CN104852797B - The photon state of polarization auto compensation method of the bit error rate and uncertain rate joint feedback - Google Patents
The photon state of polarization auto compensation method of the bit error rate and uncertain rate joint feedback Download PDFInfo
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- CN104852797B CN104852797B CN201510228202.6A CN201510228202A CN104852797B CN 104852797 B CN104852797 B CN 104852797B CN 201510228202 A CN201510228202 A CN 201510228202A CN 104852797 B CN104852797 B CN 104852797B
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- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04L—TRANSMISSION OF DIGITAL INFORMATION, e.g. TELEGRAPHIC COMMUNICATION
- H04L9/00—Cryptographic mechanisms or cryptographic arrangements for secret or secure communications; Network security protocols
- H04L9/08—Key distribution or management, e.g. generation, sharing or updating, of cryptographic keys or passwords
- H04L9/0816—Key establishment, i.e. cryptographic processes or cryptographic protocols whereby a shared secret becomes available to two or more parties, for subsequent use
- H04L9/0852—Quantum cryptography
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- H04B10/00—Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
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Abstract
A kind of photon state of polarization auto compensation method of the bit error rate and uncertain rate joint feedback, quantum key distribution system announces N positions in the primary key that length is M and is used to count the bit error rate every time, wherein N is much smaller than M, N' positions puppet key is announced in effective detection sequence where primary key to be used to count uncertain rate, the photon polarization state of receiving terminal is estimated in Poincar é balls using the bit error rate and uncertain rate, realizes and compensates two non-orthogonal polarization states simultaneously |+>With | H>.The method of the present invention can carry out accurate compensation in real time in the case where not influenceing quantum key distribution system communication efficiency and distance, do not increase system cost to two non-orthogonal photon polarization states.
Description
Technical field
The present invention relates to a kind of photon state of polarization auto compensation technology, especially with the quantum key distribution system of polarization encoder
The photon state of polarization auto compensation method of system, specifically a kind of bit error rate and uncertain rate joint feedback.
Background technology
At present, the polarization compensation scheme that known quantum key distribution system uses mainly has bidirectional optical path polarization self-complementary
Repay, interrupt compensates, time division multiplexing compensation and wavelength-division multiplex compensate [several polarization compensation skills of fiber optic quantum key distribution system
Art, Wang Jian, laser and optoelectronics progress].Based on bidirectional optical path structure Polarization scheme due to being set without outside
It is standby, Polarization is realized merely with light channel structure can, but because photon round-trip passes twice through optical fiber so that transmission distance
From being limited, system effectiveness is relatively low, and vulnerable.Interrupt polarization compensation is easily achieved, but efficiency is low, will be about using
10% time carries out polarization compensation.The polarization compensation scheme that is time-multiplexed, therefore can because reference light is identical with signal light wavelength
To reach accurate compensation to flashlight by compensating reference light, but in order to reduce interference of the reference light to quantum signal, need
System is wanted to pay larger cost on the width for improving the precision of synchronizing signal and reduction sonde door pulse.Wavelength-division multiplex polarizes
Compensation scheme can avoid the interference of reference light, reduce the bit error rate to a certain extent, have preferable stability, but due to
Wavelength is different, and polarization state develops also different, it is difficult to accurate compensation is realized to flashlight according to reference light, especially by an electricity
Dynamic Polarization Controller can only compensate two nonopiate polarization states of quantum key distribution system as much as possible.Therefore, existing quantum
The polarization compensation method of key distribution system can not be in the case where taking into account efficiency, distance and cost to two non-orthogonal photons
Polarization state is accurately compensated.
The content of the invention
The invention aims to overcome the polarization compensation method of existing quantum key distribution system can not take into account effect
The deficiency accurately compensated two non-orthogonal photon polarization states in the case of rate, distance and cost, the present invention propose one
The photon state of polarization auto compensation method of the kind bit error rate and uncertain rate joint feedback.
