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US-12621060-B2 - Method for performing quantum secure direct communication in quantum communication system, and apparatus therefor

US12621060B2US 12621060 B2US12621060 B2US 12621060B2US-12621060-B2

Abstract

The present specification provides a quantum secure direct communication (QSDC) method by which a transmitting end transmits a message on the basis of differential time coding, in a quantum communication system. More specifically, the method comprises the steps of: receiving, from a receiving end on a quantum channel, (i) at least one initial time state configured by including a time interval equal to a dead time of a single photon detector of the receiving end and (ii) at least one initial phase state; receiving, from the receiving end on a classical channel, time state location information for selecting a specific initial time state for encoding of information transmitted to the receiving end; selecting the specific initial time state for the encoding, on the basis of the time state location information: generating an encoding time state by encoding the information on the basis of the selected specific initial time state, the encoding time state being generated by applying a time shift on the basis of a value of the information being encoded; and transmitting a message including the encoding time state to the receiving end through the quantum channel, wherein the message is restored on the basis of a time difference between information on the at least one initial time state stored in the receiving end and information on the encoding time state.

Inventors

  • Byungkyu Ahn
  • Sangrim LEE
  • Hojae Lee
  • JaYeong KIM

Assignees

  • LG ELECTRONICS INC.

Dates

Publication Date
20260505
Application Date
20210721

Claims (17)

  1. 1 . A quantum secure direct communication (QSDC) method by which a transmitting end transmits a message based on differential time coding, in a quantum communication system, comprising: receiving, from a receiving end on a quantum channel, (i) at least one initial time state configured by including a time interval equal to a dead time of a single photon detector of the receiving end and (ii) at least one initial phase state; receiving, from the receiving end on a classical channel, time state location information for selecting a specific initial time state for encoding of information transmitted to the receiving end; selecting the specific initial time state for the encoding, based on the time state location information; generating an encoding time state by encoding the information, based on the selected specific initial time state, wherein the encoding time state is generated by applying a time shift based on a value of the information being encoded; and transmitting a message including the encoding time state to the receiving end through the quantum channel, wherein the message is restored based on a differential time between information on the at least one initial time state information stored in the receiving end and information on the encoding time state.
  2. 2 . The method of claim 1 , wherein some initial time states and initial phase states among the at least one initial time state and the at least one initial phase state are used for determining whether there is a eavesdropping on the quantum channel for the at least one initial time state and the at least one initial phase state.
  3. 3 . The method of claim 2 , further comprising receiving, from the receiving end on the classical channel, information on the some initial time states and initial phase states used for determining whether there is the eavesdropping on the quantum channel.
  4. 4 . The method of claim 3 , further comprising determining whether there is the eavesdropping on the quantum channel based on quantum bit error rate (QBER) estimation, based on the information on the some initial time states and initial phase states.
  5. 5 . The method of claim 4 , further comprising requesting retransmission of an initial time state and an initial phase state based on a value of QBER being equal to or more than a specific value according to a result of determining whether there is the eavesdropping.
  6. 6 . The method of claim 5 , wherein selection and encoding of the specific initial time state is performed based on the value of QBER being smaller than the specific value according to the result of determining whether there is the eavesdropping.
  7. 7 . The method of claim 1 , wherein The receiving of the time state location information is performed after receiving (i) the at least one initial time state and (ii) the at least one initial phase state.
  8. 8 . The method of claim 1 , wherein the generating of the encoding time state further includes adding, to the information, a random number used for determining whether there is a eavesdropping in a backward quantum channel, and generating a codeword by encoding the information to which the random number is added.
  9. 9 . The method of claim 8 , further comprising: transmitting, to the receiving end on the classical channel, random information including (i) a location of the random number and (ii) information on a value of the random number.
  10. 10 . The method of claim 8 , wherein the generating of the encoding time state further includes combining the specific initial time state and the codeword by applying the time shift to the codeword.
  11. 11 . The method of claim 10 , wherein different time shift values are applied to the encoding time state based on a value of the encoded information.
  12. 12 . The method of claim 11 , wherein the application of the different time shift values is performed based on a predefined mapping table, and the mapping table is related to a mapping relationship between the values of the encoded information and the time shift values.
  13. 13 . The method of claim 10 , wherein the specific initial time state and the encoding time state are configured by one or more time bins, and based on a dimension of the specific time state being the same as a dimension of the encoding time state, a length of the time bin constituting the specific initial time state is equal to a length of the time bin constituting the encoding time state.
  14. 14 . The method of claim 13 , wherein based on the dimension of the specific time state being different from the dimension of the encoding time state, the length of the time bin constituting the encoding time state is smaller than the length of the time bin constituting the specific initial time state.
  15. 15 . The method of claim 14 , further comprising: transmitting, to the receiving end, information on a dimension applied to generation of the encoding time state before generating the encoding time state, based on the dimension of the specific time state being different from the dimension of the encoding time state.
  16. 16 . A transmitting end performing quantum secure direct communication (QSDC) for transmitting a message based on differential time coding, in a quantum communication system, comprising: a transmitter for transmitting a radio signal; a receiver for receiving the radio signal; at least one processor; and at least one computer memory operably connectable to the at least one processor, and storing instructions of performing operations when executed by the at least one processor, wherein the operations include receiving, from a receiving end on a quantum channel, (i) at least one initial time state configured by including a time interval equal to a dead time of a single photon detector of the receiving end; receiving, from the receiving end on a classical channel, time state location information for selecting a specific initial time state for encoding of information transmitted to the receiving end; selecting the specific initial time state for the encoding, based on the time state location information; generating an encoding time state by encoding the information, based on the selected specific initial time state; generating the encoding time state by applying a time shift based on a value of the information being encoded; and transmitting a message including the encoding time state to the receiving end through the quantum channel, and wherein the message is restored based on a differential time between information on the at least one initial time state information stored in the receiving end and information on the encoding time state.
  17. 17 . A quantum secure direct communication (QSDC) method by which a receiving end receives a message based on differential time coding, in a quantum communication system, comprising: transmitting, to a transmitting end on a quantum channel, (i) at least one initial time state configured by including a time interval equal to a dead time of a single photon detector of the receiving end; transmitting, to the transmitting end on a classical channel, time state location information for selecting a specific initial time state for encoding of information transmitted to the transmitting end, wherein the specific initial time state for the encoding in the transmitting end is selected based on the time state location information; receiving, from the transmitting end, a message including an encoding time state generated by applying a time shift based on a value of the information encoded based on the specific initial time state; and restoring the information based on the at least one initial time state information and the encoding time state information stored in the receiving end.

