CN107195324A - A kind of high efficiency quantum storing device of continuous variable non-classical optical state - Google Patents

A kind of high efficiency quantum storing device of continuous variable non-classical optical state Download PDF

Info

Publication number
CN107195324A
CN107195324A CN201710626022.2A CN201710626022A CN107195324A CN 107195324 A CN107195324 A CN 107195324A CN 201710626022 A CN201710626022 A CN 201710626022A CN 107195324 A CN107195324 A CN 107195324A
Authority
CN
China
Prior art keywords
optical
output end
input
pulse signal
atomic
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
CN201710626022.2A
Other languages
Chinese (zh)
Inventor
闫智辉
贾晓军
彭堃墀
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Shanxi University
Original Assignee
Shanxi University
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Shanxi University filed Critical Shanxi University
Priority to CN201710626022.2A priority Critical patent/CN107195324A/en
Publication of CN107195324A publication Critical patent/CN107195324A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11CSTATIC STORES
    • G11C13/00Digital stores characterised by the use of storage elements not covered by groups G11C11/00, G11C23/00, or G11C25/00
    • G11C13/04Digital stores characterised by the use of storage elements not covered by groups G11C11/00, G11C23/00, or G11C25/00 using optical elements ; using other beam accessed elements, e.g. electron or ion beam
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B82NANOTECHNOLOGY
    • B82YSPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
    • B82Y10/00Nanotechnology for information processing, storage or transmission, e.g. quantum computing or single electron logic
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06NCOMPUTING ARRANGEMENTS BASED ON SPECIFIC COMPUTATIONAL MODELS
    • G06N10/00Quantum computing, i.e. information processing based on quantum-mechanical phenomena

Abstract

The present invention relates to a kind of high efficiency quantum storing device of continuous variable non-classical optical state.The present invention mainly solves the low technical problem of existing non-classical optical state quantum storage efficiency.The technical scheme is that:A kind of high efficiency quantum storing device of continuous variable non-classical optical state, including light source cell, atomic system and compression measuring system;The light source cell is provided with local oscillations optical signal aLOutput end, probe optical pulse signal aPOutput end and control light pulse signal aCOutput end;The probe optical pulse signal aPThe first input end connection of output end and atomic system, the control light pulse signal aCThe second input connection of output end and atomic system, the output end of atomic system is connected with compressing the first input end of measuring system, local oscillations optical signal aLOutput end is connected with compressing the second input of measuring system;The compression measuring system by optical beam-splitter, two balanced homodyne detection devices, power subtracter and numeral can storage oscillograph constitute.

