WO2018232689A1 - Time-entangled photon pair generating device - Google Patents

Time-entangled photon pair generating device Download PDF

Info

Publication number
WO2018232689A1
WO2018232689A1 PCT/CN2017/089537 CN2017089537W WO2018232689A1 WO 2018232689 A1 WO2018232689 A1 WO 2018232689A1 CN 2017089537 W CN2017089537 W CN 2017089537W WO 2018232689 A1 WO2018232689 A1 WO 2018232689A1
Authority
WO
WIPO (PCT)
Prior art keywords
waveguide structure
substrate
waveguide
entangled photon
pump light
Prior art date
Application number
PCT/CN2017/089537
Other languages
French (fr)
Chinese (zh)
Inventor
耿巍
张臣雄
Original Assignee
华为技术有限公司
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 华为技术有限公司 filed Critical 华为技术有限公司
Priority to PCT/CN2017/089537 priority Critical patent/WO2018232689A1/en
Priority to CN201780003258.9A priority patent/CN109429509A/en
Publication of WO2018232689A1 publication Critical patent/WO2018232689A1/en

Links

Images

Classifications

    • 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
    • G02F1/35Non-linear optics
    • 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
    • G02F1/35Non-linear optics
    • G02F1/365Non-linear optics in an optical waveguide structure