Description

CROSS-REFERENCE TO RELATED APPLICATIONS This application is a National Stage application under 35 U.S.C. § 371 of International Application No. PCT/KR2021/009420, filed on Jul. 21, 2021. The disclosure of the prior application is incorporated by reference in its entirety. TECHNICAL FIELD The present disclosure relates to a quantum communication system, and more particularly, to a method for high-dimensional quantum secure direct communication in a quantum communication system, and an apparatus therefor. BACKGROUND ART Wireless communication systems have been widely deployed to provide various types of communication services such as voice or data. In general, the wireless communication system is a multiple access system capable of supporting communication with multiple users by sharing available system resources (bandwidth, transmission power, etc.). Examples of multiple access systems include a Code Division Multiple Access (CDMA) system, a Frequency Division Multiple Access (FDMA) system, a Time Division Multiple Access (TDMA) system, a Space Division Multiple Access (SDMA) system, an Orthogonal Frequency Division Multiple Access (OFDMA) system, a Single Carrier Frequency Division Multiple Access (SC-FDMA) system, and an Interleave Division Multiple Access (IDMA) system. DISCLOSURE Technical Problem An object of the present disclosure is to provide a method for performing quantum secure direct communication in a quantum communication system, and an apparatus therefor. Furthermore, an object of the present disclosure is to provide a method for transmitting 2 or more bits of classical information based on a single photon in a quantum communication system, and an apparatus therefor. Furthermore, an object of the present disclosure is to provide a method for transmitting 2 or more bits of classical information without information loss based on a single photon in a quantum communication system, and an apparatus therefor. Furthermore, an object of the present disclosure is to provide a method for constructing an initial state for information transmission by considering a dead time in a single photo detector of a receiving end in a quantum communication system, and an apparatus therefor. The technical objects of the present disclosure are not limited to the aforementioned technical objects, and other technical objects, which are not mentioned above, will be apparently appreciated by a person having ordinary skill in the art from the following description. Technical Solution The present disclosure provides a method for performing quantum secure direct communication in a quantum communication system, and an apparatus therefor. More specifically, according to the present disclosure, a quantum secure direct communication (QSDC) method by which a transmitting end transmits a message based on differential time coding, in a quantum communication system includes: receiving, from a receiving end on a quantum channel, (i) at least one initial time state configured by including a time interval equal to a dead time of a single photon detector of the receiving end and (ii) at least one initial phase state; receiving, from the receiving end on a classical channel, time state location information for selecting a specific initial time state for encoding of information transmitted to the receiving end; selecting the specific initial time state for the encoding, based on the time state location information: generating an encoding time state by encoding the information, based on the selected specific initial time state, wherein the encoding time state is generated by applying a time shift based on a value of the information being encoded; and transmitting a message including the encoding time state to the receiving end through the quantum channel, and the message is restored based on a differential time between information on the at least one initial time state information stored in the receiving end and information on the encoding time state. Furthermore, according to the present disclosure, some initial time states and initial phase states among the at least one initial time state and the at least one initial phase state are used for determining whether there is a eavesdropping on the quantum channel for the at least one initial time state and the at least one initial phase state. Furthermore, according to the present disclosure, the method further includes receiving, from the receiving end on the classical channel, information on the some initial time states and initial phase states used for determining whether there is the eavesdropping on the quantum channel. Furthermore, according to the present disclosure, the method further includes determining whether there is the eavesdropping on the quantum channel based on quantum bit error rate (QBER) estimation, based on the information on the some initial time states and initial phase states. Furthermore, according to the present disclosure, the method further includes requesting ret