Patent Publication Number: US-2023142045-A1

Title: Quantum communications system using pulse divider and associated methods

Description:
FIELD OF THE INVENTION 
     The present invention relates to communications, and, more particularly, to quantum communications systems and related methods. 
     BACKGROUND OF THE INVENTION 
     In a quantum communications system, sometimes referred to as a quantum information system, information is exchanged between a transmitter node and a receiver node using encoded single photons. Each photon carries information that is encoded on a property of the photons, such as its polarization, phase, or energy in time. These quantum communications systems generally require sending information from one node to another node, such as a transmitter node, usually referred to as “Alice,” and a receiver node, usually referred to as “Bob.” The term quantum communications system encompasses multiple applications. For example a quantum key distribution (QKD) system allows the sharing of cryptographic keys between the transmitter node and receiver node, thus allowing a more secure communication between the two parties. A QKD system provides a test whether any part of the key would be known to an unauthorized third party eavesdropper, usually referred to as “Eve.” 
     Individual bits of the bit stream are transmitted using single photons. By using complementary properties to which Heisenberg’s uncertainty principle applies, information may be encoded into a photon to prevent the unauthorized third party, e.g., “Eve,” from monitoring the photon since it would disturb its state. When a secret key is established between the two parties by this QKD system, the two parties may then encrypt data transmitted over any conventional communications channel. 
     In the QKD system, the two parties as Alice and Bob at the respective transmitter node and receiver node may use two or more non-orthogonal bases to encode bit values. The laws of quantum mechanics apply to the photons and any measurement of the photons by an eavesdropper, e.g., Eve, without prior knowledge of the encoding basis of each photon, causes an unavoidable change to the state of some of the photons. These changes to the states of the photons may cause errors in the bit values sent between the transmitter node and receiver node, and by comparing a part of the common bit steam, the two parties may determine if the eavesdropper, e.g., Eve, has gained information. Photon polarization is often used to provide the complementary properties for encoding, and is used in the common QKD protocol, BB84, and may be applied to conjugate states, such as the polarization state of the quantum state. Other QKD protocols, such as E91, may be based on entanglement of photon pairs and used in a QKD system. 
     Other applications of a quantum communications system include quantum random number generator (QRNG) systems that use the inherent indeterminacy of quantum entangled photons to produce random binary digits, and quantum secure direct communication (QSDC) systems that transfer direct information between Alice and Bob without a distribution key. In QSDC systems, the transmitter node as Alice generates quantum photons that carry secure quantum information representative of the data to be communicated. The quantum photons carrying the data are decoded upon receipt at the receiver node as Bob. 
     QSDC systems are based on quantum mechanics for direct transmission of information without employing a distributed cryptographic key to encrypt the data. QSDC systems may be more efficient than some keyed communication systems because the cryptographic key development and key storage requirements are eliminated. Transmitted photons carrying data within the QSDC system may be more readily maintained in confidence without being erased, manipulated or monitored by unintended third parties, such as Eve. These QSDC systems may provide tamper evident communication links that are compatible with the direct transmission of data at the single photon level. As a result, QSDC systems may become more important as quantum computers increase in sophistication and allow conventional cryptographic keys to be more easily broken, while quantum interconnects are developed that network computers together. Improvements in QSDC systems may also provide quantum signatures and improve the efficiency and impart greater security in a quantum communications channel. 
     Current cryptographic standards may suffice for ensuring security of most types of data at the current time. It is anticipated that these standards will eventually become obsolete due to advances in quantum computing. Current techniques of QKD that use photons in prepare and measure schemes have high brightness, but have quantum bit error rates (QBER) limits on the order of about 15%. Thus, the errors in the bit rate should not exceed 15% before aborting the QKD protocol. As a result, QKD protocols are difficult to implement in noisy or turbulent communication links, and quantum communication systems that produce a large QBER may require communications equipment to be kept under strict environmental conditions, which limit the applicability of QKD. Other protocols, such as round-robin DPS protocol, have a higher QBER tolerance of about 50%, but the best key rate is about 10 Kbit/s over 50 kilometers of fiber. Other protocols have similar limitations on performance, which degrades with channel conditions. It is desirable to implement low latency, but high security communications not only in a quantum communication system such as a QSDC system, but also into a quantum communication system using QKD protocols. It would also be desirable to apply such improvements into non-quantum optical communications systems. 
     SUMMARY OF THE INVENTION 
     In general, a quantum communications system may include a transmitter node, a receiver node, and a quantum communications channel coupling the transmitter node and receiver node. The transmitter node may comprise a pulse transmitter and a pulse divider downstream therefrom. The receiver node may comprise a pulse recombiner and a pulse receiver downstream therefrom. 
