On-chip coherent conversion of photonic quantum entanglement between different degrees of freedom

Abstract

In the quantum world, a single particle can have various degrees of freedom to encode quantum information. Controlling multiple degrees of freedom simultaneously is necessary to describe a particle fully and, therefore, to use it more efficiently. Here we introduce the transverse waveguide-mode degree of freedom to quantum photonic integrated circuits, and demonstrate the coherent conversion of a photonic quantum state between path, polarization and transverse waveguide-mode degrees of freedom on a single chip. The preservation of quantum coherence in these conversion processes is proven by single-photon and two-photon quantum interference using a fibre beam splitter or on-chip beam splitters. These results provide us with the ability to control and convert multiple degrees of freedom of photons for quantum photonic integrated circuit-based quantum information process.

ARTICLE

Received 25 Feb 2016 | Accepted 18 May 2016 | Published 20 Jun 2016

Lan-Tian Feng1,2,*, Ming Zhang3,*, Zhi-Yuan Zhou1,2,*, Ming Li1,2, Xiao Xiong1,2, Le Yu1,2, Bao-Sen Shi1,2, Guo-Ping Guo1,2, Dao-Xin Dai3, Xi-Feng Ren1,2 & Guang-Can Guo1,2

In the quantum world, a single particle can have various degrees of freedom to encode quantum information. Controlling multiple degrees of freedom simultaneously is necessary to describe a particle fully and, therefore, to use it more efciently. Here we introduce the transverse waveguide-mode degree of freedom to quantum photonic integrated circuits, and demonstrate the coherent conversion of a photonic quantum state between path, polarization and transverse waveguide-mode degrees of freedom on a single chip. The preservation of quantum coherence in these conversion processes is proven by single-photon and two-photon quantum interference using a bre beam splitter or on-chip beam splitters. These results provide us with the ability to control and convert multiple degrees of freedom of photons for quantum photonic integrated circuit-based quantum information process.

DOI: 10.1038/ncomms11985 OPEN

On-chip coherent conversion of photonic quantum entanglement between different degrees of freedom

1 Key Laboratory of Quantum Information, University of Science and Technology of China, CAS, Hefei 230026, China. 2 Synergetic Innovation Center of Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei 230026, China. 3 State Key Laboratory for Modern Optical Instrumentation, Centre for Optical and Electromagnetic Research, Zhejiang Provincial Key Laboratory for Sensing Technologies, Zhejiang University, Zijingang Campus, Hangzhou 310058, China. * These authors contributed equally to this work. Correspondence and requests for materials should be addressed to D.-X.D. (email: mailto:[email protected]

Web End [email protected] ) or to X.-F.R. (email: mailto:[email protected]

Web End [email protected] ).

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Compared with free space and bre optics, photonic integrated circuits (PICs) have attracted considerable attention owing to their small footprint, scalability,

reduced power consumption and enhanced processing stability; thus, many quantum computation and quantum simulation protocols have been realized on quantum PICs19. Regarding recent investigations of quantum PICs, polarization entanglement and path entanglement are usually used. Polarization entanglement is quite important because the polarization of photons is easy to control in free space, and various proof-of-principle demonstration of quantum computation schemes were carried out based on the polarization degree of freedom1012. For the path-encoding method, it is possible to establish a higher-dimensional Hilbert space5, which means that we can encode more information per photon and increase the security of quantum systems1316. However, the path-encoding method is not easy to scale up for practical implementations.

Recently, transverse waveguide modes were introduced as a new information encoder, and they were used in multi-core17 and few-mode bres18, as well as in classical PICs19, to satisfy the increasing demand for the capacity of optical interconnects. A multi-mode waveguide can support many transverse waveguide modes, which form a set of orthogonal basis for the transverse spatial distribution of energy; thus, it is appropriate for carrying more information using photons. For example, the eight-channel information-encoding process has been demonstrated in a2.363-mm wide multi-mode waveguide20. This degree of freedom may have great potential in quantum optics, such as realizing high-dimensional quantum operation, maintaining the polarization entanglement resource in a high-birefringence integrated device.