The technical scheme is that:
A kind of photon state of polarization auto compensation method of bit error rate and uncertain rate joint feedback, it comprises the following steps:
The photon polarization state that quantum key distribution system it is expected to receive is represented with a point on Poincar é balls, in real time
Polarization state is with it is expected that the angle of polarization state just corresponds to the current bit error rate, the folder of real-time polarization state and desired nonopiate polarization state
Angle just corresponds to current uncertain rate;
Photon polarization state is to the bit error rate of itself polarization state when counting transmitting terminal and receiving terminal to base success, in Poincar é
Real-time polarization state is navigated into the relative angle for it is expected polarization state on ball to correspond on the circle of the foregoing bit error rate;
Statistics transmitting terminal and receiving terminal when failing to base photon polarization state to the uncertain rate of desired nonopiate polarization state,
Two points for further navigating to real-time polarization state on foregoing circle on Poincar é balls;
Both of the aforesaid point is all equal, random selection one to the angle of expectation polarization state and desired nonopiate polarization state
Individual point carries out exploratory compensation as real-time polarization state, if the bit error rate reduces, can determine that selection is correct, conversely, another point
It is real-time polarization state;
According to the real-time polarization state of judgement, polarized controller is adjusted according to general method, is realized to quantum key point
The compensation of hair system photon polarization state.
In the present invention, quantum key distribution system announces N positions in the primary key that length is M and is used to count error code every time
Rate, wherein N are much smaller than M, and N positions puppet key is announced in effective detection sequence where primary key and is used to count uncertain rate,
The photon polarization state of receiving terminal is estimated in Poincar é balls using the bit error rate and uncertain rate, realizes that compensation two is nonopiate simultaneously
Polarization state |+>With | H>, specifically include following steps:
(a), the receiving terminal of quantum key distribution system length be M primary key where effective detection sequence in
Machine selects result of detection of the N ' positions to base failure, referred to as pseudo- key, is disclosed by classical channel to transmitting terminal, wherein N ' >=N;
(b), by non-orthogonal two polarization states |+>With | H>It is respectively labeled as A and B;
(c), by A, corresponding point is designated as A on Poincar é balls0, A0It is expectation polarization states of the A in receiving terminal, B is existed
Corresponding point is designated as B on Poincar é balls0, B0It is expectation polarization states of the B in receiving terminal, A0With B0Angle, i.e. relevant radii
Angle, span are (0, π);
(d), in disclosed N-bit key, the bit error rate for counting A is EA;
(e) circle C, is made on Poincar é ballsESo that circle CEOn point and A0The cosine value of half-angle of angle be (1-
EA) positive square root;
(f), in disclosed N ' positions puppet key, statistics transmitting terminal is encoded to A but receiving terminal detects the probability for being B, i.e. A phases
To B uncertain rate, U is designated asA;
(g) circle C, is made on Poincar é ballsUSo that circle CUOn point and B0The cosine value of half-angle of angle be UA
Positive square root;
(h), by CEIt is designated as CEA, by CUIt is designated as CUA, then by non-orthogonal polarization state |+>With | H>B and A are respectively labeled as,
Repeat step (c)~(g), it will obtain CEIt is designated as CEB, by CUIt is designated as CUB;
(i), judge real-time polarization state according to following situations, take general method to adjust polarized controller, realization pair
The compensation of quantum key distribution system photon polarization state:
If CEAWith CUA、CEBWith CUBOnly have 1 intersection point, then put the two as A in the real-time inclined of receiving terminal
Polarization state A1With B receiving terminal real-time polarization state B1Compensate, then go to (a) and carry out next round compensation;
If CEAWith CUAThere are 1 intersection point, CEBWith CUBThere are 2 intersection points, then first by CEAWith CUAIntersection point as A in receiving terminal
Real-time polarization state A1, then to CEBWith CUB2 intersection points carry out exploratory compensation and judge real-time polarization states of the B in receiving terminal
B1, exploratory compensation is then removed, according to selected A1And B1Compensate, then go to (a) and carry out next round compensation;