     The pulse transmitter may be configured to generate temporally modulated photons. Additionally, the pulse receiver may comprise a detector to detect phase binned states. The pulse receiver may also comprise at least one single photon detector. 
     The quantum communications channel may comprise a fiber optic communications channel, and in another example, the quantum communications channel may comprise a free space optical (FSO) communications channel. The quantum communications channel may comprise an underwater communications channel. The pulse transmitter may be configured to generate spatially modulated photons and may be configured to perform optical polarization encoding. The pulse transmitter may be configured to generate a bit stream of optical pulses in a quantum key distribution (QKD) protocol. 
     A method aspect is for operating a quantum communications system using a transmitter node, a receiver node, and a quantum communications channel coupling the transmitter node and receiver node. The method may include operating the transmitter node to generate quantum pulses at a pulse transmitter, and dividing the quantum pulses at a pulse divider. The method may also include operating the receiver node to recombine the divided quantum pulses at a pulse recombiner and receiving the recombined pulses at a pulse receiver. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
       Other objects, features and advantages of the present invention will become apparent from the detailed description of the invention which follows, when considered in light of the accompanying drawings in which: 
         FIG.  1    is a block diagram of the quantum communications system having the pulse divider and pulse recombiner in accordance with a non-limiting example. 
         FIG.  2    is a schematic block diagram of the receiver node of  FIG.  1    showing phase and time basis. 
         FIG.  3    is a flowchart showing a method of operating the quantum communications system of  FIG.  1   . 
         FIG.  4    is a graph showing the improvement to prevent tampering using the quantum communications system of  FIG.  1   . 
         FIG.  5    is a chart showing the sensitivity to tampering using the quantum communications system of  FIG.  1    when employing a QKD protocol. 
         FIG.  6    is a schematic diagram illustrating the inaccuracy of a measured image in the public link of the quantum communications channel using the quantum communications system of  FIG.  1   . 
         FIG.  7    is a block diagram of a communications system using a pulse divider and pulse recombiner and incorporating an optical communications channel. 
         FIG.  8    is a graph showing a simulation of the results in the pulse divider at the transmitter node of the communications system of  FIG.  7   . 
         FIG.  9    is a graph showing a simulation of the results of the pulse recombiner at the receiver node of the communications system of  FIG.  7   . 
         FIG.  10    is a graph showing the probability of detecting a data stream at different locations in the optical communications channel of the communications system of  FIG.  7   . 
         FIG.  11    is a graph showing the probability of detecting a data stream at different locations in the optical communications channel of the optical communications system of  FIG.  7   . 
         FIG.  12    is a flowchart showing a method of operating the communications system of  FIG.  7   . 
     
    
    
     DETAILED DESCRIPTION 
     The present description is made with reference to the accompanying drawings, in which exemplary embodiments are shown. However, many different embodiments may be used, and thus, the description should not be construed as limited to the particular embodiments set forth herein. Rather, these embodiments are provided so that this disclosure will be thorough and complete. 
     Referring initially to  FIG.  1   , a quantum communications system is illustrated generally at  20  and may be operative as a quantum secure direct communications (QSDC) system, which permits direct communication, such as without use of a cryptographic key. The quantum communications system  20  includes a transmitter node  26  referred to as Alice, a receiver node  28  referred to as Bob, and a quantum communications channel  30  coupling the transmitter node and receiver node. The quantum communications system  20  may use the pulse division apparatus to place a quantum state into a superposition of time bins. Neighboring quantum states thus experience interference with each other, which scrambles the original data stream. Coupled with the he no-cloning theorem of quantum mechanics this acts as a physical layer of security that can be used to more securely transmit quantum data streams within the quantum communications channel  30  without the additional use of a cryptographic key in some embodiments. 
     Quantum states that have had their probability distribution functions broadened through the pulse divider apparatus so that these probability distribution functions interfere with neighboring states in the quantum data stream in public sections of the quantum communications channel  30  scramble the original data stream. The pulse recombiner at the receiver node  28  where Bob is located reconstructs the original data stream. The input state at the transmitter node  26  is divided into many temporal copies that are separated in time from each other which broadly redistributes its probability distribution function and spoofs attempts to gain information about it within the public sections of the quantum communications channel  30  where an eavesdropper, referred to as Eve, would be located. 
     Photon self-interference in the spatial domain and use of a spatial filter in the spatial domain may reveal data tampering. Because the spatial probability distribution function cannot be perfectly categorized, cloned and reintroduced to the public section of the quantum communications channel  30 , any attempt to monitor, misrepresent or omit temporal data may introduce spatial probability distribution changes that will not cleanly exit a spatial filter at the receiver node  28 , thus revealing tampering by an interferer within the public link of the quantum communications channel. 