We can use multiple degrees of freedom of a quantum particle simultaneously, which will certainly increase the information capacity of qubits2124. As for photons, polarization, frequency, time, orbital angular momentum and even the transverse-mode entanglement have been used in free-space quantum systems, and some of them have been used in bre quantum systems25. For example, quantum teleportation of the composite quantum states of a single photon encoded in both spin and orbital angular momentum was recently demonstrated in free-space26. Experimental realization of multi-degree-of-freedom entanglement poses signicant challenges to the coherent control of multiple degrees of freedom simultaneously and to realizing quantum logic gates between independent qubits of different degrees of freedom.

In the following, to show the potential utility of transverse waveguide modes in the quantum information process, we demonstrate that quantum coherence is preserved when photons in different transverse waveguide modes propagate in a multi-mode waveguide. We will also show the coherent on-chip conversion of quantum states between different degrees of freedom, such as path, polarization and the transverse waveguide mode. Here coherent conversion refers to the preservation of coherence of quantum state, including the indistinguishability between the single photons, the stability of relative phase of superposition state and entangled state in the processes of photon transmission and conversion between different degrees of freedom.

ResultsExperimental set-up. The transverse waveguide modes discussed in this study are the three lowest-order modes, that is, TE0, TE1 and TM0 in a multi-mode waveguide, as shown in upright inset of Fig. 1a. Here we use a silicon-on-insulator (SOI) strip waveguide with a cross-section of B750 220 nm. To effectively and

accurately excite and manipulate these transverse waveguide modes in this multi-mode waveguide, the low-loss and low-

crosstalk mode (de)multiplexer is one of the most important devices. In this work, we choose two different structures for the conversion between different degrees of freedom. The rst one is a special polarization-dependent mode converter, which can convert laser beam in TE and TM polarizations into the TE0 and

TE1 modes28,29, respectively, as shown in Supplementary Fig. 1a. The other one is a mode multiplexer, which can convert laser beam in path 1 and path 2 into the TE0 and TE1 waveguide modes27, respectively, as shown in Supplementary Fig. 1b. Although these elements work well for laser beam, they have not yet been used for quantum signals. After conversion, the TE0- and TE1-mode photons propagate in the multi-mode waveguide for a certain distance and then convert back to photons with different polarizations or different optical paths, as shown in Fig. 1b.

To test the coherent property of the two photons after undergoing different conversion processes, a HongOuMandel (HOM) interferometer is used. HOM interference is a basic type of quantum interference that reects the bosonic properties of a single particle and is generally used to test the quantum properties of single qubits30. It can be described as follows: when two indistinguishable photons enter a 50/50 beam splitter (BS) from different sides at the same time, the two photons will come out together and never be in different output ports. Experiments typically control the arrival time of two photons by adjusting the path-length difference between them and measure the photon coincidence (the case in which two photons arrive at two detectors simultaneously) of the two output ports of the BS. When two indistinguishable photons completely overlap at the BS, they give rise to the maximum interference effect and no coincidence exists. Visibility is dened as V1 (Cmax Cmin)/

Cmax, where Cmax is the maximum coincidence and Cmin is the minimum coincidence. For perfect quantum interference, Cmin 0 and V1 1. Or we can collect the photons from one

output port of the BS, send them to the second 50/50 BS, and then measure the coincidence31. In this case, a peak will be observed and the visibility is modied as follows: V2 (Cmax Cmin)/Cmin.

For perfect quantum interference, Cmax 2Cmin and V2 1.

The experimental set-up is shown in Fig. 2. The degenerate 1,558-nm photon pair source is generated using a type II phase-matched periodically poled potassium titanyl phosphate (KTiOPO4) crystal in a Sagnac interferometer pumped by a continuous-wave 779-nm laser32, which operates in a single circulation direction. Each photon is coupled into a single-mode bre and then sent to a bre array. In one arm, the bre coupler is mounted on a one-dimensional translator with a step of 10 mm.