Definitions

  • the present application relates to the field of optical communication technologies, and in particular, to a time entangled photon pair generating device.
  • Quantum entanglement refers to a phenomenon in a quantum mechanical system in which the properties of individual particles cannot be described separately due to the quantum association, which can only describe the overall nature of the system. If a pair is in a polarization entangled state The photon, if the polarization measurement for one of them is H, the polarization of the other photon must be H, and vice versa.
  • the entangled photon pair has important applications in the current quantum knock down (QKD) system.
  • QKD quantum knock down
  • the QKD of the BBM92 protocol can be performed using entangled photon pairs. To achieve ultra-long-distance QKD, it is necessary to realize quantum using entangled photon pairs. Relay (quantum relay or quantum repeater) and so on.
  • Photons can be entangled in different dimensions.
  • common entanglement coding methods include polarization entanglement, path entanglement, and time entanglement.
  • Most current patent applications are related to polarization entangled photon sources.
  • For the time entangled photon pair because its quantum state is not easily interfered by the external environment in the optical fiber, it is the most widely used coding method for the actual QKD.
  • the common way to produce time-coupled photon pairs academically is the down-conversion technique: using a laser, an unequal-arm MZ interferometer, a nonlinear material, and a system of multiple optical components, beamsplitters, and couplers to produce entangled photons. Correct.
  • the laser is used to provide pump light
  • the unequal arm MZ interferometer is usually a fiber-optic coded optical path for time-spliting the pump light to form early and late pulses, then early pulse and late pulse pumping.
  • a nonlinear material is used to generate a temporally entangled photon pair, which is then condensed using a plurality of optical elements to entangle the photon pairs, and the entangled photon pairs are split by a beam splitter and a coupler and coupled into the fiber.
  • Commonly used nonlinear materials such as barium metaborate crystal BBO, periodically poled lithium niobate crystal PPLN, etc., the preparation process or growth process can not be compatible with complementary metal oxide semiconductor (CMOS) process.
  • CMOS complementary metal oxide semiconductor
  • Materials that are compatible with CMOS processes do not contain these commonly used nonlinear materials, so these nonlinear materials cannot achieve CMOS on-chip integration.
  • Optical components are usually optical lenses. Lasers are usually large-volume independent devices with complex structures.
  • the unequal-arm MZ interferometers, optical lenses, beam splitters and couplers are also large-sized independent devices.
  • the size is too large to achieve on-chip integration. Therefore, due to the limitation of the principle of such entangled photon generation, each device selects an independent device and the size and processing process of each functional device are greatly different, and it is also difficult to be compatible with the CMOS process, so these devices cannot achieve low cost.
  • the on-chip integration results in a large overall size and high processing cost of the time entangled photon pairing system formed by these independent devices.
  • a time-entangled photon pair is generated by using a chip-down technique, and there is a large difference in size and on-chip processing technology of a time entangled photon pair generation system composed of a plurality of independent devices, which cannot be miniaturized and cannot be combined with a CMOS process.
  • CMOS process complementary metal-oxide-semiconductor
  • the embodiment of the present application provides a time entangled photon pair generating device for solving the problem that the size of the time entangled photon pair generating system in the prior art using the under-chip technology to generate a time entangled photon pair cannot be miniaturized, and cannot be combined with CMOS. Process-compatible technical issues.
  • the present application provides an entangled photon pair generating device including a substrate and a pumping source, a first waveguide structure and a second waveguide structure on the substrate; wherein the first waveguide structure and the second waveguide The structure is formed by etching a waveguide material between the pumping source and the second waveguide structure; the pumping source is configured to emit to the first waveguide structure Pumping light; the first waveguide structure for alternately outputting the first pump light pulse and the second pump light pulse after time-splitting the pump light; the second waveguide structure for The pump photons in the first pump light pulse or the second pump light pulse are converted into entangled photon pairs, the entangled photon pair comprising associated first photons and second photons.
  • the entangled photon pair generating device in the present application comprises at least a pumping light source and a first waveguide structure and a second waveguide structure on the substrate, the first waveguide structure has a time splitting function, and the second waveguide structure has a spontaneous four-wave mixing effect
  • the function of the entangled photon pair, the first waveguide structure and the second waveguide structure are formed by etching the waveguide material on the substrate, and the etching process can be compatible with the CMOS process, and the CMOS process can be used to fabricate the substrate.
  • a waveguide structure and a second waveguide structure can integrate the pump light source with the substrate by a chip process or a CMOS process, so that the size of the entangled photon pair generating device can be miniaturized.
  • the entangled photon pair generating device further includes: a third waveguide structure on the substrate, the third waveguide structure is formed by etching the waveguide material, the third waveguide structure Located between the first waveguide structure and the second waveguide structure for filtering out noise photons different from the frequency of the pump light in the first pump light pulse and the second pump light pulse.
  • the entangled photon pair generating device in the present application includes a first waveguide structure and a second waveguide structure on the substrate, and a third waveguide structure on the substrate, and the third waveguide structure has a filtering function, such as The function of the band rejection filter is capable of filtering out the first pump light pulse or the second pump before the first pump light pulse and the second pump light pulse alternately outputted by the first waveguide structure enter the second waveguide structure
  • the noise photons in the pump pulse having different frequency of the pump light are photons generated in the first waveguide structure different from the frequency of the pump light in the first pump light pulse or the second pump light pulse.
  • the entangled photon pair generating device further includes: a fourth waveguide structure on the substrate, the fourth waveguide structure is formed by etching the waveguide material, the fourth waveguide structure An output end of the second waveguide structure is configured to filter out noise photons output from the output end of the second waveguide structure different from the frequencies of the first photon and the second photon.
  • the entangled photon pair generating device in the present application includes a pumping light source and a first waveguide structure on the substrate, a second waveguide structure, a third waveguide structure, and a fourth waveguide structure, and the fourth waveguide structure has a filter function.
  • the noise photon entangled in the entangled photon pair generated by the third waveguide structure can be filtered out, and the noise photon refers to a photon generated at a frequency different from the first photon and the second photon generated during the generation of the entangled photon pair. It is beneficial to increase the content percentage of the entangled photon pair, which is beneficial to improve the signal quality when the entangled photon pair is applied in optical communication.
  • the entangled photon pair generating device further includes: a fifth waveguide structure on the substrate, the fifth waveguide structure is formed by etching the waveguide material, the fifth waveguide structure Located at an output of the fourth waveguide structure for separating the first photon and the second photon output from an output of the fourth waveguide structure.
  • the entangled photon pair generating device in the present application includes a pumping light source and a first waveguide structure on the substrate, a second waveguide structure, and a fifth waveguide structure, the fifth waveguide structure having the function of a beam splitter, capable of entanglement Photon separation in a photon pair.
  • the entangled photon pair generating device further includes: a sixth waveguide structure on the substrate, The sixth waveguide structure is formed by etching the waveguide material, and the sixth waveguide structure is located at an output end of the fifth waveguide structure for outputting the output end of the fifth waveguide structure
  • the photons are coupled into the first single mode fiber, and the second photons are coupled into the second single mode fiber.
  • the first single mode fiber and the second single mode fiber are disposed outside the substrate.
  • the entangled photon pair generating device in the present application includes a pumping light source and a first waveguide structure on the substrate, and a second waveguide structure, further including a sixth waveguide structure.
  • the sixth waveguide structure has the function of a coupler capable of coupling separate photons into a single mode fiber.
  • the substrate may be, but not limited to, an SOI (Silicon-On-Insulator) substrate.
  • the waveguide material can be, but is not limited to, silicon or silicon nitride.
  • the substrate can be, but is not limited to, an SOI substrate.
  • the pump light can excite spontaneous four-wave mixing effects and convert photons into entangled photons when passing through the second waveguide structure. .
  • the entangled photon pair generating device in the present application can be applied to the principle of time entangled photon pair generation based on non-degenerate spontaneous four-wave mixing effect, and is applicable to the principle of time entangled photon pair generation based on degenerate spontaneous four-wave mixing effect. .
  • the pump light source may be disposed on the substrate.
  • a pump light source and a plurality of waveguide structures are integrated on a substrate.
  • the substrate is an SOI substrate
  • the entangled photon pair generating device is used.
  • the size is miniaturized.
  • the plurality of waveguide structures are formed by etching the waveguide material deposited on the substrate, and the entangled photon pair generating device can be formed directly on the SOI substrate by a CMOS process, which can quantify the production of small devices and is advantageous for cost reduction.
  • the pumping source is a III-V laser diode or a vertical cavity surface emitting laser array VCSEL bonded to the substrate, or the pumping source is a Ge epitaxially grown on the substrate Laser diode.
  • the size can be guaranteed in the micrometer level, and the pumping light source can be integrated by the patch process.
  • the pumping source and the plurality of waveguide structures on the substrate is achieved, which is advantageous for reducing the volume of the entangled photon pair generating device.
  • the Ge laser diode is epitaxially grown directly on the substrate, the entangled photons are more controllable to the thickness and length and width of the generating device, and the miniaturization of the entangled photon pair generating device can be realized.
  • the device further includes a carrier, and the substrate and the pumping light source are disposed on the carrier.
  • the pump light source and the substrate are integrated on the carrier, and a plurality of waveguide structures are integrated on the substrate, which is advantageous for miniaturizing the size of the entangled photon pair generating device, for example, when the substrate is an SOI substrate, due to the SOI lining
  • the thickness of the bottom is on the order of microns such that the dimensions of the entangled photon pair generating device are on the order of microns.
  • the plurality of waveguide structures are formed by etching the waveguide material deposited on the substrate, and the entangled photon pair generating device can be formed directly on the SOI substrate by a semiconductor process, which can quantify the production of small devices and is advantageous in reducing cost.
  • the pumping source is a III-V laser diode or a vertical cavity surface emitting laser array VCSEL bonded to the carrier.
  • the size can be guaranteed in the micrometer level, and the pumping light source can be integrated by the patch process.
  • the carrier on-chip integration of the pump source and the plurality of waveguide structures on the substrate is achieved, which is advantageous for reducing the volume of the entangled photon pair generating device.
  • the device further includes a seventh waveguide structure, the seventh waveguide structure is located on the carrier and/or the substrate, and the pump light source passes through the seventh waveguide structure and the first waveguide Structural connectivity.
  • the pumping source on the carrier is connected to the first waveguide structure on the substrate through the seventh waveguide structure, so that the positional relationship between the pumping source on the carrier and the plurality of waveguide structures on the substrate is flexible, for example,
  • the positional relationship between the pump source on the carrier and the plurality of waveguide structures on the substrate may be in a horizontal arrangement; for example, the positional relationship between the pump source on the carrier and the plurality of waveguide structures on the substrate may be side by side In this case, the lateral dimension of the carrier can be further reduced.
  • FIG. 1 is a schematic diagram of a principle of generating a time pulse superposition state and a time entangled photon pair according to an embodiment of the present application
  • FIG. 2 is a schematic diagram of a schematic diagram of a degenerate spontaneous four-wave mixing effect and a non-degenerate spontaneous four-wave mixing effect according to an embodiment of the present application;
  • FIG. 3 is a schematic diagram of a principle of an entangled photon pair generating device according to an embodiment of the present application
  • FIG. 4 is a schematic cross-sectional structural view of a first entangled photon pair generating device according to an embodiment of the present application
  • FIG. 5 is a schematic top plan view of a first entangled photon pair generating device according to an embodiment of the present application
  • FIG. 6 is a schematic cross-sectional structural view of a second entangled photon pair generating device according to an embodiment of the present application.
  • FIG. 7 is a schematic cross-sectional structural view of a second entangled photon pair generating device according to an embodiment of the present application.
  • FIG. 8 is a schematic cross-sectional structural view of a second entangled photon pair generating device according to an embodiment of the present application.
  • FIG. 9 is a schematic top plan view of a second entangled photon pair generating device according to an embodiment of the present application.
  • FIG. 10 is a schematic top plan view of a second entangled photon pair generating device according to an embodiment of the present application.
  • the principle of time splitting the pump light is that a single photon passes through an unequal arm MZ interferometer to produce a time superposition of individual photons. For example, as shown in Figure 1(a), after passing through the first 50:50 fiber splitter of the unequal arm MZ interferometer, a single photon has a half chance of passing the short arm through the long arm and half the probability.
  • a single pump pulse forms an early pulse and a late pulse after passing through the first fiber splitter, and then merges with the second fiber splitter to form a superposition of the early pulse and the late pulse.
  • a commonly used principle for generating temporally entangled photon pairs is to pump time-split pump light to excite nonlinear materials to produce temporally entangled photon pairs.
  • pumps nonlinear materials such as BBO, PPLN, etc.
  • BBO bicarbonate
  • PPLN correlated photons entangled in time
  • the probability of simultaneously generating two associated photons in the early pulse and the late pulse is almost zero, which can be ignored.
  • each functional device is a separate device, and the manufacturing methods of each functional device are quite different, so these functional devices cannot achieve on-chip integration, and the entire device size cannot be reduced.
  • the principle of generating a time entangled photon pair used in the present application is: a third-order nonlinearity of a waveguide structure subjected to time-division, in a waveguide structure of a silicon-based material (such as silicon, silicon nitride, silicon dioxide, etc.) Under the influence of the effect, the pump photons of the early pulse pump optical pump are converted into time-entangled correlated photon pairs, or the pump photons of the late pulse pump optical pump are converted into time-entangled correlated photon pairs.
  • a silicon-based material such as silicon, silicon nitride, silicon dioxide, etc.
  • the silicon-based waveguide structure has a three-order nonlinear effect (spontaneous four-wave-mixing, SFWM), also known as spontaneous four-wave mixing effect.
  • Spontaneous four-wave mixing includes non-degenerate four-wave mixing and degenerate four-wave mixing.
  • the present invention provides a time entangled photon pair generating device suitable for both non-degenerate spontaneous four-wave mixing and degenerate spontaneous four-wave mixing.
  • the present application provides an entangled photon pair generating device including a pumping light source and a plurality of waveguide structures.
  • the pumping source and the plurality of waveguide structures are integrated on the same substrate surface, and the plurality of waveguide structures provide time entanglement.
  • the photon pair produces an optical path and an output optical path.
  • the substrate is an SOI substrate, and the pump light source and the plurality of waveguide structures are disposed on the same surface on the SOI substrate, wherein the pump light source provides pump light, and the plurality of waveguide structures are connected to each other and can A beam splitting path for pumping light, a pair of photons to generate an optical path, and a transmission path for entanglement of photon pairs.
  • the process of generating an entangled photon pair by the entangled photon generation device is: after the pump light source generates the pump light, the spectroscopic optical path provided by the waveguide structure performs time splitting on the pump light, and the entangled photon pair generates an optical path to excite the spontaneous four-wave mixing effect.
  • the pump light is converted into an entangled photon pair, and the transmitted optical path of the entangled photon pair filters and splits the associated photons in the entangled photon pair and is respectively coupled into the single mode fiber outside the substrate.
  • the pumping light source in the present application is capable of generating pump light of a communication band, which is a monochromatic pumping light pulse or an overlapping pump pulse of two different wavelengths.
  • the plurality of waveguide structures in the present application are silicon-based waveguide structures, such as silicon, silicon nitride or silicon dioxide waveguide structures, to generate spontaneous four-wave mixing effects on the SOI substrate.
  • silicon-based waveguide structures such as silicon, silicon nitride or silicon dioxide waveguide structures
  • waveguide structures having the above functions of other materials are also within the scope of the present application.
  • the waveguide structure can be etched through the waveguide material on the SOI substrate, and the process can be compatible with the CMOS process.
  • the SOI substrate in the present application is a silicon-based substrate, and a silicon-insulator-silicon structure SOI substrate can be obtained by ion implantation or wafer bonding.
  • the present application fabricates a plurality of waveguide structures and a pumping light source on the surface of the SOI substrate. Since the thickness of the SOI substrate is on the order of micrometers, the size of the entangled photon pair generating device is miniaturized, and a plurality of waveguide structures having the above functions can pass The waveguide material on the SOI substrate is etched, and the process can be compatible with the CMOS process. Therefore, the entangled photon pair generating device can be formed directly on the SOI substrate by a semiconductor process, which can quantify the production and contribute to cost reduction.
  • An entangled photon pair generating device provided by an embodiment of the present application includes a substrate 100, a waveguide structure 200 on the substrate 100, and a pumping light source 300.
  • the waveguide structure 200 includes: a first waveguide structure 201, The second waveguide structure 202, the third waveguide structure 203, the fourth waveguide structure 204, the fifth waveguide structure 205, and the sixth waveguide structure 206.
  • the substrate 100 may be, but not limited to, an SOI substrate.
  • the first waveguide structure 201, the second waveguide structure 202, the third waveguide structure 203, the fourth waveguide structure 204, the fifth waveguide structure 205, and the sixth waveguide structure 206 are all engraved by the waveguide material deposited on the substrate 100.
  • the etching process can be compatible with the CMOS process. Therefore, the entangled photon pair generating device can be formed directly on the substrate 100 by a semiconductor process, which can quantify the production and contribute to cost reduction.
  • the waveguide material on the substrate 100 The quality can be, but is not limited to, silicon or silicon nitride.
  • the first waveguide structure 201, the second waveguide structure 202, the third waveguide structure 203, the fourth waveguide structure 204, the fifth waveguide structure 205, and the sixth waveguide structure are combined with FIG.
  • the positional relationship, structural features and functions between 206 are described in detail.
  • the pumping light source 300 is disposed at an edge of the SOI substrate and disposed adjacent to the first waveguide structure 201 for emitting pump light to the first waveguide structure 201.
  • the pumping source 300 is a III-V laser diode or a vertical cavity surface emitting laser array VCSEL bonded to an SOI substrate.
  • the pump light source 300 is a Ge laser diode epitaxially grown on the SOI substrate. The pumping source 300 is bonded or directly grown on the SOI substrate to ensure that the size of the entangled photon generation device fabricated on the SOI substrate is on the order of millimeters.
  • the first waveguide structure 201 is directly connected to the pumping light source 300 for alternately outputting the first pumping light pulse and the second pumping light pulse after time-splitting the pumping light.
  • the first waveguide structure 201 provides two optical paths of different lengths. The two optical paths respectively meet at the input end and the output end of the first waveguide structure 201, and the first waveguide structure 201 has an optical path of unequal length, and the first waveguide structure 201 can be
  • the pump light input at the input end is time-divided to alternately output the first pump light pulse and the second pump light pulse, the first pump light pulse is an earlier output pump light pulse, and the second pump light pulse It is a pump light pulse that is output later.
  • the output of the first waveguide structure 201 is in communication with the input of the second waveguide structure 202 via a third waveguide structure 203 having a filtering effect.
  • the third waveguide structure 203 is located between the first waveguide structure 201 and the second waveguide structure 202, and the third waveguide structure 203 is configured to filter out the third photon in the first pump light pulse or the second pump light pulse.
  • the frequency of the three photons is different from the frequency of the two pump photons before the conversion of the entangled photons.
  • the shape of the third waveguide structure 203 is designed to be in the shape of an optical filter, such as the shape of a band rejection filter, which functions to alternately output the first pump light pulse and the second pump light pulse into the second waveguide structure 202.
  • noise photons of different frequency from the pump light in the first pump light pulse or the second pump light pulse are filtered out, that is, if two pumps in the first pump light pulse or the second pump light pulse
  • the frequencies of the neutrons are ⁇ p1 and ⁇ p2, respectively, and the third waveguide structure 203 removes noise photons different from ⁇ p1 and ⁇ p2 output from the first waveguide structure 201.
  • the pump light of the first pump light pulse or the second pump light pulse also has a certain probability of generating a four-wave mixing effect or a Raman effect in the first waveguide structure 201, thereby generating photons of other frequencies. Photons are noisy for entangled photons, so they are filtered out before entangled photons are generated.
  • the second waveguide structure 202 is located at the output end of the third waveguide structure and has a spiral structure.
  • the function of the second waveguide structure 202 is to provide an optical path that is as long as possible, so that the first pump light pulse and the second pump light pulse are alternately output.
  • the specific generation process is to convert two pump photons in the first pump light pulse into entangled photon pairs, or convert two pump photons in the second pump light pulse into entangled photon pairs, and generate entangled photons.
  • the pair includes the associated first photon and second photon.
  • the probability of simultaneously generating entangled photon pairs in the first pump light pulse and the second pump light pulse is negligible, because the first pump light pulse and the second pump light pulse simultaneously generate entanglement.
  • the probability of a photon pair is p 2 , which is a minimum value. Therefore, it can be considered that in the case where an entangled photon pair is generated in the first pump light pulse, no entangled photon pair is generated in the second pump light pulse, and vice versa. Also.
  • the entangled state of the generated entangled photon pair can be used Represented where e indicates that an entangled photon pair was detected in an earlier first pump light pulse position and l indicates that an entangled photon pair was detected in a later second pump light pulse.
  • the frequency relationship between the two pump photons before conversion and the converted entangled photon pair is: the frequencies defining the two pump photons are respectively ⁇ p1, ⁇ p2, and the frequencies of the first photon and the second photon are respectively ⁇ i, ⁇ s
  • the output of the second waveguide structure 202 is in communication with the input of the fifth waveguide structure 205 through the fourth waveguide structure 204.
  • the fourth waveguide structure 204 is located between the second waveguide structure 202 and the fifth waveguide structure 205 and has a structural feature similar to an optical filter, and functions to pass the second waveguide after the entangled photon pair enters the fifth waveguide structure 205.
  • the doping of the output of the structure 202 is filtered out of noise photons in the entangled photon pair, wherein the noise photons are photons that are different in frequency from the first photon and the second photon generated during the generation of the entangled photon pair.
  • the fifth waveguide structure 205 is located at the output end of the fourth waveguide structure 204, and has a structural feature similar to a beam splitter, and functions as the first photon and the second photon in the entangled photon pair outputted by the fourth waveguide structure 204, according to The optical path of the fifth waveguide structure 205 separates the first photon from the second photon.
  • the output end of the fifth waveguide structure 205 includes a first output end and a second output end. The first output end of the fifth waveguide structure 205 outputs a first photon, and the second output end of the fifth waveguide structure 205 outputs a second photon. .
  • the sixth waveguide structure 206 is located at the output end of the fifth waveguide structure 205 and has a structural feature similar to a coupler for coupling the first photon outputted from the first output end of the fifth waveguide structure 205 into the first single mode fiber.
  • the second photon outputted from the second output end of the fifth waveguide structure 205 is coupled into the second single mode fiber, and the first single mode fiber and the second single mode fiber are disposed outside the substrate 100.
  • the pumping light source 300, the first waveguide structure 201 having a spectroscopic effect, and the third waveguide structure 203 having a filtering effect have an exciting four-wave mixing effect to generate an entangled photon pair.
  • a second waveguide structure 202, a fourth waveguide structure 204 having a filtering effect, a fifth waveguide structure 205 having a splitting effect, and a sixth waveguide structure 206 having a coupling function may be integrated on the SOI substrate due to the SOI substrate
  • the thickness is on the order of micrometers, and the size is on the order of millimeters, so that the size of the entangled photon pair generating device is miniaturized, and the first waveguide structure 201, the second waveguide structure 202, the third waveguide structure 203, the fourth waveguide structure 204, and the fifth
  • the waveguide structure 205 and the sixth waveguide structure 206 are both formed by etching a waveguide material deposited on the SOI substrate.
  • the etching process can be compatible with the CMOS process. Therefore, the entangled photon pair generating device can be directly on the SOI substrate.
  • an entangled photon pair generating device as shown in FIG. 6, comprising:
  • the substrate 100 includes a waveguide structure 200 on the substrate 100 and a pumping source 300.
  • the waveguide structure 200 includes a first waveguide structure 201, a second waveguide structure 202, a third waveguide structure 203, and a fourth waveguide structure 204.
  • the fifth waveguide structure 205, the sixth waveguide structure 206 further includes a carrier 400, the substrate 100 and the pumping light source 300 are disposed on the carrier 400, and further includes a seventh waveguide structure 401, and the pumping light source 300 passes through the seventh waveguide structure 401 and A waveguide structure 201 is in communication.
  • the first waveguide structure 201, the second waveguide structure 202, the third waveguide structure 203, the fourth waveguide structure 204, the fifth waveguide structure 205, and the sixth waveguide structure 206 are all engraved by the waveguide material deposited on the substrate 100.
  • the etch process can be compatible with the CMOS process, so the entangled photon pair generating device can be directly in the SOI lining
  • the bottom is formed by a semiconductor process, which can quantify production and help reduce costs.
  • the waveguide material on the substrate 100 is made of silicon or silicon nitride to produce a spontaneous four-wave mixing effect.
  • the substrate 100 is an SOI substrate
  • the first waveguide structure 201, the second waveguide structure 202, the third waveguide structure 203, the fourth waveguide structure 204, the fifth waveguide structure 205, and the sixth waveguide structure 206 are in the SOI.
  • the specific content on the substrate is as described in the foregoing embodiment, and will not be described here.
  • the seventh waveguide structure 401 is located on the substrate 100.
  • the substrate 100 is an SOI substrate, and a seventh waveguide structure 401 is disposed at an edge of the SOI substrate.
  • the pump light source 300 on the carrier is disposed adjacent to the seventh waveguide structure 401.
  • the pump light source 300 and the seventh waveguide structure 401 are provided.
  • the first waveguide structure 201, the third waveguide structure 203, the second waveguide structure 202, the fourth waveguide structure 204, the fifth waveguide structure 205, and the sixth waveguide structure 206 (not shown in FIG. 7) are disposed laterally along the inline shape.
  • the seventh waveguide structure 401 is also fabricated together with the first waveguide structure 201, the second waveguide structure 202, the third waveguide structure 203, the fourth waveguide structure 204, the fifth waveguide structure 205, and the sixth waveguide structure 206, both of which pass through the SOI.
  • the waveguide material on the substrate is etched, and the waveguide material is a waveguide layer deposited on the SOI substrate.
  • the waveguide material on the SOI substrate is silicon, silicon nitride or silicon dioxide to generate a spontaneous four-wave mixing effect of the pump light in the waveguide material on the SOI substrate, and on the SOI substrate
  • the etching process of the waveguide material is compatible with the CMOS process, which is advantageous for the quantitative production of the entangled photon generation device and reduces the cost.
  • the seventh waveguide structure 401 is located on the carrier 400.
  • the substrate 100 is an SOI substrate, and the seventh waveguide structure 401 and the pump light source 300 are both disposed on a carrier, and the seventh waveguide structure 401, the pumping light source 300, and the first waveguide structure 201 on the SOI substrate.
  • the third waveguide structure 203, the second waveguide structure 202, the fourth waveguide structure 204, the fifth waveguide structure 205, and the sixth waveguide structure 206 (not shown in FIG. 8) are disposed laterally along the inline shape.
  • a seventh waveguide structure 401 is disposed adjacent the edge of the SOI substrate in communication with the first waveguide structure 201 at the edge of the SOI substrate.
  • the seventh waveguide structure 401 is formed by etching a waveguide material on the carrier.
  • the waveguide material on the carrier may be the same as or different from the waveguide material on the SOI substrate.
  • the waveguide material on the carrier is silicon or silicon nitride.
  • a portion of the seventh waveguide structure 401 is located on the carrier 400 and another portion is located on the substrate 100.
  • the substrate 100 is an SOI substrate
  • the pumping source 300 is disposed on the carrier
  • a portion of the seventh waveguide structure 401 is located on the carrier 400
  • another portion is located on the SOI substrate
  • the optical path of the seventh waveguide structure 401 is divided.
  • the front optical path and the rear optical path, the front optical path is located on the carrier 400, and the rear optical path is located on the substrate 100.
  • a seventh waveguide structure 401, a pumping light source 300 and a first waveguide structure 201 on the SOI substrate, a third waveguide structure 203, a second waveguide structure 202, a fourth waveguide structure 204, a fifth waveguide structure 205, and a sixth waveguide structure 206 (not shown in Fig. 8) is disposed laterally along the inline shape.
  • the pumping source 300 and the substrate 100 are arranged side by side on the carrier 400.
  • the substrate 100 is an SOI substrate
  • the SOI substrate and the pumping light source 300 are arranged side by side on the carrier
  • the shape of the seventh waveguide structure 401 for connecting the pumping light source 300 and the first waveguide structure 201 is C shape.
  • the first waveguide structure 201, the second waveguide structure 202, the third waveguide structure 203, the fourth waveguide structure 204, the fifth waveguide structure 205, and the sixth waveguide structure 206 (not shown in FIG. 8) on the SOI substrate are along a word Horizontal setting.
  • the pump light source 300 is a III-V laser diode or a vertical cavity surface emitting laser array VCSEL bonded to the carrier 400.
  • the material of the carrier may be silica or a polymer.
  • the pumping light source 300 and the SOI substrate are integrated on the same surface of the carrier, and the first waveguide structure 201 having the light splitting effect is integrated on the SOI substrate, and has a filtering effect.
  • the third waveguide structure 203 has a second waveguide structure for exciting an entangled photon pair to excite an spontaneous four-wave mixing effect, a fourth waveguide structure 204 having a filtering effect, and a fifth waveguide structure 205 having a splitting effect, having a coupling effect
  • the sixth waveguide structure, the thickness of the SOI substrate is on the order of micrometers, and the size is on the order of millimeters, so the above integrated structure makes the entangled photon pair
  • the size of the device is miniaturized, and the first waveguide structure 201, the second waveguide structure 202, the third waveguide structure 203, the fourth waveguide structure 204, the fifth waveguide structure 205, and the sixth waveguide structure 206 are all deposited on the SOI lining.
  • the etching process can be compatible with the CMOS process. Therefore, the entangled photon pair generating device can be formed directly on the SOI substrate by a semiconductor process, which can quantify the production and is advantageous for cost reduction.

