Abstract
Due to their frequency scaling and longterm coherence, frequency combs at the singlephoton level can provide a fascinating platform for developments in quantum technology. Here we demonstrate frequency comb singlephoton interferometry in an unheralded manner. We are able to induce coherence by erasing the whichway information of pathentangled photon pairs. The photon pairs are prepared using a dual parametric downconversion pumped by a highly stable frequency comb laser and an ultranarrow seed laser. This is conducted at the extremely lowconversion efficiency regime. The unique feature of our quantum interferometer is that the induced onephoton interference of the pathencoded single photons (signal), with multiple frequency components, is observed with a unit visibility without heralding conjugate photons (idler). We demonstrate that quantum information and frequency comb technology can be combined to realize quantum information platforms. We expect this will contribute to the application of quantum information and optical measurements beyond the classical limit.
Introduction
Recent developments in optical frequency comb (OFC) technology^{1,2} have led to revolutionary advances in optical frequency metrology^{3,4,5,6,7,8}, atomic spectroscopy^{9,10}, molecular spectroscopy^{11,12,13,14}, and dualcomb spectroscopy^{15,16}. Especially, a number of notable works employing quantum frequency combs, which exhibit multimodeentangled photon states^{17,18,19,20,21}, have sought to prove their usefulness in a diverse range of applications involving continuous variableentangled photons and discrete multidimensionalentangled photons in quantum information processing^{22,23,24,25,26,27,28}. Quantum frequency combs provide a promising platform for quantum information technology based on timebinencoded qubits^{29,30,31}, especially for longdistance quantum communication and cryptography^{32,33,34,35,36,37}, because frequency combs are intrinsically coherent in the time domain and scalable in the frequency domain^{38,39,40}.
Quantum pathentangled photons have also been used for optical measurements beyond the classical limits of conventional spectroscopy, metrology, and imaging^{41,42,43,44,45}. Recently, novel quantum spectroscopy and imaging with undetected photons have been reported^{46,47,48,49,50,51,52}. Experimental schemes based on pathentangled photons use the induced quantum coherence of single (signal) photons generated from two spontaneous parametric downconversion (SPDC) crystals, where the induced coherence resulted from erasing the whichpath information of their conjugate (idler) photons^{53}. The degree of induced coherence for the signal photons has a critical dependence on the degree of whichpath information for the idler photons, which is a unique feature of nonclassicality. Therefore, by placing an optical material on the idler pathway, the degree of pathindistinguishability for the generated idler photons, which depends on the amplitude and phase change of the transmitted idler field, can be controlled, and consequently the visibility of the interference fringe of the conjugate signal photons can be modulated in an unheralded way. This method utilizing the signalidler quantum entanglement enables material properties to be measured separately from probing the material via idler photon–matter interaction.
In this paper, we demonstrate experimentally and explain theoretically that, by combining the frequency comb technology and the quantum optical measurement method with undetected photons, frequency comb singlephoton interferometry (FCSPI) is feasible. This shows that the quantum interference of signal singlephoton frequency combs can be produced by erasing the whichpath information of idler photons by making the idler singlephotonadded states indistinguishable. Because the quantum state of FCSPI has high dimensionality with multiple frequency comb components, we believe that the present work paves the way for singlephoton interferometry to be applicable to not only quantum information science, but also quantum metrology through quantum spectroscopy and imaging experiments.
Results
Schematic description of FCSPI
A schematic diagram of the FCSPI experimental setup is presented in Fig. 1a. A Yb fiber laser frequency comb at 1060 nm is frequency doubled via secondharmonic generation (SHG) to produce an OFC with a center wavelength of 530 nm. Interferometry involves two stimulated parametric downconversions (StPDCs), where the SHG comb is used as a pump and an additional ultranarrow linewidth (1 Hz) CW laser at an idler wavelength of 1542 nm is used as a seed beam stimulating multiple frequency comb components at the signal wavelength. Although the PDCs are stimulated by the CW seed beam, the corresponding singlephoton emission efficiency is still very low, meaning the multiphoton generation by each StPDC can be safely ignored. The firstorder coherence of the signal field is induced by erasing the idler path information. Signal photons (at around 807 nm) are generated from each of the two nonlinear crystals (periodically poled lithium niobate; PPLN) and in turn combined at a beam splitter (BS) placed in front of the spectrometer. Therefore, the doublepathway configuration from the polarizing BS (PBS) separating the SHG comb into two (upper and lower) paths to the beamcombining BS can be considered modified quantum Mach–Zehnder interferometry (a more detailed description is provided in the “Methods).
