Abstract
The faithful storage and coherent manipulation of quantum states with mattersystems would enable the realization of largescale quantum networks based on quantum repeaters. To achieve useful communication rates, highly multimode quantum memories are required to construct a multiplexed quantum repeater. Here, we present a demonstration of ondemand storage of orbitalangularmomentum states with weak coherent pulses at the singlephotonlevel in a rareearthiondoped crystal. Through the combination of this spatial degreeoffreedom (DOF) with temporal and spectral degrees of freedom, we create a multipleDOF memory with high multimode capacity. This device can serve as a quantum mode converter with high fidelity, which is a fundamental requirement for the construction of a multiplexed quantum repeater. This device further enables essentially arbitrary spectral and temporal manipulations of spatialqutritencoded photonic pulses in real time. Therefore, the developed quantum memory can serve as a building block for scalable photonic quantum information processing architectures.
Introduction
Largescale quantum networks would enable longdistance quantum communication and optical quantum computing^{1,2,3}. Due to the exponential photon loss in optical fibers^{4}, quantum communication via groundbased optical fibers is currently limited to distances of hundred of kilometers. To overcome this problem, the idea of quantum repeater^{5,6} has been proposed to establish quantum entanglement over long distances based on quantum memories and entanglement swapping. It has been shown that to reach practical data rates using this approach, the most significant improvements can be achieved through the use of multiplexed quantum memories^{7,8,9}.
The multiplexing of quantum memories can be implemented using any degreeoffreedom (DOF) of the photons, such as those in the temporal^{10}, spectral^{11}, and spatial^{12} domains. Rareearthiondoped crystals (REIC) offer interesting possibilities as multipleDOF quantum memories for photons by virtue of their large inhomogeneous bandwidths^{11,13,14} and long coherence time^{15} at cryogenic temperatures. Recently, there have been several important demonstrations using REIC, such as the simultaneous storage of 100 temporal modes^{16} by atomic frequency comb (AFC)^{17} featuring preprogrammed delays, the storage of tens of temporal modes by spinwave AFC with ondemand readout^{18,19,20,21,22} and the storage of 26 frequency modes with feedforward controlled readout^{11}. The orbitalangularmomentum (OAM) of a photon receives much attention because of the high capacity of OAM states for information transmission and spatial multimode operations^{23}. Tremendous developments have recently been achieved in quantum memories for OAM states^{24,25,26}, paving the way to quantum networks and scalable communication architectures based on this DOF.
To date, most experiments with quantum memories have been confined to the storage of multiple modes using only one DOF, e.g., temporal, spectral, or spatial. To significantly improve the communication capacity of quantum memories and quantum channels, we consider a quantum memory using more than one DOF simultaneously^{11,27,28,29}.
Here, we report on the experimental realization of an ondemand quantum memory storing single photons encoded with threedimensional OAM states in a REIC. We present the results of a multiplexed spinwave memory operating simultaneously in temporal, spectral and spatial DOF. In addition to expanding the number of modes in the memory through parallel multiplexing, a quantum mode converter (QMC)^{30} can also be realized that can perform mode conversion in the temporal and spectral domains simultaneously and independently. Indeed, our quantum memory enables arbitrary temporal and spectral manipulations of spatialqutritencoded photonic pulses, and thus can serve as a realtime sequencer^{14}, a realtime multiplexer/demultiplexer^{31}, a realtime beam splitter^{32}, a realtime frequency shifter^{33}, a realtime temporal/spectral filter^{31}, among other functionalities.