By moving the translator, we can modify the arrival time of the single photons on BS and thus observe the HOM interference effect. The grating coupling method is used to couple the single photons into/out of the chip from/into the bre arrays. The output photon pairs collected by the second bre array are sent into a bre BS to produce the HOM interference.

The indistinguishability of the photon pairs from the source is characterized using a standard HOM interferometer with a bre BS. The dip represents the quantum interference of two photons, and the coherence length of the photons determines its width, as shown in Supplementary Fig. 2. Here we obtain a raw visibility of96.32.8% (96.82.8% with background subtraction) and an optical coherence length of 448.719.8 mm. The deviation of the visibility from 100% is attributed to the polarization distortion of the photons during the propagation in the bre, the photon source variability or both.

Single-photon state conversion. The coherent conversion of single-photon state between different degrees of freedom is tested at rst. The sketch map and charge-coupled device picture of the

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a

l = 0 l = 1 l = 2

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Figure 1 | On-chip coherent conversion of photonic quantum entanglement between different degrees of freedom. (a) Transverse waveguide mode as a new on-chip quantum information encoder. In free-space high-dimensional quantum information processes, orbital angular momentums of photons are usually used to encode information. Correspondingly, transverse waveguide mode can be used as a new degree of freedom for on-chip high-dimensional quantum information process. Inset on upright corner shows the energy distributions of the fundamental mode (TE0 and TM0) and the rst higher-order mode (TE1) in a multi-mode waveguide. The SOI strip waveguide has a cross-section of B750 220 nm. (b) On-chip coherent conversion of quantum

states between different degrees of freedom, such as path, polarization and the transverse waveguide mode, is essential for using different degrees of freedom simultaneously.

SMF

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Figure 2 | Experimental set-up for the two-photon source and sample measurement. The continuous-wave pump laser at 779 nm is from a Ti:sapphire laser (Coherent MBR 110). It is collected into single-mode bre (SMF) before entering the Sagnac-loop. A quarter wave plate (QWP) and a half wave plate (HWP) are used to control the phase and intensity of the pump beams in the Sagnac-loop. In the present experiment, the pump laser with vertical polarization is focused by a lens (L) with a focus length of 200 mm, whose beam waist is B40 mm at the centre of the PPKTP crystal. The type II PPKTP (Raicol crystals) crystal has a size of 1 2 10 mm, with a periodical poling period of 46.2 mm. The temperature of the PPKTP crystal is controlled by a

home-made temperature controller with a stability of 2 mK. After a double PBS (DPBS), the polarization of the pump beam is changed to horizontal by a double HWP (DHWP) before the PPKTP crystal. The orthogonal polarized photon pairs generated in the counterclockwise direction are separated by the DPBS and collected into SMFs by using a lens set consisting of two lenses with different focus lengths of 100 and 50 mm at each output port of the DPBS, respectively. The pump beam is removed using a long pass lter (LPF, FELH1400). We use HWPs and QWPs to control the polarizations of the photon pair before injecting into the silicon chip. The output photons from the chip are detected by two InGaAs single-photon avalanche detectors (SPAD, D220, free running single-photon detector), with polarization controlled by bre polarization controllers (PCs). The grating coupling method is used to couple the single photons into/out of the chip from/into the bre arrays.

rst sample are shown in Fig. 3a,b, respectively (see Supplementary Fig. 3 for detail). Two single photons with orthogonal polarizations from the bre array are coupled into different single-mode waveguides, that is, the TE0 and TM0 mode,

by a TE-type grating and a TM-type grating, respectively. Then, the two single-mode waveguides combine together with a polarization BS (PBS) based on a bent directional coupler28. A special mode converter based on an adiabatic taper is cascaded