In the lowcoupling regime of the well known and widely used SPDC process with a CW laser pump, the probabilistic photon detection of the BS outputs is dominated by single photons from the generated signal field, which are entangled with conjugate idler photons, thus providing a means of heralded singlephoton detection. The pathentangled photon pairs from the signal and idler modes exhibit phase coherence in twophoton interference (fourthorder interference in an electric field), as manifested by coincidence counting rate measurements^{54}. However, neither the signal nor the idler field exhibits any onephoton interference (secondorder interference in an electric field) patterns. Interestingly, only when the whichpath information of the conjugate idler photons is erased does the singlephoton coherence of the signal field appear. This can be achieved either by making the two paths of the idler photons indistinguishable by perfectly aligning the two idler beams^{53,55} or by making the photon statistics of the idler fields indistinguishable by injecting a coherent laser at the idler field frequency^{55,56,57} without heralding idler detection. The latter scheme is used in our experiment (Fig. 1a); the singlephoton coherence of the signal fields on two different paths is induced via the indistinguishability of the two singlephotonadded coherent states (SPACS)^{58} of the idler photons from the two StPDC crystals pumped by the SHG frequency comb light.
In this way, we demonstrate that singlephoton interferometry with a quantum frequency comb is feasible without detecting heralded single photons. The quantum state generated by the two StPDC crystals is a pathentangled frequency comb singlephoton state (Fig. 1b). The frequencyencoded multidimensional singlephoton state can be confirmed by changing one of the two signal paths by means of displacing the retro reflector mirror by the distance traveled by light for the time interval (ΔT) between successive pulses (Fig. 1a). The signal fields generated from the two StPDC crystals pumped by different pump pulses are then overlapped in the BS. In our experiments, we observe a strong interference pattern with a high visibility of about 0.87. This suggests that the coherence time between the single photons passing through either the short or long path is much longer than the pulsetopulse time interval (ΔT) and thus the induced coherence of the timebin photonic state persists longer than the pulse time interval. As shown below, the high visibility of the timedelayed singlephoton interference is due to the exceptionally high coherence of the signal optical frequency comb. For this experiment, we constructed highly coherent singlephoton frequency combs at the signal wavelengths from the two StPDC crystals arranged in parallel and pumped simultaneously by the same phasestabilized frequency comb laser and 1Hz CW seed laser.
We note that the degree of induced singlephoton coherence for the signal field can be modulated by the transmission coefficient of the optical sample interacting with one of the injected seed beams (Fig. 1a) because the degree of indistinguishability between the two idler fields generated by the StPDC crystals depends on the optical sample’s spatial or spectral characteristics. Furthermore, the phase information of the idler photon state can be transferred to the signal field state by means of quantum frequency conversion^{27,28,59,60,61}. This is one of the important features of our proposed frequency comb singlephoton interferometry involving two StPDC crystals that differentiates it from ordinary Mach–Zehnder singlephoton interferometry with just one singlephoton source. This double singlephoton source configuration allows the concept of quantum imaging and quantum spectroscopy with undetected photons to be implemented by inducing or modulating the intensity and phase imbalances of the two coherent CW seed beam paths.
Theoretical description of optical frequency comb and stimulated PDC
The OFC pump is a train of coherent pulses with carrier frequency ω_{p} = 2πf_{p}. The time interval between neighboring pulses is denoted as ΔT. The carrierenvelopoffset (CEO) phase shift between successive pulses is Δφ_{ceo} in the time domain. Equivalently, in the frequency domain, the OFC is a multifrequency field completely specified by the frequency interval between neighboring comb teeth that is given by f_{r} = 1/ΔT and a CEO frequency of f_{ceo} = f_{r}Δφ_{ceo}/2π^{62}. The simultaneous stabilization of both f_{r} and f_{ceo} is required for the OFC. The pulse train of our OFC is linearly polarized and propagates along the z axis. The electric field of the pulse train at z = 0 can then be written as^{63} (see Supplementary Note 1)
The pump comb frequencies are ω_{p,n} = ω_{p} + 2πnf_{r} for integer n, where the carrier frequency is ω_{p} = 2π(n_{c}f_{r} + f_{ceo}) with mode number n_{c}. The nth Fourier coefficient in Eq. (1) is given by \(A_n = \left( 1 / {\Delta T} \right) {\int}_{  \infty }^\infty {A(t)e^{  i2\pi n{\kern 1pt} t/\Delta T}{\rm{d}}t}\). Assuming that each pulse envelop is a Gaussian pulse, i.e., \(A(t) = {E}_{0}\exp \left( {  t^2{\mathrm{/}}2\delta ^2} \right)\), where δ is the pulse width, we have \(A_n = {E}_{0}\sqrt {2\pi } \delta {\mathrm{/}}\Delta T\exp (  2n^2\pi ^2\delta ^2{\mathrm{/}}\Delta T^2)\). When the input signal photon is in a vacuum state and the input idler photon is in a coherent state with frequency ω_{i}, where the seed laser is a monochromatic CW laser with amplitude α(ω_{i}) at frequency ω_{i} = ω_{seed}, the initial state can be written as \(\left {\psi (0)} \right\rangle = \left 0 \right\rangle _{s}\left {\alpha (\omega _{i})} \right\rangle _{i}\). The quantum state after a single StPDC crystal according to the perturbation theory is then given by
where \({\mathrm F}(\omega _{s,n},\omega _i)\) is a joint spectral function (Supplementary Note 1)^{64} and \(\left {\omega _{s,n}} \right\rangle _s\) represents the singlephoton Fock state of the nth mode in the signal field with frequency ω_{s,n} = ω_{p,n} − ω_{i}. The quantum state in Eq. (2) clearly shows not only the comb structure of the singlephoton signal field, but also the SPACS of the idler field at the injection frequency of ω_{i}. Here, the mode number n in ω_{s,n} of the signal frequency comb or its spectral bandwidth is mainly limited by the phasematching condition of the nonlinear crystal used.