If CEAWith CUAThere are 1 intersection point, CEBWith CUBThere is no intersection point, then first by CEAWith CUAIntersection point as A in receiving terminal
Real-time polarization state A1, then in CEBWith CUBOn take 2 nearest points of mutual distance, therefrom choose and A1Angle closest to straight
The real-time polarization state B put as B in receiving terminal at angle1, according to selected A1And B1Compensate, it is next to then go to (a) progress
Wheel compensation;
If CEAWith CUA、CEBWith CUBThere are 2 intersection points, then two first larger to bit error rate points carry out exploratory compensation
To judge a real-time polarization state A1Or B1, the A that then selects and have determined that from less two points of the bit error rate1Or B1Folder
Angle closest to right angle point as another real-time polarization state B1Or A1, exploratory compensation is then removed, according to selected A1And B1
Compensate, then go to (a) and carry out next round compensation;
If CEAWith CUAThere are 2 intersection points, CEBWith CUBThere is 1 intersection point, then first by CEBWith CUBIntersection point as B in receiving terminal
Real-time polarization state B1, then to CEAWith CUA2 intersection points carry out exploratory compensation and judge real-time polarization states of the A in receiving terminal
A1, exploratory compensation is then removed, according to selected A1And B1Compensate, then go to (a) and carry out next round compensation;
If CEAWith CUAThere are 2 intersection points, CEBWith CUBThere is no intersection point, then first to CEAWith CUA2 intersection points using exploratory
Compensate to judge A real-time polarization state A1, then in CEBWith CUBOn take 2 nearest points of mutual distance, therefrom choose and A1's
The real-time polarization state B that puts as B in receiving terminal of the angle closest to right angle1, exploratory compensation is then removed, according to selected A1
And B1Compensate, then go to (a) and carry out next round compensation;
If CEAWith CUA、CEBWith CUBThere is no intersection point, now two groups of circles respectively have the nearest point of 2 mutual distances, then first select
Take mutual distance closer to be located at CEAOr CEBOn that point be used as a real-time polarization state A1Or B1, it is then mutual from another group
The A for selecting and having determined that in 2 closest points1Or B1Angle closest to right angle point as another real-time polarization state
B1Or A1, according to selected A1And B1Compensate, then go to (a) and carry out next round compensation;
If CEAWith CUAThere is no intersection point, CEBWith CUBThere is 1 intersection point, then by CEBWith CUBIntersection point as B in receiving terminal
Real-time polarization state B1, then in CEAWith CUAOn take 2 nearest points of mutual distance, therefrom selection and B1Angle closest to right angle
Point as A receiving terminal real-time polarization state A1, according to selected A1And B1Compensate, then go to (a) and carry out next round
Compensation;
If CEAWith CUAThere is no intersection point, CEBWith CUBThere are 2 intersection points, then first to CEBWith CUB2 intersection points using exploratory
Compensate to judge B real-time polarization state B1, then in CEAWith CUAOn take 2 nearest points of mutual distance, therefrom choose and B1's
The real-time polarization state A that puts as A in receiving terminal of the angle closest to right angle1, exploratory compensation is then removed, according to selected A1
And B1Compensate, then go to (a) and carry out next round compensation.
In the present invention, 2 intersection points are carried out with exploratory compensation and judges that the method for real-time polarization state is to randomly select 1 intersection point
Compensated to the midpoint of 2 intersection points, if the bit error rate of the polarization state reduces, the point for judging to choose is real-time polarization state, conversely,
Then judge another point for real-time polarization state.
In the present invention, the method for removing exploratory compensation is the shape for reverting to polarization compensation device before exploratory compensation
State.
Beneficial effects of the present invention:
The method of the present invention can not influence quantum key distribution system communication efficiency and distance, not increase system cost
In the case of two non-orthogonal photon polarization states are carried out with accurate compensation in real time.
Brief description of the drawings
Fig. 1 is the Poincar é spherical structure schematic diagrames of the present invention.
Embodiment
The present invention is further illustrated with reference to the accompanying drawings and examples.