     In an example, the quantum communications channel  30  may include a fiber optic communications channel  34 , which may be a single mode optical fiber or a multi-mode fiber. The single mode optical fiber may be used for transmitting temporally modulated photons, and the multi-mode optical fiber may be used for transmitting both temporally and spatially modulated photons. The quantum communications channel  30  may include a free-space optical (FSO) communications channel  36  that includes satellite or line-of-sight communications, or an underwater communications channel or bulk medium  38 . 
     As illustrated, the transmitter node  26  includes a pulse transmitter  40  as a laser pulse source and a pulse divider  42  downstream therefrom, such as positioned directly at the output or further downstream. The transmitter node  26  also includes a controller  48  that operates the pulse transmitter  40  and a transceiver  50  that connects to a communication system  52  as will be explained in further detail below and which may be part of the quantum communications channel  30 . The receiver node  28  includes a pulse recombiner  54  and a pulse receiver  56  downstream. The pulse receiver  56  may include opto-electric (OE) circuitry  60  having a spatial filter  62  and a beam splitter  64  that splits signals into a phase basis or time basis at an optical detector circuit  66 , which includes a phase detector  76  and single photon detector  74 . The receiver node  24  includes a controller  78  and transceiver  80  connected thereto. The transceiver  80  is coupled to the communications system  52 . 
     The pulse transmitter  40  may be configured to generate temporally modulated photons. The pulse receiver  56  includes opto-electric (OE) circuitry  60  that detects phase bin states using the optical detector circuit  66 . The pulse receiver  56  may include at least one single photon detector  74 . The pulse transmitter  40  may also be configured to generate spatially modulated photons and perform optical polarization encoding. The pulse transmitter  40  may be configured to generate a bit stream of quantum pulses in a quantum key distribution (QKD) protocol as explained in further detail below. 
     In an example, the quantum pulses may be time bin photons and the pulse divider  42  at the transmitter node  25  may divide the pulses across other time bins. The pulse recombiner  54  at the receiver node  28  may recombine the pulses. In an example, the pulse divider  42  and pulse recombiner  54  may operate to provide a divided pulse quantum key distribution that may be applied on top of existing QKD protocols and implemented downstream of the pulse transmitter and upstream of the pulse receiver  56  to improve the performance of existing QKD protocols. 
     In an example, the transmitter node  26  may be configured to generate temporally modulated photons that are communicated over the fiber optic communications channel  34 , which may be single mode optical fiber. The transmitter node  26  may also be configured to generate spatially modulated photons that are transmitted over a multi-mode optical fiber. In both cases, the temporally or spatially modulated photons may use optical polarization encoding, and each photon may have a transmitted quantum basis. 
     The transmitter node  26  communicates with the receiver node  28  over the quantum communications channel  30 . Both transmitter and receiver nodes  26 ,  28  may communicate via the communications system  52 , which may include a classical communications channel and may be fiber optic, free-space, wired, or another conventional communications channel. This communications system  52  may be used if additional functions are desired, such as cryptographic key generation and quantum key distribution (QKD), or communication with networked devices using conventional transceivers. The quantum communications system  20  may use cryptographic key sifting or operate as a QSDC system. The quantum communications channel  30  may be part of the communication system  52  as indicated by the dashed lines connecting the two, indicating that both the quantum communications and non-quantum communications may be transmitted over any communications channel as part of the communications system  52 . 
     In an example, the optical pulse output from the pulse transmitter  40  at the transmitter node  26  may be an output bit stream of photons that are encoded bit values. The photon polarization may provide a complementary property used for encoding purposes, such as in the QKD protocol, BB84. Other protocols, such as the E91 protocol, may be used that includes the entanglement of photon pairs. Each bit of information such as a “0” or “1” may be encoded onto an individual photon by selecting from a pair of orthogonal polarization states. In the BB84 QKD protocol, two pairs of orthogonal states are used, and each pair of orthogonal states is referred to as a “basis.” The basis may provide polarization state pairs in a rectilinear basis having vertical and horizontal polarization, such as 0° and 90°, and a diagonal basis having opposite diagonal direction polarization, such as 45° and 135°. 
