WO2017214791A1 - Polarization entangled photon pair generation method and apparatus - Google Patents

Polarization entangled photon pair generation method and apparatus Download PDF

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Publication number
WO2017214791A1
WO2017214791A1 PCT/CN2016/085540 CN2016085540W WO2017214791A1 WO 2017214791 A1 WO2017214791 A1 WO 2017214791A1 CN 2016085540 W CN2016085540 W CN 2016085540W WO 2017214791 A1 WO2017214791 A1 WO 2017214791A1
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photon pair
polarization
photon
fundamental mode
conversion unit
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PCT/CN2016/085540
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French (fr)
Chinese (zh)
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柏艳飞
张臣雄
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华为技术有限公司
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Priority to CN201680080574.1A priority Critical patent/CN108604037B/en
Priority to PCT/CN2016/085540 priority patent/WO2017214791A1/en
Publication of WO2017214791A1 publication Critical patent/WO2017214791A1/en

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    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/12Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/12Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
    • G02B6/122Basic optical elements, e.g. light-guiding paths
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/21Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  by interference
    • G02F1/225Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  by interference in an optical waveguide structure

Definitions

  • the present invention relates to the field of optical communication technologies, and in particular, to a method and an apparatus for generating a polarization entangled photon pair.
  • Quantum entanglement is the most important resource in quantum information processing. It is a special quantum state in a composite system composed of multiple particles. Entanglement sources in quantum entanglement include photons, electrons, ions, and the like. Since the coherence of photons is better, entangled photons become a common source of quantum entanglement. Photons have different degrees of freedom, such as polarization degrees of freedom, path degrees of freedom, angular momentum degrees of freedom, etc. Each degree of freedom can be used to encode information. Polarization entangled photons based on polarization degrees of freedom are widely used in quantum information processing because polarization degrees of freedom can be flexibly manipulated by wave plates.
  • the optical waveguide of SOI Silicon On Insulator
  • SOI Silicon On Insulator
  • the pump photon Based on the third-order nonlinearity of silicon material, the pump photon generates a spontaneous four-wave mixing process to generate correlated photon pairs.
  • the silicon wire waveguide due to the large birefringence effect of the TE mode (Transsverse Electric mode) and the TM mode (Transsverse Magnetic mode), the TE mode polarized photon pair is more efficient than the TM mode.
  • the generation efficiency of polarized photon pairs is large, resulting in almost all of the polarized photon pairs generated in the silicon waveguides being TE mode polarized photon pairs.
  • a method of generating a polarized photon pair needs to be improved.
  • Figure 1 shows a method for generating a polarization entangled photon pair based on a spontaneous parametric down-conversion process of a second-order nonlinear crystal.
  • a spontaneous parametric down-conversion process which splits into two lower-energy photons.
  • the two photons are polarized photons in the horizontal direction and the polarized photons in the vertical direction, and the outgoing directions of the two photons are in the direction indicated by the two cones in Fig. 1, and the two conical overlapping regions Photon pair Superimposed as a polarization entangled photon pair.
  • a photon pair in only two conical overlapping regions can produce a polarization entangled photon pair, and photons in other regions cannot be utilized, resulting in a lower efficiency of the polarization entangled photon pair and a lower luminance of the entangled source.
  • the structure of the device is complicated, and all the methods using the bulk optical method require fine adjustment of the optical path and unstable phase.
  • embodiments of the present invention provide a method and an apparatus for generating a polarization entangled photon pair.
  • the technical solution is as follows:
  • a device for generating a polarization entangled photon pair comprising: a beam splitter, a photon pair generating module, a fundamental mode conversion module, and a polarization converter;
  • the beam splitter includes an input end, a first output end, and a second output end, the beam splitter splitting the photon beam input by the input end into a first photon beam and a second photon beam having the same energy, a photon beam is output through the first output end, and the second photon beam is output through the second output end;
  • the photon pair generating module includes a first photon pair generating unit and a second photon pair generating unit, the first photon pair generating unit is connected to the first output end, and can trigger the first photon beam to generate a first TE a pair of modulo polarized photons, the second photon pair generating unit being coupled to the second output end, capable of triggering the second photon beam to generate a second TE mode polarized photon pair;
  • the basic mode conversion module includes a first fundamental mode conversion unit and a second fundamental mode conversion unit, and the first fundamental mode conversion unit is connected to the first photon pair generating unit, and is capable of polarizing the first TE mode Converting to a first TE fundamental mode polarized photon pair, the second fundamental mode converting unit being coupled to the second photon pair generating unit, capable of converting the second TE mode polarized photon pair into a second TE fundamental mode polarizing Photon pair
  • the polarization converter includes a first polarization conversion unit and a second polarization conversion unit, the first polarization conversion unit being coupled to the first fundamental mode conversion unit, capable of polarizing photons of the first TE fundamental mode Coupled to the second polarization conversion unit, the second polarization conversion unit is coupled to the second fundamental mode conversion unit, capable of converting the first TE fundamental mode polarization photon pair into a first TM fundamental mode polarization a photon pair, and superimposing the first TM fundamental mode polarized photon pair and the second TE fundamental mode polarized photon pair as a polarization entangled photon pair, and outputting the polarization entangled photon pair.
  • the TE mode polarized photon pair and the TM mode polarized photon pair generated in the present invention are all used to generate polarization entangled photon pairs, and the polarization entangled photon pair has high efficiency, and the energy of the TE mode polarized photon pair and the TM mode polarized photon pair.
  • the polarization entangled photon pair obtained by the two has higher luminance when used as an entangled light source.
  • the device of the present invention has a simple structure and can be cured in a silicon-based optical waveguide chip such that the phase of the generated polarization entangled photon pair is stabilized.
  • the beam splitter is a Y-beam splitter. It not only enriches the form of the beam splitter, but also enables a processed photon to be accurately divided into two photons of the same energy.
  • the beam splitter is a multimode interferometer, the multimode interferometer further comprising a multimode waveguide region, the multimode waveguide region connection The input end, the first output end, and the second output end. It not only enriches the form of the beam splitter, but also enables a processed photon to be accurately divided into two photons of the same energy.
  • the beam splitter, the photon pair generating module, and the fundamental mode conversion Both the module and the polarization converter are comprised of a silicon dioxide cladding and silicon nanowires.
  • the silicon nanowires in the photon pair generating module are curved and surrounded by a silicon dioxide cladding layer, and
  • the first photon pair generating unit and the second photon pair generating unit have the same structure of the silicon nanowires, so that photon pairs having the same polarization state can be generated through the first photon pair generating unit and the second photon pair generating unit.
  • the silicon nanowires of the first photon pair generating unit and the second photon pair generating unit are both Spiral distribution.
  • the silicon nanowires in the basic mode conversion module are tapered, so that the upper and lower light can be
  • the TE modes in the waveguide are converted to different fundamental modes.
  • the width of the silicon nanowires in the first fundamental mode conversion unit is smaller than the second fundamental mode conversion unit The width of the silicon nanowires.
  • the polarization converter is an asymmetric directional coupler based polarization converter.
  • a method for generating a polarization entangled photon pair applying the polarization entangled photon pair generating device of the first aspect, the method comprising:
  • the beam splitter splits the photon beam input by the input end into a first photon beam and a second photon beam of the same energy, and the first output end transmits the first photon beam to the first photon pair a generating unit, the first photon pair generating unit triggering the first photon beam to generate a first TE mode polarized photon pair, and transmitting the first TE mode polarized photon pair to the first fundamental mode converting unit
  • the second output transmits the second photon beam to the second photon pair generating unit, and the second photon pair generating unit triggers the second photon beam to generate a second TE mode polarized photon pair, and Transmitting a second TE mode polarized photon pair to the second fundamental mode conversion unit;
  • the first fundamental mode conversion unit converts the first TE mode polarized photon pair into a first TE fundamental mode polarized photon pair, and transmits the first TE fundamental mode polarized photon pair to the first polarization conversion unit
  • the second fundamental mode conversion unit converts the second TE mode polarized photon pair into a second TE fundamental mode polarized photon pair, and transmits the second TE fundamental mode polarized photon pair to the second polarization conversion unit;
  • the first polarization conversion unit couples the first TE fundamental mode polarized photon pair to the second polarization conversion unit
  • the second polarization conversion unit converts the first TE fundamental mode polarization photon pair to a TM fundamental mode polarized photon pair and the first TM fundamental mode polarized photon pair and the second TE
  • the fundamental mode polarized photon pairs are superimposed as polarization entangled photon pairs, and the polarization entangled photon pairs are output.
  • the polarization entangled photon pair is further obtained by superimposing the TE mode polarized photon pair and the TM mode polarized photon pair.
  • the invention breaks through the deficiency of the polarization entangled photon pair in the prior art only in the overlapping region of the conical beam, and the generated TE mode and the TM mode polarized photon pair are all used to generate the polarization entangled photon pair, and the polarization entangled photon pair is improved.
  • the device has a simple structure and can be cured in a silicon-based optical waveguide chip, and the phase is relatively stable.
  • FIG. 2 is a schematic structural diagram of a device for generating a polarization entangled photon pair according to an embodiment of the present invention
  • FIG. 3 is a schematic structural view of a Y-type beam splitter according to another embodiment of the present invention.
  • FIG. 4 is a schematic structural view of a multimode interferometer according to another embodiment of the present invention.
  • FIG. 5 is a schematic structural view of an optical waveguide according to another embodiment of the present invention.
  • FIG. 6 is a schematic structural diagram of a polarization converter according to another embodiment of the present invention.
  • FIG. 7 is a flow chart of a method for generating a polarization entangled photon pair according to another embodiment of the present invention.
  • the reference numerals are: 1, a beam splitter; 11, an input terminal; 12, a first output terminal; 13, a second output terminal; 14, a multimode waveguide region; 2. a photon pair generating module; Photon pair generation a second photon pair generating unit; 3. a fundamental mode conversion module; 31, a first fundamental mode conversion unit; 32, a second fundamental mode conversion unit; 4. a polarization converter; 41, a first polarization conversion unit; 42. A second polarization conversion unit.
  • an embodiment of the present invention provides a device for generating a polarization entangled photon pair, the device comprising: a beam splitter 1, a photon pair generating module 2, a fundamental mode conversion module 3, and a polarization converter 4.
  • the beam splitter 1 includes an input end 11, a first output end 12 and a second output end 13, and the beam splitter 1 splits the photon beam input from the input end 11 into a first photon beam and a second photon beam of the same energy.
  • the first photon beam is output through the first output terminal 12, and the second photon beam is output through the second output terminal 13;
  • the photon pair generating module 2 includes a first photon pair generating unit 21 and a second photon pair generating unit 22, the first photon pair generating unit 21 being connected to the first output terminal 12, the first photon pair generating unit 21 being capable of triggering the first
  • the photon beam generates a first TE mode polarized photon pair and transmits the generated first TE mode polarized photon pair
  • the second photon pair generating unit 22 is coupled to the second output 13 and the second photon pair generating unit 22 is capable of triggering
  • the second photon beam generates a second TE mode polarized photon pair and transmits the generated second TE mode polarized photon pair.