Theoretical description of FCSPI
We next describe the working principle behind the singlephoton interferometry that is experimentally demonstrated in this study. Two identical StPDC crystals with exactly the same OFC pump and CW seed beams generate photons in the same quantum state described in Eq. (2). The composite quantum state at time t is given by \(\left {\psi (t)} \right\rangle = \left {\psi (t)} \right\rangle _1 \otimes \left {\psi (t)} \right\rangle _2\). It is assumed that the phasematching condition (Δk ≈ 0) at each StPDC crystal is perfect. In this case, the joint spectral function is approximated as \({\mathrm F}\left( {\omega _s,\omega _i} \right) \approx g_jtA_{j,n}\), where j ∈ {1,2} is the path index of the output fields (Supplementary Note 1). In the low StPDC efficiency regime, which is the case of our experiment, we have g_{j}tA_{j,n}^{2}α_{j}(ω_{i})^{2} << 1 . The composite quantum state can be written up to the first order in the coupling constant as
where \(\hat a_{i_j}^\dagger\) (\(\hat a_{i_j}^{}\)) is the creation (annihilation) operator of the idler photon on the jth path. Here, the probability of generating two pairs of signalidler photons from a single StPDC crystal is negligible because g_{1}g_{2}A_{1,n}A_{2,n}t^{2}^{2}α_{1}^{2}α_{2}^{2} <<1.
After combining the signal fields with the BS of our modified quantum Mach–Zehnder interferometer, the singlephoton counting rate of the signal field is measured, which is given by \(R_s = \left\langle {\psi (t)} \rightE_s^  E_s^ + \left {\psi (t)} \right\rangle\), where \(E_s^ + = \mathop {\sum}\limits_n {e^{i\varphi _{s_1}}\hat a_{s_1}^{}(\omega _{s,n}) + e^{i\varphi _{s_2}}\hat a_{s_2}^{}(\omega _{s,n})}\) and \(\hat a_{s_j}^{}\) (\(\hat a_{s_j}^\dagger\)) is the annihilation (creation) operator of the signal photon on the jth path. We further assume that the pump beams at the two nonlinear crystals have the same amplitudes but different phases, i.e., \(A_{1,n} = \left {A_n} \righte^{i\varphi _{p_1}}\) and \(A_{2,n} = \left {A_n} \righte^{i\varphi _{p_2}}\). Here, we specifically consider the case where the two seed beams at the two crystals have different phases and amplitudes, i.e., \(\alpha _1(\omega _i) = \left {\alpha (\omega _i)} \righte^{i\varphi _{i_1}}\) and \(\alpha _2(\omega _i) = \left {T(\omega _i)\alpha (\omega _i)} \righte^{i\varphi _{i_2}}\), where T(ω_{i}) is the amplitude transmission of the optical sample (Fig. 1a). The singlephoton counting rate at the photonnumber sensitive detector is then found to be
where \(\Delta \varphi _j = \varphi _{j_2}  \varphi _{j_1}\) for j = pump (p), signal (s), and seed (derivation in Supplementary Note 2). Equation (4) shows that the singlephoton (second order in the field) interference fringe depends on all the phase differences of the pump, signal, and idler fields in the interferometer. The visibility of the singlephoton interference is obtained as
Given the classical limit in which the average photon number of the seed laser is very large, i.e., α^{2} > > 1, the visibility in Eq. (5) reduces to 2T(ω_{i})/(1 + T(ω_{i})^{2}), which shows that the visibility becomes a function of T(ω_{i}) and it is always unity for T(ω_{i}) = 1.
