal (Qh), said correlation module (260) being associated with said polarization base, said correlation module (260) being further adapted to generate at least one information signal (Imk) from said correlation measurement, said information signal (1^ ) comprising entanglement information of the polarization states of said first and second quantum signals (Qn, Qh)., Receiver (20-m), according to claim 1, wherein said processing chain (Cm) comprises a control signal detection module (240) and an analysis device, the control signal detection module (240) being configured to demultiplex said at least one control signal (Rnl) and said first quantum signal (Qn) from said multiplexed optical signal (SiO n), said detection module (240) being further configured to route said demultiplexed control signal (Rnl) to the polarization analysis device (DA), the polarization analysis device (DA) comprising at least one detection unit (246) adapted to detect said control signal (Rnl) according to one of said at least one polarization state of said associated base.

3. Receiver (20-m), according to claim 2, wherein said detection module (240) further comprises a processor (248) configured to analyze said determined polarization state and to generate a servo signal (Sc) applied to a correction module (220) of polarization of said multiplexed optical signal (SiO n).

4. Receiver (20-m), according to one of claims 1 to 3, wherein said receiver (20-m) is formed from polarization maintaining fibers (PMF) and / or single mode optical fibers (SMF).

5. Transmitter (10-n) configured to transmit optical signals comprising: - a signal generator (120) configured to generate a first quantum signal (Qni), a second quantum signal (Qn2), and a polarization state control signal (Rni), said first quantum signal (Qni) and said second quantum signal (Qn2) being mutually entangled quantum signals, - a signal integrator (140) configured to generate a multiplexed optical signal (Sio-ni), the multiplexed signal comprising said first control signal (Rnl) and said first quantum signal (Qn1), said transmitter (10-n) being configured to transmit through a transmission channel (50), said multiplexed optical signal (SiO ni) and an optical signal (Sio-n2) comprising said second quantum signal (Qn2).

6. A quantum communication system (1) comprising a plurality of transmitters (10-n) according to claim 5, and at least one receiver (20-m) according to one of claims 1 to 4.

7. System (1), according to claim 6, wherein said plurality of transmitters comprises at least a first transmitter and a second transmitter, and said system (1) further comprises a plurality of auxiliary receivers comprising a first auxiliary receiver (30-1) configured to receive an optical signal (SiO n) comprising a quantum signal (Qn) transmitted by the first transmitter (10-n), and a second auxiliary receiver (30-2) configured to receive an optical signal (Sio_h) comprising a quantum signal (Qh) transmitted by the second transmitter (10-h), each auxiliary receiver (30-1; 30-2) being associated with a measurement polarization base composed of at least one polarization state and adapted to measure said associated quantum signal (Qn; Qh) according to at least one of said at least one polarization state of said associated measurement polarization base, and wherein each auxiliary receiver (30-1, 30-2) is configured to receive an entanglement information signal (Imi; Im2 or Ip2) comprising entanglement information of polarization states of quantum signals transmitted by said at least one receiver (20-m; 20-p), each auxiliary receiver (30-1; 30-2) being configured to determine a shared quantum encryption key from said measurement of said associated quantum signal (Qn; Qh) and said entanglement information of polarization states of quantum signals.

8. System (1), according to claim 7, wherein, for one or both auxiliary receivers (30-1, 30-2), said optical signal (Si0.n; Sio-h) received by said auxiliary receiver (30-1; 30-2) is a multiplexed optical signal further comprising a polarization state control signal (Rnl), said auxiliary receiver(s) (30-1; 30-2) comprising a processing chain (Ck) associated with said measurement polarization base and adapted to determine the polarization state of said polarization state control signal (Rni) and to modify the polarization of said multiplexed optical signal (Si0.n; Sio-h) so as to align said determined polarization state with respect to one of said at least one polarization state of said associated measurement polarization base.

9. System (1), according to one of claims 6 to 8, in which said multiplexed signals are frequency multiplexed signals.

10. System (1) according to claim 9, wherein the absolute value of the wavelength difference between the quantum wavelength (XQ) of a quantum signal and the reference wavelength (kR) of a control signal is greater than or equal to a minimum wavelength difference value (ÔX).

11. Method for determining at least one information signal in response to the reception of a multiplexed optical signal (Si0.n) and an optical signal (Sio_h) transmitted independently through a transmission channel (50), said multiplexed optical signal (SiO n) comprising a first quantum signal (Qn), said optical signal (Sio-h) comprising a second quantum signal (Qh), said multiplexed optical signal (Sio-n) further comprising at least one polarization state control signal (Rnl), said method comprising a processing phase (Cm), associated with a polarization base composed of at least one polarization state, for determining the polarization state of said at least one polarization state control signal (Rni) and for modifying the polarization of said multiplexed optical signal (SiO n) so as to align said determined polarization state with respect to one of said at least one polarization state of said associated base, the method further comprising a correlation step comprising a correlation measurement between said first quantum signal (Qni) from said multiplexed optical signal (SiO n) with modified polarization and said second quantum signal (Qh), said correlation measurement being associated with said polarization base,said correlation step (260) further comprising generating said at least one information signal (1^) from said correlation measurement, said information signal (1^) comprising entanglement information of the polarization states of said first and second quantum signals (Qn, Qh).,

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