     It is also possible to use a circular basis of left-handedness and right-side handedness depending on what other bases are used that are conjugate to each other. The quantum communications system  20  may use an unencrypted non-quantum communications channel, such as the communications system  52 , for the key exchange or key sifting process, as key exchange is commonly called. It is possible to use a continuous-variable QKD (CV-QKD) protocol or a discrete-variable (DV-QKD) protocol. Single protons may be generated for the DV-QKD protocol, usually as optical pulses, and requires single photon detectors  74  at the receiver node  28 , for example, as an array of single photon optical detectors. In contrast to the DV-QKD protocol, the CV-QKD protocol may use conjugate-continuous degrees of freedom (field quadratures) of a light pulse prepared in a Gaussian (coherent or squeezed) state to transmit signals that constitute a shared randomness. At the receiver node  28 , the field quadratures of each light pulse may be measured using as an example, shot-noise limited, balanced homodyne or heterodyne detectors, such as phase detectors  76 , which have an advantage of not requiring single photon detection and operating at high GHz speed detection rates. In the CV-QKD protocol, often a local oscillator (OL) signal may be generated at the transmitter node  26  and the CV-QKD protocol may involve polarization encoding and multiplexing techniques. 
     As noted before, the transceiver  50  at the transmitter node and the transceiver  80  at the receiver node  28  may communicate with the communications system  52 , which may be a conventional or non-quantum communications system. For example, Bob as the party at the receiver node  28  may communicate with Alice as the party at the transmitter node  26  over the conventional communications system  52 , and transmit data regarding the basis in which each photon was received at the receiver node  28 . The transmitter node  26 , e.g., Alice, may transmit data about the basis in which each photon was transmitted to the receiver node  28 , e.g., Bob, using the communications system  52 . Any bits having a different basis may be discarded, leaving the remaining bits as the basis for a shared cryptographic key in the key verification or key shifting phase. The subset of shared bits used by both parties, e.g., Alice and Bob as to the respective transmitter node  26  and receiver node  28 , may be used to check against eavesdropping by the unauthorized party, e.g., Eve, which would have introduced errors into the communications stream of bits. 
     The transmitter node  26  with the pulse transmitter  40  may include other components not illustrated in detail, such as a spatial light modulator (SLM) that imposes a spatially varying modulation by modulating intensity and phase, a waveguide array and circuitry that generates phase bin states, and an attenuation filter. 
     As noted before, the transmitter node  26  includes the pulse transmitter  40  for generating a bit stream of “quantum” optical pulses. Although a pulse transmitter  40  as a laser is described, it should be understood that other sources of the pulses may be used that generate the bit stream of pulses. 
     The pulse output from the transmitter node  26  is an output bit stream of photons that are encoded bit values. The photons may be temporally or spatially modulated photons and have a transmitted quantum basis that includes time and phase parameters, including optical polarization encoding. The photon polarization provides the complementary property used for encoding purposes and in the quantum communications system  20  as described, with optical pulses arranged in time bins in this example, photon polarization may be applied to conjugate states, such as phase encoding. The quantum communications system  20  may use entanglement of photon pairs. Each bit of information such as a “0” or “1” may be encoded onto an individual photon by selecting from a pair of orthogonal polarization states. In an example, two pairs of orthogonal states may be used, and each pair of orthogonal states may be referred to as a “basis.” The bases may provide polarization state pairs in a rectilinear basis having vertical and horizontal polarization, such as 0° and 90°, and a diagonal basis having opposite diagonal direction polarization, such as 45° and 135°. It is also possible to use a circular basis of left-handedness and right-handedness depending on what other bases are used that are conjugate to each other. 
     The transmitter node  26  includes its controller  48  operatively connected to the laser pulse transmitter  40  and other components at the transmitter node  26  for controlling their operation, such that the pulse transmitter is controlled for transmitting a photon in a polarization state defined by the bit and basis and in time bins, and record the time the photon was transmitted. This process is repeated for the string of bits as a stream of photons. The transmitter node  26  may include its transceiver  50  connected to the controller  48  and operative to communicate with conventional networked components via the communications system  52 . Additional functions for Quantum Key Distribution (QKD) with the receiver node  28  may be provided via the communications system  52 . 
     The transmitter node  26  may transmit the stream of pulses via the pulse divider  42  over the quantum communications channel  30 , such as the fiber optic communications channel  34 , and as either separate or a part of the communications system  52 , and either as temporally modulated photons or spatially modulated photons in an example. It is possible to use the same fiber optic communications channel  34  for both quantum communications and conventional communications. 
     The receiver node  28  includes the pulse recombiner  54  that recombines the pulses and the pulse receiver  56  includes in this example the opto-electronic (OE) circuitry  60  that receives the bit stream of pulses from the transmitter node  26  over the quantum communications channel  30 . This OE circuitry  60  may include a spatial filter  62  and a beam splitter  64  for splitting the optical signal into an optical phase or time streams for measurement in the phase basis or time basis as explained below. The spatial filter  62  may be used to “clean up” the stream of optical pulses and produce a smooth intensity profile as a cleaner Gaussian signal that has unwanted multiple-order energy peaks removed such that the central maximum of a diffraction energy pattern will be passed through the OE circuitry  60 . The spatial filter  62  may include a microscopic objective lens, a pinhole aperture and a positioning mechanism having precision X-Y movement at the center of the pinhole that operates as the focal point of the objective lens in a non-limiting example. The spatial filter  62  may also be advantageous because it operates as a filter for the spatial probability distribution function that may not be characterized, cloned and reintroduced to the public portion of the quantum communications channel  30 . Thus, any spatial probability distribution disturbances that are introduced may not cleanly exit the spatial filter  62 , and thus, Bob at the receiver node  28  may use this information as a metric to reveal tampering. 