Complementarity relation, indistinguishability, and visibility
In the proposed frequency comb singlephoton interferometry, the coherence of the signal fields in the two paths is induced via the indistinguishability of the two conjugate idler fields that are in either an unchanged injected coherent state, \(\left \alpha \right\rangle\), or the SPACS, \(\hat a_{}^\dagger \left \alpha \right\rangle\). When the coherent seed laser has a very large average photon number, i.e., α^{2} > > 1, it is not possible to distinguish between the two cases where a single photon is added either to the coherent seed beam in the upper path or to that in the lower path.
To further quantify this argument, let us consider the experimental situation in more detail. For the sake of notational simplicity, let us denote the coherent state and the singlephoton state as \(\left \alpha \right\rangle\) and \(\left 1 \right\rangle\), respectively. The SPACS of the idler beam after one of the two StPDC crystals is defined as \(\left {\alpha _j,1} \right\rangle = \hat a_j^\dagger \left {\alpha _j} \right\rangle /\sqrt {1 + \alpha _j^2}\) for j = 1 and 2. The overlap (F) between the two idler states \(\left {\alpha _1,1} \right\rangle _{i_1}\left {\alpha _2} \right\rangle _{i_2}\) and \(\left {\alpha _1} \right\rangle _{i_1}\left {\alpha _2,1} \right\rangle _{i_2}\) created by the two nonlinear crystals is given by
As both α_{1}^{2} and α_{2}^{2} increase, overlap F approaches unity. Therefore, it becomes in principle impossible to discriminate between a single photon being added to the idler field on the upper path and one being added to the idler field on the lower path. In other words, the critical whichpath information of the SPACS in the idler fields is erased due to the indistinguishability within the photon statistics. This is the origin of the induced coherence in the singlephoton doubleslit experiment implemented using the proposed frequency comb singlephoton interferometry with two StPDC crystals working in the quantum mechanical regime.
To examine the relationship between indistinguishability and complementary, in this subsection we assume a monochromatic signal field for notational simplicity. When an optical sample with transmission coefficient T is on the seed beam (upper) path 2 (Fig. 1a), the quantum state of the signal and idler photons in our interferometer can be written as
When the upper seed beam path (Fig. 1a) is blocked, i.e., T = 0, \(\left {T\alpha ,1} \right\rangle = \left 1 \right\rangle\) and the overlap F vanishes, which means that the source of a singlephoton generation, either from crystal 1 or crystal 2, can be completely distinguishable. Therefore, when T = 0, there is no coherence between the corresponding two signal beams, which leads to zero visibility. Now, consider T = 1, where the two seed beams have equal amplitudes α for both paths. In this case, the firstorder interference between the signal single photons from the two independent sources (crystals 1 and 2) would exhibit visibility V = α^{2}/(1 + α^{2}). For a more general case of a finite T, the visibility is V = 2Tα^{2}/(2 + α^{2} + Tα^{2}). Because visibility V (wave nature) and distinguishability K (particle nature) should satisfy the complementary relation, i.e., V^{2} + K^{2} = 1^{65,66}, the distinguishability between the signal photons from the two StPDC crystals is given by
The detailed derivation of Eq. (8) can be found in the “Methods” section. Equation (8) clearly indicates that the signal photon generated by the upper StPDC can be completely distinguishable from that by the lower StPDC when no coherent seed beams are injected into the PDC crystals in the stimulating process.
Signal field interference measurements
To examine the induced coherence of the signal fields, we measured their firstorder singlephoton interference. The singlephoton counting rate given in Eq. (4) predicts perfect interference with V = 1 given that α^{2} > > 1. To adjust the path lengths or equivalently the relative phase differences of the pump, seed, or signal beams in the two paths, three piezoelectric transducers (PZTs) were used (Fig. 1a). To obtain highcontrast interference fringes, we optimized the spatial and temporal modes of the two signal beams and overlapped the singlephoton spectra in the two paths, with the corresponding spectrum measured using the spectrometer and EMCCD with an instrumentlimited spectral width of 0.1 nm (Supplementary Note 3). Here, the spectrum of each signal beam at around 807.2 nm could be finely tuned by adjusting the phasematching temperature of the PPLN crystal. To confirm the maximum spectral overlap between the two signal fields, we compared our experimental data with analytic values from the Sellmeier equation for the PPLN crystal (Supplementary Note 3 and Supplementary Fig. 1). Unlike previous work that has used CW lasers, the generated signal field also has an optical frequency comb structure with exactly the same repetition rate f_{r} as the pump frequency comb (Supplementary Notes 1 and 4). Therefore, it should be emphasized that the perfect spectral overlap of the signal beams from the two StPDC crystals is critical to the measurement of the singlephoton interference fringe whose visibility is close to unity (Supplementary Note 4).