Abstract

An entangled photon pair generating device, comprising a substrate, a pump light source, and a first waveguide structure and a second waveguide structure located on the substrate. The pump light source is used for transmitting pump light to the first waveguide structure. The first waveguide structure is used for alternately outputting a first pump light pulse and a second pump light pulse after time division is performed on the pump light. The second waveguide structure is used for converting two pumped photons in the first pump light pulse or in the second pump light pulse into an entangled photon pair. Integrating the first waveguide structure, the second waveguide structure, and the pump light source on one substrate can reduce device size. The first waveguide structure and the second waveguide structure on the substrate are both formed by etching the same waveguide material on the substrate; therefore, a manufacturing process thereof is compatible with a CMOS process, facilitating mass production of devices and cost reduction.

Description

一种时间纠缠光子对产生装置Time entangled photon pair generating device 技术领域Technical field
本申请涉及光通信技术领域,尤其涉及一种时间纠缠光子对产生装置。The present application relates to the field of optical communication technologies, and in particular, to a time entangled photon pair generating device.
背景技术Background technique
量子纠缠是指在一个量子力学系统里,其中各个粒子的性质由于出现量子关联,从而无法对其进行单独描述,只能描述系统整体性质的现象。如一对处在偏振纠缠态
Figure PCTCN2017089537-appb-000001
的光子,如果对其中一个的偏振测量结果为H,则另一个光子的偏振必定为H,反之亦然。纠缠光子对在当前量子密钥分发(quick knock down,QKD)系统中具有重要应用,如:可以使用纠缠光子对进行BBM92协议的QKD;为实现超长距离的QKD,需要利用纠缠光子对实现量子中继(quantum relay或quantum repeater)等。
Quantum entanglement refers to a phenomenon in a quantum mechanical system in which the properties of individual particles cannot be described separately due to the quantum association, which can only describe the overall nature of the system. If a pair is in a polarization entangled state
Figure PCTCN2017089537-appb-000001
The photon, if the polarization measurement for one of them is H, the polarization of the other photon must be H, and vice versa. The entangled photon pair has important applications in the current quantum knock down (QKD) system. For example, the QKD of the BBM92 protocol can be performed using entangled photon pairs. To achieve ultra-long-distance QKD, it is necessary to realize quantum using entangled photon pairs. Relay (quantum relay or quantum repeater) and so on.
光子可在不同的维度上产生纠缠,比如常见的纠缠编码方式有偏振态纠缠、路径纠缠、时间纠缠等。当前大部分专利申请是关于偏振纠缠光子源的。对于时间纠缠光子对,由于其量子态在光纤中不易受到外界环境的干扰,为实际QKD应用最广泛的一种编码方式。Photons can be entangled in different dimensions. For example, common entanglement coding methods include polarization entanglement, path entanglement, and time entanglement. Most current patent applications are related to polarization entangled photon sources. For the time entangled photon pair, because its quantum state is not easily interfered by the external environment in the optical fiber, it is the most widely used coding method for the actual QKD.
但目前时间纠缠光子对的产生方式只在学术上有所研究。学术上产生时间纠缠光子对的普遍方式为片下的下转换技术:使用激光器、不等臂MZ干涉仪、非线性材料以及多个光学元件、分束器和耦合器构成的系统来产生纠缠光子对。其中,激光器用来提供泵浦光,不等臂MZ干涉仪通常是使用光纤搭建的编码光路,用来将泵浦光进行时间分光,形成早脉冲和晚脉冲,然后早脉冲和晚脉冲泵浦非线性材料,来产生时间纠缠光子对,之后利用多个光学元件纠缠光子对进行会聚,利用分束器和耦合器将纠缠光子对分束后,耦合进光纤。通常采用的非线性材料,如偏硼酸钡晶体BBO、周期性极化铌酸锂晶体PPLN等,其制备工艺或生长工艺都无法与互补金属氧化物半导体元件制程(complementary metal oxide semiconductor,CMOS)兼容,与CMOS工艺兼容的材料不包含这些常用的非线性材料,所以这些非线性材料无法实现CMOS片上集成。光学元件通常是光学透镜,激光器通常是结构复杂的大体积独立器件,不等臂MZ干涉仪、光学透镜,分束器和耦合器也都是大尺寸独立器件,尺寸太大无法实现片上集成。因此,受此种纠缠光子对产生原理的限制,各个器件选择的都是独立的器件且各个功能器件的尺寸与加工工艺存在较大差异,也难以与CMOS工艺兼容,所以这些器件无法实现低成本的片上集成,导致由这些独立器件构成的时间纠缠光子对产生系统的整体尺寸较大、加工成本高。However, the current generation of entangled photon pairs has only been studied academically. The common way to produce time-coupled photon pairs academically is the down-conversion technique: using a laser, an unequal-arm MZ interferometer, a nonlinear material, and a system of multiple optical components, beamsplitters, and couplers to produce entangled photons. Correct. Among them, the laser is used to provide pump light, and the unequal arm MZ interferometer is usually a fiber-optic coded optical path for time-spliting the pump light to form early and late pulses, then early pulse and late pulse pumping. A nonlinear material is used to generate a temporally entangled photon pair, which is then condensed using a plurality of optical elements to entangle the photon pairs, and the entangled photon pairs are split by a beam splitter and a coupler and coupled into the fiber. Commonly used nonlinear materials, such as barium metaborate crystal BBO, periodically poled lithium niobate crystal PPLN, etc., the preparation process or growth process can not be compatible with complementary metal oxide semiconductor (CMOS) process. Materials that are compatible with CMOS processes do not contain these commonly used nonlinear materials, so these nonlinear materials cannot achieve CMOS on-chip integration. Optical components are usually optical lenses. Lasers are usually large-volume independent devices with complex structures. The unequal-arm MZ interferometers, optical lenses, beam splitters and couplers are also large-sized independent devices. The size is too large to achieve on-chip integration. Therefore, due to the limitation of the principle of such entangled photon generation, each device selects an independent device and the size and processing process of each functional device are greatly different, and it is also difficult to be compatible with the CMOS process, so these devices cannot achieve low cost. The on-chip integration results in a large overall size and high processing cost of the time entangled photon pairing system formed by these independent devices.
综上,现有技术中采用片下技术产生时间纠缠光子对,存在着由多个独立器件构成的时间纠缠光子对产生系统的尺寸与片上加工工艺存在较大差异无法小型化,无法与CMOS工艺兼容的技术问题。In summary, in the prior art, a time-entangled photon pair is generated by using a chip-down technique, and there is a large difference in size and on-chip processing technology of a time entangled photon pair generation system composed of a plurality of independent devices, which cannot be miniaturized and cannot be combined with a CMOS process. Compatible technical issues.
发明内容Summary of the invention
本申请实施例提供了一种时间纠缠光子对产生装置,用以解决现有技术中采用片下技术产生时间纠缠光子对存在的时间纠缠光子对产生系统的尺寸无法小型化,无法与CMOS 工艺兼容的技术问题。The embodiment of the present application provides a time entangled photon pair generating device for solving the problem that the size of the time entangled photon pair generating system in the prior art using the under-chip technology to generate a time entangled photon pair cannot be miniaturized, and cannot be combined with CMOS. Process-compatible technical issues.
本申请提供一种纠缠光子对产生装置,包括衬底和泵浦光源,位于所述衬底上的第一波导结构和第二波导结构;其中,所述第一波导结构和所述第二波导结构是通过对波导材质刻蚀后形成的,所述第一波导结构位于所述泵浦光源和所述第二波导结构之间;所述泵浦光源,用于向所述第一波导结构发射泵浦光;所述第一波导结构,用于对所述泵浦光进行时间分光后交替输出第一泵浦光脉冲和第二泵浦光脉冲;所述第二波导结构,用于将所述第一泵浦光脉冲或所述第二泵浦光脉冲中的泵浦光子转化为纠缠光子对,所述纠缠光子对包括关联的第一光子和第二光子。The present application provides an entangled photon pair generating device including a substrate and a pumping source, a first waveguide structure and a second waveguide structure on the substrate; wherein the first waveguide structure and the second waveguide The structure is formed by etching a waveguide material between the pumping source and the second waveguide structure; the pumping source is configured to emit to the first waveguide structure Pumping light; the first waveguide structure for alternately outputting the first pump light pulse and the second pump light pulse after time-splitting the pump light; the second waveguide structure for The pump photons in the first pump light pulse or the second pump light pulse are converted into entangled photon pairs, the entangled photon pair comprising associated first photons and second photons.
本申请中的纠缠光子对产生装置至少包括泵浦光源和衬底上的第一波导结构和第二波导结构,第一波导结构具有时间分光功能,第二波导结构具有自发四波混频效应产生纠缠光子对的功能,第一波导结构,第二波导结构均是对衬底上的波导材质刻蚀后形成的,此刻蚀工艺可以与CMOS工艺兼容,采用CMOS工艺即可在衬底上制作第一波导结构和第二波导结构,采用贴片工艺或CMOS工艺即可将泵浦光源与衬底集成,进而使得纠缠光子对产生装置的尺寸可以小型化。The entangled photon pair generating device in the present application comprises at least a pumping light source and a first waveguide structure and a second waveguide structure on the substrate, the first waveguide structure has a time splitting function, and the second waveguide structure has a spontaneous four-wave mixing effect The function of the entangled photon pair, the first waveguide structure and the second waveguide structure are formed by etching the waveguide material on the substrate, and the etching process can be compatible with the CMOS process, and the CMOS process can be used to fabricate the substrate. A waveguide structure and a second waveguide structure can integrate the pump light source with the substrate by a chip process or a CMOS process, so that the size of the entangled photon pair generating device can be miniaturized.
进一步的,所述纠缠光子对产生装置还包括:位于所述衬底上的第三波导结构,所述第三波导结构是通过对所述波导材质刻蚀后形成的,所述第三波导结构位于所述第一波导结构和所述第二波导结构之间,用于滤除与所述第一泵浦光脉冲、所述第二泵浦光脉冲中的泵浦光频率不同的噪声光子。Further, the entangled photon pair generating device further includes: a third waveguide structure on the substrate, the third waveguide structure is formed by etching the waveguide material, the third waveguide structure Located between the first waveguide structure and the second waveguide structure for filtering out noise photons different from the frequency of the pump light in the first pump light pulse and the second pump light pulse.
本申请中的纠缠光子对产生装置除了包括泵浦光源和衬底上的第一波导结构和第二波导结构,还包括衬底上的第三波导结构,第三波导结构具有滤光功能,如具有带阻滤波器的功能,能够在第一波导结构交替输出的第一泵浦光脉冲和第二泵浦光脉冲进入第二波导结构之前,滤除与第一泵浦光脉冲或第二泵浦光脉冲中的泵浦光频率不同的噪声光子,这些噪声光子是在第一波导结构中产生的与第一泵浦光脉冲或第二泵浦光脉冲中的泵浦光频率不同的光子。The entangled photon pair generating device in the present application includes a first waveguide structure and a second waveguide structure on the substrate, and a third waveguide structure on the substrate, and the third waveguide structure has a filtering function, such as The function of the band rejection filter is capable of filtering out the first pump light pulse or the second pump before the first pump light pulse and the second pump light pulse alternately outputted by the first waveguide structure enter the second waveguide structure The noise photons in the pump pulse having different frequency of the pump light are photons generated in the first waveguide structure different from the frequency of the pump light in the first pump light pulse or the second pump light pulse.
进一步的,所述纠缠光子对产生装置还包括:位于所述衬底上的第四波导结构,所述第四波导结构是通过对所述波导材质刻蚀后形成的,所述第四波导结构位于所述第二波导结构的输出端,用于滤除从所述第二波导结构的输出端输出的与所述第一光子、所述第二光子的频率不同的噪声光子。Further, the entangled photon pair generating device further includes: a fourth waveguide structure on the substrate, the fourth waveguide structure is formed by etching the waveguide material, the fourth waveguide structure An output end of the second waveguide structure is configured to filter out noise photons output from the output end of the second waveguide structure different from the frequencies of the first photon and the second photon.
本申请中的纠缠光子对产生装置除了包括泵浦光源和衬底上的第一波导结构,第二波导结构,第三波导结构,还包括第四波导结构,第四波导结构具有滤波器的功能,能够将第三波导结构产生的缠杂在纠缠光子对中的噪声光子滤除,这些噪声光子是指在纠缠光子对产生过程中产生的与第一光子、第二光子的频率不同的光子,有利于提升纠缠光子对的含量百分比,在纠缠光子对应用在光通信中时,有利于提升信号质量。The entangled photon pair generating device in the present application includes a pumping light source and a first waveguide structure on the substrate, a second waveguide structure, a third waveguide structure, and a fourth waveguide structure, and the fourth waveguide structure has a filter function. The noise photon entangled in the entangled photon pair generated by the third waveguide structure can be filtered out, and the noise photon refers to a photon generated at a frequency different from the first photon and the second photon generated during the generation of the entangled photon pair. It is beneficial to increase the content percentage of the entangled photon pair, which is beneficial to improve the signal quality when the entangled photon pair is applied in optical communication.
进一步的,所述纠缠光子对产生装置还包括:位于所述衬底上的第五波导结构,所述第五波导结构是通过对所述波导材质刻蚀后形成的,所述第五波导结构位于所述第四波导结构的输出端,用于将从第四波导结构的输出端输出的所述第一光子、所述第二光子分离。Further, the entangled photon pair generating device further includes: a fifth waveguide structure on the substrate, the fifth waveguide structure is formed by etching the waveguide material, the fifth waveguide structure Located at an output of the fourth waveguide structure for separating the first photon and the second photon output from an output of the fourth waveguide structure.
本申请中的纠缠光子对产生装置除了包括泵浦光源和衬底上的第一波导结构,第二波导结构,还包括第五波导结构,第五波导结构具有分束器的功能,能够将纠缠光子对中的光子分离。The entangled photon pair generating device in the present application includes a pumping light source and a first waveguide structure on the substrate, a second waveguide structure, and a fifth waveguide structure, the fifth waveguide structure having the function of a beam splitter, capable of entanglement Photon separation in a photon pair.
进一步的,所述纠缠光子对产生装置还包括:位于所述衬底上的第六波导结构,所述 第六波导结构是通过对所述波导材质刻蚀后形成的,所述第六波导结构位于所述第五波导结构的输出端,用于将所述第五波导结构的输出端输出的第一光子耦合进第一单模光纤内,将所述第二光子耦合进第二单模光纤内,所述第一单模光纤、所述第二单模光纤设置在所述衬底外部。Further, the entangled photon pair generating device further includes: a sixth waveguide structure on the substrate, The sixth waveguide structure is formed by etching the waveguide material, and the sixth waveguide structure is located at an output end of the fifth waveguide structure for outputting the output end of the fifth waveguide structure The photons are coupled into the first single mode fiber, and the second photons are coupled into the second single mode fiber. The first single mode fiber and the second single mode fiber are disposed outside the substrate.