     The optical detector circuit  66  receives the bit stream of optical pulses from the OE circuitry  60  and detects the optical pulses and generates signals that may be processed at the controller  78 , which processes and demodulates the signals representative of the optical pulses depending on the communications protocol. At the receiver node  28 , the optical detector circuit  66  may be formed as a single photon detector  74  for measuring photons in the time basis and in respective time bins, where the optical pulses are transmitted in respective time bins for data encoding. In an example, the optical detector circuit  66  may include an array of single photon detectors  74 . The optical detector circuit  66  may also include a phase detector apparatus  76  for measuring the photons in the phase basis. 
     The controller  78  at the receiver node  28  may be connected to the conventional transceiver  80 , also located at the receiver node  28 . This transceiver  80  may communicate via the conventional or non-quantum communications system  52  with the other networked components or to the transceiver  50  located at the transmitter node  26 . The transmitter node  26  may include other components not illustrated in detail, such as a spatial light modulator (SLM) that imposes a spatially varying modulation by modulating intensity and phase, a waveguide array that increases bit generation and phase bin states, and an attenuation filter. These components may be used to transmit temporally modulated photons or spatially modulated photons and perform optical polarization encoding. 
     As noted before, the OE circuitry  60  at the receiver node  28  may include a spatial filter  62  and a beam splitter  64  to split any incoming optical pulse streams for time processing and phase processing as explained in greater detail below. The optical detector circuit  66  may include the phase detector apparatus  76  and single photon detector  74  for phase basis and time basis measurements, respectively. 
     Generally, an eigenstate |Ψ〉 as a photon of a particular basis is prepared and transmitted from the transmitter node  26  as Alice over the quantum communications channel  30  to the receiver node  28  as Bob. In a conventional QKD system, if the eigenstate |Ψ〉 was prepared in the same photon basis that Eve or Bob as the receiver node  28  chooses to measure the quantum state in, both will measure the same state that Alice at the transmitter node  26  initially prepared. If Eve or Bob at the receiver node  28  choose a different basis than the one Alice at the receiver node  26  initially prepared the quantum state in, both would collapse the eigenstate |Ψ〉 into one of the eigenstates of the basis they were measuring in, and would have a 50% chance in a d=2 data structure, for example, corresponding to a random guess, of correctly identifying the associated bit value of the state that Alice sent. 
     This use of mutually unbiased bases, and the impact of preparing and measuring in inconsistent bases, is used to establish a more secure communications link between Alice as the transmitter node  26  and Bob as the receiver node  28  over the quantum communications channel  30 . As Eve is forced to annihilate the state Alice  26  has prepared as a single photon in order to gain any information about it, and as Eve must randomly choose a basis to measure the state in, on average Eve will choose the wrong basis 50% of the time, both resulting in measurements which do not provide Eve information about the original state, and revealing Eve’s presence to Bob as the receiver node  28  downstream through a quantum bit error rate (QBER) that is higher than a certain threshold value. 
     It is generally assumed that the eigenstate |Ψ〉 prepared in a particular basis, does not change as it propagates. Thus, If Eve and Bob as the receiver node  28  choose the same basis to measure the state that Alice as the transmitter node  26  initially used to prepare the state in, Eve and Bob will both measure it accurately. For a 4-state transmission, however, Eve has on average a 75% chance of correctly retrieving the bit value that Alice as the transmitter node  26  sends, as she has a 50% chance of correctly choosing the right basis and 100% accuracy of retrieving the associated bit value in the correct basis, and a 50% chance of choosing the wrong basis, and a 50% accuracy of retrieving the associated bit value when measuring in the wrong basis. The amount of error that Bob  28  can tolerate before knowing that the quantum communications channel  30  is insecure and that Eve is present, is in part dependent on this probability, which essentially reflects the amount of information that Eve has access to. 
     Increasing the maximum threshold of the quantum bit error rate (QBER) that Bob  28  can tolerate before concluding that the quantum communications channel  30  is insecure may increase secure link lengths, increase secure bit rates, and enable more efficient and cost effective implementations of the quantum communications system  20  in existing communication links and better enable secure communications for QKD systems, and transmission of quantum information in general, for instance for distributed quantum computing or sensing applications. 