Description

A kind of high efficiency quantum storing device of continuous variable non-classical optical state
Technical field
The present invention relates to a kind of high efficiency quantum storing device of continuous variable non-classical optical state.It belongs to a kind of by continuously The quantum state storage of variable compression state light field is measured into the spin wave quantum state of atom assemblage, and by optical resonator raising The equipment of sub- storage efficiency.
Background technology
With the development of quantum information science, the quantum information network being made up of quantum optics passage and atom quantum nodes It is the guarantee of practical application.Wherein, the just ideal carrier of quantum information long-distance transmissions;Atom assemblage is due to thick with optics The big advantage for going with coherence of degree, is to realize one of Effective medium of quantum nodes, it is possible to achieve the storage of quantum information and place Reason.Therefore, the quantum state of light is stored in atom assemblage, is the important foundation for realizing quantum information network.
Non-classical optical state is the core resource for realizing quantum information.Wherein, squeezed light is a kind of important non-classical optical state, And it can be coupled into by optical beam-splitter and tangle light.At present, the transparent mechanism of electromagnetically induced is to realize one kind of quantum storage Effective ways, can realize the mutual mapping between the quantum state of light and the spin state of atom.Electricity particularly in atom assemblage Magnetic guidance clearing process has the advantages that noise is small, therefore this method is applied to the quantum storage of non-classical optical state.Meanwhile, Gao Bao True quantum information processing needs efficient quantum storage.Therefore, the quantum state of squeezed light is expeditiously stored into atom system Comprehensive spin state, is the key of the practical development of quantum information network.
2012, Japanese Kozuma seminar realized compression using the transparent mechanism of electromagnetically induced in cold atom assemblage The quantum storage of light, in Phys.Rev.Lett.100, entitled " Storage and Retrieval are delivered in 093601 (2008) Of a Squeezed Vacuum " paper.The same year, Canadian Lvovsky seminar also achieves in pyrogen subensemble The quantum storage of squeezed light, in Phys.Rev.Lett.100, entitled " Quantum Memory for are delivered in 093602 (2008) Squeezed Light " paper.
Two above research work realize squeezed light atom assemblage quantum store, solve non-classical optical state The problem of quantum is stored is realized in atom assemblage, but the quantum storage efficiency of the above method is most in 10-20% or so, and they are deposited In the low technical problem of quantum storage efficiency.
The content of the invention
Present invention aim to address the low technical problem of existing non-classical optical state quantum storage efficiency, there is provided a kind of reliable Property the good and high continuous variable non-classical optical state of storage efficiency high efficiency quantum storing device.
In order to solve the above technical problems, the technical solution adopted by the present invention is:A kind of height of continuous variable non-classical optical state Efficiency quantum storing device, including light source cell, atomic system and compression measuring system;The light source cell is provided with local oscillations Optical signal aLOutput end, probe optical pulse signal aPOutput end and control light pulse signal aCOutput end;The spy of the horizontal polarization Pin light pulse signal aPThe first input end connection of output end and atomic system, the control light pulse signal a polarized verticallyC The second input connection of output end and atomic system, the first input end of the output end and compression measuring system of atomic system connects Connect, local oscillations optical signal aLOutput end is connected with compressing the second input of measuring system;The compression measuring system is by light Learning beam splitter, two balanced homodyne detection devices, power subtracter and numeral can storage oscillograph composition.
The light source cell is by tunable laser, the optical beam-splitter arrays of 1x 3, optical parametric amplifier, four sets of acousto-optics Modulating system is constituted.The output end of the tunable laser is connected with the input of 1x3 optical beam-splitter arrays, 1x3 optics The first output end output local oscillations optical signal a of beam splitter arrayL, the second output end of 1x3 optical beam-splitter arrays and The input connection of one acousto-optic modulation system, the output end of the first acousto-optic modulation system and the input of optical parametric amplifier connect Connect, the output end of optical parametric amplifier is connected with the input of the 3rd acousto-optic modulation system, the output of the 3rd acousto-optic modulation system Probe optical pulse signal aP, the 3rd output end of 1x3 optical beam-splitter arrays is connected with the input of rising tone light modulation system, The output end of rising tone light modulation system is connected with the input of falling tone light modulation system, the output control of falling tone light modulation system Light pulse signal a processedC;The tunable laser uses low noise, narrow linewidth, ti sapphire laser;The optical parameter is put Big device produces the compressed state optical field with Atomic absorption lines matching;Described first, the 3rd, falling tone light modulation system is by a pair of acousto-optics Modulator is constituted;The rising tone light modulation system is made up of two double secondary acousto-optic modulators passed through.
The atomic system is made up of atomic components and optical resonator, and the optical resonator is by the flat hysteroscope of two panels, two The concavees lens composition that the plano-concave hysteroscope and a piece of focal length that plate curvature radius is 1000mm are 30mm;The optical resonator uses four Mirror ring cavity structure, a length of 1456mm of its chamber;First flat hysteroscope is as input and output coupling mirror, and the transmitance to probe light is 20%;Second flat hysteroscope is high to probe light anti-;Two panels plano-concave hysteroscope is high to probe light anti-, and a piece of plano-concave hysteroscope is fixed On piezoelectric ceramics;The atomic components are located in the middle of two plano-concave hysteroscopes of optical resonator.