本申请中的纠缠光子对产生装置除了包括泵浦光源和衬底上的第一波导结构,第二波导结构,还包括第六波导结构。第六波导结构具有耦合器的功能,能够将分离的光子耦合进单模光纤。The entangled photon pair generating device in the present application includes a pumping light source and a first waveguide structure on the substrate, and a second waveguide structure, further including a sixth waveguide structure. The sixth waveguide structure has the function of a coupler capable of coupling separate photons into a single mode fiber.
所述衬底可以但不限于为SOI(Silicon-On-Insulator,绝缘衬底上的硅)衬底。所述波导材质可以但不限于为硅或氮化硅。衬底可以但不限于为SOI衬底,衬底上的波导材质为硅或氮化硅时,泵浦光经过第二波导结构时,能够激发自发四波混频效应,将光子转换为纠缠光子。The substrate may be, but not limited to, an SOI (Silicon-On-Insulator) substrate. The waveguide material can be, but is not limited to, silicon or silicon nitride. The substrate can be, but is not limited to, an SOI substrate. When the waveguide material on the substrate is silicon or silicon nitride, the pump light can excite spontaneous four-wave mixing effects and convert photons into entangled photons when passing through the second waveguide structure. .
本申请实施例中,所述两个泵浦光子的频率分别为ωp1、ωp2,所述第一光子和所述第二光子的频率分别为ωi、ωs,若ωp1=ωp2,则ωs≠ωi,且满足ωs+ωi=2×ωp1=2×ωp2;若ωp1≠ωp2,则ωs=ωi,且满足ωp1+ωp2=2×ωs=2×ωi。本申请中的纠缠光子对产生装置即可适用于基于非简并自发四波混频效应的时间纠缠光子对产生原理,又适用于基于简并自发四波混频效应的时间纠缠光子对产生原理。In the embodiment of the present application, the frequencies of the two pump photons are respectively ωp1 and ωp2, and the frequencies of the first photon and the second photon are respectively ωi and ωs, and if ωp1=ωp2, ωs≠ωi, And ωs+ωi=2×ωp1=2×ωp2 is satisfied; if ωp1≠ωp2, ωs=ωi, and ωp1+ωp2=2×ωs=2×ωi is satisfied. The entangled photon pair generating device in the present application can be applied to the principle of time entangled photon pair generation based on non-degenerate spontaneous four-wave mixing effect, and is applicable to the principle of time entangled photon pair generation based on degenerate spontaneous four-wave mixing effect. .
可选的,本申请实施例中,所述泵浦光源可以设置于所述衬底上。本申请中,将泵浦光源和多个波导结构集成在衬底上,例如,衬底是SOI衬底时,因SOI衬底的厚度在微米级,尺寸在毫米级,使得纠缠光子对产生装置的尺寸小型化。此外,多个波导结构是对沉积在衬底上的波导材质刻蚀后形成的,纠缠光子对产生装置可以直接在SOI衬底上通过CMOS工艺形成,能够量化生产小型器件,有利于降低成本。Optionally, in the embodiment of the present application, the pump light source may be disposed on the substrate. In the present application, a pump light source and a plurality of waveguide structures are integrated on a substrate. For example, when the substrate is an SOI substrate, since the thickness of the SOI substrate is on the order of micrometers and the size is on the order of millimeters, the entangled photon pair generating device is used. The size is miniaturized. In addition, the plurality of waveguide structures are formed by etching the waveguide material deposited on the substrate, and the entangled photon pair generating device can be formed directly on the SOI substrate by a CMOS process, which can quantify the production of small devices and is advantageous for cost reduction.
进一步的,所述泵浦光源为粘合在所述衬底上的III-V族激光二极管或垂直腔面发射激光器阵列VCSEL,或者所述泵浦光源为外延生长在所述衬底上的Ge激光二极管。Further, the pumping source is a III-V laser diode or a vertical cavity surface emitting laser array VCSEL bonded to the substrate, or the pumping source is a Ge epitaxially grown on the substrate Laser diode.
本申请中,对于泵浦光源来说,无论是选择III-V族激光二极管,还是选择垂直腔面发射激光器阵列VCSEL,其尺寸都能保证在微米级,可采用贴片工艺将泵浦光源集成在衬底上,实现泵浦光源和多个波导结构在衬底上的集成,有利于缩小纠缠光子对产生装置的体积。若选择直接在衬底上外延生长Ge激光二极管,纠缠光子对产生装置的厚度和长宽尺寸更加可控,能够实现纠缠光子对产生装置的小型化。In the present application, for the pump light source, whether the III-V laser diode or the vertical cavity surface emitting laser array VCSEL is selected, the size can be guaranteed in the micrometer level, and the pumping light source can be integrated by the patch process. On the substrate, integration of the pumping source and the plurality of waveguide structures on the substrate is achieved, which is advantageous for reducing the volume of the entangled photon pair generating device. If the Ge laser diode is epitaxially grown directly on the substrate, the entangled photons are more controllable to the thickness and length and width of the generating device, and the miniaturization of the entangled photon pair generating device can be realized.
可选的,所述装置还包括载体,所述衬底和泵浦光源设置于所述载体上。Optionally, the device further includes a carrier, and the substrate and the pumping light source are disposed on the carrier.
本申请中,将泵浦光源和衬底集成在载体上,衬底上集成多个波导结构,有利于纠缠光子对产生装置的尺寸小型化,例如,衬底是SOI衬底时,因SOI衬底的厚度在微米级,使得纠缠光子对产生装置的尺寸为微米级。此外,多个波导结构是对沉积在衬底上的波导材质刻蚀后形成的,纠缠光子对产生装置可以直接在SOI衬底上通过半导体工艺形成,能够量化生产小型器件,有利于降低成本。In the present application, the pump light source and the substrate are integrated on the carrier, and a plurality of waveguide structures are integrated on the substrate, which is advantageous for miniaturizing the size of the entangled photon pair generating device, for example, when the substrate is an SOI substrate, due to the SOI lining The thickness of the bottom is on the order of microns such that the dimensions of the entangled photon pair generating device are on the order of microns. In addition, the plurality of waveguide structures are formed by etching the waveguide material deposited on the substrate, and the entangled photon pair generating device can be formed directly on the SOI substrate by a semiconductor process, which can quantify the production of small devices and is advantageous in reducing cost.
进一步的,所述泵浦光源为粘合在所述载体上的III-V族激光二极管或垂直腔面发射激光器阵列VCSEL。Further, the pumping source is a III-V laser diode or a vertical cavity surface emitting laser array VCSEL bonded to the carrier.
本申请中,对于泵浦光源来说,无论是选择III-V族激光二极管,还是选择垂直腔面发射激光器阵列VCSEL,其尺寸都能保证在微米级,可采用贴片工艺将泵浦光源集成在载体上,实现泵浦光源和衬底上的多个波导结构的片上集成,有利于缩小纠缠光子对产生装置的体积。 In the present application, for the pump light source, whether the III-V laser diode or the vertical cavity surface emitting laser array VCSEL is selected, the size can be guaranteed in the micrometer level, and the pumping light source can be integrated by the patch process. On the carrier, on-chip integration of the pump source and the plurality of waveguide structures on the substrate is achieved, which is advantageous for reducing the volume of the entangled photon pair generating device.
进一步的,所述装置还包括第七波导结构,所述第七波导结构位于所述载体和/或所述衬底上,所述泵浦光源通过所述第七波导结构与所述第一波导结构连通。Further, the device further includes a seventh waveguide structure, the seventh waveguide structure is located on the carrier and/or the substrate, and the pump light source passes through the seventh waveguide structure and the first waveguide Structural connectivity.
本申请中,通过第七波导结构将载体上的泵浦光源与衬底上的第一波导结构连通,使得载体上的泵浦光源与衬底上的多个波导结构的位置关系灵活,例如,载体上的泵浦光源与衬底上的多个波导结构的位置关系可以为呈一字型横向设置;例如,载体上的泵浦光源与衬底上的多个波导结构的位置关系可以为并排设置,此时,可以进一步的缩小载体的横向尺寸。In the present application, the pumping source on the carrier is connected to the first waveguide structure on the substrate through the seventh waveguide structure, so that the positional relationship between the pumping source on the carrier and the plurality of waveguide structures on the substrate is flexible, for example, The positional relationship between the pump source on the carrier and the plurality of waveguide structures on the substrate may be in a horizontal arrangement; for example, the positional relationship between the pump source on the carrier and the plurality of waveguide structures on the substrate may be side by side In this case, the lateral dimension of the carrier can be further reduced.
附图说明DRAWINGS
图1为本申请实施例提供的时间脉冲叠加态和时间纠缠光子对的产生原理示意图;1 is a schematic diagram of a principle of generating a time pulse superposition state and a time entangled photon pair according to an embodiment of the present application;
图2为本申请实施例提供的一种简并自发四波混频效应和非简并自发四波混频效应的原理示意图;2 is a schematic diagram of a schematic diagram of a degenerate spontaneous four-wave mixing effect and a non-degenerate spontaneous four-wave mixing effect according to an embodiment of the present application;
图3为本申请实施例提供的一种纠缠光子对产生装置的原理示意图;3 is a schematic diagram of a principle of an entangled photon pair generating device according to an embodiment of the present application;
图4为本申请实施例提供的第一种纠缠光子对产生装置的剖面结构示意图;4 is a schematic cross-sectional structural view of a first entangled photon pair generating device according to an embodiment of the present application;
图5为本申请实施例提供的第一种纠缠光子对产生装置的俯视结构示意图;5 is a schematic top plan view of a first entangled photon pair generating device according to an embodiment of the present application;
图6为本申请实施例提供的第二种纠缠光子对产生装置的剖面结构示意图;6 is a schematic cross-sectional structural view of a second entangled photon pair generating device according to an embodiment of the present application;
图7为本申请实施例提供的第二种纠缠光子对产生装置的剖面结构示意图;7 is a schematic cross-sectional structural view of a second entangled photon pair generating device according to an embodiment of the present application;
图8为本申请实施例提供的第二种纠缠光子对产生装置的剖面结构示意图;8 is a schematic cross-sectional structural view of a second entangled photon pair generating device according to an embodiment of the present application;
图9为本申请实施例提供的第二种纠缠光子对产生装置的俯视结构示意图;9 is a schematic top plan view of a second entangled photon pair generating device according to an embodiment of the present application;
图10为本申请实施例提供的第二种纠缠光子对产生装置的俯视结构示意图。FIG. 10 is a schematic top plan view of a second entangled photon pair generating device according to an embodiment of the present application.
具体实施方式Detailed ways
下面将结合附图对本申请实施例作进一步地详细描述。The embodiments of the present application will be further described in detail below with reference to the accompanying drawings.
对泵浦光进行时间分光的原理为:单个光子经过一个不等臂MZ干涉仪会产生单个光子的时间叠加态。例如,如图1(a)所示,单个光子在经过不等臂MZ干涉仪的第一个50:50的光纤分束器后,有一半的几率通过长臂、一半的几率通过短臂。单个泵浦脉冲经过第一个光纤分束器后形成早脉冲和晚脉冲,再经过第二个光纤分束器的合束后形成早脉冲和晚脉冲的叠加态。The principle of time splitting the pump light is that a single photon passes through an unequal arm MZ interferometer to produce a time superposition of individual photons. For example, as shown in Figure 1(a), after passing through the first 50:50 fiber splitter of the unequal arm MZ interferometer, a single photon has a half chance of passing the short arm through the long arm and half the probability. A single pump pulse forms an early pulse and a late pulse after passing through the first fiber splitter, and then merges with the second fiber splitter to form a superposition of the early pulse and the late pulse.
通常采用的一种产生时间纠缠光子对的原理是:将进行时间分光后的泵浦光激发非线性材料从而产生时间纠缠光子对。如图1(b)所示,单个泵浦脉冲经过相同的不等臂MZ干涉仪后,泵浦非线性材料,如BBO、PPLN等材料,在此过程中,有相同的概率在早脉冲或在晚脉冲中形成时间纠缠的两个关联光子,而在早脉冲和晚脉冲中同时产生两个关联光子的概率几乎为0,可忽略。受这种原理的限制,各个功能器件都是独立的器件,且各个功能器件的制作方法存在较大差异,所以这些功能器件无法实现片上集成,导致整个器件尺寸无法缩小。A commonly used principle for generating temporally entangled photon pairs is to pump time-split pump light to excite nonlinear materials to produce temporally entangled photon pairs. As shown in Figure 1(b), after a single pump pulse passes through the same unequal-arm MZ interferometer, pumps nonlinear materials such as BBO, PPLN, etc., in the process, with the same probability in early pulses or Two correlated photons entangled in time are formed in the late pulse, and the probability of simultaneously generating two associated photons in the early pulse and the late pulse is almost zero, which can be ignored. Limited by this principle, each functional device is a separate device, and the manufacturing methods of each functional device are quite different, so these functional devices cannot achieve on-chip integration, and the entire device size cannot be reduced.
本申请采用的产生时间纠缠光子对的原理为:令进行时间分光后的泵浦光,在受硅基材质(如硅、氮化硅、二氧化硅等材料)的波导结构的三阶非线性效应的影响下,将早脉冲泵浦光泵的泵浦光子转换为时间纠缠的关联光子对,或者将晚脉冲泵浦光泵的泵浦光子转换为时间纠缠的关联光子对。The principle of generating a time entangled photon pair used in the present application is: a third-order nonlinearity of a waveguide structure subjected to time-division, in a waveguide structure of a silicon-based material (such as silicon, silicon nitride, silicon dioxide, etc.) Under the influence of the effect, the pump photons of the early pulse pump optical pump are converted into time-entangled correlated photon pairs, or the pump photons of the late pulse pump optical pump are converted into time-entangled correlated photon pairs.
其中,硅基材质的波导结构的硅线三阶非线性效应(spontaneous four-wave-mixing, SFWM),也称自发四波混频效应。自发四波混频包括非简并发四波混频和简并发四波混频。Among them, the silicon-based waveguide structure has a three-order nonlinear effect (spontaneous four-wave-mixing, SFWM), also known as spontaneous four-wave mixing effect. Spontaneous four-wave mixing includes non-degenerate four-wave mixing and degenerate four-wave mixing.
非简并自发四波混频的原理为:参见图2(a),若转化前的两个泵浦光子的频率相同(用ωp表示),则这两个泵浦光子受硅基波导的硅线三阶非线性效应影响,能够转换为两个频率不同的关联光子(分别用ωs和ωi表示),并且这两个关联光子满足:2ωp=ωsiThe principle of non-degenerate spontaneous four-wave mixing is: see Figure 2(a), if the two pump photons before the conversion have the same frequency (indicated by ω p ), then the two pump photons are subjected to the silicon-based waveguide. The third-order nonlinear effect of the silicon line can be converted into two correlated photons with different frequencies (represented by ω s and ω i , respectively), and the two associated photons satisfy: 2ω p = ω s + ω i .
简并自发四波混频的原理为:参见图2(b),若转化前的两个泵浦光子的频率不同(分别用ωp1和ωp2表示),则这两个泵浦光子受硅基波导的硅线三阶非线性效应影响,能够转换为两个频率相同的关联光子(用ωs,i表示),并且这两个关联光子满足:ωp1p2=2ωs,iThe principle of degenerate spontaneous four-wave mixing is as follows: See Figure 2(b). If the two pump photons before the conversion have different frequencies (represented by ω p1 and ω p2 respectively), the two pump photons are subjected to silicon. The third-order nonlinear effect of the silicon waveguide of the fundamental waveguide can be converted into two associated photons of the same frequency (represented by ω s, i ), and the two associated photons satisfy: ω p1p2 =2ω s,i .
本申请提供的一种时间纠缠光子对产生装置,既适用于非简并自发四波混频,也适用于简并自发四波混频。The present invention provides a time entangled photon pair generating device suitable for both non-degenerate spontaneous four-wave mixing and degenerate spontaneous four-wave mixing.