In Fig. 2a, the experimentally measured singlephoton counting rate R_{s}, where the EMCCD exposure time was set to 10 ms, is plotted against the pathlength differences Δx_{p}, Δx_{s}, and Δx_{seed}, which are related to the corresponding phase differences as Δφ_{m} = 2πΔx_{m}/λ_{m} (for m = p, s, and seed). In all three cases, the fringe visibility is close to 1.
Stimulated PDC efficiency
To carry out FCSPI experiments in a very low parametric downconversion regime where the number of signal photons generated by one pump pulse is much smaller than unity, we attenuated the 530 nm pump power (3.5 mW) and the intensity of the seed beam (4 mW). From Fig. 2a, the singlephoton counting rate is about 1 million photons per second with a 10 μm width slit placed in front of the spectrometer (reducing the intensity to 1%). It should be mentioned that the EMCCD with an integration time of 10 ms integrates signals over 2.5 × 10^{6} pulses. Without phase coherence between pulses, the interference fringe should be washed out due to fluctuations in the pulsetopulse phase difference Δφ_{ceo} because the integration time (10 ms) of the detector is much longer than the pulse interval ΔT (4 ns). This clearly shows the absolute necessity of OFC for the pump in our FSSPI. From the measured singlephoton counting rate, the StPDC efficiency of each nonlinear crystal can now be estimated as η_{StPDC} ≈ 5.2 × 10^{−10}. Consequently, the possibility of each StPDC crystal generating two or more pairs of signal and idler photons can be safely ignored and the photon detection at the BS output is truly dominated by singlephoton events. Furthermore, noting that the repetition rate f_{r} of the pump beam is 250.0 MHz, the filling factor per pulse is ~0.02, which means that each generated signal pulse contains 0.02 photons.
In addition, we measure the spontaneous PDC efficiency of our nonlinear crystals and find that η_{SPDC} ≈ 5.3 × 10^{−12}. Thus, by using the relation between η_{StPDC} and η_{SPDC}, i.e., η_{StPDC} ≈ η_{SPDC}(α^{2} + 1), the average photon number of the coherent seed beam is found to be α^{2} ≈ 97. This experimentally measured average photon number is consistent with the value calculated by considering the effective seed beam power. Although the injected seed beam power at each arm is about 4 mW (~10^{16} photons/s), only a fraction (2.1 × 10^{−3}) of the incident CW seed photons contributes to the StPDC process at each nonlinear crystal because the StPDC process most effectively occurs when the CW seed beam and each pump pulse overlap spatially and temporally. Noting that the repetition rate of the pump pulses and the temporal width of each pump pulse are 4 ns (= 1/f_{rep}) and 8.4 ps, respectively, the number of effective seed beam photons should be in the order of 10^{13} photons/s (≈ 10^{16} photons/s × 8.4 ps × f_{rep}). The average photon number of the injected seed beam per unit of downconverted bandwidth can thus be estimated as \(\left \alpha \right^2 \approx \frac{{{\rm{Average}}\;{\rm{photon}}\;{\rm{number}}\,{\mathrm{/}}{\rm{s}}}}{{{\rm{bandwidth}}}}\sim 10^2\), where the bandwidth of the idler beam is ~50 GHz, which corresponds to the frequency resolution (0.1 nm) of our spectrometer on the signal beam path. This numerical calculation for the average photon number of the seed beam is in quantitative agreement with our experimentally measured values from the spontaneous and stimulated PDC efficiencies. Thus, the experimentally measured signal field interference in Fig. 2a is in a deep singlephoton regime in which the idler whichpath information is erased because α^{2} > > 1.
Quantum optical measurement with undetected photons
Although a few different research groups have employed experimental setups similar to ours and have already demonstrated quantum spectroscopy or quantum imaging with undetected photons, the FCSPI method has not been developed for quantum optical measurement with undetected photons. Here, the visibility V is measured for different values of the amplitude transmission coefficient T of the optical sample placed on one of the seed beam paths, which in turn modulates the distinguishability of the two idler fields after the nonlinear crystals (Fig. 1a). A variable neutral density filter (VND) was used to change T experimentally. Figure 2b depicts the experimentally measured visibility with respect to T. The solid line is the theoretical prediction, i.e., V = 2T/(1 + T^{2}). The agreement between the experimental data and the theory is very close, clearly indicating that the FCSPI is a useful quantum optical measurement method for detecting sample transmission coefficient T at the wavelength of undetected idler photons by measuring the visibility of the signal singlephoton interference. The observation that the visibility depends only on T is consistent with the fact that the average photon number of the coherent seed beam is much larger than unity, i.e., α^{2} > > 1.