     The quantum communications system  20  increases the maximum QBER threshold where an initial state |Ψ&gt;has its temporal probability distribution is broadened so that it interferes with other neighboring bits in the bit stream, and scrambles the state and bit stream in the public link of the quantum communications channel  30  that Eve has access to. This results in any measurements made at a location other than where Alice as the transmitting node  26  and Bob as the receiving node  28  are located will reduce the information available to Eve, even if Eve chooses to measure |Ψ〉 in the same basis that the state was initially prepared in. The quantum communications system  20  may reduce Eve’s information about the eigenstate |Ψ〉 in the public segment of the quantum communications channel  30  even for measurements she conducts in the correct basis. The QBER threshold required for unconditional security may be increased even when Eve chooses the right basis. The probability that Eve will measure the state Alice at the transmitter node  26  initially sent is reduced. As a result, using the quantum communications system  20  of  FIG.  1    as a QSDC system, Alice  26  and Bob  28  may tolerate higher system losses, increase communication link distances, relax optical detector requirements, and more easily adapt the system into existing telecom networks. 
     Further details of pulse detection occurring at the receiver node  28  are explained relative to  FIG.  2   , where a schematic block diagram is illustrated, and showing the optical detector circuit  66  having a phase basis section as part of the phase detector  76 , which includes detectors D1 and D2 for phase basis measurements, and in this example, a single photon detector  74  for time basis measurements and including detector D3. The quantum communications system  20  results in the correct determination of the state for the quantum basis it is intended to be measured in, and inconclusive results of the state when measured in an unintended basis. As shown in  FIG.  2   , the phase detector  76  includes detectors D1 and D2, and the single photon detector  74  includes detector D3 and operating to measure the time bin photons. Time basis measurements may be performed with direct detection to resolve the arrival times of pulses associated with the various bit values that Alice  26  sends. It is also possible to use the time to frequency conversion as disclosed in commonly assigned U.S. Pat. Application Serial No. 16/583,346 filed Sep. 26, 2019, under the title, “Quantum Communication System Having Time to Frequency Conversion and Associated Methods,” the disclosure which is hereby incorporated by reference in its entirety. 
     An incoming photon may be randomly directed by the beam splitter  64  to either a time basis measurement at the single photon detector  74  (D3) or a phase basis measurement at the phase detector apparatus  76  (D1 and D2). For time basis measurements, detector D3 as the single photon detector  74  detects the arrival time of the photon, which correlates with a particular time bin and associated bit value. 
     Phase basis measurements may be performed by passing the single photon state through a Mach-Zender interferometer  84 , which has a delay set by the time bin width of a protocol for the quantum communications system  20  or a half width of the waveguide for the quantum communications system. Single photon interference occurs in a central time window, which the two outputs of the Mach-Zender interferometer  84  resolve constructively or destructively depending on the eigenstate of the phase basis that was sent. For example, if phase state 1 was sent with an associated bit value 0, the phase detector  76  would yield a detection event for Pl on Detector 1, and no detection event on P1 of Detector 2. There is a non-zero probability amplitude of a detection event in the other arrival time bins (P2 and P3) for both of detectors D1 and D2 in the phase basis. However, detection events in these time bins do not help discriminate between the two states, and so they are not used to make state determinations, e.g., only the central time bins “Pl” are used. 
     A flowchart illustrating a method of operating the quantum communication system is illustrated in  FIG.  3    at  100 . The process starts (Block  102 ), and the method includes operating the transmitter node  26  to generate quantum pulses at a pulse transmitter  40  (Block  104 ). The method further includes dividing the quantum pulses at the pulse divider  42  (Block  106 ), operating the receiver node  28  to recombine the quantum pulses at the pulse recombiner  54  (Block  108 ), and receiving the recombined pulses at the pulse receiver  56  (Block  110 ). The process ends (Block  112 ). 
     Referring now to  FIG.  4   , there is illustrated at  110  a graph showing the improvements resulting from the quantum communications system  20  to resist any tampering such as by Eve, when the pulse divider  42  and pulse recombiner  54  are employed. As illustrated as point A1 on the graph, Eve’s measurements are reduced to random and Eve’s ability to recreate the state is impossible without a matched receiver. As shown at point B1 on the graph, Alice and Bob may receive the same bits after sifting. 
     As shown in the chart of  FIG.  5   , the improvements for increased sensitivity to tampering such as by Eve indicates that the use of the pulse divider  42  and pulse recombiner  54  may potentially tolerate up to four times more bit errors than other protocols, from sources such as channel degradation, and still be operable. The state-of-the-art for a conventional quantum system without use of pulse dividers  42  and pulse recombiners  54  is shown in the first column and the use of the pulse combiner and pulse recombiner as a divided pulse QKD in an example with four stages, and assuming Eve does not have a matched receiver, is shown in the second column. The QBER without Eve is shown in the first row, and the QBER with Eve is shown in the second row, and the relative throughput indicated. 