Results
Experimental setup
A scheme of our experimental setup and relevant atomic level structure of Pr^{3+} ions is presented in Fig. 1. The memory crystal (MC) and filter crystal (FC) used in this setup are 3 × 6 × 3 mm crystals of 0.05% doped Pr^{3+} :Y_{2}SiO_{5}, which are cooled to 3.2 K using a cryogenfree cryostat (Montana Instruments Cryostation). In order to maximize absorption, the polarization of input light is close to the D_{2}axis of Y_{2}SiO_{5} crystal. To realize reliable quantum storage with high multimode capacity, we created a highcontrast AFC in MC (the AFC structure is shown in Supplementary Note 1). Spinwave storage is employed to enable ondemand retrieval and extend storage time^{17}. The control and input light are steered towards the MC in opposite directions with an angular offset ~4^{°} to reject the strong control field and avoid the detection of free induction decay noise^{34}. To achieve a low noise floor, we increase the absorption depth of the FC by employing a doublepass configuration. Figure 2a presents the time histograms of the input photons (blue) and the photons retrieved at 12.68 μs (green) with a spinwave storage efficiency η_{SW} = 5.51%. For an input with a mean photon number μ = 1.12 per pulse, we have measured a signaltonoise ratio (SNR) ~39.7 ± 6.7 with the input photons in the Gaussian mode.
Quantum process tomography
The ability to realize the ondemand storage of photonic OAM superposition states in solidstate systems is crucial for the construction of OAMbased highdimensional quantum networks^{24}. Quantum process tomography for qutrit operations^{35} benchmarks the storage performance for OAM qutrit in our solidstate quantum memory. The qutrit states are prepared in the following basis of OAM states: \(\left {{\mathrm{LG}}_{p = 0}^{l =  1}} \right\rangle\), \(\left {{\mathrm{LG}}_{p = 0}^{l = 0}} \right\rangle\), \(\left {{\mathrm{LG}}_{p = 0}^{l = 1}} \right\rangle\). Here, \(\left {{\mathrm{LG}}_p^l} \right\rangle\) corresponds to OAM states defined as LaguerreGaussian (LG) modes, where l and p are the azimuthal and radial indices, respectively. In the following, we use the kets L〉, G〉, and R〉 to denote the OAM states \(\left {{\mathrm{LG}}_{p = 0}^{l = 1}} \right\rangle\), \(\left {{\mathrm{LG}}_{p = 0}^{l = 0}} \right\rangle\), and \(\left {{\mathrm{LG}}_{p = 0}^{l =  1}} \right\rangle\), respectively. For μ = 1.12, we first characterized the input states before the quantum memory using quantum state tomography (see Methods section for details). The reconstructed density matrices of input are not ideal because of imperfect preparation and measurements based on spatial light modulators and singlemode fibers^{26}. We then characterized the memory operation using quantum process tomography. Figure 2b presents the real part of the experimentally reconstructed process matrix χ. It is found to have a fidelity of 0.909 ± 0.010 with respect to the Identity operation. This fidelity exceeds the classical bound of 0.831 (see Supplementary Note 4 for details), thereby confirming the quantum nature of the memory operation. The nonunity value of the memory fidelity may be caused by the limited beam waist of the pump/control light, which may result in imperfect overlap with different OAM modes. Moreover, we noted that the memory performance for superposition states of L〉 and R〉 is much better than that achieved here (as detailed in Supplementary Note 2). The visibility of such twodimensional superposition states is higher than the fidelity of the memory process in all three dimensions. This result indicates that the storage efficiency is balanced for the symmetrical LG modes but is not balanced for all the three considered spatial modes.
Multiplexing storage in multiple DOF
Carrying information in multiple DOF on photons can expand the channel capacity of quantum communication protocols^{11,36}. Here, we show that our solidstate memory can be simultaneously multiplexed in temporal, spectral, and spatial DOF. As shown in Fig. 3a, two AFC are created in the MC with an interval of 80 MHz between them to achieve spectral multiplexing. The two AFC have the same peak spacing of Δ = 200 kHz and the same bandwidth of Γ_{AFC} = 2 MHz. The spinwave storage efficiencies are 5.05% and 5.13%, for the first AFC and the second AFC, respectively. The temporal multimode capacity of an AFC is limited by Γ_{AFC}/Δ^{17}. However, increasing the number of modes, the time interval between the last control pulse and the first output signal pulse will be reduced. Therefore, we employed only two temporal modes to reduce the noise caused by the last control pulse. The spatial multiplexing is realized by using three independent paths as input as shown in Fig. 3b. These paths, s_{1}, s_{2}, and s_{3}, correspond to the OAM states as L〉, R〉, and G〉 defined above. By combining all three DOF together, we obtain 2 × 2 × 3 = 12 modes in total. The FC is employed to select out the desired spectral modes. Figure 3c illustrates the results of multimode storage over these three DOF for μ = 1.04. The minimum crosstalk as obtained from mode crosstalk for each mode is 19.7 ± 3.41, which is calculated as one takes the counts in the diagonal term as the signal and then locates the large peaks over the range of output modes as the noise.