基于上述原理,本申请提供一种纠缠光子对产生装置,包括泵浦光源和多个波导结构,泵浦光源和多个波导结构集成在同一衬底表面,多个波导结构提供了形成时间纠缠的光子对的产生光路和输出光路。如图3所示,衬底为SOI衬底,泵浦光源和多个波导结构设置于SOI衬底上的同一表面,其中,泵浦光源提供泵浦光,多个波导结构相互连通,并能提供泵浦光的分光光路、缠光子对产生光路,以及纠缠光子对的传输光路。该纠缠光子对产生装置产生纠缠光子对的过程为:泵浦光源产生泵浦光之后,波导结构提供的分光光路对泵浦光进行时间分光,纠缠光子对产生光路激发自发四波混频效应,将泵浦光转化成纠缠光子对,纠缠光子对的传输光路对纠缠光子对中关联光子进行滤波和分束后分别耦合进衬底外的单模光纤中。Based on the above principle, the present application provides an entangled photon pair generating device including a pumping light source and a plurality of waveguide structures. The pumping source and the plurality of waveguide structures are integrated on the same substrate surface, and the plurality of waveguide structures provide time entanglement. The photon pair produces an optical path and an output optical path. As shown in FIG. 3, the substrate is an SOI substrate, and the pump light source and the plurality of waveguide structures are disposed on the same surface on the SOI substrate, wherein the pump light source provides pump light, and the plurality of waveguide structures are connected to each other and can A beam splitting path for pumping light, a pair of photons to generate an optical path, and a transmission path for entanglement of photon pairs. The process of generating an entangled photon pair by the entangled photon generation device is: after the pump light source generates the pump light, the spectroscopic optical path provided by the waveguide structure performs time splitting on the pump light, and the entangled photon pair generates an optical path to excite the spontaneous four-wave mixing effect. The pump light is converted into an entangled photon pair, and the transmitted optical path of the entangled photon pair filters and splits the associated photons in the entangled photon pair and is respectively coupled into the single mode fiber outside the substrate.
需要说明的是,本申请中的泵浦光源,能够产生一个通信波段的泵浦光,泵浦光为单色泵浦光脉冲或者两种不同波长的重叠泵浦脉冲。It should be noted that the pumping light source in the present application is capable of generating pump light of a communication band, which is a monochromatic pumping light pulse or an overlapping pump pulse of two different wavelengths.
需要说明的是,本申请中的多个波导结构为硅基材质的波导结构,如硅,氮化硅或者是二氧化硅材质的波导结构,以便在SOI衬底上产生自发四波混频效应,但不限于这三种,其他材质的具有上述功能的波导结构也在本申请的保护范围之内。此外,波导结构可以通过SOI衬底上的波导材质刻蚀而成,工艺上能够与CMOS工艺兼容。It should be noted that the plurality of waveguide structures in the present application are silicon-based waveguide structures, such as silicon, silicon nitride or silicon dioxide waveguide structures, to generate spontaneous four-wave mixing effects on the SOI substrate. However, it is not limited to these three types, and waveguide structures having the above functions of other materials are also within the scope of the present application. In addition, the waveguide structure can be etched through the waveguide material on the SOI substrate, and the process can be compatible with the CMOS process.
需要说明的是,本申请中的SOI衬底是一种硅基的衬底,可通过离子注入或晶圆键合等方式获得硅-绝缘体-硅结构的SOI衬底。It should be noted that the SOI substrate in the present application is a silicon-based substrate, and a silicon-insulator-silicon structure SOI substrate can be obtained by ion implantation or wafer bonding.
本申请将多个波导结构和泵浦光源制作在SOI衬底表面,因SOI衬底的厚度在微米级,使得纠缠光子对产生装置的尺寸小型化,而且具有上述功能的多个波导结构可以通过SOI衬底上的波导材质刻蚀而成,此工艺可以与CMOS工艺兼容,因此,纠缠光子对产生装置可以直接在SOI衬底上通过半导体工艺形成,能够量化生产,有利于降低成本。The present application fabricates a plurality of waveguide structures and a pumping light source on the surface of the SOI substrate. Since the thickness of the SOI substrate is on the order of micrometers, the size of the entangled photon pair generating device is miniaturized, and a plurality of waveguide structures having the above functions can pass The waveguide material on the SOI substrate is etched, and the process can be compatible with the CMOS process. Therefore, the entangled photon pair generating device can be formed directly on the SOI substrate by a semiconductor process, which can quantify the production and contribute to cost reduction.
基于上述发明构思,下面结合具体的实施例说明本申请实施例提供的纠缠光子对产生装置。本申请提供的一种纠缠光子对产生装置,如图4所示,包括衬底100,位于衬底100上的波导结构200和泵浦光源300,波导结构200包括:第一波导结构201,第二波导结构202,第三波导结构203,第四波导结构204,第五波导结构205,第六波导结构206。Based on the above inventive concept, an entangled photon pair generating device provided by an embodiment of the present application will be described below with reference to specific embodiments. An entangled photon pair generating device provided by the present application, as shown in FIG. 4, includes a substrate 100, a waveguide structure 200 on the substrate 100, and a pumping light source 300. The waveguide structure 200 includes: a first waveguide structure 201, The second waveguide structure 202, the third waveguide structure 203, the fourth waveguide structure 204, the fifth waveguide structure 205, and the sixth waveguide structure 206.
其中衬底100可以但不限于为SOI衬底。The substrate 100 may be, but not limited to, an SOI substrate.
上述第一波导结构201,第二波导结构202,第三波导结构203,第四波导结构204,第五波导结构205,第六波导结构206均是通过对沉积在衬底100上的波导材质刻蚀后形成的,此刻蚀工艺可以与CMOS工艺兼容,因此,纠缠光子对产生装置可以直接在衬底100上通过半导体工艺形成,能够量化生产,有利于降低成本。可选的,衬底100上的波导材 质可以但不限于为硅或氮化硅。The first waveguide structure 201, the second waveguide structure 202, the third waveguide structure 203, the fourth waveguide structure 204, the fifth waveguide structure 205, and the sixth waveguide structure 206 are all engraved by the waveguide material deposited on the substrate 100. After the etching, the etching process can be compatible with the CMOS process. Therefore, the entangled photon pair generating device can be formed directly on the substrate 100 by a semiconductor process, which can quantify the production and contribute to cost reduction. Optionally, the waveguide material on the substrate 100 The quality can be, but is not limited to, silicon or silicon nitride.
下面以衬底100为SOI衬底为例,结合图5对第一波导结构201,第二波导结构202,第三波导结构203,第四波导结构204,第五波导结构205,第六波导结构206之间的位置关系、结构特征和功能进行详细说明。Taking the substrate 100 as an SOI substrate as an example, the first waveguide structure 201, the second waveguide structure 202, the third waveguide structure 203, the fourth waveguide structure 204, the fifth waveguide structure 205, and the sixth waveguide structure are combined with FIG. The positional relationship, structural features and functions between 206 are described in detail.
在图5中,SOI衬底上的泵浦光源300、第一波导结构201,第三波导结构203,第二波导结构202,第四波导结构204,第五波导结构205,第六波导结构206(图8未示出)沿一字型横向设置。In FIG. 5, a pumping source 300, a first waveguide structure 201, a third waveguide structure 203, a second waveguide structure 202, a fourth waveguide structure 204, a fifth waveguide structure 205, and a sixth waveguide structure 206 on an SOI substrate. (not shown in Fig. 8) is arranged laterally along the inline shape.
泵浦光源300,设置在SOI衬底的边缘,且靠近第一波导结构201设置,用于向第一波导结构201发射泵浦光。可选的,泵浦光源300为粘合在SOI衬底上的III-V族激光二极管或垂直腔面发射激光器阵列VCSEL。可选的,泵浦光源300为外延生长在SOI衬底上的Ge激光二极管。泵浦光源300粘合在或直接生长在SOI衬底上,都可以保证SOI衬底上制作的纠缠光子对产生装置的尺寸在毫米级。The pumping light source 300 is disposed at an edge of the SOI substrate and disposed adjacent to the first waveguide structure 201 for emitting pump light to the first waveguide structure 201. Optionally, the pumping source 300 is a III-V laser diode or a vertical cavity surface emitting laser array VCSEL bonded to an SOI substrate. Optionally, the pump light source 300 is a Ge laser diode epitaxially grown on the SOI substrate. The pumping source 300 is bonded or directly grown on the SOI substrate to ensure that the size of the entangled photon generation device fabricated on the SOI substrate is on the order of millimeters.
第一波导结构201,直接与泵浦光源300连通,用于对泵浦光进行时间分光后交替输出第一泵浦光脉冲和第二泵浦光脉冲。第一波导结构201提供两条不同长度的光路,两条光路分别在第一波导结构201的输入端、输出端汇合,第一波导结构201不等长度的光路,可将第一波导结构201的输入端输入的泵浦光进行时间分光,以便交替输出第一泵浦光脉冲和第二泵浦光脉冲,第一泵浦光脉冲为较早输出的泵浦光脉冲,第二泵浦光脉冲为较晚输出的泵浦光脉冲。第一波导结构201的输出端通过具有滤波作用的第三波导结构203与第二波导结构202的输入端连通。The first waveguide structure 201 is directly connected to the pumping light source 300 for alternately outputting the first pumping light pulse and the second pumping light pulse after time-splitting the pumping light. The first waveguide structure 201 provides two optical paths of different lengths. The two optical paths respectively meet at the input end and the output end of the first waveguide structure 201, and the first waveguide structure 201 has an optical path of unequal length, and the first waveguide structure 201 can be The pump light input at the input end is time-divided to alternately output the first pump light pulse and the second pump light pulse, the first pump light pulse is an earlier output pump light pulse, and the second pump light pulse It is a pump light pulse that is output later. The output of the first waveguide structure 201 is in communication with the input of the second waveguide structure 202 via a third waveguide structure 203 having a filtering effect.
第三波导结构203,位于第一波导结构201和第二波导结构202之间,第三波导结构203用于滤除第一泵浦光脉冲或第二泵浦光脉冲中的第三光子,第三光子的频率与纠缠光子对转化前的两个泵浦光子的频率不同。第三波导结构203的形状设计为一个光学滤波器的形状,如带阻滤波器的形状,其作用是在交替输出的第一泵浦光脉冲和第二泵浦光脉冲进入第二波导结构202之前,将与第一泵浦光脉冲或第二泵浦光脉冲中的泵浦光频率不同的噪声光子滤除,即若第一泵浦光脉冲或第二泵浦光脉冲中的两个泵浦光子的频率分别为ωp1、ωp2,则第三波导结构203将第一波导结构201输出的与ωp1、ωp2不同的噪声光子去除。这是因为第一泵浦光脉冲或第二泵浦光脉冲的泵浦光在第一波导结构201中也有一定概率发生四波混频效应或者拉曼效应,从而产生一些其他频率的光子,这些光子对于纠缠光子来说是噪声,因此在产生纠缠光子之前要把这些光子滤掉。The third waveguide structure 203 is located between the first waveguide structure 201 and the second waveguide structure 202, and the third waveguide structure 203 is configured to filter out the third photon in the first pump light pulse or the second pump light pulse. The frequency of the three photons is different from the frequency of the two pump photons before the conversion of the entangled photons. The shape of the third waveguide structure 203 is designed to be in the shape of an optical filter, such as the shape of a band rejection filter, which functions to alternately output the first pump light pulse and the second pump light pulse into the second waveguide structure 202. Previously, noise photons of different frequency from the pump light in the first pump light pulse or the second pump light pulse are filtered out, that is, if two pumps in the first pump light pulse or the second pump light pulse The frequencies of the neutrons are ωp1 and ωp2, respectively, and the third waveguide structure 203 removes noise photons different from ωp1 and ωp2 output from the first waveguide structure 201. This is because the pump light of the first pump light pulse or the second pump light pulse also has a certain probability of generating a four-wave mixing effect or a Raman effect in the first waveguide structure 201, thereby generating photons of other frequencies. Photons are noisy for entangled photons, so they are filtered out before entangled photons are generated.
第二波导结构202,位于第三波导结构的输出端,其结构特征呈螺旋状,其作用是可以提供尽可能长的光路,使交替输出的第一泵浦光脉冲和第二泵浦光脉冲在通过第二波导结构202的过程中,有足够的时间分别以一定概率p在该光路中受自发四波混频效应的影响产生纠缠光子对。具体的产生过程是将第一泵浦光脉冲中的两个泵浦光子转化为纠缠光子对,或者将第二泵浦光脉冲中的两个泵浦光子转化为纠缠光子对,产生的纠缠光子对包括关联的第一光子和第二光子。The second waveguide structure 202 is located at the output end of the third waveguide structure and has a spiral structure. The function of the second waveguide structure 202 is to provide an optical path that is as long as possible, so that the first pump light pulse and the second pump light pulse are alternately output. In the process of passing through the second waveguide structure 202, there is sufficient time to generate an entangled photon pair by a certain probability p in the optical path by the effect of the spontaneous four-wave mixing effect. The specific generation process is to convert two pump photons in the first pump light pulse into entangled photon pairs, or convert two pump photons in the second pump light pulse into entangled photon pairs, and generate entangled photons. The pair includes the associated first photon and second photon.
需要说明的是,在第一泵浦光脉冲和第二泵浦光脉冲中同时产生纠缠光子对的概率可以忽略不计,这是由于第一泵浦光脉冲和第二泵浦光脉冲同时产生纠缠光子对的概率为p2,是一个极小值,因此,可以认为在第一泵浦光脉冲中产生纠缠光子对的情况下,第二泵浦光脉冲中就不会产生纠缠光子对,反之亦然。It should be noted that the probability of simultaneously generating entangled photon pairs in the first pump light pulse and the second pump light pulse is negligible, because the first pump light pulse and the second pump light pulse simultaneously generate entanglement. The probability of a photon pair is p 2 , which is a minimum value. Therefore, it can be considered that in the case where an entangled photon pair is generated in the first pump light pulse, no entangled photon pair is generated in the second pump light pulse, and vice versa. Also.
其中,产生的纠缠光子对的纠缠态可以用
Figure PCTCN2017089537-appb-000002
表示,其中,e表示在 较早的第一泵浦光脉冲位置中探测到纠缠光子对,l表示在较晚的第二泵浦光脉冲中探测到纠缠光子对。
Wherein, the entangled state of the generated entangled photon pair can be used
Figure PCTCN2017089537-appb-000002
Represented where e indicates that an entangled photon pair was detected in an earlier first pump light pulse position and l indicates that an entangled photon pair was detected in a later second pump light pulse.
其中,转化前的两个泵浦光子与转换后的纠缠光子对的频率关系为:定义两个泵浦光子的频率分别为ωp1、ωp2,第一光子和第二光子的频率分别为ωi、ωs,那么如果按照非简并自发四波混频原理产生纠缠光子对,则ωp1=ωp2,ωs≠ωi,且满足ωs+ωi=2×ωp1=2×ωp2;如果按照简并自发四波混频原理产生纠缠光子对,则ωp1≠ωp2,ωs=ωi,且满足ωp1+ωp2=2×ωs=2×ωi。Wherein, the frequency relationship between the two pump photons before conversion and the converted entangled photon pair is: the frequencies defining the two pump photons are respectively ωp1, ωp2, and the frequencies of the first photon and the second photon are respectively ωi, ωs Then, if an entangled photon pair is generated according to the non-degenerate spontaneous four-wave mixing principle, then ωp1=ωp2, ωs≠ωi, and satisfy ωs+ωi=2×ωp1=2×ωp2; if the four-wave mixing is performed according to degenerate spontaneous The principle produces an entangled photon pair, then ωp1 ≠ ωp2, ωs = ωi, and satisfies ωp1 + ωp2 = 2 × ωs = 2 × ωi.
此外,第二波导结构202的输出端通过第四波导结构204与第五波导结构205的输入端连通。Furthermore, the output of the second waveguide structure 202 is in communication with the input of the fifth waveguide structure 205 through the fourth waveguide structure 204.