  • the first TE mode polarized photon pair and the second TE mode polarized photon pair have the same Correlated photon pairs of polarization states, the two are identical, only the transmission paths are different;
  • the fundamental mode conversion module 3 includes a first fundamental mode conversion unit 31 and a second fundamental mode conversion unit 32, and the first fundamental mode conversion unit 31 is connected to the first photon pair generation unit 21 for receiving the first photon pair generation unit 21 Generating a first TE mode polarized photon pair and converting the first TE mode polarized photon pair into a first TE fundamental mode polarized photon pair, thereby transmitting a first TE fundamental mode polarized photon pair; and a second fundamental mode conversion unit 32 is connected to the second photon pair generating unit 22 for receiving the second TE mode polarized photon pair generated by the second photon pair generating unit 22, and converting the second TE mode polarized photon pair into the second TE mode polarized photon And, in turn, transmitting a second TE fundamental mode polarized photon pair;
  • the polarization converter 4 includes a first polarization conversion unit 41 and a second polarization conversion unit 42, which is connected to the first fundamental mode conversion unit 31 for receiving the first transmission of the first fundamental mode conversion unit 31.
  • the TE fundamental mode polarizes the photon pair and couples the first TE fundamental mode polarized photon pair to the second polarization unit; the second polarization conversion unit 42 is coupled to the second TE fundamental mode polarized photon pair for receiving the second fundamental mode
  • the second TE fundamental mode polarized photon pair transmitted by the polarization conversion unit 32, the effective polarization of the first TE fundamental mode polarized photon pair in the first polarization conversion unit 41 and the TM fundamental mode polarized photon pair in the second deflection conversion unit 42
  • the first TE fundamental mode polarized photon pair is converted into a first TM fundamental mode polarized photon pair, and the first TM fundamental mode polarized photon pair and the second TE fundamental mode polarized photon pair are superimposed into polarization
  • the beam splitter 1 can be a Y-beam splitter.
  • the beam splitter 1 is a Y-type beam splitter
  • the positional relationship of the input terminal 11, the first output terminal 12 and the second output terminal 13 in the Y-type beam splitter is as shown in FIG.
  • the beam splitter 1 can also be a multimode interferometer.
  • the multimode interferometer includes an input terminal 11, a first output terminal 12, a second output terminal 13 and a multimode waveguide region 14, the multimode waveguide region 14 being connected to the input terminal 11, The first output terminal 12 and the second output terminal 13 are provided.
  • the width and length of the multimode waveguide region 14 are set as desired to ensure that the light field achieves a 50/50 splitting effect, i.e., the input photon beam can be split into first and second photon beams of the same energy.
  • the generating device for the polarization entangled photon pair shown in FIG. 2 may be an optical waveguide.
  • the optical waveguide is mainly composed of a silicon dioxide cladding layer and silicon nanowires. Therefore, the beam splitting shown in FIG.
  • the photon pair generation module 2, the fundamental mode conversion module 3, and the polarization converter 4 are each composed of a silicon dioxide cladding layer and silicon nanowires.
  • the input end 11, the first output end 12 and the second output end 13 of the beam splitter 1 are also composed of a silicon dioxide cladding and silicon nanowires;
  • the first photon pair included in the photon pair generating module 2 The generating unit 21 and the second photon pair generating unit 22 are also composed of a silicon dioxide cladding layer and silicon nanowires;
  • the first fundamental mode converting unit 31 and the second fundamental mode converting unit 32 included in the fundamental mode converting module 3 are also composed of two The silicon oxide cladding layer and the silicon nanowires are formed;
  • the second polarization conversion unit 42 is also composed of a silicon dioxide cladding layer and silicon nanowires.
  • the light beam in the optical waveguide is mainly transmitted along the silicon nanowire.
  • the silicon nanowires constituting the functional modules in the device are shown in the optical waveguide chip. Distribution.
  • the silicon nanowires in the photon pair generating module 2 are curved and surrounded in the silicon dioxide cladding layer, and the structure is compact and the length meets the design requirement, so that the light beam is in the photon.
  • the spontaneous four-wave mixing process of the silicon nanowire waveguide can be used to generate a TE mode polarized photon pair.
  • the silicon nanowires in the first photon pair generating unit 21 and the second photon pair generating unit 22 have the same size.
  • the silicon photon in the first photon pair generating unit 21 and the second photon pair generating unit 22 are symmetrically distributed and spiral, of course, the first photon pair generating unit 21 and the second photon pair generating unit 22
  • the shape of the silicon nanowires may also be other shapes, which is not specifically limited in this embodiment.
  • the silicon nanowires in the fundamental mode conversion module 3 are tapered, the width of the silicon nanowires in the first fundamental mode conversion unit 31 is gradually tapered, and the silicon nanometers in the second fundamental mode conversion unit 32 are tapered.
  • the width of the line is gradually thickened, so that the first fundamental mode conversion unit 31 becomes a fine optical waveguide, and the second fundamental mode conversion unit 32 becomes a thick waveguide.
  • the width of the silicon nanowires in the first fundamental mode conversion unit 31 can be Gradually thickening
  • the width of the silicon nanowires in the second fundamental mode conversion unit 32 may be tapered such that the first fundamental mode conversion unit 31 becomes a coarse optical waveguide and the second fundamental mode conversion unit 32 becomes a fine optical waveguide.
  • the width of the silicon nanowires in the fundamental mode conversion module 3 is determined by the width of the silicon nanowires in the polarization converter 4, specifically, the width of the silicon nanowires in the first polarization conversion unit 41 is determined.
  • the width of the silicon nanowires in the first fundamental mode conversion unit 31, and the width of the silicon nanowires in the second polarization conversion unit 42 determine the width of the silicon nanowires in the second fundamental mode conversion unit 32, when in the polarization converter 4 As the width of the silicon nanowires changes, the width of the silicon nanowires in the fundamental mode conversion module 3 needs to be redesigned as needed.
  • the first fundamental mode conversion unit 31 converts the mode of the first TE mode deflection photon pair into a corresponding fundamental mode according to the width of the self silicon nanowire, and obtains the first TE fundamental mode polarized photon pair.
  • the second photon pair generating unit 22 transmits the generated second TE mode polarized photon pair to the second fundamental mode converting unit 32
  • the second fundamental mode converting unit 32 sets the second TE mode according to the width of the self silicon nanowire.
  • the mode of the polarized photon pair is converted to the corresponding fundamental mode, resulting in a second TE fundamental mode polarized photon pair. Since the optical waveguides corresponding to the first fundamental mode conversion unit 31 and the second fundamental mode conversion unit 32 are different, the first TE fundamental mode polarized photon pair and the second TE fundamental mode polarized photon pair obtained after the conversion are also different.
  • the polarization converter 4 is a polarization converter of an asymmetric directional coupler, and the length and width of the silicon nanowires in the first polarization conversion unit 41 and the second polarization conversion unit 42 are also different.
  • the length of the silicon nanowires in the first polarization conversion unit 41 may be smaller than the length of the silicon nanowires in the second polarization conversion unit 42, and the silicon nanowires in the first polarization conversion unit 41
  • the width is smaller than the width of the silicon nanowires in the second polarization conversion unit 42, at which time the first polarization conversion unit 41 does not output a polarization entangled photon pair, which can serve as a test port, and the second polarization conversion unit 42 serves as an output terminal to output polarization entanglement.
  • the length of the silicon nanowires in the first polarization conversion unit 41 may be greater than the length of the silicon nanowires in the second polarization conversion unit 42, and the silicon nanometers in the first polarization conversion unit 41 The width of the line is greater than the width of the silicon nanowires in the second polarization conversion unit 42.
  • the first polarization conversion unit 41 can be made Corresponding to the first TE fundamental mode polarized photon pair in the optical waveguide and the second TM polarization converting unit 42 corresponding to the second TM fundamental mode polarized photon pair in the optical waveguide, the effective refractive index is equal, and according to the coupled mode theory, the finer light can be
  • the TE fundamental mode polarized photon pair in the waveguide is coupled into the coarser optical waveguide and converted into a TM fundamental mode polarized photon pair in the coarser optical waveguide, while the TE fundamental mode polarized photon pair in the coarser optical waveguide still propagates therein.
  • the TE fundamental mode can be expressed as a TE 0 mode
  • the TM fundamental mode can be expressed as a TM 0 mode.
  • the length of the coupling region is 36.8 um
  • the fine optical waveguide can be The TE 0 mode photon pair is coupled into the coarse optical waveguide, and the TE 0 mode photon pair in the coarse optical waveguide still propagates in the coarse optical waveguide.
  • Figure 6 (b) is a cross-sectional view of the polarization converter, where w1 is the width of the thin optical waveguide, w2 is the width in the coarse optical waveguide, and g is the distance between the thin waveguide and the thick waveguide, h is The height of the thick and thin optical waveguide.
  • W1 may be 330 nm
  • w2 may be 600 nm
  • g may be 100 nm
  • h may be 250 nm.
  • the above structural parameters may be specifically designed according to requirements, and are not limited to the above listed data, as long as the fine optical waveguide is satisfied.
  • the TE 0 mode in the middle is equal to the effective refractive index of the TM 0 mode in the coarse optical waveguide, and the length of the coupling region needs to ensure that most of the TE 0 mode in the thin optical waveguide is converted into the TM 0 mode in the thick waveguide.
  • the first photon pair generating unit 21, the first fundamental mode converting unit 31, and the first polarizing converting unit 41 may constitute an on-path optical waveguide, and the second photon pair generating unit 22 and the second fundamental mode converting unit may be configured.
  • 32 and the second polarization conversion unit 42 constitute a lower optical waveguide.
  • the device provided by the embodiment of the present invention divides one input photon into two photons of the same energy, and converts the two photons into TE-mode polarized photon pairs having the same polarization state, thereby polarizing one of the TE modes.
  • the photon pair is converted into a TM mode polarized photon pair, and the polarization entangled photon pair is further obtained by superimposing the TE mode polarized photon pair and the TM mode polarized photon pair.
  • the invention breaks through the deficiency of the polarization entangled photon pair in the prior art only in the overlapping region of the conical beam, and the generated TE mode and the TM mode polarized photon pair are all used to generate the polarization entangled photon pair, and the polarization entangled photon pair is improved.
  • the efficiency of the generation, and the energy of the TE mode and the TM mode polarized photon pair are the same, and thus the brightness of the entangled light source is high.
  • the device has a simple structure and can be cured in a silicon-based optical waveguide chip, and the phase is relatively stable.
  • the embodiment of the present invention provides a method for generating a polarization entangled photon.