The present invention uses above-mentioned technical proposal, and orthogonal point of light field in electromagnetically induced clearing process is strengthened using optical resonator The interaction of amount and atom assemblage collective spin wave, and then quantum storage efficiency is improved, to realize the efficient of non-classical optical state Rate quantum is stored.The transparent mechanism of electromagnetically induced is using the coherence between two ground state levels of atom, in the effect of control light Under, there is Transparency Phenomenon in probe light, and due to slower rays phenomenon caused by dispersion, this is provided for the realization that quantum is stored can Energy.Theoretical according to dark-state extremely son, in the presence of light is write, quantum state can be mapped to atom assemblage from light field;Reading the work of light Under, quantum state can be mapped to light field from atom assemblage.Moreover, the noise very little that electromagnetically induced clearing process is introduced, especially Suitable for the quantum storage of non-classical optical state.In addition, repeatedly passing through atom in optical resonance intracavitary light field, can effectively it strengthen The interaction of light and atom, and then improve quantum storage efficiency.The present invention can realize the high efficiency storage of compressed state optical field And release, the quantum state of compressed state optical field is expeditiously stored in atom assemblage.Compared with background technology, the present invention has Storage efficiency is high, the advantage of good reliability.The quantum storing device of the present invention has following beneficial effect:
1st, the present invention mutually ties optical resonator technology with based on the transparent atom assemblage quantum memory technology of electromagnetically induced Close, the high efficiency quantum storage of non-classical optical state can be realized.
2nd, the optical resonator that the present invention is utilized can make probe light repeatedly pass through atom assemblage, interact, Improve quantum storage efficiency.
3rd, the optical resonance intracavitary that the present invention is utilized places concavees lens, for waist class in enlarged cavity, to increase light and original The region of son interaction, improves quantum storage efficiency.
The present invention is to be improved the quantum storage efficiency of continuous variable non-classical optical state by optical resonator, is adapted to application In the processing of quantum information network, particularly high-fidelity quantum information comprising atomic node.
Brief description of the drawings
Fig. 1 the structural representation of present invention;
The structural representation of Fig. 2 light source cells of the present invention;
The energy level schematic diagram of Fig. 3 atom assemblages of the present invention;
The control sequential figure of Fig. 4 optical signals of the present invention;
The structural representation of Fig. 5 atomic systems of the present invention;
The structural representation of Fig. 6 present invention compression measuring systems.
Embodiment
The present invention is described in further detail with reference to the accompanying drawings and examples.
As shown in figure 1, a kind of high efficiency quantum storing device of continuous variable non-classical optical state in the present embodiment, including Light source cell 1, atomic system 2 and compression measuring system 3;The light source cell 1 is provided with local oscillations optical signal aLOutput end, spy Pin light pulse signal aPOutput end and control light pulse signal aCOutput end;The probe optical pulse signal a of the horizontal polarizationPIt is defeated Go out end to be 1. connected with the first input end of atomic system 2, the control light pulse signal a polarized verticallyCOutput end and atom 2. second input of system 2 connects, and 1. the output end of atomic system 2 is connected with compressing the first input end of measuring system 3, this Ground oscillating optical signal aL2. output end is connected with compressing the second input of measuring system 3.
As shown in Fig. 2 the light source cell is by tunable laser 11, the optical beam-splitter arrays 12 of 1x 3, optical parameter Amplifier 13 and four sets of acousto-optic modulation system 14-17 compositions.The output end of the tunable laser 11 and 1x3 optical beam-splitters 1. the input connection of array 12, the first output end of 1x3 optical beam-splitters array 12 exports local oscillations optical signal aL, 1x3 Input of second output end of optical beam-splitter array 12 2. with the first acousto-optic modulation system 14 is connected, the first acousto-optic modulation system The output end of system 14 is connected with the input of optical parametric amplifier 13, the output end of optical parametric amplifier 13 and the 3rd acousto-optic The input connection of modulating system 16, the 3rd acousto-optic modulation system 16 output probe optical pulse signal aP, 1x3 optical beam-splitters battle array Input of 3rd output end of row 12 3. with rising tone light modulation system 15 is connected, the output end of rising tone light modulation system 15 It is connected with the input of falling tone light modulation system 17, the output control light pulse signal a of falling tone light modulation system 17C.It is described Tunable laser 11 is using low noise, narrow linewidth, ti sapphire laser, and the laser exports 795nm laser, corresponding to rubidium The Absorption Line of atom.Optical parametric amplifier 13 produces the compressed state optical field with rubidium Atomic absorption lines matching.Firstth, the 3rd acousto-optic Modulating system 14,16, opens the light for being realized to laser, obtains probe optical pulse signal aP.Secondth, falling tone light modulation system 15th, 17, for realizing frequency displacement to laser and opening the light, obtain control light pulse signal aC.First acousto-optic modulation system 14 is by a pair 100MHz acousto-optic modulators are constituted, for producing the analog optical signal that optical parametric amplifier 13 and atomic system 2 are locked.Second Acousto-optic modulation system 15 is made up of two double secondary 1.7GHz acousto-optic modulators passed through, the shift frequency for realizing laser 6.8GHz. 3rd, falling tone light modulation system 16,17 is made up of a pair of 100MHz acousto-optic modulators, for the sequential control in storing process System.