Here, the temporal, spectral and spatial DOF are employed as classical DOF for multiplexing. One can choose any DOF to carry quantum information. As a typical example, now we use the temporal and spectral DOF for multiplexing and each channel is encoded with spatialqutrit state of \(\left {\psi _1} \right\rangle = \left( {\left L \right\rangle + \left G \right\rangle + \left R \right\rangle } \right)/\sqrt 3\). Each channel is labeled as f_{i}t_{j}, where f_{i} represent spectral modes i and t_{j} similarly represent temporal modes j. Figure 4a shows the experimental results for μ = 1.04. The minimum crosstalk as obtained from the mode crosstalk is approximately 15.2. We measured the fidelities of the spatialqutrit state for each channel as shown in Fig. 4b.
A QMC can transfer photonic pulses to a target temporal or spectral mode without distorting the photonic quantum states. A realtime QMC that can operate on many DOF is essential for linking the components of a quantum network^{30,37}. By adjusting the timing of the control pulse, one can specify the recall time in an ondemand manner to realize the temporal mode conversion. The twoAOM gate in our system can be used as a highspeed frequency shifter by tuning its driving frequency. Therefore, spectral and temporal mode conversion can be realized independently and simultaneously. Figure 4c presents the results of QMC operation for μ = 1.04. We can convert from f_{i} to f_{j} and from t_{i} to t_{j}, where these notations represent all different spectral modes and temporal modes. The noise level is significantly weaker than the strength of the converted signal, which indicates that the QMC operates quietly enough to avoid introducing any mode crosstalk. All these modes are encoded with OAM spatialqutrit of ψ_{1}〉. To demonstrate that the qutrit state coherence is well preserved after QMC operation, we measured the fidelities (see Methods for details) between the input and converted states. The results, presented in Fig. 4d, indicate that the QMC can convert arbitrary temporal and spectral modes in realtime while preserving their quantum properties. Our device is expected to find applications in quantum networks comprising two quantum memories, in which mismatched spectral or temporal photon modes may need to be converted^{30}. This device can ensure the indistinguishability of the photons which are retrieved from any quantum memory. This device could find application in many photonic information processing protocols, e.g., a Bellstate measurement^{11}, and quantum memoryassisted multiphoton generation^{9}.
Arbitrary manipulations in real time
The precise and arbitrary manipulation of photonic pulses while preserving photonic coherence is an important requirement for many proposed photonic technologies^{31}. In addition to the QMC functionality demonstrated above, the developed quantum memory can enable arbitrary manipulations of photonic pulses in the temporal and spectral domains in real time. As an example, we prepared the OAM qutrit state ψ_{1}〉 in the f_{1}t_{1} and f_{2}t_{2} modes (Fig. 5a) as the input. Four typical operations were demonstrated, i.e., exchange of the readout times for the f_{1} and f_{2} photons, the simultaneous retrieval of the f_{1} and f_{2} photons at t_{1}, shifting the frequency of f_{1} photons to f_{2} but keeping the frequency of f_{2} photons unchanged and temporal beam splitting the f_{1} photons but filtering out the f_{2} photons. These operations correspond to output of \(\left {\psi _1} \right\rangle _{f_1t_2,f_2t_1}\), \(\left {\psi _1} \right\rangle _{f_1t_1,f_2t_1}\), \(\left {\psi _1} \right\rangle _{f_2t_1,f_2t_2}\), and \(\left {\psi _1} \right\rangle _{f_1t_1,f_1t_2}\), respectively. Another example was implemented with the OAM qutrit state \(\left {\psi _2} \right\rangle = \left( {\left L \right\rangle + \left G \right\rangle  {\mathrm{i}}\left R \right\rangle } \right)/\sqrt 3\) encoded in the f_{1}t_{2} and f_{2}t_{2} modes as the input, as shown in Fig. 5b with same output. The retrieved states were then characterized via quantum state tomography as usual (see Methods). Table 1 shows the fidelities between output states and input states.