第四波导结构204,位于第二波导结构202和第五波导结构205之间,其结构特征类似一个光学滤波器,其作用是在纠缠光子对进入第五波导结构205之前,将从第二波导结构202的输出端输出的掺杂在纠缠光子对中的噪声光子滤除,其中,这些噪声光子是指在纠缠光子对产生过程中产生的与第一光子、第二光子的频率不同的光子。The fourth waveguide structure 204 is located between the second waveguide structure 202 and the fifth waveguide structure 205 and has a structural feature similar to an optical filter, and functions to pass the second waveguide after the entangled photon pair enters the fifth waveguide structure 205. The doping of the output of the structure 202 is filtered out of noise photons in the entangled photon pair, wherein the noise photons are photons that are different in frequency from the first photon and the second photon generated during the generation of the entangled photon pair.
第五波导结构205,位于第四波导结构204的输出端,其结构特征类似一个分束器,其作用是第四波导结构204输出的纠缠光子对中的第一光子、第二光子分离,按照第五波导结构205的光路将第一光子和第二光子分离。其中,第五波导结构205的输出端包括第一输出端和第二输出端,第五波导结构205的第一输出端输出第一光子,第五波导结构205的第二输出端输出第二光子。The fifth waveguide structure 205 is located at the output end of the fourth waveguide structure 204, and has a structural feature similar to a beam splitter, and functions as the first photon and the second photon in the entangled photon pair outputted by the fourth waveguide structure 204, according to The optical path of the fifth waveguide structure 205 separates the first photon from the second photon. The output end of the fifth waveguide structure 205 includes a first output end and a second output end. The first output end of the fifth waveguide structure 205 outputs a first photon, and the second output end of the fifth waveguide structure 205 outputs a second photon. .
第六波导结构206,位于第五波导结构205的输出端,其结构特征类似一个耦合器,用于将第五波导结构205的第一输出端输出的第一光子耦合进第一单模光纤内,将第五波导结构205的第二输出端输出的第二光子耦合进第二单模光纤内,第一单模光纤、第二单模光纤设置在衬底100外部。The sixth waveguide structure 206 is located at the output end of the fifth waveguide structure 205 and has a structural feature similar to a coupler for coupling the first photon outputted from the first output end of the fifth waveguide structure 205 into the first single mode fiber. The second photon outputted from the second output end of the fifth waveguide structure 205 is coupled into the second single mode fiber, and the first single mode fiber and the second single mode fiber are disposed outside the substrate 100.
本申请提供的上述纠缠光子对产生装置中,泵浦光源300、具有分光作用的第一波导结构201,具有滤光作用的第三波导结构203,具有激发自发四波混频效应产生纠缠光子对的第二波导结构202、具有滤光作用的第四波导结构204,具有分束作用的第五波导结构205,具有耦合作用的第六波导结构206可以集成在SOI衬底上,因SOI衬底的厚度在微米级,尺寸在毫米级,使得纠缠光子对产生装置的尺寸小型化,而且上述第一波导结构201,第二波导结构202,第三波导结构203,第四波导结构204,第五波导结构205,第六波导结构206均是对沉积在SOI衬底上的波导材质刻蚀后形成的,此刻蚀工艺可以与CMOS工艺兼容,因此,纠缠光子对产生装置可以直接在SOI衬底上通过半导体工艺形成,能够量化生产,有利于降低成本。In the above entangled photon pair generating device provided by the present application, the pumping light source 300, the first waveguide structure 201 having a spectroscopic effect, and the third waveguide structure 203 having a filtering effect have an exciting four-wave mixing effect to generate an entangled photon pair. a second waveguide structure 202, a fourth waveguide structure 204 having a filtering effect, a fifth waveguide structure 205 having a splitting effect, and a sixth waveguide structure 206 having a coupling function may be integrated on the SOI substrate due to the SOI substrate The thickness is on the order of micrometers, and the size is on the order of millimeters, so that the size of the entangled photon pair generating device is miniaturized, and the first waveguide structure 201, the second waveguide structure 202, the third waveguide structure 203, the fourth waveguide structure 204, and the fifth The waveguide structure 205 and the sixth waveguide structure 206 are both formed by etching a waveguide material deposited on the SOI substrate. The etching process can be compatible with the CMOS process. Therefore, the entangled photon pair generating device can be directly on the SOI substrate. Through the formation of a semiconductor process, it is possible to quantify production and contribute to cost reduction.
基于相同的发明构思,本申请还提供一种纠缠光子对产生装置,如图6所示,包括:Based on the same inventive concept, the present application further provides an entangled photon pair generating device, as shown in FIG. 6, comprising:
包括衬底100,位于衬底100上的波导结构200和泵浦光源300,波导结构200包括:第一波导结构201,第二波导结构202,第三波导结构203,第四波导结构204,第五波导结构205,第六波导结构206,还包括载体400,衬底100和泵浦光源300设置于载体400上,还包括第七波导结构401,泵浦光源300通过第七波导结构401与第一波导结构201连通。The substrate 100 includes a waveguide structure 200 on the substrate 100 and a pumping source 300. The waveguide structure 200 includes a first waveguide structure 201, a second waveguide structure 202, a third waveguide structure 203, and a fourth waveguide structure 204. The fifth waveguide structure 205, the sixth waveguide structure 206, further includes a carrier 400, the substrate 100 and the pumping light source 300 are disposed on the carrier 400, and further includes a seventh waveguide structure 401, and the pumping light source 300 passes through the seventh waveguide structure 401 and A waveguide structure 201 is in communication.
上述第一波导结构201,第二波导结构202,第三波导结构203,第四波导结构204,第五波导结构205,第六波导结构206均是通过对沉积在衬底100上的波导材质刻蚀后形成的,此刻蚀工艺可以与CMOS工艺兼容,因此,纠缠光子对产生装置可以直接在SOI衬 底上通过半导体工艺形成,能够量化生产,有利于降低成本。可选的,衬底100上的波导材质为硅或氮化硅,以便产生自发四波混频效应。The first waveguide structure 201, the second waveguide structure 202, the third waveguide structure 203, the fourth waveguide structure 204, the fifth waveguide structure 205, and the sixth waveguide structure 206 are all engraved by the waveguide material deposited on the substrate 100. After the etch, the etch process can be compatible with the CMOS process, so the entangled photon pair generating device can be directly in the SOI lining The bottom is formed by a semiconductor process, which can quantify production and help reduce costs. Alternatively, the waveguide material on the substrate 100 is made of silicon or silicon nitride to produce a spontaneous four-wave mixing effect.
可选的,衬底100为SOI衬底时,第一波导结构201,第二波导结构202,第三波导结构203,第四波导结构204,第五波导结构205、第六波导结构206在SOI衬底上的具体内容参见前述实施例,此处不再累述。Optionally, when the substrate 100 is an SOI substrate, the first waveguide structure 201, the second waveguide structure 202, the third waveguide structure 203, the fourth waveguide structure 204, the fifth waveguide structure 205, and the sixth waveguide structure 206 are in the SOI. The specific content on the substrate is as described in the foregoing embodiment, and will not be described here.
可选的,第七波导结构401位于衬底100上。参照图7,衬底100为SOI衬底,第七波导结构401设置在SOI衬底的边缘,载体上的泵浦光源300靠近第七波导结构401设置,泵浦光源300、第七波导结构401、第一波导结构201,第三波导结构203,第二波导结构202,第四波导结构204,第五波导结构205,第六波导结构206(图7未示出)沿一字型横向设置。第七波导结构401还与第一波导结构201,第二波导结构202,第三波导结构203,第四波导结构204,第五波导结构205,第六波导结构206一起制作,都是通过对SOI衬底上的波导材质进行刻蚀形成,波导材质为在SOI衬底上沉积的波导层。可选的,SOI衬底上的波导材质为硅,氮化硅或二氧化硅,以便使泵浦光在SOI衬底上的波导材质中产生自发四波混频效应,而且SOI衬底上的波导材质的刻蚀工艺与CMOS工艺兼容,有利于纠缠光子对产生装置的量化生产,降低成本。Optionally, the seventh waveguide structure 401 is located on the substrate 100. Referring to FIG. 7, the substrate 100 is an SOI substrate, and a seventh waveguide structure 401 is disposed at an edge of the SOI substrate. The pump light source 300 on the carrier is disposed adjacent to the seventh waveguide structure 401. The pump light source 300 and the seventh waveguide structure 401 are provided. The first waveguide structure 201, the third waveguide structure 203, the second waveguide structure 202, the fourth waveguide structure 204, the fifth waveguide structure 205, and the sixth waveguide structure 206 (not shown in FIG. 7) are disposed laterally along the inline shape. The seventh waveguide structure 401 is also fabricated together with the first waveguide structure 201, the second waveguide structure 202, the third waveguide structure 203, the fourth waveguide structure 204, the fifth waveguide structure 205, and the sixth waveguide structure 206, both of which pass through the SOI. The waveguide material on the substrate is etched, and the waveguide material is a waveguide layer deposited on the SOI substrate. Optionally, the waveguide material on the SOI substrate is silicon, silicon nitride or silicon dioxide to generate a spontaneous four-wave mixing effect of the pump light in the waveguide material on the SOI substrate, and on the SOI substrate The etching process of the waveguide material is compatible with the CMOS process, which is advantageous for the quantitative production of the entangled photon generation device and reduces the cost.
可选的,第七波导结构401位于载体400上。参照图8,衬底100为SOI衬底,第七波导结构401和泵浦光源300都设置在载体上,并且第七波导结构401、泵浦光源300与SOI衬底上的第一波导结构201,第三波导结构203,第二波导结构202,第四波导结构204,第五波导结构205,第六波导结构206(图8未示出)沿一字型横向设置。第七波导结构401靠近SOI衬底的边缘设置,与位于SOI衬底边缘的第一波导结构201连通。第七波导结构401是对载体上的波导材质刻蚀形成。载体上的波导材质可以与SOI衬底上的波导材质相同,也可以不同。可选的,载体上的波导材质为硅或氮化硅。Optionally, the seventh waveguide structure 401 is located on the carrier 400. Referring to FIG. 8, the substrate 100 is an SOI substrate, and the seventh waveguide structure 401 and the pump light source 300 are both disposed on a carrier, and the seventh waveguide structure 401, the pumping light source 300, and the first waveguide structure 201 on the SOI substrate. The third waveguide structure 203, the second waveguide structure 202, the fourth waveguide structure 204, the fifth waveguide structure 205, and the sixth waveguide structure 206 (not shown in FIG. 8) are disposed laterally along the inline shape. A seventh waveguide structure 401 is disposed adjacent the edge of the SOI substrate in communication with the first waveguide structure 201 at the edge of the SOI substrate. The seventh waveguide structure 401 is formed by etching a waveguide material on the carrier. The waveguide material on the carrier may be the same as or different from the waveguide material on the SOI substrate. Optionally, the waveguide material on the carrier is silicon or silicon nitride.
可选的,第七波导结构401的一部分位于载体400上,另一部分位于衬底100上。参见图9,衬底100为SOI衬底,泵浦光源300设置在载体上,第七波导结构401的一部分位于载体400上,另一部分位于SOI衬底上,第七波导结构401的光路分为前段光路和后段光路,前段光路位于载体400上,后段光路位于衬底100上。第七波导结构401、泵浦光源300与SOI衬底上的第一波导结构201,第三波导结构203,第二波导结构202,第四波导结构204,第五波导结构205,第六波导结构206(图8未示出)沿一字型横向设置。Optionally, a portion of the seventh waveguide structure 401 is located on the carrier 400 and another portion is located on the substrate 100. Referring to FIG. 9, the substrate 100 is an SOI substrate, the pumping source 300 is disposed on the carrier, a portion of the seventh waveguide structure 401 is located on the carrier 400, and another portion is located on the SOI substrate, and the optical path of the seventh waveguide structure 401 is divided. The front optical path and the rear optical path, the front optical path is located on the carrier 400, and the rear optical path is located on the substrate 100. a seventh waveguide structure 401, a pumping light source 300 and a first waveguide structure 201 on the SOI substrate, a third waveguide structure 203, a second waveguide structure 202, a fourth waveguide structure 204, a fifth waveguide structure 205, and a sixth waveguide structure 206 (not shown in Fig. 8) is disposed laterally along the inline shape.
可选的,为了减小芯片的横向尺寸,泵浦光源300与衬底100在载体400上并排设置。如图10所示,衬底100为SOI衬底,SOI衬底与泵浦光源300在载体上并排设置,用来连通泵浦光源300和第一波导结构201的第七波导结构401的形状为C形。SOI衬底上的第一波导结构201,第二波导结构202,第三波导结构203,第四波导结构204,第五波导结构205,第六波导结构206(图8未示出)沿一字型横向设置。Alternatively, in order to reduce the lateral dimension of the chip, the pumping source 300 and the substrate 100 are arranged side by side on the carrier 400. As shown in FIG. 10, the substrate 100 is an SOI substrate, and the SOI substrate and the pumping light source 300 are arranged side by side on the carrier, and the shape of the seventh waveguide structure 401 for connecting the pumping light source 300 and the first waveguide structure 201 is C shape. The first waveguide structure 201, the second waveguide structure 202, the third waveguide structure 203, the fourth waveguide structure 204, the fifth waveguide structure 205, and the sixth waveguide structure 206 (not shown in FIG. 8) on the SOI substrate are along a word Horizontal setting.
可选的,泵浦光源300为粘合在载体400上的III-V族激光二极管或垂直腔面发射激光器阵列VCSEL。可选的,载体的材质可以为二氧化硅或者聚合物。Optionally, the pump light source 300 is a III-V laser diode or a vertical cavity surface emitting laser array VCSEL bonded to the carrier 400. Alternatively, the material of the carrier may be silica or a polymer.
本申请提供的上述纠缠光子对产生装置中,泵浦光源300和SOI衬底都集成在载体的同一表面,并且SOI衬底上集成有具有分光作用的第一波导结构201,具有滤光作用的第三波导结构203,具有激发自发四波混频效应产生纠缠光子对的第二波导结构、具有滤光作用的第四波导结构204,具有分束作用的第五波导结构205,具有耦合作用的第六波导结构,SOI衬底的厚度在微米级,尺寸在毫米级,因此上述集成结构使得纠缠光子对产生 装置的尺寸小型化,而且上述第一波导结构201,第二波导结构202,第三波导结构203,第四波导结构204,第五波导结构205,第六波导结构206均是对沉积在SOI衬底上的波导材质刻蚀后形成的,此刻蚀工艺可以与CMOS工艺兼容,因此,纠缠光子对产生装置可以直接在SOI衬底上通过半导体工艺形成,能够量化生产,有利于降低成本。 In the above entangled photon pair generating device provided by the present application, the pumping light source 300 and the SOI substrate are integrated on the same surface of the carrier, and the first waveguide structure 201 having the light splitting effect is integrated on the SOI substrate, and has a filtering effect. The third waveguide structure 203 has a second waveguide structure for exciting an entangled photon pair to excite an spontaneous four-wave mixing effect, a fourth waveguide structure 204 having a filtering effect, and a fifth waveguide structure 205 having a splitting effect, having a coupling effect The sixth waveguide structure, the thickness of the SOI substrate is on the order of micrometers, and the size is on the order of millimeters, so the above integrated structure makes the entangled photon pair The size of the device is miniaturized, and the first waveguide structure 201, the second waveguide structure 202, the third waveguide structure 203, the fourth waveguide structure 204, the fifth waveguide structure 205, and the sixth waveguide structure 206 are all deposited on the SOI lining. After the waveguide material on the bottom is etched, the etching process can be compatible with the CMOS process. Therefore, the entangled photon pair generating device can be formed directly on the SOI substrate by a semiconductor process, which can quantify the production and is advantageous for cost reduction.