As shown in figure 1, quantum key distribution system it is expected the photon polarization state of reception with Poincar é balls by the present invention
A point represent that real-time polarization state is with it is expected that the angle of polarization state just corresponds to the current bit error rate, real-time polarization state and expectation
The angle of nonopiate polarization state just correspond to current uncertain rate.Photon during by counting transmitting terminal and receiving terminal to base success
Real-time polarization state is navigated to the relative folder for it is expected polarization state by polarization state to the bit error rate of itself polarization state on Poincar é balls
Angle is corresponded on the circle of the foregoing bit error rate.Photon polarization state is to desired anon-normal when being failed by counting transmitting terminal and receiving terminal to base
Hand over the uncertain rate of polarization state, two points for further navigating to real-time polarization state on foregoing circle on Poincar é balls.This
The angle of two points to expectation polarization state and desired nonopiate polarization state is all equal.One point of random selection is as real-time
Polarization state carries out exploratory compensation, if the bit error rate reduces, can determine that selection is correct, conversely, another point is real-time polarization
State.According to the real-time polarization state of judgement, polarized controller is adjusted according to general method, so that it may realize to quantum key distribution
The compensation of system photon polarization state.
During specific implementation:
Using the quantum key distribution system of BB84 agreements, encoded with two groups of linear polarizations, be respectively 0 ° and 90 °, 45 ° and
135 °, it is seen that be non-orthogonal between two groups of polarization states, and be orthogonal between every group of two polarization states.Such quantum is close
Key dissemination system carries out polarization compensation, two non-orthogonal polarization states, such as 0 ° and 45 ° is compensated simultaneously, Fig. 1's
On Poincar é balls, 0 ° of corresponding points A0, 45 ° of corresponding points B0。
In length it is that quantum key that key length disclosed in M primary key is N (be much smaller than M) divides when assessing the bit error rate
Hair system, the photon state of polarization auto compensation method of feedback is combined using the bit error rate and uncertain rate, while compensation two is non-orthogonal
0 ° and 45 ° of polarization state, comprises the following steps:
(a), receiving terminal selects N ' positions in effective detection sequence where length is M primary key and base is failed at random
Result of detection, referred to as pseudo- key, disclosed by classical channel to transmitting terminal;
(b) A, is labeled as by 0 °, B is labeled as by 45 °;
(c), by A, corresponding point is designated as A on Poincar é balls0, A0It is expectation polarization states of the A in receiving terminal, B is existed
Corresponding point is designated as B on Poincar é balls0, B0It is expectation polarization states of the B in receiving terminal, A0With B0Angle, i.e. relevant radii
Angle, span are (0, π);
(d), in disclosed N-bit key, the bit error rate for counting A is EA;
(e) circle C, is made on Poincar é ballsESo that CEOn point and A0The cosine value of half-angle of angle be (1-EA)
Positive square root;
(f), in disclosed N ' positions puppet key, statistics transmitting terminal is encoded to A but receiving terminal detects the probability for being B, i.e. A phases
To B uncertain rate, U is designated asA;
(g) circle C, is made on Poincar é ballsUSo that CUOn point and B0The cosine value of half-angle of angle be UAJust
Square root;
(h), by CEIt is designated as CEA, by CUIt is designated as CUA, B then is labeled as by 0 °, A is labeled as by 45 °, repeat step (c)~
(g) C that, will be obtainedEIt is designated as CEB, the C that will obtainUIt is designated as CUB, as shown in Figure 1;
(i), because CEAWith CUA、CEBWith CUBThere are 2 intersection points, and CEBThe corresponding bit error rate is larger, so first to CEBWith
CUB2 intersection points carry out exploratory compensation and judge the real-time polarization state B of receiving terminal1, then from CEAWith CUA2 intersection points in
The B for selecting and having determined that1Angle closest to right angle point as another real-time polarization state A1, exploratory compensation is then removed,
According to selected A1And B1Compensate, then go to (a) and carry out next round compensation;
The present invention is to CEBWith CUB2 intersection points carry out it is exploratory compensation judge real-time polarization state method be:Randomly select
1 intersection point compensates to the midpoint of 2 intersection points, if the bit error rate reduces, the point for judging to choose is real-time polarization state, conversely, then
Judge another point for real-time polarization state.
Part that the present invention does not relate to is same as the prior art or can be realized using prior art.