Discussion
In conclusion, we have experimentally demonstrated a multiplexed solidstate quantum memory that operates simultaneously in three DOF. The currently achieved multimode capacity is certainly not the fundamental limit for the physical system. Pr^{3+} :Y_{2}SiO_{5} has an inhomogeneous linewidth of 5 GHz, which can support more than 60 independent spectral modes. The number of temporal modes that can be achieved using the AFC protocol^{17} is proportional to the number of absorption in the comb, which has already been improved to 50 in Eu^{3+} :Y_{2}SiO_{5}^{22}. There is no fundamental limit on the multimode capacity in the OAM DOF since it is independent on the AFC bandwidth. The capacity in this DOF is simply determined by the useful size of the memory in practice. We have recently demonstrated the faithful storage of 51 OAM spatial modes in a Nd^{3+} :YVO_{4} crystal^{26}. The combination of these stateoftheart technologies could result in a multimode capacity of 60 × 50 × 51 = 1,53,000 modes. This large capacity could greatly enhance the data rate in memorybased quantum networks and in portable quantum hard drives with extremely long lifetimes^{15}.
The developed multipleDOF quantum memory can serve as a QMC, which is a fundamental requirement for the construction of scalable networks based on multiplexed quantum repeaters. Although it is not demonstrated in the current work, mode conversion in the spatial domain should also be feasible using a highspeed digital micromirror device^{38}. QMC can also find applications in linear optical quantum computations. One typical example is to solve the mode mismatch caused by fiberloop length effects and the time jitter of the photon sources in a boson sampling protocol^{39,40}.
Quantum communication and quantum computation in a largescale quantum network rely on the ability to faithfully store and manipulate photonic pulses carrying quantum information. The presented quantum memory can apply arbitrary temporal and spectral manipulations to photonic pulses in real time, which indicates that this single device can serve as a variable temporal beam splitter^{32,41} and a relative phase shifter^{42} that enables arbitrary control of splitting ratio and phase for each output. Therefore, this device can perform arbitrary singlequbit operations^{43}. Combining with the recent achievements on generation of heralded single photons^{44,45}, this device should provide the sufficient set of operations to allow for universal quantum computing in the Knill–Laflamme–Milburn scheme^{46}. Our results are expected to find applications in largescale memorybased quantum networks and advanced photonic information processing architectures.
Methods
AFC preparation
We tailored the absorption spectrum of Pr^{3+} ions to prepare the AFC using spectral hole burning^{42}. The frequency of the pump light was first scanned over 16 MHz to create a wide transparent window in the Pr^{3+} absorption line. Then, a 1.6 MHz sweep was performed outside the pit to prepare the atoms into the 1/2g state. The burnback procedure created an absorbing feature of 2 MHz in width resonant with the 1/2g–3/2e transition, but simultaneously populated the 3/2g state, which, in principle, must be empty for spinwave storage. Thus, a clean pulse was applied at the 3/2g–3/2e transition to empty this ground state. After the successful preparation of absorbing band in the 1/2g state, a stream of holeburning pulses was applied on the 1/2g–3/2e transition. An AFC structure with a periodicity of Δ = 200 kHz is prepared in this step. These pulses burned the desired spectral comb of ions on the 1/2g–3/2e transition and antiholes at the 3/2g–3/2e transition; thus, a short burst of clean pulses was applied to maintain the emptiness of the 3/2g state. For AFC preparation, the remaining 5/2g ground state is used as an auxiliary state, which stores those atoms which do not contribute to the AFC components. To reduce the noise generated by the control pulses during spinwave storage, we applied 100 control pulses separated by 25 μs and another 50 control pulses with a separation of 100 μs after the preparation of the comb^{21}. An example of the AFC with a periodicity Δ = 200 kHz is illustrated in Fig. 3a. A detailed estimation of the structure and storage efficiency of the AFC memory is presented in Supplementary Note 1. The signal photons are mapped onto the AFC, leading to an AFC echo after a time 1/Δ. Spinwave storage is achieved by applying two onresonance control pulses to induce reversible transfer between the 3/2e state and 3/2g state before the AFC echo emission. The complete storage time is 12.68 μs in our experiment which includes an AFC storage time of 5 μs and a spinwave storage time of 7.68 μs.
