We report the first entanglement generation experiment using an on-chip slow light device. With highly efficient spontaneous four-wave mixing enhanced by the slow light effect in a coupled resonator optical waveguide based on a silicon photonic crystal, we generated 1.5-μm-band high-dimensional time-bin entangled photon pairs. We undertook two-photon interference experiments and observed the coincidence fringes with visibilities >74%. The present result enables us to realize an on-chip entanglement source with a very small footprint, which is an essential function for quantum information processing based on integrated quantum photonics.
Slow light waveguides are now being intensively studied as a way of realizing various functionalities such as optical switches and buffers with very small footprints on a chip1,2. Slow light waveguides are also attracting attention as a way of obtaining a huge nonlinear optical effect. For example, the third order nonlinear coefficient is proportional to the square of the group index ng3, which means that we can significantly enhance the four-wave mixing efficiency by using a slow light waveguide4. Thus, a slow light waveguide is a promising candidate as a nonlinear optical device for all-optical signal processing. The slow-light enhanced nonlinearity is also useful for integrated quantum photonics, in which photonic quantum information processing functions are integrated on an optical waveguide5. With the aim of realizing integrated photon sources on a chip, several correlated photon pair generation experiments based on slow-light enhanced spontaneous four-wave mixing (SFWM) have already been reported6,7,8. Xiong et al. demonstrated the first correlated pair generation enhanced by a slow light waveguide, using a dispersion-engineered silicon photonic crystal waveguide6. This experiment was followed by one that used a coupled resonator optical waveguide (CROW)9 based on silicon ring cavities as a slow-light device7. Recently, our group reported a correlated pair generation experiment using a CROW based on silicon photonic crystal cavities8. These experiments achieved a significant enhancement of pair generation efficiency compared with conventional photon pair sources based on SFWM. However, none of the experiments have achieved the generation of an entangled state, or in other words, confirmed the coherence of two-photon states.
In this paper, we report the first entanglement generation experiment to use a slow-light waveguide. We utilized slow-light enhanced SFWM in a CROW consisting of 200 silicon photonic crystal nanocavities10 pumped by a coherent pulse train to generate a high-dimensional time-bin entangled state11. We undertook two-photon interference measurements using a Franson interferometer12 and observed the coincidence fringes with visibilities exceeding the limit of the violation of Bell's inequality.
CROW based on silicon photonic crystal
A CROW is a one-dimensional array of identical optical cavities, where adjacent cavities are coupled to each other to form an extended mode along the waveguide. A CROW exhibits a transmission bandwidth that is far larger than those of the individual cavities, while the group velocity is significantly reduced inside the band. Figure 1 (a) shows a schematic of our CROW fabricated on a silicon chip. The CROW is based on a width-modulated line defect cavity in a silicon photonic crystal (PhC) with a two-dimensional triangular-lattice of air holes13. The Q of each cavity is ~106, and the intercavity distance is 5a, where a is the lattice constant of our PhC waveguide (420 nm). The air hole diameter is a/2. The number of cavities is 200, which means that the total length of the CROW is 420 μm. PhC line-defect waveguides are equipped at the both ends of the CROW. The PhC section is integrated with silicon wire waveguides (SWW) from which we can optically access the CROW. The waveguide loss of the CROW section was ~2 dB/mm8. Lensed fibers are used to couple light to the silicon chip with a coupling efficiency of ~−9 dB per point. Figure 1 (b) shows the transmission spectra of the CROW at a temperature of 32.8°C. The formation of a broad transmission band was clearly observed from 1543 to 1550 nm.