Distinguishability of idler photons with an attenuated CW seed laser
Within the quantum description of the doubleStPDC scheme, the visibility of signal onephoton interference is also related to the average photon number of the injected seed beam in idler mode (Eq. 5). This is because the visibility of signal onephoton interference corresponds to the indistinguishability (F) of the idler photons generated by the two NL crystals (Eq. 6). To confirm that this quantum optical description of singlephoton interferometry is valid even with a pulsed (frequency comb) pump and a highly coherent seed laser in a significantly lowcoupling regime compared to previous work^{57}, we carried out a series of visibility measurements by attenuating the injected seed laser intensity with a variable neutral density (VND) filter for balanced seed beams (T = 1), where the seed beam intensities at the two NL crystals are the same. Our experimentally measured visibilities are quantitatively describable by theory, i.e., V = α^{2}/(1 + α^{2}), as can be seen in Fig. 3. This indicates that our experiment occurs in a regime that can be only explained using a quantum mechanical description^{56,57}.
Comb structure of generated signal photons
Despite the high visibility of the signal field interference, the nature of the generated signal photons needs to be characterized. More specifically, to confirm that each StPDC generates signal photons with a comb structure in the frequency domain, the spectral width of the resulting signal pulse in the time domain needs to be measured. This first requires the estimation of the temporal width of each pump pulse, which is achieved by monitoring the variation in the interference envelop as a function of the pump beam path difference Δx_{p} (Fig. 4a). The experimental results suggest that the Gaussian pulse width (FWHM) of each pump is 8.4 ps, which results in the optical bandwidth of the pulse being 52.3 GHz. Therefore, there are ~209 modes (comb teeth) in the generated signal frequency comb.
Here, the linewidth of an individual comb tooth of the signal singlephoton frequency combs from each PPLN crystal can be measured using (i) a stronger pump beam than the one used for FCSPI to enhance the signaltonoise ratio and (ii) a fast photodiode detector (see Supplementary Fig. 2). The linewidth of a signal comb tooth is estimated to be about 1 Hz, which is limited by the frequency resolution of the RF spectrum analyzer used here. The measured combtooth linewidth (<1 Hz) is almost five orders of magnitude narrower than that of the pump frequency comb, whose linewidth is about 100 kHz. This dramatic narrowing in the linewidth of the generated signal comb teeth is due to the stimulated emission process in the StPDC crystal with the exceptionally narrow (1 Hz) CW seed laser. Therefore, the revival of coherence when the pathlength difference is an integer multiple of 1.2 m can be observed in the interference fringe even when the interference pattern is obtained by accumulating over 1 million photons with time delays up to the coherence time (1 s), which is the inverse linewidth (1 Hz) of each signal singlephoton frequency comb tooth (Supplementary Note 4).
Longterm coherence of FCSPI
The path lengths of the two arms in our modified quantum Mach–Zehnder interferometer were adjusted to be the same in the above FCSPI measurements (see Supplementary Note 5 and Supplementary Fig. 3). However, to measure the timebin coherence of the FCSPI, we deliberately increased the length of the lower signal beam path by 1.2 m. In contrast to the widely used method to generate timebin photonic states, we did not use beam splitters to split a single pulse from a conventional modelocked laser into multiple pulses. The pulse trains here were generated by two different PPLN crystals and they propagate along two different paths, which critically differ from the case in which a single pulse is spatially split into two (or multiple) pulses. In our doubleStPDC interferometer, the seed laser with a frequency in idler mode is a highly coherent CW beam with an exceptionally narrow (1 Hz) linewidth and the frequency comb pump laser is highly phasestabilized, with both the repetition rate and the CEO frequency precisely and actively stabilized with reference to the GPSdisciplined Rb atomic clock. Consequently, the pump beam has a phase coherence that is maintained over the entire train of pulses within the 10ms detector exposure time used in our experiment. Therefore, the singlephoton interference between the (n + m)th pulsed signal field from PPLN1 (nonlinear crystal 1) and the nth pulsed signal field from PPLN2 is expected to be observed when the pathlength difference is adjusted to be m×cΔT (m is the difference integer). In the present work, we set m = 1 (Fig. 1a) and found that the visibility is still very high, i.e., 0.87 (see Fig. 4b). We attribute this slight reduction in visibility to a nonzero (20 MHz) CEO phase. In measuring the visibility of each signal path difference (Δx_{s}) near m = 1 in Fig. 4b, about 5 × 10^{4} signal photons are detected during each detector exposure period (10 ms) while the pump path difference is periodically modulated. We estimate that, in our extremely lowcoupling regime, only one photon can be found approximately every 50 pulses generated from each StPDC crystal. Thus, the filling factor is estimated to be 1/50. When the detection period is as long as 10 ms, it is impossible to measure singlephoton interference between the successive pulses with high visibility, e.g., 0.87, if a conventional modelocked laser is used without the active phaselocking of f_{ceo}. This is because the phasecoherence time of a typical modelocked laser is several orders of magnitude shorter than that of our frequency comb laser.