  • the method flow provided by the embodiment includes:
  • the beam splitter divides the photon beam input at the input end into a first photon beam and a second photon beam having the same energy, and the first output end transmits the first photon beam to the first photon pair generating unit, and the first photon pair generates
  • the unit triggers the first photon beam to generate a first TE mode polarized photon pair, and transmits the first TE mode polarized photon pair to the first fundamental mode conversion unit, and the second output transmits the second photon beam to the second photon pair generating unit
  • the second photon pair generating unit triggers the second photon beam to generate a second TE mode polarized photon pair, and transmits the second TE mode polarized photon pair to the second fundamental mode converting unit.
  • the first fundamental mode conversion unit converts the first TE mode polarized photon pair into a first TE fundamental mode polarized photon pair, and transmits the first TE fundamental mode polarized photon pair to the first polarization conversion unit
  • the second fundamental mode conversion The unit converts the second TE mode polarized photon pair into a second TE fundamental mode polarized photon pair and transmits the second TE fundamental mode polarized photon pair to the second polarization converting unit.
  • the first polarization conversion unit couples the first TE fundamental mode polarization photon pair into the second polarization conversion unit
  • the second polarization conversion unit converts the first TE fundamental mode polarization photon pair into the first TM fundamental mode polarization photon pair. And superimposing the first TM fundamental mode polarized photon pair and the second TE fundamental mode polarized photon pair into a polarization entangled photon pair, and outputting a polarization entangled photon pair.
  • the above process of generating the polarization entangled photon pair based on the optical waveguide is as follows:
  • the pump photons are input from the off-chip into the SOI optical chip, and are split into two photon beams of the same energy through the beam splitter and transmitted to the upper and lower optical waveguides.
  • the third-order nonlinearity of the silicon wire waveguide is used to generate a spontaneous four-wave mixing process, and the upper and lower optical waveguides respectively generate TE-mode polarized photon pairs having the same polarization state.
  • the tapered optical waveguide converts the mode of the TE mode polarized photon pair into a fundamental mode TE 0 mode in the coarse and fine optical waveguide.
  • the TE 0 mode photon in the thin waveguide is converted into the TM 0 mode photon in the thick waveguide by using a polarization converter, and the TE 0 mode photon pair in the coarse waveguide and the converted TM 0 mode photon pair are superposed.
  • the polarization entangles the pair of photons, which in turn outputs a pair of polarization entangled photons.
  • the method provided by the embodiment of the present invention divides one input photon into two photons of the same energy, and converts the two photons into TE-mode polarized photon pairs having the same polarization state, thereby polarizing one of the TE modes.
  • the photon pair is converted into a TM mode polarized photon pair, and the polarization entangled photon pair is further obtained by superimposing the TE mode polarized photon pair and the TM mode polarized photon pair.
  • the invention breaks through the deficiency of the polarization entangled photon pair in the prior art only in the overlapping region of the conical beam, and the generated TE mode and the TM mode polarized photon pair are all used to generate the polarization entangled photon pair, and the polarization entangled photon pair is improved.
  • the efficiency of the generation, and the energy of the TE mode and the TM mode polarized photon pair are the same, and thus the brightness of the entangled light source is high.
  • the device has a simple structure and can be cured in a silicon-based optical waveguide chip, and the phase is relatively stable.
  • the device for generating a polarization entangled photon pair provided by the above embodiment is only exemplified by the division of the above functional modules when generating a polarization entangled photon pair. In practical applications, the function may be allocated according to needs.
  • the different functional modules are completed, that is, the internal structure of the polarization entangled photon pair generating device is divided into different functional modules to complete all or part of the functions described above.
  • the apparatus for generating a polarization entangled photon pair provided by the above embodiment is the same as the embodiment of the method for generating a polarization entangled photon pair. The specific implementation process is described in detail in the method embodiment, and details are not described herein again.
  • a person skilled in the art may understand that all or part of the steps of implementing the above embodiments may be completed by hardware, or may be instructed by a program to execute related hardware, and the program may be stored in a computer readable storage medium.
  • the storage medium mentioned may be a read only memory, a magnetic disk or an optical disk or the like.

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Abstract

A polarization entangled photon pair generation method and apparatus, falling within the technical field of optical communications. The method comprises: dividing a beam of input photons into two beams of photons with the same energy, converting the two beams of photons into TE mode polarization photon pairs with the same polarization state, then converting one of the TE mode polarization photon pairs into a TM mode polarization photon pair, and further obtaining a polarization entangled photon pair by superposing the TE mode polarization photon pair and the TM mode polarization photon pair. The present invention breaks through the shortcoming in the prior art that a polarization entangled photon pair is only generated in a conical beam overlapping area, and the generated TE mode and TM mode polarization photon pairs are fully used to generate the polarization entangled photon pair, thereby improving the generation efficiency of the polarization entangled photon pair; moreover, the energies of the TE mode and TM mode polarization photon pairs are the same, and thus the brightness of an entangled light source is relatively high. In addition, the apparatus is simple in structure and can be solidified in a silicon-based optical waveguide chip, and the phase is relatively stable.

Description

偏振纠缠光子对的产生方法及装置Method and device for generating polarization entangled photon pair 技术领域Technical field
本发明涉及光通信技术领域,特别涉及一种偏振纠缠光子对的产生方法及装置。The present invention relates to the field of optical communication technologies, and in particular, to a method and an apparatus for generating a polarization entangled photon pair.
背景技术Background technique
量子纠缠是量子信息处理中最为重要的资源,它是多粒子构成的复合系统中的一类特殊量子态。量子纠缠中的纠缠源包括光子、电子、离子等。由于光子的相干性比较好,纠缠光子成为常用的量子纠缠源。光子具有不同自由度,例如,偏振自由度、路径自由度、角动量自由度等,每个自由度都可以用来编码信息。由于偏振自由度可以通过波片进行灵活地操控,因而基于偏振自由度的偏振纠缠光子对在量子信息处理中得到了广泛应用。Quantum entanglement is the most important resource in quantum information processing. It is a special quantum state in a composite system composed of multiple particles. Entanglement sources in quantum entanglement include photons, electrons, ions, and the like. Since the coherence of photons is better, entangled photons become a common source of quantum entanglement. Photons have different degrees of freedom, such as polarization degrees of freedom, path degrees of freedom, angular momentum degrees of freedom, etc. Each degree of freedom can be used to encode information. Polarization entangled photons based on polarization degrees of freedom are widely used in quantum information processing because polarization degrees of freedom can be flexibly manipulated by wave plates.
当前主要利用SOI(Silicon On Insulator,绝缘体上的硅)的光波导,基于硅材料的三阶非线性,泵浦光子发生自发四波混频过程,产生关联光子对。然而在硅线波导中,由于TE模(Transsverse Electric mode,横电模)和TM模(Transsverse Magnetic mode,横磁模)存在较大的双折射效应,TE模偏振光子对的产生效率比TM模偏振光子对的产生效率要大,导致硅线波导中产生的偏振光子对几乎全部为TE模偏振光子对。为了获取到偏振纠缠光子对,需要对偏振光子对的产生方法进行改进。At present, the optical waveguide of SOI (Silicon On Insulator) is mainly used. Based on the third-order nonlinearity of silicon material, the pump photon generates a spontaneous four-wave mixing process to generate correlated photon pairs. However, in the silicon wire waveguide, due to the large birefringence effect of the TE mode (Transsverse Electric mode) and the TM mode (Transsverse Magnetic mode), the TE mode polarized photon pair is more efficient than the TM mode. The generation efficiency of polarized photon pairs is large, resulting in almost all of the polarized photon pairs generated in the silicon waveguides being TE mode polarized photon pairs. In order to obtain a polarization entangled photon pair, a method of generating a polarized photon pair needs to be improved.
图1示出了一种基于二阶非线性晶体的自发参量下转换过程产生偏振纠缠光子对的方法。参见图1,当一束波长较短的泵浦光子入射到二阶非线性晶体上,光子发生自发参量下转换过程,劈裂为两个能量较低的光子。这两个光子一个为水平方向的偏振光子,另一个为竖直方向的偏振光子,且两个光子的出射方向为图1中的两个圆锥所指示的方向,两个圆锥交叠的区域的光子对能够 叠加为偏振纠缠光子对。Figure 1 shows a method for generating a polarization entangled photon pair based on a spontaneous parametric down-conversion process of a second-order nonlinear crystal. Referring to Figure 1, when a short beam of pump photons is incident on a second-order nonlinear crystal, the photons undergo a spontaneous parametric down-conversion process, which splits into two lower-energy photons. The two photons are polarized photons in the horizontal direction and the polarized photons in the vertical direction, and the outgoing directions of the two photons are in the direction indicated by the two cones in Fig. 1, and the two conical overlapping regions Photon pair Superimposed as a polarization entangled photon pair.
在实现本发明的过程中,发明人发现现有技术至少存在以下问题:In the process of implementing the present invention, the inventors have found that the prior art has at least the following problems:
仅两个圆锥交叠区域内的光子对才能产生偏振纠缠光子对,其他区域的光子无法被利用,导致偏振纠缠光子对的产生效率较低,纠缠光源的亮度较低。且该装置结构复杂,全部利用体块光学的方法,光路需要精细调节,相位不稳定。A photon pair in only two conical overlapping regions can produce a polarization entangled photon pair, and photons in other regions cannot be utilized, resulting in a lower efficiency of the polarization entangled photon pair and a lower luminance of the entangled source. Moreover, the structure of the device is complicated, and all the methods using the bulk optical method require fine adjustment of the optical path and unstable phase.
