Quantum key distribution using a thermal source

1. A passive continuous variable quantum key distribution comprising:

splitting, at a transmitter, an output of a thermal source into a first beam of the output of the thermal source and a second beam of the output of the thermal source, wherein the output of the thermal source has quantum noise;

attenuating the first beam at the transmitter;

communicating the attenuated first beam across a quantum communication channel from the transmitter to a receiver;

measuring, at the receiver, a quantum state of the attenuated first beam by performing homodyne detection on the attenuated first beam to measure either in-phase component or quadrature component randomly;

measuring, at the transmitter, a quantum state of the second beam by performing either

homodyne detection on the second beam to measure either in-phase component or quadrature component randomly, or

conjugate homodyne detection on the second beam to measure both in-phase component and quadrature component of the second beam; and

establishing, at the receiver and at the transmitter, a shared key based on the measured quantum state of the first beam and the measured quantum state of the second beam.

2. A passive continuous variable quantum key distribution comprising:

splitting, at a transmitter, an output of a thermal source into a first beam of the output of the thermal source and a second beam of the output of the thermal source, wherein the output of the thermal source has quantum noise;

attenuating the first beam at the transmitter;

communicating the attenuated first beam across a quantum communication channel from the transmitter to a receiver;

measuring, at the receiver, a quantum state of the attenuated first beam by performing conjugate homodyne detection on the attenuated first beam to measure both in-phase component and quadrature component of the attenuated first beam;

measuring, at the transmitter, a quantum state of the second beam by performing either

conjugate homodyne detection on the second beam to measure both in-phase component and quadrature component of the second beam, or

homodyne detection on the second beam to measure either in-phase component or quadrature component randomly; and

establishing, at the receiver and at the transmitter, a shared key based on the measured quantum state of the first beam and the measured quantum state of the second beam.

3. The passive continuous variable quantum key distribution method of claim 2 , wherein said splitting and said attenuating are accomplished by at least one of a) an asymmetric beam splitter, and b) a combination of a beam splitter and an attenuator.

4. The passive continuous variable quantum key distribution method of claim 2 , wherein

the thermal source is configured to emit light having a multiwavelength spectrum,

measuring the quantum state of the attenuated first beam includes aligning a central wavelength of a first local oscillator within the multiwavelength spectrum, and

measuring the quantum state of the second beam includes aligning a central wavelength of a second local oscillator within the multiwavelength spectrum.

5. The passive continuous variable quantum key distribution method of claim 1 wherein said splitting and said attenuating are accomplished by at least one of a) an asymmetric beam splitter, and b) a combination of a beam splitter and an attenuator.

6. The passive continuous variable quantum key distribution method of claim 1 wherein

the thermal source is configured to emit light having a multiwavelength spectrum,

measuring the quantum state of the attenuated first beam includes aligning a central wavelength of a first local oscillator within the multiwavelength spectrum, and

measuring the quantum state of the second beam includes aligning a central wavelength of a second local oscillator within the multiwavelength spectrum.

7. A passive continuous variable quantum key distribution system comprising:

a transmitter system comprising

a thermal source configured to generate an output having quantum noise,

a beam splitter unit that splits the output of the thermal source into a first beam and a second beam, wherein

the first beam is weaker than the second beam,

a transmission system configured to transmit the first beam over a quantum communication channel, and

a detector system configured to detect a quantum state of the second beam comprising a homodyne detection system configured to detect randomly either in-phase component or quadrature component of the second beam;

a receiver system configured to receive over the quantum communication channel the weaker first beam and determine information about the quantum state of the weaker first beam; and

a control unit operably coupled to said detector system of the transmitter system and the receiver system, said control unit configured to establish a shared private key based on the quantum state of the second beam and the information about the quantum state of the weaker first beam.

8. A passive continuous variable quantum key distribution system comprising:

a transmitter system comprising

a thermal source configured to generate an output having quantum noise,

a beam splitter unit that splits the output of the thermal source into a first beam and a second beam, wherein

the first beam is weaker than the second beam,

a transmission system configured to transmit the first beam over a quantum communication channel, and

a detector system configured to detect a quantum state of the second beam comprising a conjugate homodyne detection system configured to detect both in-phase component or quadrature component of the second beam second beam;

a receiver system configured to receive over the quantum communication channel the weaker first beam and determine information about the quantum state of the weaker first beam includes either

information about both in-phase component and quadrature component of the weaker first beam, or

information about randomly either in-phase component or quadrature component of the weaker first beam; and

a control unit operably coupled to said detector system of the transmitter system and the receiver system, said control unit configured to establish a shared private key based on the quantum state of the second beam and the information about the quantum state of the weaker first beam.