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Figure 3 | Single-photon state conversion. (a,b) The sketch map and CCD (charge-coupled device) picture (scale bar, 250 mm) of the rst sample, respectively. Two single photons with orthogonal polarizations from the bre array are coupled into different single-mode waveguide as TE0 and TM0 modes, respectively, by a TE-type grating and a TM-type grating and then converted to different transverse waveguide modes, that, the TE0 and TE1 modes, by a mode converter after a PBS. After propagating along the multi-mode waveguide for 870 mm, the two photons are converted back with different polarizations and are coupled out to a bre BS to produce a HOM interference. Coincidence measurement is performed when adjusting the position of the one-dimensional translator. (c,d) The sketch map and CCD picture (scale bar, 250 mm) of the second sample, respectively. Two single photons with the same polarization from the bre array are coupled into different single-mode waveguides, both having the TE0 mode, by two TE-type gratings, respectively. Then, with a mode multiplexer, photons in different optical paths are converted to different transverse waveguide modes. After propagating along the multi-mode waveguide for 30 mm, the two photons are divided into two distinct single-mode waveguides by a reversed process. HOM interference occurs on an on-chip BS (3-dB coupler), which was performed on the path degree of freedom. (e) HOM interference between the two photons, which undergo different conversion processes via a bre BS for the rst sample. The raw visibility is 92.35.0% (94.85.0% with background subtraction), which proves unambiguously the preservation of quantum coherence in the process of polarization to transverse waveguide mode and back to polarization. (f) HOM interference between two photons undergoing different conversion processes using an on-chip BS for the second sample. The visibility is 96.03.3%(97.33.3% with background subtraction), which proves unambiguously the preservation of quantum coherence in the process of path to transverse waveguide mode and back to path. Error bar comes from the Poisson statistical distribution. The experimental data are tted with a triangle function.

and polarization-dependent mode conversion happens, as reported previously29. The TM0 mode is then converted into the TE1 mode after propagating along this adiabatic taper while there is no mode conversion for the TE0 mode. As a result, photons with different polarizations are converted to different transverse waveguide modes (that is, the TE0 and TE1 modes).

This is experimentally proven by a near-eld scanning optical microscope, which can measure the evanescent eld distribution of the guided mode in an optical waveguide. The results are shown in Supplementary Fig. 4, which clearly prove the function of the PBS and the mode converter. The two photons in the TE0 mode and the TE1 mode propagate along the multi-mode waveguide for 870 mm and are converted back to different polarizations by a similar mode converter structure. We collect the two output photons from the two different gratings and then send them to the HOM test system. By moving the one-dimensional translator, we can control the arrival time difference between the two photons and thus get the relation between the

coincidence and the path length difference. Figure 3e gives the measured HOM interference between the two photons undergoing different conversion processes. The raw visibility is92.35.0% (94.85.0% with background subtraction) and the coherent length is 458.737.8 mm, which proves unambiguously the preservation of quantum coherence during the conversion from the polarization to the transverse waveguide mode and back to polarization process.

Then, we tested the single-photon state conversion between the optical path and transverse waveguide-mode degrees of freedom with sample 2, as shown in Fig. 3c,d (see Supplementary Fig. 5 for detail). In this case, two photons with the same polarization from the bre array are coupled into different single-mode waveguides, both having the TE0 mode, by two TE-type gratings, respectively.

Then, the two single-mode waveguides combine together with a mode multiplexer such that one TE0 mode is converted to the TE1 mode in the bus waveguide while the other TE0 mode is kept unchanged. Thus, photons in different optical paths are converted

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to different transverse waveguide modes. The two photons in the TE0 mode and the TE1 mode propagate along the multi-mode waveguide for 30 mm, and then are converted back to the TE0 mode in two distinct single-mode waveguides with a mode demultiplexer. Unlike the rst sample, HOM interference occurs on an on-chip BS (3-dB coupler). Figure 3f gives the result with a raw visibility of 96.03.3% (97.33.3% with background subtraction), and the coherent length is 460.228.1 mm, which illustrates the coherent conversion of quantum signals from path encoding to transverse waveguide-mode encoding.