As shown in figure 3, the atomic system 2 is using the 5 of the atom of rubidium 872S1/2F=1 and F=2 and 52P1/2F '=1 Hyperfine energy level.Using the tuning characteristic and the shift frequency characteristic of second sound-optic modulator 15 of ti sapphire laser 11, phase is obtained Answer the optical signal of wavelength.Control light pulse signal aCFrequency and 52S1/2F=1 to 52P1/2The transition absorption line of F '=1 have Δ=700MHz single photon off resonance;Probe optical pulse signal aPWith local oscillations optical signal aLFrequency it is identical, the frequency and 52S1/2F=2 to 52P1/2The transition absorption line of F '=1 have Δ=700MHz single photon off resonance and δ=0.5MHz double light Sub- mismatching angle.
As shown in figure 4, using first, the 3rd, the switching characteristic of falling tone optical modulator 14,16,17, when realizing corresponding Sequence is controlled.Whole controlling cycle takes 1 millisecond.Local oscillations optical signal aLWithout acousto-optic modulator, in normally open.In light In 10 microseconds of atomic interaction, using acousto-optic modulator 14 by probe optical pulse signal aPClose, remaining time opens And strong simulated light is exported, for the locking to optical resonator in optical parametric amplifier and quantum storage;In probe light In pulse signal and atomic interaction time, using acousto-optic modulator 16 by probe optical pulse signal aPOpened for 500 nanoseconds, use In quantum storage.While probe optical pulse signal is opened, light pulse signal a will be controlled using acousto-optic modulator 17COpen 1 Microsecond, realizes probe optical pulse signal aPQuantum storage;After the storage time of 1 microsecond, using acousto-optic modulator 17 again Open control light pulse signal aC, the quantum state of atomic system is read, release light pulse signal a ' is converted toP
As shown in figure 5, the atomic system 2 is made up of atomic components and optical resonator, wherein, atomic components are by atom Air chamber 21, magnetic shielding system and temperature control system 24 are constituted, and the magnetic shielding system is made up of magnetic cup wallpaper 22 and magnetic shielding cylinder 23; The atomic air chamber 21 is coated with accordingly filled with atomic gas and a certain amount of inert buffer gas in the light pass surface of atomic air chamber 21 The antireflective film of optical maser wavelength, the outer layer magnetic screen paper 22 of atomic air chamber 21 is wrapped up, and is positioned over the magnetic shielding cylinder 23 of metal It is interior, set former to rubidium using the temperature control system 24 of heating tape, insulation material and temperature control instrument composition in the outer layer of magnetic shielding cylinder 23 Son heating and accurate temperature controlling;The optical resonator is by the flat hysteroscope 25 of two panels, 26, the plano-concave that two panels radius of curvature is 1000mm Hysteroscope 27,28 and a piece of focal length constitute for 30mm concavees lens 29;The optical resonator uses four mirror ring cavity structures, its chamber A length of 1456mm;First flat hysteroscope 25 is located at probe optical pulse signal a as input and output coupling mirrorPInput path and go out Penetrate in light path, the transmitance to probe light is 20%;Second flat hysteroscope 26 is located at probe optical pulse signal aPInput path In to probe optical pulse signal aPIt is high anti-;Two panels plano-concave hysteroscope 27,28 is located at the both sides of atomic system 2 and positioned at probe optical pulse Signal aPReflected light path on to probe optical pulse signal aPHeight is anti-, and a piece of plano-concave hysteroscope 28 is fixed on piezoelectric ceramics, For optical resonator chamber length, probe optical pulse signal aPWith control light pulse signal aCThe locking of resonance;Concavees lens 29 are located at To probe optical pulse signal a in the middle of a piece of flat hysteroscope 25 and second flat hysteroscope 26PIt is high thoroughly to amplify intracavitary hot spot, to increase The region of light and atomic interaction;The atomic components are located in the middle of two plano-concave hysteroscopes 27,28 of optical resonator.
As shown in fig. 6, the compression measuring system is by optical beam-splitter 31, balanced homodyne detection device 32,33, power subtraction Device 34 and numeral can storage oscillograph 35 constitute;The probe optical pulse a ' of releasePWith local oscillations optical signal aLThrough optical beam-splitter 31 interference, interference signal can 35 pairs of releases of storage oscillograph by balanced homodyne detection device 32,33, power subtracter 34 and numeral Probe optical pulse a 'PThe quantum noise of quadrature component measure, store and analyze, and it is interfered using simulated light Position difference is locked.
Optical parametric amplifier 13 is operated in the anti-magnifying state of parameter, produces a branch of orthogonal amplitude squeezed light;By first, 3rd acousto-optic modulator 14,16 is converted into compression probe optical pulse signal aP;In control light pulse signal aCWrite-in effect Under, by above-mentioned compression probe optical pulse signal aPStore in atomic system 2;In control light pulse signal aCReading effect under, The quantum state of above-mentioned atomic system 2 is mapped to release probe optical pulse a 'PIn, and utilize local oscillations optical signal aLAnd pressure Contracting measuring system 3 discharges light pulse signal to it and measured.
The present invention is not limited to the above embodiments, without departing from the scope of the invention, enters according to the above description Capable improvement and conversion should all belong to the protection domain of the claims in the present invention.