发明内容Summary of the invention
为了解决现有技术的问题,本发明实施例提供了一种偏振纠缠光子对的产生方法及装置。所述技术方案如下:In order to solve the problems of the prior art, embodiments of the present invention provide a method and an apparatus for generating a polarization entangled photon pair. The technical solution is as follows:
第一方面,提供了一种偏振纠缠光子对的产生装置,所述装置包括:分束器、光子对产生模块、基模转换模块及偏振转换器;In a first aspect, a device for generating a polarization entangled photon pair is provided, the device comprising: a beam splitter, a photon pair generating module, a fundamental mode conversion module, and a polarization converter;
所述分束器包括输入端、第一输出端及第二输出端,所述分束器将所述输入端输入的光子束分成能量相同的第一光子束和第二光子束,所述第一光子束经所述第一输出端输出,所述第二光子束经所述第二输出端输出;The beam splitter includes an input end, a first output end, and a second output end, the beam splitter splitting the photon beam input by the input end into a first photon beam and a second photon beam having the same energy, a photon beam is output through the first output end, and the second photon beam is output through the second output end;
所述光子对产生模块包括第一光子对产生单元和第二光子对产生单元,所述第一光子对产生单元与所述第一输出端相连,能够触发所述第一光子束生成第一TE模偏振光子对,所述第二光子对产生单元与所述第二输出端相连,能够触发所述第二光子束生成第二TE模偏振光子对;The photon pair generating module includes a first photon pair generating unit and a second photon pair generating unit, the first photon pair generating unit is connected to the first output end, and can trigger the first photon beam to generate a first TE a pair of modulo polarized photons, the second photon pair generating unit being coupled to the second output end, capable of triggering the second photon beam to generate a second TE mode polarized photon pair;
所述基模转换模块包括第一基模转换单元和第二基模转换单元,所述第一基模转换单元与所述第一光子对产生单元相连,能够将所述第一TE模偏振光子对转换为第一TE基模偏振光子对,所述第二基模转换单元与所述第二光子对产生单元相连,能够将所述第二TE模偏振光子对转换为第二TE基模偏振光子对;The basic mode conversion module includes a first fundamental mode conversion unit and a second fundamental mode conversion unit, and the first fundamental mode conversion unit is connected to the first photon pair generating unit, and is capable of polarizing the first TE mode Converting to a first TE fundamental mode polarized photon pair, the second fundamental mode converting unit being coupled to the second photon pair generating unit, capable of converting the second TE mode polarized photon pair into a second TE fundamental mode polarizing Photon pair
所述偏振转换器包括第一偏振转换单元和第二偏振转换单元,所述第一偏振转换单元与所述第一基模转换单元相连,能够将所述第一TE基模偏振光子 对耦合到所述第二偏振转换单元中,所述第二偏振转换单元与所述第二基模转换单元相连,能够将所述第一TE基模偏振光子对转换为第一TM基模偏振光子对,并将所述第一TM基模偏振光子对和所述第二TE基模偏振光子对叠加为偏振纠缠光子对,输出所述偏振纠缠光子对。The polarization converter includes a first polarization conversion unit and a second polarization conversion unit, the first polarization conversion unit being coupled to the first fundamental mode conversion unit, capable of polarizing photons of the first TE fundamental mode Coupled to the second polarization conversion unit, the second polarization conversion unit is coupled to the second fundamental mode conversion unit, capable of converting the first TE fundamental mode polarization photon pair into a first TM fundamental mode polarization a photon pair, and superimposing the first TM fundamental mode polarized photon pair and the second TE fundamental mode polarized photon pair as a polarization entangled photon pair, and outputting the polarization entangled photon pair.
本发明中所产生的TE模偏振光子对和TM模偏振光子对全部用于生成偏振纠缠光子对,偏振纠缠光子对的产生效率较高,且TE模偏振光子对和TM模偏振光子对的能量相同,以二者所得到的偏振纠缠光子对作为纠缠光源时亮度较高。进一步地,本发明中的装置结构简单,可固化在硅基光波导芯片中,使得所生成的偏振纠缠光子对的相位稳定。The TE mode polarized photon pair and the TM mode polarized photon pair generated in the present invention are all used to generate polarization entangled photon pairs, and the polarization entangled photon pair has high efficiency, and the energy of the TE mode polarized photon pair and the TM mode polarized photon pair. Similarly, the polarization entangled photon pair obtained by the two has higher luminance when used as an entangled light source. Further, the device of the present invention has a simple structure and can be cured in a silicon-based optical waveguide chip such that the phase of the generated polarization entangled photon pair is stabilized.
结合第一方面,在第一方面的第一种可能的实现方式中,所述分束器为Y型分束器。不仅丰富了分束器的形式,而且使得处理后的一束光子能够精确地分为能量相同的两束光子。In conjunction with the first aspect, in a first possible implementation of the first aspect, the beam splitter is a Y-beam splitter. It not only enriches the form of the beam splitter, but also enables a processed photon to be accurately divided into two photons of the same energy.
结合第一方面,在第一方面的第二种可能的实现方式中,所述分束器为多模干涉器,所述多模干涉器还包括多模波导区域,所述多模波导区域连接所述输入端、所述第一输出端及所述第二输出端。不仅丰富了分束器的形式,而且使得处理后的一束光子能够精确地分为能量相同的两束光子。In conjunction with the first aspect, in a second possible implementation of the first aspect, the beam splitter is a multimode interferometer, the multimode interferometer further comprising a multimode waveguide region, the multimode waveguide region connection The input end, the first output end, and the second output end. It not only enriches the form of the beam splitter, but also enables a processed photon to be accurately divided into two photons of the same energy.
结合第一方面至第一方面的第二种可能的实现方式中,在第一方面的第三种可能的实现方式中,所述分束器、所述光子对产生模块、所述基模转换模块及所述偏振转换器均由二氧化硅包层和硅纳米线构成。In a second possible implementation manner of the first aspect, in the third possible implementation manner of the first aspect, the beam splitter, the photon pair generating module, and the fundamental mode conversion Both the module and the polarization converter are comprised of a silicon dioxide cladding and silicon nanowires.
结合第一方面的第三种可能的实现方式,在第一方面的第四种可能的实现方式,所述光子对产生模块中的硅纳米线弯曲环绕在二氧化硅包层内,且所述第一光子对产生单元和所述第二光子对产生单元中的硅纳米线的结构相同,从而经过第一光子对产生单元和第二光子对产生单元可产生具有相同偏振态的光子对。In conjunction with the third possible implementation of the first aspect, in a fourth possible implementation manner of the first aspect, the silicon nanowires in the photon pair generating module are curved and surrounded by a silicon dioxide cladding layer, and The first photon pair generating unit and the second photon pair generating unit have the same structure of the silicon nanowires, so that photon pairs having the same polarization state can be generated through the first photon pair generating unit and the second photon pair generating unit.
结合第一方面的第四种可能的实现方式,在第一方面的第五种可能的实现方式中,所述第一光子对产生单元和所述第二光子对产生单元的硅纳米线均呈 螺旋分布。In conjunction with the fourth possible implementation of the first aspect, in a fifth possible implementation manner of the first aspect, the silicon nanowires of the first photon pair generating unit and the second photon pair generating unit are both Spiral distribution.
结合第一方面的第三种可能的实现方式,在第一方面的第六种可能的实现方式中,所述基模转换模块中的硅纳米线呈锥形分布,从而能够将上下两路光波导中的TE模转换为不同的基模。In conjunction with the third possible implementation of the first aspect, in a sixth possible implementation manner of the first aspect, the silicon nanowires in the basic mode conversion module are tapered, so that the upper and lower light can be The TE modes in the waveguide are converted to different fundamental modes.
结合第一方面的第六种可能的实现方式,在第一方面的第七种可能的实现方式,所述第一基模转换单元中的硅纳米线的宽度小于所述第二基模转换单元中的硅纳米线的宽度。In conjunction with the sixth possible implementation of the first aspect, in a seventh possible implementation manner of the first aspect, the width of the silicon nanowires in the first fundamental mode conversion unit is smaller than the second fundamental mode conversion unit The width of the silicon nanowires.
结合第一方面,在第一方面的第八种可能的实现方式,所述偏振转换器为基于不对称定向耦合器的偏振转换器。In conjunction with the first aspect, in an eighth possible implementation of the first aspect, the polarization converter is an asymmetric directional coupler based polarization converter.
第二方面,提供了一种偏振纠缠光子对的产生方法,所述方法应用上述第一方面所述的偏振纠缠光子对的产生装置,所述方法包括:In a second aspect, a method for generating a polarization entangled photon pair is provided, the method applying the polarization entangled photon pair generating device of the first aspect, the method comprising:
所述分束器将所述输入端输入的光子束分为能量相同的第一光子束和第二光子束,所述第一输出端将所述第一光子束传输至所述第一光子对产生单元,所述第一光子对产生单元触发所述第一光子束生成第一TE模偏振光子对,并将所述第一TE模偏振光子对传输至所述第一基模转换单元,所述第二输出端将所述第二光子束传输至所述第二光子对产生单元,所述第二光子对产生单元触发所述第二光子束生成第二TE模偏振光子对,并将所述第二TE模偏振光子对传输至所述第二基模转换单元;The beam splitter splits the photon beam input by the input end into a first photon beam and a second photon beam of the same energy, and the first output end transmits the first photon beam to the first photon pair a generating unit, the first photon pair generating unit triggering the first photon beam to generate a first TE mode polarized photon pair, and transmitting the first TE mode polarized photon pair to the first fundamental mode converting unit The second output transmits the second photon beam to the second photon pair generating unit, and the second photon pair generating unit triggers the second photon beam to generate a second TE mode polarized photon pair, and Transmitting a second TE mode polarized photon pair to the second fundamental mode conversion unit;
所述第一基模转换单元将所述第一TE模偏振光子对转换为第一TE基模偏振光子对,并将所述第一TE基模偏振光子对传输至所述第一偏振转换单元,所述第二基模转换单元将所述第二TE模偏振光子对转换为第二TE基模偏振光子对,并将所述第二TE基模偏振光子对传输至所述第二偏振转换单元;The first fundamental mode conversion unit converts the first TE mode polarized photon pair into a first TE fundamental mode polarized photon pair, and transmits the first TE fundamental mode polarized photon pair to the first polarization conversion unit The second fundamental mode conversion unit converts the second TE mode polarized photon pair into a second TE fundamental mode polarized photon pair, and transmits the second TE fundamental mode polarized photon pair to the second polarization conversion unit;
所述第一偏振转换单元将所述第一TE基模偏振光子对耦合到所述第二偏振转换单元中,所述第二偏振转换单元将所述第一TE基模偏振光子对转换为第一TM基模偏振光子对,并将所述第一TM基模偏振光子对和所述第二TE 基模偏振光子对叠加为偏振纠缠光子对,输出所述偏振纠缠光子对。The first polarization conversion unit couples the first TE fundamental mode polarized photon pair to the second polarization conversion unit, and the second polarization conversion unit converts the first TE fundamental mode polarization photon pair to a TM fundamental mode polarized photon pair and the first TM fundamental mode polarized photon pair and the second TE The fundamental mode polarized photon pairs are superimposed as polarization entangled photon pairs, and the polarization entangled photon pairs are output.
本发明实施例提供的技术方案带来的有益效果是:The beneficial effects brought by the technical solutions provided by the embodiments of the present invention are:
通过将输入的一束光子分为相同能量的两束光子,并将两束光子转换成具有相同偏振态的TE模偏振光子对,进而将其中一束TE模偏振光子对转换为TM模偏振光子对,进一步通过将TE模偏振光子对和TM模偏振光子对叠加得到偏振纠缠光子对。本发明突破了现有技术中偏振纠缠光子对仅产生于圆锥形光束交叠区域的不足,所产生的TE模和TM模偏振光子对全部用于生成偏振纠缠光子对,提高了偏振纠缠光子对的产生效率,且TE模和TM模偏振光子对的能量相同,因而纠缠光源的亮度较高。另外,该装置结构简单且可固化在硅基光波导芯片中,相位相对稳定。By dividing one input photon into two photons of the same energy and converting the two photons into TE mode polarized photon pairs having the same polarization state, one of the TE mode polarized photon pairs is converted into a TM mode polarized photon. Yes, the polarization entangled photon pair is further obtained by superimposing the TE mode polarized photon pair and the TM mode polarized photon pair. The invention breaks through the deficiency of the polarization entangled photon pair in the prior art only in the overlapping region of the conical beam, and the generated TE mode and the TM mode polarized photon pair are all used to generate the polarization entangled photon pair, and the polarization entangled photon pair is improved. The efficiency of the generation, and the energy of the TE mode and the TM mode polarized photon pair are the same, and thus the brightness of the entangled light source is high. In addition, the device has a simple structure and can be cured in a silicon-based optical waveguide chip, and the phase is relatively stable.