Quantum entanglement conversion. Coherent conversion of the quantum-entangled state is also proven in our experiment using the third and fourth samples shown in Fig. 4ad (see Supplementary Figs 6 and 7 for detail), respectively. For the third sample, two single photons with the same polarization are coupled to single-mode waveguides by two gratings, respectively. Then, they interfere at the BS and generate a two-photon quantum NOON state33, encoded on the path as

j2i0j0i1 j0i0j2i1= 2

p , where jnii denotes n photons in path

i, for n 0, 1, 2, and i 0, 1. With a mode multiplexer, the state

will be changed to j2iTE1j0iTE0 j0iTE1j2iTE0= 2

p because the

photons in path 0 will be in the TE1 mode while photons in path 1 will be in the TE0 mode. After propagation in the multi-mode waveguide for a distance of 30 mm, this transverse waveguide-mode two-photon NOON state is changed back to a path NOON state. Two-photon interference, or two-photon NOON state interference, is measured by using the second on-chip BS, as shown in Fig. 4e (red dots). The phase between the two arms is adjusted by using a thermal-tuning method. Classical interference is also measured for comparison with a visibility of 99.97.8% (black dots). We observe a entangled state interference visibility of 90.37.8% (94.08.2% with background subtraction) with a period (heater power 32.50.7 mW) approximately half of the classical interference (heater power period is 66.82.8 mW).

Finally, to show that these conversion processes can be cascaded, we combine several structures together on a single chip, and a two-photon quantum NOON state is converted between these three degrees of freedom. The sample is shown in Fig. 4c,d. Two single photons with the same polarization are coupled to single-mode waveguides and then interfere at the on-chip BS, generating a quantum-entangled state encoded on the path as

j2i0j0i1 j0i0j2i1= 2

p . It is rst converted to a transverse

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Figure 4 | Quantum-entangled state conversion. (a,b) The sketch map and CCD (charge-coupled device) picture (scale bar, 250 mm) of the third sample, respectively. Two single photons with the same polarization are coupled to single-mode waveguides by two gratings, respectively. Then, they interference at the rst BS (3-dB coupler) and generate a two-photon quantum NOON state, encoded on the path as 2

j i0 0

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2

p . With a mode multiplexer,

the state will be changed to 2

. 2

p . After propagation in the multi-mode waveguide for a distance of 30 mm, this transverse waveguide-mode NOON state is changed back to a path NOON state. Two-photon interference, or two-photon NOON state interference, is measured by using the second on-chip BS, as shown in e (red dots). Classical interference is also measured for comparison (black dots). We observe a raw interference visibility of 90.37.8% (94.08.2% with background subtraction) with a period approximately half of the classical interference. (c,d) are the sketch map and CCD picture (scale bar 250 mm) of the fourth sample, respectively. A quantum two-photon NOON state is generated by an on-chip BS and then converted between the three degrees of freedom (path, transverse waveguide mode and polarization). (f,g) HOM interference patterns between the two photons from TE and TM outputs of the sample, respectively. Error bar comes from the Poisson statistical distribution. The raw visibilities are 96.87.8%(98.27.9% with background subtraction) and 96.78.3% (98.38.5% with background subtraction), respectively. These results prove unambiguously the preservation of quantum coherence in the conversion of quantum-entangled state between different degrees of freedom. It should be noted that all the measurements of the HOM interference were performed on the path degree of freedom for the sake of simplication.