Claims (3)

1. a kind of high efficiency quantum storing device of continuous variable non-classical optical state, it is characterised in that:Including light source cell, atom System and compression measuring system;The light source cell is provided with local oscillations optical signal aLOutput end, probe optical pulse signal aPOutput End and control light pulse signal aCOutput end;The probe optical pulse signal a of the horizontal polarizationPThe of output end and atomic system One input is connected, the control light pulse signal a polarized verticallyCThe second input connection of output end and atomic system, The output end of atomic system is connected with compressing the first input end of measuring system, local oscillations optical signal aLOutput end is surveyed with compression The second input connection of amount system;The compression measuring system is subtracted by optical beam-splitter, two balanced homodyne detection devices, power Musical instruments used in a Buddhist or Taoist mass and numeral can storage oscillograph compositions.
2. a kind of high efficiency quantum storing device of continuous variable non-classical optical state according to claim 1, its feature exists In:The light source cell is by tunable laser, 1x3 optical beam-splitters array, optical parametric amplifier and four sets of acousto-optic modulations System is constituted;The output end of the tunable laser is connected with the input of 1x3 optical beam-splitter arrays, 1x3 optical beam splittings The first output end output local oscillations optical signal a of device arrayL, the second output end and the first sound of 1x3 optical beam-splitter arrays The input connection of light modulation system, the output end of the first acousto-optic modulation system and the input of optical parametric amplifier are connected, The output end of optical parametric amplifier is connected with the input of the 3rd acousto-optic modulation system, the 3rd acousto-optic modulation system output probe Light pulse signal aP, the 3rd output end of 1x3 optical beam-splitter arrays is connected with the input of rising tone light modulation system, and second The output end of acousto-optic modulation system is connected with the input of falling tone light modulation system, falling tone light modulation system output control light Pulse signal aC;The tunable laser uses low noise, narrow linewidth, ti sapphire laser;The optical parametric amplifier Produce the compressed state optical field with Atomic absorption lines matching;Described first, the 3rd, falling tone light modulation system is by a pair of acousto-optic modulations Device is constituted;The rising tone light modulation system is made up of two double secondary acousto-optic modulators passed through.
3. a kind of high efficiency quantum storing device of continuous variable non-classical optical state according to claim 1, its feature exists In:The atomic system is made up of atomic components and optical resonator, and the optical resonator is by the flat hysteroscope of two panels, two plate curvatures The concavees lens composition that the plano-concave hysteroscope and a piece of focal length that radius is 1000mm are 30mm;The optical resonator is using four mirrors annular Cavity configuration, a length of 1456mm of its chamber;First flat hysteroscope is as input and output coupling mirror, and the transmitance to probe light is 20%; Second flat hysteroscope is high to probe light anti-;Two panels plano-concave hysteroscope is high to probe light anti-, and a piece of plano-concave hysteroscope is fixed on pressure On electroceramics;The atomic components are located in the middle of two plano-concave hysteroscopes of optical resonator.
CN201710626022.2A 2017-07-27 2017-07-27 A kind of high efficiency quantum storing device of continuous variable non-classical optical state Pending CN107195324A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201710626022.2A CN107195324A (en) 2017-07-27 2017-07-27 A kind of high efficiency quantum storing device of continuous variable non-classical optical state