9. The passive continuous variable quantum key distribution system of claim 8 wherein the beam splitter unit comprises a beam splitter and an attenuator.

10. The passive continuous variable quantum key distribution system of claim 8 wherein

the thermal source is configured to emit light having a multiwavelength spectrum, and

said detector system is configured to align a central wavelength of a local oscillator within the multiwavelength spectrum.

11. The passive continuous variable quantum key distribution system of claim 10 , wherein the thermal source comprises an amplified spontaneous emission source.

12. The passive continuous variable quantum key distribution system of claim 11 , wherein the amplified spontaneous emission source comprises a superluminescent light emitting diode.

13. The passive continuous variable quantum key distribution system of claim 7 wherein the beam splitter unit comprises a beam splitter and an attenuator.

14. The passive continuous variable quantum key distribution system of claim 7 wherein

the thermal source is configured to emit light having a multiwavelength spectrum, and

said detector system is configured to align a central wavelength of a local oscillator within the multiwavelength spectrum.

15. The passive continuous variable quantum key distribution system of claim 14 , wherein the thermal source comprises an amplified spontaneous emission source.

16. The passive continuous variable quantum key distribution system of claim 15 , wherein the amplified spontaneous emission source comprises a superluminescent light emitting diode.

17. A method of generating shared random numbers in a transmitter and a receiver using a thermal source, an output of the thermal source having quantum noise, the method comprising:

splitting, at the transmitter, the output of the thermal source into a first beam and a second beam;

attenuating, at the transmitter, the first beam by an attenuation amount;

communicating the attenuated first beam across a quantum communication channel from the transmitter to the receiver;

measuring, at the transmitter, a quantum state of the attenuated first beam by performing homodyne detection on the attenuated first beam;

generating, at the receiver, random numbers based on the quantum state of the attenuated first beam;

measuring, at the transmitter, a quantum state of the second beam by performing either homodyne detection or conjugate homodyne detection on the second beam; and

generating, at the transmitter, random numbers based on the quantum state of the second beam,

wherein at least a portion of the random numbers generated based on the measured quantum state of the attenuated first beam is correlated to at least a portion of the random numbers generated based on the measured quantum state of the second beam.

18. A method of generating shared random numbers in a transmitter and a receiver using a thermal source, an output of the thermal source having quantum noise, the method comprising:

splitting, at the transmitter, the output of the thermal source into a first beam and a second beam;

attenuating, at the transmitter, the first beam by an attenuation amount;

communicating the attenuated first beam across a quantum communication channel from the transmitter to the receiver;

measuring, at the transmitter, a quantum state of the attenuated first beam by performing conjugate homodyne detection on the attenuated first beam;

generating, at the receiver, random numbers based on the quantum state of the attenuated first beam;

measuring, at the transmitter, a quantum state of the second beam by performing either conjugate homodyne detection or homodyne detection on the second beam; and

generating, at the transmitter, random numbers based on the quantum state of the second beam,

wherein at least a portion of the random numbers generated based on the measured quantum state of the attenuated first beam is correlated to at least a portion of the random numbers generated based on the measured quantum state of the second beam.

19. The method of generating shared random numbers of claim 18 , wherein said splitting and attenuating are accomplished by at least one of a) an asymmetric beam splitter, and b) a combination of a beam splitter and an attenuator.

20. The method of generating shared random numbers of claim 18 , wherein

the thermal source is configured to emit light having a multiwavelength spectrum,

measuring the quantum state of the attenuated first beam includes aligning a central wavelength of a first local oscillator within the multiwavelength spectrum, and

measuring the quantum state of the second beam includes aligning a central wavelength of a second local oscillator within the multiwavelength spectrum.

21. The method of generating shared random numbers of claim 17 wherein said splitting and attenuating are accomplished by at least one of a) an asymmetric beam splitter, and b) a combination of a beam splitter and an attenuator.

22. The method of generating shared random numbers of claim 17 wherein

the thermal source is configured to emit light having a multiwavelength spectrum,

measuring the quantum state of the attenuated first beam includes aligning a central wavelength of a first local oscillator within the multiwavelength spectrum, and

measuring the quantum state of the second beam includes aligning a central wavelength of a second local oscillator within the multiwavelength spectrum.