Claims (13)

  1. 一种纠缠光子对产生装置,其特征在于,包括衬底和泵浦光源,位于所述衬底上的第一波导结构和第二波导结构;An entangled photon pair generating device, comprising: a substrate and a pumping source, a first waveguide structure and a second waveguide structure on the substrate;
    其中,所述第一波导结构和所述第二波导结构是通过对所述衬底上的波导材质刻蚀后形成的,所述第一波导结构位于所述泵浦光源和所述第二波导结构之间;Wherein the first waveguide structure and the second waveguide structure are formed by etching a waveguide material on the substrate, the first waveguide structure being located at the pumping source and the second waveguide Between structures;
    所述泵浦光源,用于向所述第一波导结构发射泵浦光;The pumping light source for transmitting pump light to the first waveguide structure;
    所述第一波导结构,用于对所述泵浦光进行时间分光后交替输出第一泵浦光脉冲和第二泵浦光脉冲;The first waveguide structure is configured to alternately output the first pump light pulse and the second pump light pulse after performing time splitting on the pump light;
    所述第二波导结构,用于将所述第一泵浦光脉冲或所述第二泵浦光脉冲中的两个泵浦光子转化为纠缠光子对,所述纠缠光子对包括关联的第一光子和第二光子。The second waveguide structure is configured to convert two pump photons of the first pump light pulse or the second pump light pulse into an entangled photon pair, the entangled photon pair including an associated first Photons and second photons.
  2. 如权利要求1所述的纠缠光子对产生装置,其特征在于,还包括:位于所述衬底上的第三波导结构,所述第三波导结构是通过对所述波导材质刻蚀后形成的,所述第三波导结构位于所述第一波导结构和所述第二波导结构之间,用于滤除所述第一波导结构输出的与所述第一泵浦光脉冲、所述第二泵浦光脉冲中的泵浦光频率不同的噪声光子。The entangled photon pair generating apparatus according to claim 1, further comprising: a third waveguide structure on said substrate, said third waveguide structure being formed by etching said waveguide material The third waveguide structure is located between the first waveguide structure and the second waveguide structure for filtering out the first waveguide structure output and the first pump light pulse, the second The noise photons of different pump light frequencies in the pump light pulse.
  3. 如权利要求1所述的纠缠光子对产生装置,其特征在于,还包括:位于所述衬底上的第四波导结构,所述第四波导结构是通过对所述波导材质刻蚀后形成的,所述第四波导结构位于所述第二波导结构的输出端,用于滤除从所述第二波导结构的输出端输出的与所述第一光子、所述第二光子的频率不同的噪声光子。The entangled photon pair generating apparatus according to claim 1, further comprising: a fourth waveguide structure on said substrate, said fourth waveguide structure being formed by etching said waveguide material The fourth waveguide structure is located at an output end of the second waveguide structure, and is configured to filter out a frequency different from a frequency of the first photon and the second photon output from an output end of the second waveguide structure. Noise photons.
  4. 如权利要求3所述的纠缠光子对产生装置,其特征在于,还包括:位于所述衬底上的第五波导结构,所述第五波导结构是通过对所述波导材质刻蚀后形成的,所述第五波导结构位于所述第四波导结构的输出端,用于将从第四波导结构的输出端输出的所述第一光子、所述第二光子分离。The entangled photon pair generating apparatus according to claim 3, further comprising: a fifth waveguide structure on said substrate, said fifth waveguide structure being formed by etching said waveguide material The fifth waveguide structure is located at an output end of the fourth waveguide structure for separating the first photon and the second photon outputted from an output end of the fourth waveguide structure.
  5. 如权利要求4所述的纠缠光子对产生装置,其特征在于,还包括:位于所述衬底上的第六波导结构,所述第六波导结构是通过对所述波导材质刻蚀后形成的,所述第六波导结构位于所述第五波导结构的输出端,用于将所述第五波导结构的输出端输出的第一光子耦合进第一单模光纤内,将所述第二光子耦合进第二单模光纤内,所述第一单模光纤、所述第二单模光纤设置在所述衬底外部。The entangled photon pair generating device according to claim 4, further comprising: a sixth waveguide structure on the substrate, wherein the sixth waveguide structure is formed by etching the waveguide material The sixth waveguide structure is located at an output end of the fifth waveguide structure for coupling a first photon outputted from an output end of the fifth waveguide structure into the first single mode fiber, and the second photon is Coupled into the second single mode fiber, the first single mode fiber and the second single mode fiber are disposed outside of the substrate.
  6. 如权利要求1至5中任一项所述的纠缠光子对产生装置,其特征在于,所述衬底为SOI衬底。The entangled photon pair generating apparatus according to any one of claims 1 to 5, wherein the substrate is an SOI substrate.
  7. 如权利要求1至6中任一项所述的纠缠光子对产生装置,其特征在于,所述波导材质为硅或氮化硅。The entangled photon pair generating device according to any one of claims 1 to 6, wherein the waveguide material is silicon or silicon nitride.
  8. 如权利要求1至6中任一项所述的纠缠光子对产生装置,其特征在于,所述两个泵浦光子的频率分别为ωp1、ωp2,所述第一光子和所述第二光子的频率分别为ωi、ωs,The entangled photon pair generating device according to any one of claims 1 to 6, wherein the frequencies of the two pump photons are ωp1, ωp2, respectively, of the first photon and the second photon The frequencies are ωi, ωs, respectively.
    若ωp1=ωp2,则ωs≠ωi,且满足ωs+ωi=2×ωp1=2×ωp2;If ωp1=ωp2, then ωs≠ωi, and satisfy ωs+ωi=2×ωp1=2×ωp2;
    若ωp1≠ωp2,则ωs=ωi,且满足ωp1+ωp2=2×ωs=2×ωi。If ωp1 ≠ ωp2, ωs = ωi, and ωp1 + ωp2 = 2 × ωs = 2 × ωi is satisfied.
  9. 如权利要求1所述的纠缠光子对产生装置,其特征在于,所述泵浦光源设置于所述衬底上。The entangled photon pair generating apparatus according to claim 1, wherein said pumping light source is disposed on said substrate.
  10. 如权利要求9所述的纠缠光子对产生装置,其特征在于,所述泵浦光源为粘合在所述衬底上的III-V族激光二极管或垂直腔面发射激光器阵列VCSEL,或者所述泵浦光源 为外延生长在所述衬底上的Ge激光二极管。The entangled photon pair generating device according to claim 9, wherein said pumping source is a III-V laser diode or a vertical cavity surface emitting laser array VCSEL bonded to said substrate, or said Pump source A Ge laser diode for epitaxial growth on the substrate.
  11. 如权利要求1所述的纠缠光子对产生装置,其特征在于,所述装置还包括载体,所述衬底和泵浦光源设置于所述载体上。The entangled photon pair generating apparatus according to claim 1, wherein said apparatus further comprises a carrier, and said substrate and said pumping light source are disposed on said carrier.
  12. 如权利要求11所述的纠缠光子对产生装置,其特征在于,所述泵浦光源为粘合在所述载体上的III-V族激光二极管或垂直腔面发射激光器阵列VCSEL。The entangled photon pair generating apparatus according to claim 11, wherein said pumping source is a III-V laser diode or a vertical cavity surface emitting laser array VCSEL bonded to said carrier.
  13. 如权利要求12所述的纠缠光子对产生装置,其特征在于,所述装置还包括第七波导结构,所述第七波导结构位于所述载体和/或所述衬底上,所述泵浦光源通过所述第七波导结构与所述第一波导结构连通。 The entangled photon pair generating apparatus according to claim 12, wherein said apparatus further comprises a seventh waveguide structure, said seventh waveguide structure being located on said carrier and/or said substrate, said pump A light source is in communication with the first waveguide structure through the seventh waveguide structure.
PCT/CN2017/089537 2017-06-22 2017-06-22 Time-entangled photon pair generating device WO2018232689A1 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
PCT/CN2017/089537 WO2018232689A1 (en) 2017-06-22 2017-06-22 Time-entangled photon pair generating device
CN201780003258.9A CN109429509A (en) 2017-06-22 2017-06-22 A kind of time entangled photon pairs generation device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
PCT/CN2017/089537 WO2018232689A1 (en) 2017-06-22 2017-06-22 Time-entangled photon pair generating device