Figure 2 shows the experimental setup. A 1545.4-nm continuous wave light from an external cavity laser diode was modulated into a 60-ps, 1-GHz clock pulse train using a lithium niobate intensity modulator. The pulse train was then amplified by an erbium-doped fiber amplifier (EDFA), and input into optical bandpass filters to eliminate the amplified spontaneous emission noise from the EDFA. The pulse train was launched into the silicon chip that contained the CROW through a lensed fiber. The chip temperature was set at 32.8°C. At this temperature, the group index of the CROW for the pump wavelength was around 4014. Through the slow-light enhanced SFWM in the CROW, high-dimensional time-bin entangled photon pairs were generated, whose quantum state is approximately given by11 Here N is the number of pump pulses where coherence is preserved, and |k〉x denotes a quantum state where there is a photon at the k th time slot in the mode x ( = s: signal, i: idler). The photons from the chip were collected by another lensed fiber, passed through fiber Bragg gratings to suppress the pump photons, and input into an arrayed waveguide grating to separate the signal and idler channels. The wavelengths of the signal and idler channels were 1544.6 and 1546.2 nm, respectively, and both had a 0.1 nm (12.5 GHz) bandwidth. The transmission spectra of the signal and idler channels with respect to the CROW band are plotted in Fig. 1 (b). The total channel losses were 6.0 and 6.7 [dB] for the signal and idler, respectively. The signal and idler photons were passed through optical bandpass filters to suppress the pump photons further, and launched into 1-bit delayed Mach-Zehnder interferometers made using silica-on-silicon waveguides15. The phase differences between the two arms of the interferometers were tuned by changing the waveguide temperature: a π phase shift was attained with ~0.4°C temperature change. With these interferometers, a state |k〉x is converted to , where ϕx is the phase difference induced in the interferometer for channel x. Then, Eq. (1) is converted to where only the terms that contributed to the coincidence detection are shown and the normalizing term is discarded for simplicity. By ignoring the first and the last terms on the right hand side of the above equation, we obtain the coincidence probability P as where V is the two-photon interference visibility. Then, the photons from the interferometers were received by superconducting single photon detectors (SSPD), and the coincidences were counted using a time interval analyzer. The detection efficiency of both SSPDs was set at 20%, and at this condition, the dark count rates were 50 and 10 Hz for the signal and idler channels, respectively.
To investigate the degree of temporal correlation, we first removed the waveguide interferometers from the setup and undertook a coincidence-to-accidentals ratio (CAR) measurement. The result is shown in Fig. 3 (a). We obtained the maximum CAR of 8.7 ± 1.0 when we set the average photon number per pulse at 0.001. The improvement in the CAR compared with our previous experiment8 can be mainly attributed to the fact that we halved the photon pair bandwidth and reduced the pump pulse width (details are provided in Method). Using the method reported in16, we can estimate the portions of correlated pairs and the noise photons from the CAR and count rate measurement results. The estimated correlated and noise photons per pulse as a function of peak coupled pump power are shown in Fig. 3 (b). The average number of correlated photon pairs per pulse (μc) is proportional to the square of the pump power, which is a clear signature of the SFWM process. μc can be approximately obtained as 8, where Δν, Δt, , Pp are the bandwidth of the signal and idler photons, the pulse width, the effective nonlinear coefficient, and the peak power of the pump pulse, respectively. Leff denotes the effective length defined by (1 − e−αL)/α, where α is the attenuation coefficient of the waveguide. With this equation and the result shown in Fig. 3 (b), we estimated that the effective nonlinear coefficient of our CROW was ~5900 [1/W/m], which is comparable to values reported for the previous experiments6,7,8 and larger than that of a conventional SWW by an order of magnitude17. On the other hand, the noise photons were dominant in our experiment, which severely limited the maximum CAR. The average numbers of noise photons for the signal (μsn) and the idler (μin) are almost proportional to the pump power. Note that similar noise photon generation at small detunings was also observed in an SWW18.
We then inserted waveguide interferometers into the setup and undertook a two photon interference experiment. The average photon number per pulse was set at 0.004. Figure 3 (c) shows the coincidences as a function of the signal interferometer phase, where the squares and circles correspond to the data obtained when we set the idler interferometer phase at 0 and π/2, respectively. We observed clear sinusoidal modulations of coincidences for two nonorthogonal measurement bases for the idler photons, and the visibilities of the fitted curves were 78.0 ± 3.9% (idler interferometer phase 0) and 74.1 ± 4.8% (π/2). This result indicates that, although we obtained a visibility value larger than that associated with the violation of Bell's inequality (), the excess of the visibility was less than one standard deviation. However, when we subtracted the accidental coincidences (which were mainly caused by noise photons), the visibilities were 99.9 ± 7.6% (idler interferometer phase 0) and 99.6 ± 7.4% (π/2), which exceeded by 3.8 standard deviations. The coincidence fringes with the accidental coincidences subtracted are shown in Supplementary Figure S1. Thus, we confirmed the generation of a time-bin entangled state that can violate the Bell's inequality.