j iTE 0

j iTE 0

j iTE 2

j iTE

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waveguide-mode NOON state j2iTE1j0iTE0 j0iTE1j2iTE0= 2

p

Methods

Sample design and fabrication. The chip includes some key components, including the PBSs, the mode multiplexers and the mode converters. All the components are designed according to the optical waveguide theory and the coupled-mode theory. The simulation tools include the Fimmprop (PhotoDesign, Oxford, UK) using an eigenmode expansion and the matching method, and Lumerical software (Lumerical Solutions, Inc., London, UK) with the 3D time-domain nite-difference method. The PBS is designed with a bent directional coupler consisting of two parallel bent waveguides28. These two bent waveguides have different core widths and could be designed to satisfy the phase-matching condition for the coupling of TM polarization; consequently, TM-polarized light could be coupled to the cross port completely when choosing the length of the coupling region appropriately. On the other hand, for TE polarization, the phase-matching condition is not satised because of the birefringence of the waveguides. Thus, TE-polarized light goes through without any signicant coupling. In this way, TE- and TM-polarized lights are separated within a very short length that is close to the coupling length of TM polarization. The mode multiplexer is designed with an asymmetric directional coupler, which consists of a narrow access waveguide close to the wide bus waveguide27. The widths of the narrow access waveguide and the wide bus waveguide are chosen optimally to satisfy the phase-matching condition so that the fundamental mode of the narrow access waveguide can be coupled to the rst higher-order mode in the bus waveguide completely. On the other hand, there is almost no coupling from the fundamental mode of the wide bus waveguide to any modes in the narrow access waveguide. The mode converter is designed with an adiabatic taper based on SOI strip waveguides with an air upper-cladding29. For an SOI strip waveguide whose cross-section has vertical asymmetry, mode hybridization happens when choosing some special core width wco0. The hybridized modes have comparable x and y components for the electrical elds. Such mode hybridization will introduce a mode conversion when light propagates along an adiabatic taper structure whose end widths w1 and w2 are chosen such that w1owco0ow2.

For the fabrication of the present sample, the process started from an SOI wafer with a 220-nm-thick top silicon layer. An E-beam lithography process with the MA-N2403 photoresist was carried out to make the pattern of waveguides, which was then transferred to the top silicon layer via an inductively coupled-plasma-etching process. Grating couplers were made using a second etching process to achieve an efcient bre-chip coupling.

Grating coupling method. Grating couplers are very popular for realizing efcient coupling between the chip and bres at the input/output ends39. Here we use two types of grating couplers, that is, TE type and TM type, which are designed for TE- and TM-polarized lights, respectively. In our design, the grating periods are chosen as 640 and 1040 nm for the TE- and TM-type grating couplers, respectively. To avoid reection at the waveguide-grating interface, light is coupled in (out) at a small angle (15 in our experiment) with respect to the vertical direction. The peak coupling efciencies are about 30%.

Photon source. The continuous-wave pump laser at 779 nm is from a Ti: sapphire laser (Coherent MBR 110). It is collected into single-mode bre before entering the Sagnac-loop. A quarter-wave plate and a half-wave plate (HWP) are used to control the phase and intensity of the pump beams in the Sagnac-loop. In the present experiment, the pump laser with vertical polarization is focused by a lens with a focus length of 200 mm, whose beam waist is B40 mm at the centre of the periodically poled potassium titanyl phosphate (PPKTP) crystal. The type II PPKTP (Raicol crystals) crystal has a size of 1 2 10 mm, with a periodical

poling period of 46.2 mm. The temperature of the PPKTP crystal is controlled by a home-made temperature controller with a stability of 2 mK. After a double PBS (DPBS), the polarization of the pump beam is changed to horizontal by a double HWP before the PPKTP crystal. The orthogonal polarized photon pairs generated in the counterclockwise direction are separated by the DPBS and collected into single-mode bres by using a lens set consisting of two lenses with different focus lengths of 100 and 50 mm at each output port of the DPBS, respectively. The pump beam is removed using a long pass lter (FELH1400). We use HWPs and quarter-wave plates to control the polarizations of the photon pair before injecting into the silicon chip. The output photons from the chip are detected by two InGaAs single-photon avalanche detectors (D220, free running single-photon detector).