Publications (1)

Publication Number Publication Date
WO2018232689A1 true WO2018232689A1 (en) 2018-12-27

Family

ID=64735434

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/CN2017/089537 WO2018232689A1 (en) 2017-06-22 2017-06-22 Time-entangled photon pair generating device

Country Status (2)

Country Link
CN (1) CN109429509A (en)
WO (1) WO2018232689A1 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US11588613B1 (en) 2021-10-26 2023-02-21 Eagle Technology, Llc Systems and methods for synchronization of photons over quantum channels with co-propagating clock pulses

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111323986B (en) * 2019-12-18 2022-07-22 西南技术物理研究所 System for generating three-photon polarization entangled GHZ state based on Sagnac optical fiber loop
CN112946968B (en) * 2021-02-01 2022-01-07 电子科技大学 Hybrid integrated optical communication waveband on-chip quantum entanglement source

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101398590A (en) * 2008-11-06 2009-04-01 天津大学 All-optical frequency entangled photon source
WO2009093391A1 (en) * 2008-01-25 2009-07-30 Japan Science And Technology Agency Non-degenerate polarization-entangled photon pairs generation device and non-degenerate polarization-entangled photon pairs generation method
CN102130418A (en) * 2011-01-26 2011-07-20 清华大学 Polarization-entangled quantum light source
US8265280B2 (en) * 2004-11-05 2012-09-11 Nucrypt Llc System and method of entangled photons generation
CN103959704A (en) * 2011-09-30 2014-07-30 中央科学研究中心 Method and device for synchronizing entanglement sources for a quantum communication network
CN104330938A (en) * 2014-10-16 2015-02-04 南京大学 Optical superlattice- and waveguide light path-based quantum light source chip

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CA2680245A1 (en) * 2007-03-08 2008-09-12 Qutools Gmbh Generation of quantum-correlated and/or polarization-entangled photon pairs with unequal wavelengths
JP5723260B2 (en) * 2011-11-18 2015-05-27 日本電信電話株式会社 Polarization-entangled photon pair generator
CN103901700B (en) * 2014-05-06 2016-06-29 天津大学 Wavelength tunable and frequency spectrum controllable small-sized Quantum Correlation photon pair source and the method for generation

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8265280B2 (en) * 2004-11-05 2012-09-11 Nucrypt Llc System and method of entangled photons generation
WO2009093391A1 (en) * 2008-01-25 2009-07-30 Japan Science And Technology Agency Non-degenerate polarization-entangled photon pairs generation device and non-degenerate polarization-entangled photon pairs generation method
CN101398590A (en) * 2008-11-06 2009-04-01 天津大学 All-optical frequency entangled photon source
CN102130418A (en) * 2011-01-26 2011-07-20 清华大学 Polarization-entangled quantum light source
CN103959704A (en) * 2011-09-30 2014-07-30 中央科学研究中心 Method and device for synchronizing entanglement sources for a quantum communication network
CN104330938A (en) * 2014-10-16 2015-02-04 南京大学 Optical superlattice- and waveguide light path-based quantum light source chip

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
LV , NING: "1.5µm Polarization Entanglement Generation Based on Silicon Wire Waveguides", CHINESE MASTER'S THESES FULL-TEXT DATABASE, 15 July 2015 (2015-07-15), ISSN: 1674-0246 *

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US11588613B1 (en) 2021-10-26 2023-02-21 Eagle Technology, Llc Systems and methods for synchronization of photons over quantum channels with co-propagating clock pulses

Also Published As

Publication number Publication date
CN109429509A (en) 2019-03-05

Similar Documents

Publication Publication Date Title
EP2788863B1 (en) Integrated quantum-random noise generator using quantum vacuum states of light
Snijders et al. Fiber-coupled cavity-QED source of identical single photons
CN104170189B (en) Luminescent semiconductor device
WO2018232689A1 (en) Time-entangled photon pair generating device
Doerr et al. O, E, S, C, and L band silicon photonics coherent modulator/receiver
JP6924198B2 (en) Integrated Microwave-Optical Single Photon Transducer with Distortion-Induced Electro-Optical Material
CN111999959A (en) Narrow-bandwidth entangled photon pair generation device based on periodically polarized lithium niobate thin-film waveguide
CN103292800A (en) One-chip type integrated optical gyroscope and manufacturing method thereof
Lukin et al. Two-emitter multimode cavity quantum electrodynamics in thin-film silicon carbide photonics
JP2014165292A (en) Light-emitting element, manufacturing method of the same and optical transmitter/receiver
CN104466620A (en) Frequency stabilization type photoproduction microwave signal source based on optical microcavity
JP2015184528A (en) Integrated optical circuit and manufacturing method of the same
JP2014228639A (en) Optical amplifier
Srinivasan et al. Heterogeneous SISCAP microring modulator for high-speed optical communication
US20160291442A1 (en) Quantum wave-converter
CN212846292U (en) Efficient entanglement photon pair generation device
Pinguet et al. Silicon photonics multicore transceivers
Riedel et al. Efficient photonic integration of diamond color centers and thin-film lithium niobate
US9618709B2 (en) Hybrid integration of edge-coupled chips
KR100916659B1 (en) Photon-pair generator
US11101616B2 (en) Brillouin laser
CN1752834A (en) Photoswitch and the light wave shape monitoring device that utilizes photoswitch
Serafini et al. Tunable, High Purity Two-Photon Interference From Independent Sources On a Silicon Photonic Chip
JP5758779B2 (en) Optical hybrid circuit, optical receiver and optical coupler
CN114362829B (en) PPLN-based polarization independent frequency conversion method, device and single photon detector

Legal Events

Date Code Title Description
121 Ep: the epo has been informed by wipo that ep was designated in this application

Ref document number: 17914987

Country of ref document: EP

Kind code of ref document: A1

NENP Non-entry into the national phase

Ref country code: DE

122 Ep: pct application non-entry in european phase

Ref document number: 17914987

Country of ref document: EP

Kind code of ref document: A1