Claims (3)
1. a kind of photon state of polarization auto compensation method of bit error rate and uncertain rate joint feedback, it is characterised in that including following step
Suddenly:
The photon polarization state that quantum key distribution system it is expected to receive is represented with a point on Poincar é balls, real-time polarization
State is with it is expected that the angle of polarization state just corresponds to the current bit error rate, and the angle of real-time polarization state and desired nonopiate polarization state is just
Corresponding current uncertain rate;
Photon polarization state is to the bit error rate of itself polarization state when counting transmitting terminal and receiving terminal to base success, on Poincar é balls
Real-time polarization state is navigated into the relative angle for it is expected polarization state to correspond on the circle of the foregoing bit error rate;
Statistics transmitting terminal and receiving terminal when failing to base photon polarization state to the uncertain rate of desired nonopiate polarization state,
Two points for further navigating to real-time polarization state on foregoing circle on Poincar é balls;
Both of the aforesaid point is all equal to the angle of expectation polarization state and desired nonopiate polarization state, randomly chooses a point
Exploratory compensation is carried out as real-time polarization state, if the bit error rate reduces, can determine that selection is correct, conversely, another point is
Real-time polarization state;
According to the real-time polarization state of judgement, polarized controller is adjusted according to general method, is realized to quantum key distribution system
The compensation for photon polarization state of uniting;
Wherein;Quantum key distribution system announces N positions in the primary key that length is M and is used to count the bit error rate, wherein N every time
Much smaller than M, N positions puppet key is announced in effective detection sequence where primary key and is used to count uncertain rate, utilizes error code
Rate and uncertain rate are in the photon polarization state of Poincar é balls estimation receiving terminal, two non-orthogonal polarization states of realization while compensation
|+>With | H>, specifically include following steps:
(a), the receiving terminal of quantum key distribution system is chosen at random in effective detection sequence where length is M primary key
N ' positions are selected referred to as pseudo- key, to disclose, wherein N ' >=N the result of detection of base failure to transmitting terminal by classical channel;
(b), by non-orthogonal two polarization states |+>With | H>It is respectively labeled as A and B;
(c), by A, corresponding point is designated as A on Poincar é balls0, A0It is expectation polarization states of the A in receiving terminal, by B in Poincar
Corresponding point is designated as B on é balls0, B0It is expectation polarization states of the B in receiving terminal, A0With B0Angle, i.e. relevant radii angle, take
It is (0, π) to be worth scope;
(d), in disclosed N-bit key, the bit error rate for counting A is EA;
(e) circle C, is made on Poincar é ballsESo that circle CEOn point and A0The cosine value of half-angle of angle be (1-EA)
Positive square root;
(f), in disclosed N ' positions puppet key, it is B probability that statistics transmitting terminal, which is encoded to A but receiving terminal detection, i.e., A is with respect to B
Uncertain rate, be designated as UA;
(g) circle C, is made on Poincar é ballsUSo that circle CUOn point and B0The cosine value of half-angle of angle be UAIt is just flat
Root;
(h), by CEIt is designated as CEA, by CUIt is designated as CUA, then by non-orthogonal polarization state |+>With | H>B and A are respectively labeled as, is repeated
Step (c)~(g), it will obtain CEIt is designated as CEB, by CUIt is designated as CUB;
(i), judge real-time polarization state according to following situations, take general method to adjust polarized controller, realize to quantum
The compensation of key distribution system photon polarization state:
If CEAWith CUA、CEBWith CUBOnly have 1 intersection point, then the two are put to the real-time polarization state as A in receiving terminal
A1With B receiving terminal real-time polarization state B1Compensate, then go to (a) and carry out next round compensation;
If CEAWith CUAThere are 1 intersection point, CEBWith CUBThere are 2 intersection points, then first by CEAWith CUAIntersection point as A receiving terminal reality
When polarization state A1, then to CEBWith CUB2 intersection points carry out exploratory compensation and judge real-time polarization state Bs of the B in receiving terminal1,
Then exploratory compensation is removed, according to selected A1And B1Compensate, then go to (a) and carry out next round compensation;