     Referring now to  FIG.  6   , there is illustrated a schematic diagram showing inaccuracy of a measured image as in the public link of the quantum communications channel  30  using the quantum communication system  20  of  FIG.  1   . For example, the original image is shown at the transmitter node  26  (Alice) and is shown relative to the measured image  120  in the public link when the pulse divider  42  and pulse recombiner  54  are employed. The image is shown after recombination at the receiver node  28  and corresponding to the image at the transmitter node  26 . The measured image  120  in the public link cannot be discerned even if Eve somehow correctly chose the frequency of the data. The optical communication system  20  as described provides high security, tamper evident communications, and low probability of interception/detection that are compatible with optical fiber, free space and underwater links and achieved with, for example, pulse division techniques using the pulse divider  42  and pulse recombiner  54 . 
     Referring now to  FIG.  7   , there is illustrated at  200  a communications system that is not a quantum communication system that includes a transmitter node  226 , receiver node  228 , and an optical communications channel  230  coupling the transmitter node and the receiver node. The transmitter node  226  includes a pulse transmitter  240  and a pulse divider  242  downstream therefrom and the receiver node  238  includes the pulse recombiner  254  and pulse receiver  256  downstream therefrom. The optical communications channel  230  may be a free-space optical communications channel  236 , an underwater communications channel  238 , or fiber optic communications channel  234 , such as a single mode fiber or a multi-mode fiber. 
     The pulse transmitter  240  may include pulse generation circuitry  241  that is configured to generate an optical signal carrying communications data and amplified simultaneous emission (ASE) noise, which may be in the spectral and temporal domains. the pulse divider  242  may include birefringent elements  243 , that divide the pulses received from the pulse transmitter  240  into a first group of pulses having a first polarization and a second group of pulses having a second orthogonal polarization. These first and seconds of pulses may be interleaved with each other. The pulse receiver  256  may include a photoelectric detector  260  and a signal processor  264  coupled to the photoelectric detector and configured to separate the amplified spontaneous emission (ASE) noise from the communications data. The transmitter node  226  may include a controller  248  connected to the pulse transmitter  240  and controlling operation of the pulse transmitter. The receiver node  228  may include a controller  278  connected to the pulse receiver  256  and controlling operation of the pulse receiver, including the signal processor  264 . 
     The data signal from the pulse transmitter  240  is passed through the pulse divider  242 , which may create copies of each bit and distribute them into neighboring time bins, foiling attempts to extract information about the data. As the power in the data signal is reduced and the pulse copies are increased, security of the data increases. The broad probability distribution function of the data created by the pulse divider  242  may be compatible with frequency hopping techniques and classical encryption techniques and may provide an integrated and added layer of physical security. 
     Different pulse dividers  242  and pulse recombiners  254  may be used for both the quantum communications system  20  of  FIG.  1    and the communications system  200  shown as a non-quantum optical communication system in  FIG.  7   . The description relative to components described in  FIG.  7    may also apply to the pulse divider  42  and pulse recombiner  54  in  FIG.  1   . 
     The pulse divider  242  may receive an input pulse of a first energy level and divide the pulse into a sequence of temporally spaced lower-energy pulses. The pulse recombiner  254  may combine the temporally spaced pulses for input into the pulse receiver  256 . The pulse divider  242  may be formed from a sequence of M birefringent elements  243 , which divide an initial pulse into a sequence of 2 M  pulses. This sequence of pulses may include a first group of pulses that have a first polarization, and a second group of pulses that have a second orthogonal polarization. It is possible that the pulses in the first and second groups are interleaved with one another, so that the sequence of pulses have alternating linear polarizations. 
     The birefringent elements  243  may be formed from a sequence of birefringent crystals 1, 2, ... , N. Crystals at odd-numbered positions in the sequence may have their optic axes oriented at a 45-degree angle to a direction of linear polarization of the pulse, while crystals at the even-numbered positions may be oriented in the same direction as the linear polarization of the pulse, so that at each crystal, a pulse is split into two equal-intensity pulses, one as an ordinary (o) wave pulse and a second as an extraordinary (e) wave pulse. The o and e pulses are separated in time by Δt=|1/ve - 1/vo|L, where vo and v e  are the group velocities of the o- and e-waves and L is the crystal length. The length of the shortest crystal in the sequence of crystals may be chosen so that At exceeds the pulse duration. The length of the m th  crystal in the sequence may be L,m=2 m-1 L 1  to produce equally spaced pulses. 