附图说明DRAWINGS
为了更清楚地说明本发明实施例中的技术方案,下面将对实施例描述中所需要使用的附图作简单地介绍,显而易见地,下面描述中的附图仅仅是本发明的一些实施例,对于本领域普通技术人员来讲,在不付出创造性劳动的前提下,还可以根据这些附图获得其他的附图。In order to more clearly illustrate the technical solutions in the embodiments of the present invention, the drawings used in the description of the embodiments will be briefly described below. It is obvious that the drawings in the following description are only some embodiments of the present invention. Other drawings may also be obtained from those of ordinary skill in the art in light of the inventive work.
图1是本发明提供的一种现有的偏振纠缠光子对的产生方法;1 is a method of generating a prior art polarization entangled photon pair provided by the present invention;
图2是本发明一个实施例示出的一种偏振纠缠光子对的产生装置结构示意图;2 is a schematic structural diagram of a device for generating a polarization entangled photon pair according to an embodiment of the present invention;
图3是本发明另一个实施例示出的一种Y型分束器的结构示意图;3 is a schematic structural view of a Y-type beam splitter according to another embodiment of the present invention;
图4是本发明另一个实施例示出的一种多模干涉器的结构示意图;4 is a schematic structural view of a multimode interferometer according to another embodiment of the present invention;
图5是本发明另一个实施例示出的光波导的结构示意图;FIG. 5 is a schematic structural view of an optical waveguide according to another embodiment of the present invention; FIG.
图6是本发明另一个实施例提供的一种偏振转换器的结构示意图;6 is a schematic structural diagram of a polarization converter according to another embodiment of the present invention;
图7本发明另一个施例提供的一种偏振纠缠光子对的产生方法的流程图。FIG. 7 is a flow chart of a method for generating a polarization entangled photon pair according to another embodiment of the present invention.
其中,附图标记为:1、分束器;11、输入端;12、第一输出端;13、第二输出端;14、多模波导区域;2、光子对产生模块;21、第一光子对产生单 元;22、第二光子对产生单元;3、基模转换模块;31、第一基模转换单元;32、第二基模转换单元;4、偏振转换器;41、第一偏振转换单元;42、第二偏振转换单元。Wherein, the reference numerals are: 1, a beam splitter; 11, an input terminal; 12, a first output terminal; 13, a second output terminal; 14, a multimode waveguide region; 2. a photon pair generating module; Photon pair generation a second photon pair generating unit; 3. a fundamental mode conversion module; 31, a first fundamental mode conversion unit; 32, a second fundamental mode conversion unit; 4. a polarization converter; 41, a first polarization conversion unit; 42. A second polarization conversion unit.
具体实施方式detailed description
为使本发明的目的、技术方案和优点更加清楚,下面将结合附图对本发明实施方式作进一步地详细描述。The embodiments of the present invention will be further described in detail below with reference to the accompanying drawings.
参见图2,本发明实施例提供了一种偏振纠缠光子对的产生装置,该装置包括:分束器1、光子对产生模块2、基模转换模块3及偏振转换器4。Referring to FIG. 2, an embodiment of the present invention provides a device for generating a polarization entangled photon pair, the device comprising: a beam splitter 1, a photon pair generating module 2, a fundamental mode conversion module 3, and a polarization converter 4.
其中,分束器1包括输入端11、第一输出端12及第二输出端13,该分束器1将输入端11输入的光子束分成能量相同的第一光子束和第二光子束,该第一光子束经第一输出端12输出,第二光子束经第二输出端13输出;The beam splitter 1 includes an input end 11, a first output end 12 and a second output end 13, and the beam splitter 1 splits the photon beam input from the input end 11 into a first photon beam and a second photon beam of the same energy. The first photon beam is output through the first output terminal 12, and the second photon beam is output through the second output terminal 13;
光子对产生模块2包括第一光子对产生单元21和第二光子对产生单元22,该第一光子对产生单元21与第一输出端12相连,该第一光子对产生单元21能够触发第一光子束生成第一TE模偏振光子对,并传输所生成的第一TE模偏振光子对;该第二光子对产生单元22与第二输出端13相连,该第二光子对产生单元22能够触发第二光子束生成第二TE模偏振光子对,并传输所生成的第二TE模偏振光子对,在本实施例中,第一TE模偏振光子对和第二TE模偏振光子对为具有相同偏振态的关联光子对,二者完全相同,仅传输路径不同;The photon pair generating module 2 includes a first photon pair generating unit 21 and a second photon pair generating unit 22, the first photon pair generating unit 21 being connected to the first output terminal 12, the first photon pair generating unit 21 being capable of triggering the first The photon beam generates a first TE mode polarized photon pair and transmits the generated first TE mode polarized photon pair; the second photon pair generating unit 22 is coupled to the second output 13 and the second photon pair generating unit 22 is capable of triggering The second photon beam generates a second TE mode polarized photon pair and transmits the generated second TE mode polarized photon pair. In this embodiment, the first TE mode polarized photon pair and the second TE mode polarized photon pair have the same Correlated photon pairs of polarization states, the two are identical, only the transmission paths are different;
基模转换模块3包括第一基模转换单元31和第二基模转换单元32,该第一基模转换单元31与第一光子对产生单元21相连,用于接收第一光子对产生单元21所产生的第一TE模偏振光子对,并将该第一TE模偏振光子对转换为为第一TE基模偏振光子对,进而传输第一TE基模偏振光子对;第二基模转换单元32与第二光子对产生单元22相连,用于接收第二光子对产生单元22所产生的第二TE模偏振光子对,并将该第二TE模偏振光子对转换为第二TE模偏振光子对,进而传输第二TE基模偏振光子对; The fundamental mode conversion module 3 includes a first fundamental mode conversion unit 31 and a second fundamental mode conversion unit 32, and the first fundamental mode conversion unit 31 is connected to the first photon pair generation unit 21 for receiving the first photon pair generation unit 21 Generating a first TE mode polarized photon pair and converting the first TE mode polarized photon pair into a first TE fundamental mode polarized photon pair, thereby transmitting a first TE fundamental mode polarized photon pair; and a second fundamental mode conversion unit 32 is connected to the second photon pair generating unit 22 for receiving the second TE mode polarized photon pair generated by the second photon pair generating unit 22, and converting the second TE mode polarized photon pair into the second TE mode polarized photon And, in turn, transmitting a second TE fundamental mode polarized photon pair;
偏振转换器4包括第一偏振转换单元41和第二偏振转换单元42,该第一偏振转换单元41与第一基模转换单元31相连,用于接收第一基模转换单元31传输的第一TE基模偏振光子对,并将该第一TE基模偏振光子对耦合到第二偏振单元中;第二偏振转换单元42与第二TE基模偏振光子对相连,用于接收第二基模偏振转换单元32传输的第二TE基模偏振光子对,在第一偏振转换单元41中的第一TE基模偏振光子对与第二偏转转换单元42中的TM基模偏振光子对的有效折射率相等的情况下,将第一TE基模偏振光子对转换为第一TM基模偏振光子对,并将第一TM基模偏振光子对和第二TE基模偏振光子对叠加为偏振纠缠光子对,进而将偏振纠缠光子对输出。The polarization converter 4 includes a first polarization conversion unit 41 and a second polarization conversion unit 42, which is connected to the first fundamental mode conversion unit 31 for receiving the first transmission of the first fundamental mode conversion unit 31. The TE fundamental mode polarizes the photon pair and couples the first TE fundamental mode polarized photon pair to the second polarization unit; the second polarization conversion unit 42 is coupled to the second TE fundamental mode polarized photon pair for receiving the second fundamental mode The second TE fundamental mode polarized photon pair transmitted by the polarization conversion unit 32, the effective polarization of the first TE fundamental mode polarized photon pair in the first polarization conversion unit 41 and the TM fundamental mode polarized photon pair in the second deflection conversion unit 42 When the rates are equal, the first TE fundamental mode polarized photon pair is converted into a first TM fundamental mode polarized photon pair, and the first TM fundamental mode polarized photon pair and the second TE fundamental mode polarized photon pair are superimposed into polarization entangled photons. Then, the polarization entangled photon pair is output.
在本发明的一个实施例中,参见图3,分束器1可以为Y型分束器。当分束器1为Y型分束器时,输入端11、第一输出端12及第二输出端13在Y型分束器中的位置关系如图3所示。In one embodiment of the invention, referring to Figure 3, the beam splitter 1 can be a Y-beam splitter. When the beam splitter 1 is a Y-type beam splitter, the positional relationship of the input terminal 11, the first output terminal 12 and the second output terminal 13 in the Y-type beam splitter is as shown in FIG.
在发明的另一个实施例中,参见图4,分束器1还可以为多模干涉器。当分束器1为多模干涉器时,该多模干涉器包括输入端11、第一输出端12、第二输出端13及多模波导区域14,该多模波导区域14连接输入端11、第一输出端12及第二输出端13。多模波导区域14的宽度和长度根据需要设置,以保证光场达到50/50分束效果,也即是可将输入的光子束分为能量相同的第一光子束和第二光子束。In another embodiment of the invention, referring to Figure 4, the beam splitter 1 can also be a multimode interferometer. When the beam splitter 1 is a multimode interferometer, the multimode interferometer includes an input terminal 11, a first output terminal 12, a second output terminal 13 and a multimode waveguide region 14, the multimode waveguide region 14 being connected to the input terminal 11, The first output terminal 12 and the second output terminal 13 are provided. The width and length of the multimode waveguide region 14 are set as desired to ensure that the light field achieves a 50/50 splitting effect, i.e., the input photon beam can be split into first and second photon beams of the same energy.