Furthermore, we demonstrate that the visibility of our singlephoton interferometer for varying interpulse time differences or pathlength differences has a critical dependence on the phase noise (or linewidth) of the generated signal frequency comb teeth. Indeed, the linewidth of the RF beat notes of the generated frequency comb at the signal wavelength exhibits an instrumentlimited linewidth of about 1 Hz, which is comparable to that of a highly coherent seed laser (see Supplementary Fig. 2). Thus, we believe that the longterm phase coherence of the StPDCgenerated signal photon frequency comb at the singlephoton level is a prerequisite for the present FCSPI. The quantum state of the signal field generated by each PPLN crystal is indeed a singlephoton frequencyencoded qudit. The singlephoton interference revival shown in Fig. 4b is the key measurement confirming that a singlephoton frequency qudit state is generated.
By following Islam et al. (refs^{67},^{68}), the number of timebin bases in our system can be increased by adding more nonlinear crystals in a parallel configuration and maintaining pathlength differences between signal photons generated from two different crystals to be an integer multiple of cΔT. This is currently under investigation. Nonetheless, it is well known that quantum communication technology requires a robust system for longdistance optical fiber communication with minimized decoherence. Thus, it would be desirable to develop multidimensional qudit technology for quantum communication with highrate data processing^{67,68,69}. In this regard, it is believed that the frequencyencoded highdimensional singlephoton state demonstrated here could be a useful framework for the future development of fast, robust, secure, and efficient quantum communication technology.
Discussion
In this study we have demonstrated frequency comb singlephoton interferometry using a pair of pathentangled photons. Coherence between the two StPDCgenerated signal fields can be induced by making their conjugate idler photon statistics indistinguishable, which is in contrast to previously reported quantum spectroscopy^{46} and imaging^{47} schemes based on induced coherence via the indistinguishability of idler beam paths. The succinct expression of this generated signal singlephoton frequency comb state is \(\left \psi \right\rangle _s = \mathop {\sum}\nolimits_{n = 1}^N {C_n\left( {\left {\omega _{s,n}} \right\rangle _1\left 0 \right\rangle _2 + C^\prime e^{i\Delta \phi }\left 0 \right\rangle _1\left {\omega _{s,n}} \right\rangle _2} \right)}\), which is a frequencyencoded pathentangled singlephoton state. Here, we found that the mode number of the signal frequency comb is N ≈ 209 with a frequency of ω_{s,n} and the same frequency interval of ω_{r} as the pump frequency comb. The frequency degrees of freedom of the generated multimode singlephoton state could be accessible in quantum information technology if combtoothresolved detection becomes possible in the future, something which can be realized with a frequency comb pump laser with a high repetition rate. In the present work, we have demonstrated that the coherence of generated signal field frequency modes can be verified in the time domain by measuring the singlephoton interference revivals with imbalanced (in arm length) FCSPI.
Because the amplitude and phase of the signal comb state can be modulated by the intensity imbalance and/or the pathlength difference of the seed beams, it could be possible to engineer a quantum state of photons remotely with differently colored conjugate photons based on the concept of quantum imaging and quantum spectroscopy with undetected photons^{46,47,48,49,50}. Therefore, we anticipate that our FCSPI utilizing photons in a frequencyencoded multidimensional qudit state has potential applications in (i) remote quantum measurement with undetected photons, (ii) longdistance remote quantum state engineering by means of frequency conversion, and (iii) quantum information science and technology that requires high dimensionality to increase key rates (refs.^{23,28,40,67,68} and references therein) and that requires long coherence length and highdimensional photons for decoherencefree, efficient, and secure communication based on highrate data processing with the capability of frequency resolving all of the comb teeth.