     The pulse recombiner  254  may be formed from a second sequence of birefringent crystals, which may be formed from Yttrium vanadate. Any alternating pulses with orthogonal polarizations may be separated with a polarizing beam splitter, and counter-propagate through a gain medium that requires a specific direction of linear polarization. A wave plate may exchange the direction of polarization of the counterpropagating beams, ensuring the correct polarizations for the beam entering the gain medium, and reverse the pulse replicas before the replicas are recombined into a final output pulse. 
     A mirror may be employed at the pulse recombiner  254  to rotate the polarization of the divided pulses by 90 degrees before they are fully recombined so that all pulses experience the same total delay and recombine into the output pulse. The pulse divider  242  and the pulse recombiner  254  may be implemented by a single stack of birefringent crystals  243 . For pulse division, a pulse may be passed in a first direction through a stack of crystals and for pulse recombination, a sequence of pulses may be passed in a second, opposite direction through a stack of birefringent crystals. 
     Examples and descriptions of different pulse dividers  42  and pulse recombiners  54  that may be used with the quantum communications system  20  of  FIG.  1   , and pulse dividers  242  and pulse recombiners  253  that may be used with optical communications system  20  of  FIG.  7    are disclosed in U.S. Pat. Nos. 8,456,736; 10,109,976; and 10,374,376; and in the articles: Zhou et al., “Divided-Pulse Amplification of Ultrashort Pulses,” Optics Letters, 32(7), 2007, pp. 871-873; Zhang et al., “Divided Pulse Soliton Self-Frequency Shift: A Multi-Color, Dual-Polarization, Power-Scalable, Broadly Tunable Optical Source,” Optics Letters, 42(3), 2017, pp. 502-505; and Lamb et al., “Divided-Pulse Lasers,” Optics Letters, 39(9), 2014, pp. 2775-2777, all of the disclosures which are hereby incorporated by reference in their entirety. 
     Referring now to  FIG.  8   , there is illustrated a graph at  290  showing a simulation of the results in pulse division at the transmitter node  226  using the conventional optical communication system  20  of  FIG.  7   . The pulse division is shown in the graph of  FIG.  8   , and the recombining is shown in the graph of  FIG.  9    at  292 . The different stages in both graphs  290 , 292  are illustrated as letters A-F. 
     Referring now to the graphs of  FIGS.  10  and  11   , shown respectively at  294  and  296 , there are illustrated the probabilities of currently detecting an original data stream at different locations in the optical communications channel  230  using the communications system  200  of  FIG.  7   . Bob and the Public link graph lines are shown as “A” and “B” respectively. 
     The communications system  200  having the optical communications channel  230  and employment of the pulse dividers  242  and pulse recombiners  254  provides a low probability of detection where weak pulses are hid in tailored noise and makes the probability of detection low. There is a low probability of intercept because each bit is divided into many copies and distributing each copy into bins provides a system  200  where no useful information about the original message is gained. The system  200  is tamper evident because attempts to measure the data mid-link may be detected by the intended recipient and it is compatible with existing methods of data encryption with added potential for protecting against the attacks. Simulations have been based on “OOK” at 10 Gb/s to send an image from the transmitter node  226  to the receiver node  228  with a five-stage version of the divided pulse communications link. Similar performance may be expected as in a demonstrated free-space optical communications channel  236  that is greater than 25 km and greater than 1 Gb/s for communications between ship-shore and underwater up to 100 Mb/S and 100 meter range. A single system may enable communications over multiple link types with different wavelengths and distances. Use of the pulse divider  242  and pulse recombiner  254  are compatible with existing methods of data encryption and compatible with active link monitoring techniques and phase front shaping for increasing link performance and scattering media. 
     Referring now to  FIG.  12   , there is illustrated a flowchart generally at  300  that shows the method of operating the communications system  200  shown in  FIG.  7   . The process starts (Block  302 ). The transmitter node  226  is operated to generate optical pulses at the pulse transmitter  240  (Block  304 ). The optical pulses are divided at the pulse divider  242  (Block  306 ). The receiver node  228  is operated to recombine the optical pulses at the pulse recombiner  254  (Block  308 ). The recombined pulses are received at the pulse receiver  256  (Block  310 ). The process ends (Block  312 ). 
     This application is related to copending patent application entitled, “COMMUNICATIONS SYSTEM USING PULSE DIVIDER AND ASSOCIATED METHODS,” which is filed on the same date and by the same assignee and inventors, the disclosure which is hereby incorporated by reference. 
     Many modifications and other embodiments of the invention will come to the mind of one skilled in the art having the benefit of the teachings presented in the foregoing descriptions and the associated drawings. Therefore, it is understood that the invention is not to be limited to the specific embodiments disclosed, and that modifications and embodiments are intended to be included within the scope of the appended claims.