在本实施例中,上述图2所示的偏振纠缠光子对的产生装置可以为光波导,通常光波导主要由二氧化硅包层和硅纳米线构成,因此,图2中所示的分束器1、光子对产生模块2、基模转换模块3及偏振转换器4均由二氧化硅包层和硅纳米线构成。相应地,分束器1所包括的输入端11、第一输出端12及第二输出端13也由二氧化硅包层和硅纳米线构成;光子对产生模块2所包括的第一光子对产生单元21和第二光子对产生单元22也由二氧化硅包层和硅纳米线构成;基模转换模块3所包括的第一基模转换单元31和第二基模转换单元32也由二氧化硅包层和硅纳米线构成;偏振转换器4所包括的第一偏振转换单元41 和第二偏振转换单元42也由二氧化硅包层和硅纳米线构成。通常光波导中光束主要沿着硅纳米线进行传输的,为了直观地展示光束在光波导中的传输路径,如图5示出了构成装置内各个功能模块的硅纳米线在光波导芯片中的分布情况。In this embodiment, the generating device for the polarization entangled photon pair shown in FIG. 2 may be an optical waveguide. Generally, the optical waveguide is mainly composed of a silicon dioxide cladding layer and silicon nanowires. Therefore, the beam splitting shown in FIG. The photon pair generation module 2, the fundamental mode conversion module 3, and the polarization converter 4 are each composed of a silicon dioxide cladding layer and silicon nanowires. Correspondingly, the input end 11, the first output end 12 and the second output end 13 of the beam splitter 1 are also composed of a silicon dioxide cladding and silicon nanowires; the first photon pair included in the photon pair generating module 2 The generating unit 21 and the second photon pair generating unit 22 are also composed of a silicon dioxide cladding layer and silicon nanowires; the first fundamental mode converting unit 31 and the second fundamental mode converting unit 32 included in the fundamental mode converting module 3 are also composed of two The silicon oxide cladding layer and the silicon nanowires are formed; the first polarization conversion unit 41 included in the polarization converter 4 The second polarization conversion unit 42 is also composed of a silicon dioxide cladding layer and silicon nanowires. Generally, the light beam in the optical waveguide is mainly transmitted along the silicon nanowire. In order to visually display the transmission path of the light beam in the optical waveguide, as shown in FIG. 5, the silicon nanowires constituting the functional modules in the device are shown in the optical waveguide chip. Distribution.
当图2所示的偏振纠缠光子对的产生装置为光波导时,光子对产生模块2中的硅纳米线弯曲环绕在二氧化硅包层内,结构紧凑且长度满足设计需求,使得光束在光子对产生模块2传输时,能够利用硅纳米线波导的三阶非线性发生自发四波混频过程,产生TE模偏振光子对。为了确保第一光子对产生单元21和第二光子对产生单元22所产生的偏振光子对具有相同偏振态,第一光子对产生单元21和第二光子对产生单元22中的硅纳米线尺寸相同,且对称分布。如图5所示,第一光子对产生单元21和第二光子对产生单元22中的硅纳米线对称分布且呈螺旋形,当然,第一光子对产生单元21和第二光子对产生单元22中的硅纳米线的形状还可以为其他形状,本实施例对此不作具体的限定。When the generating device of the polarization entangled photon pair shown in FIG. 2 is an optical waveguide, the silicon nanowires in the photon pair generating module 2 are curved and surrounded in the silicon dioxide cladding layer, and the structure is compact and the length meets the design requirement, so that the light beam is in the photon. When the generating module 2 is transmitted, the spontaneous four-wave mixing process of the silicon nanowire waveguide can be used to generate a TE mode polarized photon pair. In order to ensure that the polarized photon pairs generated by the first photon pair generating unit 21 and the second photon pair generating unit 22 have the same polarization state, the silicon nanowires in the first photon pair generating unit 21 and the second photon pair generating unit 22 have the same size. And symmetrically distributed. As shown in FIG. 5, the silicon photon in the first photon pair generating unit 21 and the second photon pair generating unit 22 are symmetrically distributed and spiral, of course, the first photon pair generating unit 21 and the second photon pair generating unit 22 The shape of the silicon nanowires may also be other shapes, which is not specifically limited in this embodiment.
在本实施例中,基模转换模块3中的硅纳米线呈锥形分布,第一基模转换单元31中的硅纳米线的宽度逐渐变细,第二基模转换单元32中的硅纳米线的宽度逐渐变粗,使得第一基模转换单元31变为细光波导,第二基模转换单元32变为粗波导,当然,第一基模转换单元31中的硅纳米线的宽度可以逐渐变粗,第二基模转换单元32中的硅纳米线的宽度可以逐渐变细,使得第一基模转换单元31变为粗光波导,第二基模转换单元32变为细光波导。总之,只要保证基模转换模块3中的两路光波导的粗细不同即可。在本实施例中,基模转换模块3中的硅纳米线的宽度由偏振转换器4中的硅纳米线的宽度决定,具体来说,第一偏振转换单元41中的硅纳米线的宽度决定第一基模转换单元31中的硅纳米线的宽度,第二偏振转换单元42中的硅纳米线的宽度决定第二基模转换单元32中硅纳米线的宽度,当偏振转换器4中的硅纳米线的宽度改变,则基模转换模块3中硅纳米线的宽度需要根据需求重新设计。In this embodiment, the silicon nanowires in the fundamental mode conversion module 3 are tapered, the width of the silicon nanowires in the first fundamental mode conversion unit 31 is gradually tapered, and the silicon nanometers in the second fundamental mode conversion unit 32 are tapered. The width of the line is gradually thickened, so that the first fundamental mode conversion unit 31 becomes a fine optical waveguide, and the second fundamental mode conversion unit 32 becomes a thick waveguide. Of course, the width of the silicon nanowires in the first fundamental mode conversion unit 31 can be Gradually thickening, the width of the silicon nanowires in the second fundamental mode conversion unit 32 may be tapered such that the first fundamental mode conversion unit 31 becomes a coarse optical waveguide and the second fundamental mode conversion unit 32 becomes a fine optical waveguide. In short, it is only necessary to ensure that the thicknesses of the two optical waveguides in the fundamental mode conversion module 3 are different. In the present embodiment, the width of the silicon nanowires in the fundamental mode conversion module 3 is determined by the width of the silicon nanowires in the polarization converter 4, specifically, the width of the silicon nanowires in the first polarization conversion unit 41 is determined. The width of the silicon nanowires in the first fundamental mode conversion unit 31, and the width of the silicon nanowires in the second polarization conversion unit 42 determine the width of the silicon nanowires in the second fundamental mode conversion unit 32, when in the polarization converter 4 As the width of the silicon nanowires changes, the width of the silicon nanowires in the fundamental mode conversion module 3 needs to be redesigned as needed.
当第一光子对生成单元21将所生成的第一TE模偏振光子对传输至第一基 模转换单元31时,第一基模转换单元31根据自身硅纳米线的宽度,将第一TE模偏转光子对的模式转换为相应基模,得到第一TE基模偏振光子对。当第二光子对生成单元22将所生成的第二TE模偏振光子对传输至第二基模转换单元32时,第二基模转换单元32根据自身硅纳米线的宽度,将第二TE模偏振光子对的模式转换为相应基模,得到第二TE基模偏振光子对。由于第一基模转换单元31和第二基模转换单元32对应的光波导不同,因而转换后得到的第一TE基模偏振光子对和第二TE基模偏振光子对也不相同。When the first photon pair generating unit 21 transmits the generated first TE mode polarized photon pair to the first base In the mode conversion unit 31, the first fundamental mode conversion unit 31 converts the mode of the first TE mode deflection photon pair into a corresponding fundamental mode according to the width of the self silicon nanowire, and obtains the first TE fundamental mode polarized photon pair. When the second photon pair generating unit 22 transmits the generated second TE mode polarized photon pair to the second fundamental mode converting unit 32, the second fundamental mode converting unit 32 sets the second TE mode according to the width of the self silicon nanowire. The mode of the polarized photon pair is converted to the corresponding fundamental mode, resulting in a second TE fundamental mode polarized photon pair. Since the optical waveguides corresponding to the first fundamental mode conversion unit 31 and the second fundamental mode conversion unit 32 are different, the first TE fundamental mode polarized photon pair and the second TE fundamental mode polarized photon pair obtained after the conversion are also different.
在本实施例中,偏振转换器4为不对称定向耦合器的偏振转换器,第一偏振转换单元41和第二偏振转换单元42中的硅纳米线的长度和宽度也是不同的。在本发明的一个实施例中,第一偏振转换单元41中的硅纳米线的长度可以小于第二偏振转换单元42中的硅纳米线的长度,且第一偏振转换单元41中的硅纳米线的宽度小于第二偏振转换单元42中的硅纳米线的宽度,此时第一偏振转换单元41不会输出偏振纠缠光子对,可作为测试端口,第二偏振转换单元42作为输出端输出偏振纠缠光子对。在本发明的另一个实施例中,第一偏振转换单元41中的硅纳米线的长度可以大于第二偏振转换单元42中的硅纳米线的长度,且第一偏振转换单元41中的硅纳米线的宽度大于第二偏振转换单元42中的硅纳米线的宽度,此时第一偏振转换单元41作为输出端输出偏振纠缠光子对,第二偏振转换单元42不会输出偏振纠缠光子对,可作为测试端口。In the present embodiment, the polarization converter 4 is a polarization converter of an asymmetric directional coupler, and the length and width of the silicon nanowires in the first polarization conversion unit 41 and the second polarization conversion unit 42 are also different. In one embodiment of the present invention, the length of the silicon nanowires in the first polarization conversion unit 41 may be smaller than the length of the silicon nanowires in the second polarization conversion unit 42, and the silicon nanowires in the first polarization conversion unit 41 The width is smaller than the width of the silicon nanowires in the second polarization conversion unit 42, at which time the first polarization conversion unit 41 does not output a polarization entangled photon pair, which can serve as a test port, and the second polarization conversion unit 42 serves as an output terminal to output polarization entanglement. Photon pair. In another embodiment of the present invention, the length of the silicon nanowires in the first polarization conversion unit 41 may be greater than the length of the silicon nanowires in the second polarization conversion unit 42, and the silicon nanometers in the first polarization conversion unit 41 The width of the line is greater than the width of the silicon nanowires in the second polarization conversion unit 42. At this time, the first polarization conversion unit 41 outputs a polarization entangled photon pair as an output terminal, and the second polarization conversion unit 42 does not output a polarization entangled photon pair. As a test port.