If CEAWith CUAThere are 1 intersection point, CEBWith CUBThere is no intersection point, then first by CEAWith CUAIntersection point as A receiving terminal reality
When polarization state A1, then in CEBWith CUBOn take 2 nearest points of mutual distance, therefrom choose and A1Angle closest to right angle
Put the real-time polarization state B in receiving terminal as B1, according to selected A1And B1Compensate, then go to (a) and carry out next round benefit
Repay;
If CEAWith CUA、CEBWith CUBThere are 2 intersection points, then two first larger to bit error rate points carry out exploratory compensation to sentence
A fixed real-time polarization state A1Or B1, the A that then selects and have determined that from less two points of the bit error rate1Or B1Angle most
Close to right angle point as another real-time polarization state B1Or A1, exploratory compensation is then removed, according to selected A1And B1Carry out
Compensation, then go to (a) and carry out next round compensation;
If CEAWith CUAThere are 2 intersection points, CEBWith CUBThere is 1 intersection point, then first by CEBWith CUBIntersection point as B receiving terminal reality
When polarization state B1, then to CEAWith CUA2 intersection points carry out exploratory compensation and judge real-time polarization state As of the A in receiving terminal1,
Then exploratory compensation is removed, according to selected A1And B1Compensate, then go to (a) and carry out next round compensation;
If CEAWith CUAThere are 2 intersection points, CEBWith CUBThere is no intersection point, then first to CEAWith CUA2 intersection points use exploratory compensation
To judge A real-time polarization state A1, then in CEBWith CUBOn take 2 nearest points of mutual distance, therefrom choose and A1Angle
Closest to the real-time polarization state B put as B in receiving terminal at right angle1, exploratory compensation is then removed, according to selected A1And B1
Compensate, then go to (a) and carry out next round compensation;
If CEAWith CUA、CEBWith CUBThere is no intersection point, now two groups of circles respectively have the nearest point of 2 mutual distances, then first choose phase
Mutual edge distance closer to be located at CEAOr CEBOn that point be used as a real-time polarization state A1Or B1, then from another group of mutual distance
The A for selecting and having determined that in 2 nearest points1Or B1Angle closest to right angle point as another real-time polarization state B1Or
A1, according to selected A1And B1Compensate, then go to (a) and carry out next round compensation;
If CEAWith CUAThere is no intersection point, CEBWith CUBThere is 1 intersection point, then by CEBWith CUBIntersection point as B in the real-time of receiving terminal
Polarization state B1, then in CEAWith CUAOn take 2 nearest points of mutual distance, therefrom selection and B1Angle closest to right angle point
As A receiving terminal real-time polarization state A1, according to selected A1And B1Compensate, then go to (a) and carry out next round benefit
Repay;
If CEAWith CUAThere is no intersection point, CEBWith CUBThere are 2 intersection points, then first to CEBWith CUB2 intersection points use exploratory compensation
To judge B real-time polarization state B1, then in CEAWith CUAOn take 2 nearest points of mutual distance, therefrom choose and B1Angle
Closest to the real-time polarization state A put as A in receiving terminal at right angle1, exploratory compensation is then removed, according to selected A1And B1
Compensate, then go to (a) and carry out next round compensation.
2. the photon state of polarization auto compensation method of the bit error rate according to claim 1 and uncertain rate joint feedback, its feature
It is, 2 intersection points is carried out with exploratory compensation and judges that the method for real-time polarization state randomly selects 1 intersection point to 2 intersection points
Midpoint compensates, if the bit error rate of the polarization state reduces, the point for judging to choose is real-time polarization state, conversely, then judging another
Individual point is real-time polarization state.
3. the photon state of polarization auto compensation method of the bit error rate according to claim 1 and uncertain rate joint feedback, its feature
It is, the method for removing exploratory compensation is the state for reverting to polarization compensation device before exploratory compensation.
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CN108173647B (en) * | 2017-12-28 | 2021-02-02 | 中国人民解放军陆军工程大学 | Polarization state ambiguity elimination method during incomplete evolution reconstruction |
CN108173646B (en) * | 2017-12-28 | 2021-02-02 | 中国人民解放军陆军工程大学 | Photon polarization state compensation method based on evolution history reconstruction |
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