Here, we also demonstrate that timebin qubit state measurement is feasible by simply modifying the interferometer setup to have an armlength difference that is an integer multiple of the pulsetopulse separation, which is possible due to the exceptionally longterm phase coherence and intrinsic frequency scalability of the generated signal frequency comb. This longterm phase coherence of a singlephoton pulse train can be of use when conducting timedomain double or multipleslit experiments with single photons without a Franson interferometer. The high dimensionality of the frequencyencoded photonic state in our FCSPI can overcome a critical limitation of conventional quantum telecommunication technology: the utilization of a pulsed laser with limited phase stability. Nonetheless, a challenging issue related to the degree of coherence of a signal singlephoton frequency comb with a critical dependence on the phase coherence of the pump and seed beams remains to be overcome. Thus, we are currently investigating the effects of the linewidth of a CW seed laser and of the phase noise of a pump frequency comb on the visibility of FCSPI.
We anticipate that FCSPI with frequency comb photons at the singlephoton level could be useful in a variety of applications in quantum information science because it consists of pathentangled and frequencyencoded qudits that are modulated by undetected photons. In addition, the FCSPI developed and experimentally demonstrated here can be used to study the fundamental physics of quantum entanglement and to develop novel quantum optical measurement methods with undetected photons, where only the onephoton interference of the signal fields needs to be measured without heralded detections of the entangled idler fields.
Methods
Experimental details
A schematic diagram of our singlephoton interferometer is given in Fig. 1a. An optical frequency comb (Menlo Systems) at 1060 nm with a spectral bandwidth of 46 nm is frequency doubled using an LBO crystal. The secondharmonicgenerated beam with a center wavelength of 530 nm is used to pump the two StPDC crystals. The repetition rate f_{r} and carrieroffset frequency f_{ceo} of the frequency comb are phaselocked to be 250.0 MHz and 20.0 MHz, respectively, with reference to a GPSdisciplined Rb atomic clock. The spectral width of the pump beam at 530 nm, which is estimated to be about 3 nm, is much narrower than that of the injecting OFC beam due to the noncritical phasematching bandwidth of the LBO crystal at 143 °C and the output power is 7 mW. The pump beam is divided into two paths using a combination of a halfwave plate and PBS. The PDC crystal is periodically poled lithium niobate (PPLN) with type0 phasematching, a size of 15 × 7.9 × 0.5 mm^{3}, and a grating width of 7.3 μm. A stream of entangled singlephoton pairs, each consisting of a signal photon and an idler photon, are then generated from both crystals through the SPDC process at a phasematching temperature of 121.5 ^{o}C. The emitted SPDC signal photons have a broad bandwidth of over 20 nm.
In the present work, to build a singlephoton frequency comb interferometer, we inject a monochromatic laser with a linewidth of 1 Hz (OE waves) along the two paths of the pump beams using two dichroic beam splitters (DM in Fig. 1a). The wavelength of the seed laser is 1542.384 nm. Because the seed beam frequency overlaps with the emission spectrum of the idler photons generated from the PDC crystals, the PDC processes at the two crystals are stimulated. After each StPDC crystal, only the signal field in a singlephoton state with a wavelength of 807.2 nm is transmitted through the DM, and the pump and seed beams and generated idler photons are all reflected by the DM. Finally, a beam splitter (BS) combines the signal photons generated from the two StPDC crystals. Singlephoton statistics and singlephoton interference fringes at both exit ports of the interferometer are measured with a singlephotonsensitive twodimensional EMCCD camera (Andor Technology) attached to the output port of a spectrometer (Shamrock SR303iB, Andor Technology) with a wavelength resolution of 0.1 nm.
Complementary relation
Based on the quantum state in Eq. (7), the reduced density matrix for the signal photon state is written as
where
and
The distinguishability^{65,66} is then given by
where the normalization factor C^{2} = [(1 + α^{2}) + (1 + Tα^{2})]^{−1}. Using Eq. (9), we obtain visibility V and distinguishability K, and confirm the complementary relationship discussed in the main text.
Data availability
The data that supports the findings of this study are available from the corresponding authors on request.
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Acknowledgements
We thank Prof. M. Choi for stimulating discussion on singlephoton interferometry. This work was supported by IBSR023D1
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M.C. and T.H.Y. conceived this experiment. S.K.L. developed the idea, performed theoretical analysis, experiment, and data analysis. N.S.H. helped the experiment of RF spectrum analysis. All the authors interpreted experimental results and wrote the manuscript.
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Lee, S.K., Han, N.S., Yoon, T.H. et al. Frequency comb singlephoton interferometry. Commun Phys 1, 51 (2018). https://doi.org/10.1038/s4200501800512
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DOI: https://doi.org/10.1038/s4200501800512
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