在本实施例中,基于不对称定向耦合器的偏振转换器,当第一偏振转换单元41和第二偏振转换单元42中硅纳米线的宽度满足一定条件时,可使第一偏振转换单元41对应光波导中第一TE基模偏振光子对和第二偏振转换单元42对应光波导中的第二TM基模偏振光子对的有效折射率相等,此时根据耦合模理论,可将较细光波导中的TE基模偏振光子对耦合到较粗的光波导中,转换为较粗光波导中的TM基模偏振光子对,而较粗光波导中的TE基模偏振光子对依然在其中传播。TE基模可以表示为TE0模,TM基模可以表示为TM0模。 例如,图6中(a)图所示,耦合区域的长度为36.8um,当细光波导中的TE0模与粗光波导中TM0模的有效折射率相等时,可将细光波导中TE0模光子对耦合到粗光波导中,粗光波导中的TE0模光子对依然在粗光波导中传播。图6中的(b)图为偏振转换器的横截面图,其中,w1为细光波导的宽度,w2为粗光波导中的宽度,g为细波导和粗波导之间的距离,h为粗细光波导的高度。w1可以为330nm,w2可以为600nm,g可以为100nm,h可以为250nm,当然,在实际应用中,上述结构参数可根据需求具体设计,并不限于上述所列的数据,只要满足细光波导中的TE0模与粗光波导中TM0模的有效折射率相等,耦合区域的长度需要保证细光波导中的TE0模大部分转换为粗波导中的TM0模即可。In the present embodiment, based on the polarization converter of the asymmetric directional coupler, when the width of the silicon nanowires in the first polarization conversion unit 41 and the second polarization conversion unit 42 satisfies certain conditions, the first polarization conversion unit 41 can be made Corresponding to the first TE fundamental mode polarized photon pair in the optical waveguide and the second TM polarization converting unit 42 corresponding to the second TM fundamental mode polarized photon pair in the optical waveguide, the effective refractive index is equal, and according to the coupled mode theory, the finer light can be The TE fundamental mode polarized photon pair in the waveguide is coupled into the coarser optical waveguide and converted into a TM fundamental mode polarized photon pair in the coarser optical waveguide, while the TE fundamental mode polarized photon pair in the coarser optical waveguide still propagates therein. . The TE fundamental mode can be expressed as a TE 0 mode, and the TM fundamental mode can be expressed as a TM 0 mode. For example, as shown in (a) of FIG. 6, the length of the coupling region is 36.8 um, and when the TE 0 mode in the thin optical waveguide is equal to the effective refractive index of the TM 0 mode in the coarse optical waveguide, the fine optical waveguide can be The TE 0 mode photon pair is coupled into the coarse optical waveguide, and the TE 0 mode photon pair in the coarse optical waveguide still propagates in the coarse optical waveguide. Figure 6 (b) is a cross-sectional view of the polarization converter, where w1 is the width of the thin optical waveguide, w2 is the width in the coarse optical waveguide, and g is the distance between the thin waveguide and the thick waveguide, h is The height of the thick and thin optical waveguide. W1 may be 330 nm, w2 may be 600 nm, g may be 100 nm, and h may be 250 nm. Of course, in practical applications, the above structural parameters may be specifically designed according to requirements, and are not limited to the above listed data, as long as the fine optical waveguide is satisfied. The TE 0 mode in the middle is equal to the effective refractive index of the TM 0 mode in the coarse optical waveguide, and the length of the coupling region needs to ensure that most of the TE 0 mode in the thin optical waveguide is converted into the TM 0 mode in the thick waveguide.
在本实施例中,可将第一光子对产生单元21、第一基模转换单元31及第一偏振转换单元41构成上路光波导,将第二光子对产生单元22、第二基模转换单元32及第二偏振转换单元42构成下路光波导。通过在上路光波导和下路光波导中添加金属电极,施加电压之后,可利用光热效应,调节上下两路波导中光子的相对相位,得到偏振纠缠态为|ψ>=a|TE,TE>+be|TM,TM>的偏振纠缠光子对。其中,ψ为偏振纠缠态,θ为相对相位,a和b为任意参数,且a和b满足归一化条件|a|2+|b|2=1。In this embodiment, the first photon pair generating unit 21, the first fundamental mode converting unit 31, and the first polarizing converting unit 41 may constitute an on-path optical waveguide, and the second photon pair generating unit 22 and the second fundamental mode converting unit may be configured. 32 and the second polarization conversion unit 42 constitute a lower optical waveguide. By adding a metal electrode to the upper optical waveguide and the lower optical waveguide, after applying a voltage, the relative phase of the photons in the upper and lower waveguides can be adjusted by using the photothermal effect, and the polarization entangled state is |ψ>=a|TE, TE> +be |TM, TM> polarization entangled photon pairs. Where ψ is the polarization entangled state, θ is the relative phase, a and b are arbitrary parameters, and a and b satisfy the normalization condition |a| 2 +|b| 2 =1.
本发明实施例提供的装置,通过将输入的一束光子分为相同能量的两束光子,并将两束光子转换成具有相同偏振态的TE模偏振光子对,进而将其中一束TE模偏振光子对转换为TM模偏振光子对,进一步通过将TE模偏振光子对和TM模偏振光子对叠加得到偏振纠缠光子对。本发明突破了现有技术中偏振纠缠光子对仅产生于圆锥形光束交叠区域的不足,所产生的TE模和TM模偏振光子对全部用于生成偏振纠缠光子对,提高了偏振纠缠光子对的产生效率,且TE模和TM模偏振光子对的能量相同,因而纠缠光源的亮度较高。另外,该装置结构简单且可固化在硅基光波导芯片中,相位相对稳定。 The device provided by the embodiment of the present invention divides one input photon into two photons of the same energy, and converts the two photons into TE-mode polarized photon pairs having the same polarization state, thereby polarizing one of the TE modes. The photon pair is converted into a TM mode polarized photon pair, and the polarization entangled photon pair is further obtained by superimposing the TE mode polarized photon pair and the TM mode polarized photon pair. The invention breaks through the deficiency of the polarization entangled photon pair in the prior art only in the overlapping region of the conical beam, and the generated TE mode and the TM mode polarized photon pair are all used to generate the polarization entangled photon pair, and the polarization entangled photon pair is improved. The efficiency of the generation, and the energy of the TE mode and the TM mode polarized photon pair are the same, and thus the brightness of the entangled light source is high. In addition, the device has a simple structure and can be cured in a silicon-based optical waveguide chip, and the phase is relatively stable.
基于上述图2所示的偏振纠缠光子的产生装置,本发明实施例提供了一种偏振纠缠光子的产生方法,参见图7,本实施例提供的方法流程包括:The method for generating a polarization entangled photon according to the above-mentioned FIG. 2, the embodiment of the present invention provides a method for generating a polarization entangled photon. Referring to FIG. 7, the method flow provided by the embodiment includes:
701、分束器将输入端输入的光子束分为能量相同的第一光子束和第二光子束,第一输出端将第一光子束传输至第一光子对产生单元,第一光子对产生单元触发第一光子束生成第一TE模偏振光子对,并将第一TE模偏振光子对传输至第一基模转换单元,第二输出端将第二光子束传输至第二光子对产生单元,第二光子对产生单元触发第二光子束生成第二TE模偏振光子对,并将第二TE模偏振光子对传输至第二基模转换单元。701. The beam splitter divides the photon beam input at the input end into a first photon beam and a second photon beam having the same energy, and the first output end transmits the first photon beam to the first photon pair generating unit, and the first photon pair generates The unit triggers the first photon beam to generate a first TE mode polarized photon pair, and transmits the first TE mode polarized photon pair to the first fundamental mode conversion unit, and the second output transmits the second photon beam to the second photon pair generating unit The second photon pair generating unit triggers the second photon beam to generate a second TE mode polarized photon pair, and transmits the second TE mode polarized photon pair to the second fundamental mode converting unit.
702、第一基模转换单元将第一TE模偏振光子对转换为第一TE基模偏振光子对,并将第一TE基模偏振光子对传输至第一偏振转换单元,第二基模转换单元将第二TE模偏振光子对转换为第二TE基模偏振光子对,并将第二TE基模偏振光子对传输至第二偏振转换单元。702. The first fundamental mode conversion unit converts the first TE mode polarized photon pair into a first TE fundamental mode polarized photon pair, and transmits the first TE fundamental mode polarized photon pair to the first polarization conversion unit, and the second fundamental mode conversion The unit converts the second TE mode polarized photon pair into a second TE fundamental mode polarized photon pair and transmits the second TE fundamental mode polarized photon pair to the second polarization converting unit.
703、第一偏振转换单元将第一TE基模偏振光子对耦合到第二偏振转换单元中,第二偏振转换单元将第一TE基模偏振光子对转换为第一TM基模偏振光子对,并将第一TM基模偏振光子对和第二TE基模偏振光子对叠加为偏振纠缠光子对,输出偏振纠缠光子对。703. The first polarization conversion unit couples the first TE fundamental mode polarization photon pair into the second polarization conversion unit, and the second polarization conversion unit converts the first TE fundamental mode polarization photon pair into the first TM fundamental mode polarization photon pair. And superimposing the first TM fundamental mode polarized photon pair and the second TE fundamental mode polarized photon pair into a polarization entangled photon pair, and outputting a polarization entangled photon pair.
以偏振纠缠光子对的产生装置为光波导为例,上述基于光波导产生偏振纠缠光子对的过程如下:Taking the generating device of the polarization entangled photon pair as an example of the optical waveguide, the above process of generating the polarization entangled photon pair based on the optical waveguide is as follows:
第一步,泵浦光子从片外输入进SOI光学芯片,经过分束器分为两束相同能量的光子束,传输到上下光波导中。In the first step, the pump photons are input from the off-chip into the SOI optical chip, and are split into two photon beams of the same energy through the beam splitter and transmitted to the upper and lower optical waveguides.
第二步,利用硅线波导的三阶非线性发生自发四波混频过程,上下两路光波导分别产生具有相同偏振态的TE模偏振光子对。In the second step, the third-order nonlinearity of the silicon wire waveguide is used to generate a spontaneous four-wave mixing process, and the upper and lower optical waveguides respectively generate TE-mode polarized photon pairs having the same polarization state.
第三步,锥形光波导将TE模偏振光子对的模式转换为粗、细光波导中的基模TE0模。In the third step, the tapered optical waveguide converts the mode of the TE mode polarized photon pair into a fundamental mode TE 0 mode in the coarse and fine optical waveguide.
第四步,利用偏振转换器将细波导中的TE0模光子转换为粗波导中的TM0模光子,将粗波导中的TE0模光子对和转换得到的TM0模光子对叠加,得到偏 振纠缠光子对,进而输出偏振纠缠光子对。In the fourth step, the TE 0 mode photon in the thin waveguide is converted into the TM 0 mode photon in the thick waveguide by using a polarization converter, and the TE 0 mode photon pair in the coarse waveguide and the converted TM 0 mode photon pair are superposed. The polarization entangles the pair of photons, which in turn outputs a pair of polarization entangled photons.
本发明实施例提供的方法,通过将输入的一束光子分为相同能量的两束光子,并将两束光子转换成具有相同偏振态的TE模偏振光子对,进而将其中一束TE模偏振光子对转换为TM模偏振光子对,进一步通过将TE模偏振光子对和TM模偏振光子对叠加得到偏振纠缠光子对。本发明突破了现有技术中偏振纠缠光子对仅产生于圆锥形光束交叠区域的不足,所产生的TE模和TM模偏振光子对全部用于生成偏振纠缠光子对,提高了偏振纠缠光子对的产生效率,且TE模和TM模偏振光子对的能量相同,因而纠缠光源的亮度较高。另外,该装置结构简单且可固化在硅基光波导芯片中,相位相对稳定。The method provided by the embodiment of the present invention divides one input photon into two photons of the same energy, and converts the two photons into TE-mode polarized photon pairs having the same polarization state, thereby polarizing one of the TE modes. The photon pair is converted into a TM mode polarized photon pair, and the polarization entangled photon pair is further obtained by superimposing the TE mode polarized photon pair and the TM mode polarized photon pair. The invention breaks through the deficiency of the polarization entangled photon pair in the prior art only in the overlapping region of the conical beam, and the generated TE mode and the TM mode polarized photon pair are all used to generate the polarization entangled photon pair, and the polarization entangled photon pair is improved. The efficiency of the generation, and the energy of the TE mode and the TM mode polarized photon pair are the same, and thus the brightness of the entangled light source is high. In addition, the device has a simple structure and can be cured in a silicon-based optical waveguide chip, and the phase is relatively stable.