As stated above, there were a significant number of noise photons, which limited the CAR and visibilities in the two photon interference measurements. Although the origin of the noise photons is not yet clear, the generation efficiency of the similar noise photons observed in an SWW exhibited temperature dependence, suggesting that those photons were generated by the scattering of the pump photons on thermal bath of excitations18. Therefore, we may be able to reduce the noise by cooling the device, which constitutes important future work. Also, as discussed in Method, we can improve the visibility by using narrower filters, at the expense of source brightness.
The source presented here, whose device length is only 420 μm, is the smallest entanglement source yet reported. Although the efficiency is worse than the 1.15-cm SWW with and a waveguide loss of ~0.1 dB/mm reported in19, the pair generation efficiency of the CROW is significantly better than that of the SWW at a fixed device length in the low-pump power regime where two-photon absorption and free carrier absorption can be neglected. For example, when the peak pump power and the device length are set at 0.01 W and 1 mm, the CROW generates pulsed photon pairs with an average photon pair number per pulse of 2 × 10−3, while the SWW generates ~10−5 pairs per pulse.
It is also important to compare these devices not only in terms of device length but also in terms of area. While the device width of a typical SWW is as small as 1 μm20, the PhC CROW device presented here consists of 12 rows of air holes on each side of a line defect, which means that the device width is (including the area occupied by the air holes). Even with this difference in the device widths, the PhC CROW can achieve a smaller footprint than the SWW. For example, to generate 10−3 pairs per pulse with a 0.01-W peak pump power, the required areas are ~5600 μm2 for the PhC CROW and ~12000 μm2 for the SWW. We can reduce the device footprint even further by optimizing the CROW parameters. For example, we can decrease the cavity coupling by employing a larger intercavity distance, which results in an increased ng9.
In summary, we have reported the first entanglement generation using SFWM in an on-chip slow light device. Thanks to SFWM enhanced by the slow-light effect in a silicon PhC CROW, we realized an on-chip time-bin entangled photon pair source with a device length as short as 420 μm. The two-photon-interference experimental results showed that we could generate an entanglement that can violate Bell's inequality.
Dependence of CAR on filter and pump pulse width
In many previous SFWM experiments, noise photons caused by the spontaneous Raman scattering (SpRS) process degraded the quantum correlation. Inoue and Shimizu studied the effect of SpRS noise photons on photon pair generation based on SFWM with a pulsed pump21. They pointed out that, at a fixed average photon number per pulse, the portion of SFWM photons increases as we reduce the filter bandwidth or the pump pulse width. Here we show the formula that relates CAR, filter bandwidth and pump pulse width.
In the presence of noise photons whose number increases linearly with the pump power, the average photon number per pulse μ is expressed as follows. Here, p is the peak pump power and μc(p) and μn(p) are the average correlated and noise photon per pulse, which are given by where a and b denote coefficients representing the efficiencies of SFWM and the noise-photon generation process, respectively. Δf and Δt are the filter bandwidth and the pump pulse width, respectively. In these equations, we assumed the numbers of noise photons to be the same for the signal and idler channels. Equation (4) implies that the peak pump power p can be expressed with the following equation at a fixed μ. On the other hand, assuming Poisson-distributed photon-pairs, CAR can be related to μc(p) and μn(p) with the following equation16. Here, α and d denote the coupling efficiency (including detection efficiency) of photons and the dark count probability of the detectors, respectively, assuming that these values are the same for both signal and idler channels. With Eqs. (7) and (8), we obtain the following equation. It is clear that we can observe a better CAR if we reduce ΔfΔt.
With the experimental data shown in Fig. 3 (b), we obtain a = 5.78 and b = 1.03 at μ = 0.004. In our previous experiment reported in8, Δf, Δt and d were 25 [GHz], 100 [ps] and 7 × 10−6, respectively. If we use these values together with a and b shown above to calculate CAR using Eq. (9), we obtain 2.2, which is close to the value presented in8 (~2). On the other hand, the calculated CAR is 3.1 if we use the SSPDs with the filter and pump pulse width shown above. This consideration implies that the CAR enhancement in the present experiment can be mainly attributed to the reduction of the filter and pump pulse widths.
This work was supported by the Japan Society for the Promotion of Science with a Grant-in-Aid for Scientific Research (No. 22360034).
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