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201710626022.2A CN107195324A (en) 2017-07-27 2017-07-27 A kind of high efficiency quantum storing device of continuous variable non-classical optical state

Publications (1)

Publication Number Publication Date
CN107195324A true CN107195324A (en) 2017-09-22

Family

ID=59884058

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201710626022.2A Pending CN107195324A (en) 2017-07-27 2017-07-27 A kind of high efficiency quantum storing device of continuous variable non-classical optical state

Country Status (1)

Country Link
CN (1) CN107195324A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109856888A (en) * 2019-02-25 2019-06-07 山西大学 A kind of device and method enhancing the continuous variable compressed state optical field degree of compression
CN110133941A (en) * 2019-04-28 2019-08-16 山西大学 A kind of quasi-continuous quantum Squeezed Vacuum generation device
CN112994691A (en) * 2021-02-23 2021-06-18 北京无线电计量测试研究所 Preparation method of non-Hermite system spin compression state
CN113014257A (en) * 2021-02-23 2021-06-22 北京无线电计量测试研究所 Preparation method of cold atom system spin compression state

Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101286616A (en) * 2008-05-30 2008-10-15 中国科学院上海光学精密机械研究所 2 mu m complete solid state pulse ring laser
US7518784B2 (en) * 2007-05-18 2009-04-14 Wisconsin Alumni Research Foundation Apparatus and method of producing quantum-entangled, up-converted light beams
CN102175429A (en) * 2011-01-11 2011-09-07 山西大学 Method for measuring thermal focus length of laser
CN103091933A (en) * 2013-01-30 2013-05-08 山西大学 Generating device for continuous variable polychrome entangled optical field
US20130301094A1 (en) * 2012-05-10 2013-11-14 The Mitre Corporation Method and Apparatus for Quantum Mechanical Entanglement Protection
CN104283101A (en) * 2014-11-12 2015-01-14 核工业理化工程研究院 All-solid-state single-frequency tunable red laser
CN105652555A (en) * 2016-02-05 2016-06-08 山西大学 Continuous variable light and atom ensemble entanglement production device
CN105676559A (en) * 2016-02-05 2016-06-15 山西大学 Generating device for entanglement of continuous variable atom ensemble
CN105807535A (en) * 2016-05-16 2016-07-27 山西大学 Generation device of quantum entanglement among three atomic ensembles
CN105954010A (en) * 2016-05-17 2016-09-21 山西大学 Measurement method of nonlinear crystal thermal lens focal length