需要说明的是:上述实施例提供的偏振纠缠光子对的产生装置在产生偏振纠缠光子对时,仅以上述各功能模块的划分进行举例说明,实际应用中,可以根据需要而将上述功能分配由不同的功能模块完成,即将偏振纠缠光子对的产生装置的内部结构划分成不同的功能模块,以完成以上描述的全部或者部分功能。另外,上述实施例提供的偏振纠缠光子对的产生装置与偏振纠缠光子对的产生方法实施例属于同一构思,其具体实现过程详见方法实施例,这里不再赘述。It should be noted that the device for generating a polarization entangled photon pair provided by the above embodiment is only exemplified by the division of the above functional modules when generating a polarization entangled photon pair. In practical applications, the function may be allocated according to needs. The different functional modules are completed, that is, the internal structure of the polarization entangled photon pair generating device is divided into different functional modules to complete all or part of the functions described above. In addition, the apparatus for generating a polarization entangled photon pair provided by the above embodiment is the same as the embodiment of the method for generating a polarization entangled photon pair. The specific implementation process is described in detail in the method embodiment, and details are not described herein again.
本领域普通技术人员可以理解实现上述实施例的全部或部分步骤可以通过硬件来完成,也可以通过程序来指令相关的硬件完成,所述的程序可以存储于一种计算机可读存储介质中,上述提到的存储介质可以是只读存储器,磁盘或光盘等。A person skilled in the art may understand that all or part of the steps of implementing the above embodiments may be completed by hardware, or may be instructed by a program to execute related hardware, and the program may be stored in a computer readable storage medium. The storage medium mentioned may be a read only memory, a magnetic disk or an optical disk or the like.
以上所述仅为本发明的较佳实施例,并不用以限制本发明,凡在本发明的精神和原则之内,所作的任何修改、等同替换、改进等,均应包含在本发明的保护范围之内。 The above are only the preferred embodiments of the present invention, and are not intended to limit the present invention. Any modifications, equivalents, improvements, etc., which are within the spirit and scope of the present invention, should be included in the protection of the present invention. Within the scope.

Claims (10)

  1. 一种偏振纠缠光子对的产生装置,其特征在于,所述装置包括:分束器、光子对产生模块、基模转换模块及偏振转换器;A device for generating a polarization entangled photon pair, characterized in that the device comprises: a beam splitter, a photon pair generating module, a fundamental mode conversion module and a polarization converter;
    所述分束器包括输入端、第一输出端及第二输出端,所述分束器将所述输入端输入的光子束分成能量相同的第一光子束和第二光子束,所述第一光子束经所述第一输出端输出,所述第二光子束经所述第二输出端输出;The beam splitter includes an input end, a first output end, and a second output end, the beam splitter splitting the photon beam input by the input end into a first photon beam and a second photon beam having the same energy, a photon beam is output through the first output end, and the second photon beam is output through the second output end;
    所述光子对产生模块包括第一光子对产生单元和第二光子对产生单元,所述第一光子对产生单元与所述第一输出端相连,能够触发所述第一光子束生成第一TE模偏振光子对,所述第二光子对产生单元与所述第二输出端相连,能够触发所述第二光子束生成第二TE模偏振光子对;The photon pair generating module includes a first photon pair generating unit and a second photon pair generating unit, the first photon pair generating unit is connected to the first output end, and can trigger the first photon beam to generate a first TE a pair of modulo polarized photons, the second photon pair generating unit being coupled to the second output end, capable of triggering the second photon beam to generate a second TE mode polarized photon pair;
    所述基模转换模块包括第一基模转换单元和第二基模转换单元,所述第一基模转换单元与所述第一光子对产生单元相连,能够将所述第一TE模偏振光子对转换为第一TE基模偏振光子对,所述第二基模转换单元与所述第二光子对产生单元相连,能够将所述第二TE模偏振光子对转换为第二TE基模偏振光子对;The basic mode conversion module includes a first fundamental mode conversion unit and a second fundamental mode conversion unit, and the first fundamental mode conversion unit is connected to the first photon pair generating unit, and is capable of polarizing the first TE mode Converting to a first TE fundamental mode polarized photon pair, the second fundamental mode converting unit being coupled to the second photon pair generating unit, capable of converting the second TE mode polarized photon pair into a second TE fundamental mode polarizing Photon pair
    所述偏振转换器包括第一偏振转换单元和第二偏振转换单元,所述第一偏振转换单元与所述第一基模转换单元相连,能够将所述第一TE基模偏振光子对耦合到所述第二偏振转换单元中,所述第二偏振转换单元与所述第二基模转换单元相连,能够将所述第一TE基模偏振光子对转换为第一TM基模偏振光子对,并将所述第一TM基模偏振光子对和所述第二TE基模偏振光子对叠加为偏振纠缠光子对,输出所述偏振纠缠光子对。The polarization converter includes a first polarization conversion unit and a second polarization conversion unit, the first polarization conversion unit being coupled to the first fundamental mode conversion unit, capable of coupling the first TE fundamental mode polarization photon pair to In the second polarization conversion unit, the second polarization conversion unit is connected to the second fundamental mode conversion unit, and is capable of converting the first TE fundamental mode polarization photon pair into a first TM fundamental mode polarization photon pair. And superposing the first TM fundamental mode polarized photon pair and the second TE fundamental mode polarized photon pair into a polarization entangled photon pair, and outputting the polarization entangled photon pair.
  2. 根据权利要求1所述的装置,其特征在于,所述分束器为Y型分束器。The device of claim 1 wherein said beam splitter is a Y-beam splitter.
  3. 根据权利要求1所述的装置,其特征在于,所述分束器为多模干涉器,所述多模干涉器还包括多模波导区域,所述多模波导区域连接所述输入端、所 述第一输出端及所述第二输出端。The apparatus according to claim 1, wherein said beam splitter is a multimode interferometer, said multimode interferometer further comprising a multimode waveguide region, said multimode waveguide region connecting said input end, said The first output end and the second output end are described.
  4. 根据权利要求1至3中任一项所述的装置,其特征在于,所述分束器、所述光子对产生模块、所述基模转换模块及所述偏振转换器均由二氧化硅包层和硅纳米线构成。The apparatus according to any one of claims 1 to 3, wherein the beam splitter, the photon pair generating module, the fundamental mode conversion module, and the polarization converter are all packaged by silicon dioxide. The layer is composed of silicon nanowires.
  5. 根据权利要求4所述的装置,其特征在于,所述光子对产生模块中的硅纳米线弯曲环绕在二氧化硅包层内,且所述第一光子对产生单元和所述第二光子对产生单元中的硅纳米线的结构相同。The apparatus according to claim 4, wherein the silicon nanowires in the photon pair generating module are curved to surround the silicon dioxide cladding, and the first photon pair generating unit and the second photon pair The structure of the silicon nanowires in the generating unit is the same.
  6. 根据权利要求5所述的装置,其特征在于,所述第一光子对产生单元和所述第二光子对产生单元的硅纳米线均呈螺旋分布。The apparatus according to claim 5, wherein the silicon photon of the first photon pair generating unit and the second photon pair generating unit are spirally distributed.
  7. 根据权利要求4所述的装置,其特征在于,所述基模转换模块中的硅纳米线呈锥形分布。The apparatus according to claim 4, wherein the silicon nanowires in the fundamental mode conversion module are tapered.
  8. 根据权利要求7所述的装置,其特征在于,所述第一基模转换单元中的硅纳米线的宽度小于所述第二基模转换单元中的硅纳米线的宽度。The apparatus according to claim 7, wherein a width of the silicon nanowires in the first fundamental mode conversion unit is smaller than a width of the silicon nanowires in the second fundamental mode conversion unit.
  9. 根据权利要求1所述的装置,其特征在于,所述偏振转换器为基于不对称定向耦合器的偏振转换器。The apparatus of claim 1 wherein said polarization converter is a polarization converter based on an asymmetric directional coupler.
  10. 一种偏振纠缠光子对的产生方法,其特征在于,所述方法应用上述权利要求1至9所述的偏振纠缠光子对的产生装置,所述方法包括:A method for generating a polarization entangled photon pair, wherein the method uses the polarization entangled photon pair generating device according to any one of claims 1 to 9, the method comprising:
    所述分束器将所述输入端输入的光子束分为能量相同的第一光子束和第二光子束,所述第一输出端将所述第一光子束传输至所述第一光子对产生单元,所述第一光子对产生单元触发所述第一光子束生成第一TE模偏振光子对,并将 所述第一TE模偏振光子对传输至所述第一基模转换单元,所述第二输出端将所述第二光子束传输至所述第二光子对产生单元,所述第二光子对产生单元触发所述第二光子束生成第二TE模偏振光子对,并将所述第二TE模偏振光子对传输至所述第二基模转换单元;The beam splitter splits the photon beam input by the input end into a first photon beam and a second photon beam of the same energy, and the first output end transmits the first photon beam to the first photon pair a generating unit, the first photon pair generating unit triggering the first photon beam to generate a first TE mode polarized photon pair, and The first TE mode polarized photon pair is transmitted to the first fundamental mode conversion unit, and the second output transmits the second photon beam to the second photon pair generating unit, the second photon pair Generating unit triggers the second photon beam to generate a second TE mode polarized photon pair, and transmits the second TE mode polarized photon pair to the second fundamental mode conversion unit;
    所述第一基模转换单元将所述第一TE模偏振光子对转换为第一TE基模偏振光子对,并将所述第一TE基模偏振光子对传输至所述第一偏振转换单元,所述第二基模转换单元将所述第二TE模偏振光子对转换为第二TE基模偏振光子对,并将所述第二TE基模偏振光子对传输至所述第二偏振转换单元;The first fundamental mode conversion unit converts the first TE mode polarized photon pair into a first TE fundamental mode polarized photon pair, and transmits the first TE fundamental mode polarized photon pair to the first polarization conversion unit The second fundamental mode conversion unit converts the second TE mode polarized photon pair into a second TE fundamental mode polarized photon pair, and transmits the second TE fundamental mode polarized photon pair to the second polarization conversion unit;
    所述第一偏振转换单元将所述第一TE基模偏振光子对耦合到所述第二偏振转换单元中,所述第二偏振转换单元将所述第一TE基模偏振光子对转换为第一TM基模偏振光子对,并将所述第一TM基模偏振光子对和所述第二TE基模偏振光子对叠加为偏振纠缠光子对,输出所述偏振纠缠光子对。 The first polarization conversion unit couples the first TE fundamental mode polarized photon pair to the second polarization conversion unit, and the second polarization conversion unit converts the first TE fundamental mode polarization photon pair to A TM fundamental mode polarized photon pair, and the first TM fundamental mode polarized photon pair and the second TE fundamental mode polarized photon pair are superimposed into a polarization entangled photon pair, and the polarization entangled photon pair is output.
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US20150261058A1 (en) * 2013-02-19 2015-09-17 The University Of Bristol Optical source

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