Data availability. The authors declare that the data supporting the ndings of this study are available within the article and its Supplementary Information les.

and then changed to j2iTM0j0iTE0 j0iTM0j2iTE0= 2

p , which is a polarization NOON state. To show that the whole process is actually the same as what we described above, it is important to show that the two photons at the output are either both in H polarization or in V polarization and never have different polarizations. We collect the output photons from each grating coupler and conduct the HOM interference test with a bre BS. As shown in Fig. 4f,g, peaks are observed as the two photons arrive at the on-chip BS simultaneously. The raw visibilities are 96.87.8% (98.27.9% with background subtraction) and96.78.3% (98.38.5% with background subtraction), and the coherent lengths are 446.137.0 and 407.731.2 mm, respectively. This means that when the two-photon path NOON state is generated, there are two photons at output 1 or at output 2, as we predicted.

DiscussionWe conclude that our experiment demonstrates unambiguously the coherent propagation of quantum signals encoded on transverse waveguide modes and the on-chip coherent conversion of quantum entanglement between different degrees of freedom. Although only two lower transverse waveguide modes are discussed, this newly introduced degree of freedom shows us the possibility of encoding quantum information within a higher-dimensional Hilbert space, which is useful for the investigation of the on-chip high-dimensional quantum information process, such as teleportation using qudits13,14, quantum dense coding15 and quantum key distribution16. For example, a two-photon three-dimensional (3D) path-entangled state can be converted to a 3D transverse waveguide-mode-entangled state easily using our mode converters (similar demonstration between path and orbital angular momentum was recently realized in free space34).

The on-chip coherent conversion of quantum-entangled state that is encoded onto path, polarization and the transverse waveguide mode, shows us the ability to control these degrees of freedom, which has great potential in on-chip hyper-entangled quantum systems. Hyper-entanglement21,35, where qubits are entangled in two or more degrees of freedom, has shown advantages in quantum information applications. Using hyper-entanglement will make it much easier to perform quantum logic gates36, and will also enable new capabilities in quantum information process, such as remote preparation of entangled states, full Bell-state analysis and improved super-dense coding22,23, as well as the possibility of quantum communication with larger alphabets24. Path-polarization hyper-entangled and cluster states of photons on a chip were recently realized37.

The chips we used are based on SOI waveguides, which have been developed well and used widely because of the complementary metal oxide semiconductor (CMOS) compatibility and the ultra-small footprint. The operation wavelength of the silicon chip lies in the whole telecom band, which is compatible with present bre communication networks. Quantum information processing based on silicon photonic chip will be a good candidate of quantum processor for quantum communication networks. Note that because different transverse waveguide modes have different effective refractive indices, relative phases will be generated when photons in different transverse waveguide modes propagate along the multi-mode waveguide. For the on-chip quantum information process, this phase can be adjusted by using a thermal-tuning method. In our experiment, all the measurements of the HOM interference were performed on the path degree of freedom for the sake of simplication.

While this report was being written, quantum interference between transverse waveguide modes was realized38.

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Acknowledgements

This work was funded by NBRP (grant nos 2011CBA00200 and 2011CB921200), the Innovation Funds from the Chinese Academy of Sciences (grant no. 60921091), NNSFC (grant nos11374289, 61590932, 61422510, 11374263, 61431166001 and 61525504), the Fundamental Research Funds for the Central Universities, the Open Fund of the State Key Laboratory on Integrated Optoelectronics and the Doctoral Fund of the Ministry of Education of China (no. 20120101110094).

Author contributions

All authors contributed extensively to the work presented in this paper; M.Z. and D.-X.D; prepared the samples; L.-T.F., Z.-Y.Z., B.-S.S. and X.-F.R. performed the measurements and data analysis; M.L., X.X., L.Y., G.-P.G. and G.-C.G. conducted theoretical analysis;X.-F.R. and D.-X.D. wrote the manuscript and supervised the project.

Additional information

Supplementary Information accompanies this paper at http://www.nature.com/naturecommunications

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How to cite this article: Feng, L.-T. et al. On-chip coherent conversion of photonic quantum entanglement between different degrees of freedom. Nat. Commun. 7:11985 doi: 10.1038/ncomms11985 (2016).

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