Patent Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7518784B2 (en) * 2007-05-18 2009-04-14 Wisconsin Alumni Research Foundation Apparatus and method of producing quantum-entangled, up-converted light beams
CN101286616A (en) * 2008-05-30 2008-10-15 中国科学院上海光学精密机械研究所 2 mu m complete solid state pulse ring laser
CN102175429A (en) * 2011-01-11 2011-09-07 山西大学 Method for measuring thermal focus length of laser
US20130301094A1 (en) * 2012-05-10 2013-11-14 The Mitre Corporation Method and Apparatus for Quantum Mechanical Entanglement Protection
CN103091933A (en) * 2013-01-30 2013-05-08 山西大学 Generating device for continuous variable polychrome entangled optical field
CN104283101A (en) * 2014-11-12 2015-01-14 核工业理化工程研究院 All-solid-state single-frequency tunable red laser
CN105652555A (en) * 2016-02-05 2016-06-08 山西大学 Continuous variable light and atom ensemble entanglement production device
CN105676559A (en) * 2016-02-05 2016-06-15 山西大学 Generating device for entanglement of continuous variable atom ensemble
CN105807535A (en) * 2016-05-16 2016-07-27 山西大学 Generation device of quantum entanglement among three atomic ensembles
CN105954010A (en) * 2016-05-17 2016-09-21 山西大学 Measurement method of nonlinear crystal thermal lens focal length

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
闫智辉: "连续变量量子纠缠操控的理论与实验研究", 《中国博士学位论文全文数据库基础科学辑》 *

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109856888A (en) * 2019-02-25 2019-06-07 山西大学 A kind of device and method enhancing the continuous variable compressed state optical field degree of compression
CN110133941A (en) * 2019-04-28 2019-08-16 山西大学 A kind of quasi-continuous quantum Squeezed Vacuum generation device
CN112994691A (en) * 2021-02-23 2021-06-18 北京无线电计量测试研究所 Preparation method of non-Hermite system spin compression state
CN113014257A (en) * 2021-02-23 2021-06-22 北京无线电计量测试研究所 Preparation method of cold atom system spin compression state
CN112994691B (en) * 2021-02-23 2022-05-20 北京无线电计量测试研究所 Preparation method of non-Hermite system spin compression state
CN113014257B (en) * 2021-02-23 2022-05-20 北京无线电计量测试研究所 Preparation method of cold atom system spin compression state

Similar Documents

Publication Publication Date Title
CN107195324A (en) A kind of high efficiency quantum storing device of continuous variable non-classical optical state
CN104316180B (en) Based on two optical frequency com optical imaging methods of continuous Frequency Stabilized Lasers
CN105807535B (en) The generation device of quantum entanglement between a kind of three atom assemblages
CN105814452A (en) Laser radar device
CN105652555B (en) The generation device that a kind of continuous variable light and atom assemblage tangle
Heersink et al. Polarization squeezing of intense pulses with a fiber-optic Sagnac interferometer
CN107272299B (en) The generation device of continuous variable quantum entanglement between multiple atom assemblages
CN109494559A (en) Orphan's frequency comb generation device and operating method
CN102426279A (en) All-optical high-voltage voltage transformer
Liu et al. Two-beam pumped cascaded four-wave-mixing process for producing multiple-beam quantum correlation
CN105676559A (en) Generating device for entanglement of continuous variable atom ensemble
CN108227247A (en) The 8 journey frequency shifters based on acousto-optic modulation
Zhu et al. Coherent optical memory based on a laser-written on-chip waveguide
CN203490436U (en) Electro-optics Q-switch optical switch
CN204256335U (en) A kind of nonlinear interferometer based on optical parameter process
CN107346086B (en) The generation device of continuous variable quantum entanglement between quantum channel and quantum nodes
CN108011286B (en) Device for generating sub-kHz low-frequency intensity difference compression based on cesium atom ensemble
CN104698720A (en) Generating set of continuous-variable multi-component polarized entangled optical field
CN205985740U (en) Four ways laser beam combining system
CN207751871U (en) A kind of measuring device of nonlinear refraction coefficient of materials rate coefficient
CN105719719A (en) Device for non-classical state teleportation between continuous variable quantum storage nodes
CN217007473U (en) Ultra-wideband microwave signal spectrum measurement system
Guo et al. Single photon at a configurable quantum-memory-based beam splitter
CN107678189A (en) It is a kind of can the quick optics cavity output signal interference of light of accurate adjustment two device
Zhang et al. Interfacing a two-photon NOON state with an atomic quantum memory

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
RJ01 Rejection of invention patent application after publication

Application publication date: 20170922

RJ01 Rejection of invention patent application after publication