Filtering the noise
In order to achieve a low noise floor, temporal, spectral, and spatial filter methods are employed. The input and control beams are sent to the MC in opposite directions with a small angular offset for spatial filtering. Temporal filtering is achieved by means of a temporal gate implemented with two AOM. This AOM gate temporally blocked the strong control pulses. This is important to avoid burning a spectral hole in the FC and to avoid blinding the singlephoton detector. We used two 2nm bandpass filters at 606 nm to filter out incoherent fluorescence noise. The spectral of the filter mode was achieved by narrowband spectral filter in the FC (shown by the dashed black line in Fig. 3a), which is created by 0.8 MHz sweep around the input light frequency, leading to a transparent window of approximately 1.84 MHz due to the power broadening effect. Furthermore, the FC is implemented in a doublepass configuration to achieve high absorption.
Quantum tomography
To characterize the memory performance for threedimensional OAM states, quantum process tomography for the quantum memory operation is performed. Reconstructing the process matrix χ of any threedimensional state requires nine linearly independent measurements. We chose three OAM eigenstates and six OAM superposition states as our nine input states, which are listed as follows: \(\left L \right\rangle ,\left G \right\rangle ,\left R \right\rangle ,\left( {\left L \right\rangle + \left G \right\rangle } \right)/\sqrt 2\), \(\left( {\left R \right\rangle + \left G \right\rangle } \right)/\sqrt 2\), \(\left( {i\left L \right\rangle + \left G \right\rangle } \right)/\sqrt 2\), \(\left( {  i\left R \right\rangle + \left G \right\rangle } \right)/\sqrt 2\), \(\left( {\left L \right\rangle + \left R \right\rangle } \right)/\sqrt 2\), and \(\left( {\left L \right\rangle  i\left R \right\rangle } \right)/\sqrt 2\)^{26}. The complete operators for the reconstruction of the matrix χ are as follows:^{26,47}
Here, λ_{1} is the identity operation. The process matrix χ can be expressed on the basis of λ_{i} and maps an input matrix ρ_{in} onto the output matrix ρ_{out}^{47,48}. Density matrices of the input states ρ_{in} and density matrices of the output states ρ_{out} are reconstructed using quantum state tomography^{47,48}. For a given qutrit state (ψ〉), we used ρ=ψ〉〈ψ to reconstruct the density matrix ρ from the measurement results. As examples, we presented graphical representations of the reconstructed density matrices for the OAM qutrit states ψ_{1}〉 and ψ_{2}〉 in Supplementary Note 3.The fidelities of the output states with respect to the input states can be calculated based on the reconstructed density matrices using the formula \(Tr\left( {\sqrt {\sqrt {\rho _{{\mathrm{out}}}} \rho _{{\mathrm{in}}}\sqrt {\rho _{{\mathrm{out}}}} } } \right)^2\).
Data availability
The data that support the findings of this study are available from the corresponding authors on request.
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Acknowledgments
This work was supported by the National Key R&D Program of China (No. 2017YFA0304100), the National Natural Science Foundation of China (Nos. 61327901, 11774331, 11774335, 61490711, 11504362, and 11654002), Anhui Initiative in Quantum Information Technologies (No. AHY020100), Key Research Program of Frontier Sciences, CAS (No. QYZDYSSWSLH003), the Fundamental Research Funds for the Central Universities (Nos. WK2470000023 and WK2470000026).
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Z.Q.Z. and C.F.L. designed experiment. T.S.Y. and Z.Q.Z. carried out the experiment assisted by Y.L.H., X.L., Z.F.L., P.Y.L., Y.M., C.L., P.J.L., Y.X.X., J.H., and X.L., T.S.Y. and Z.Q.Z. wrote the paper with input from other authors. C.F.L. and G.C.G supervised the project. All authors discussed the experimental procedures and results.
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Yang, T., Zhou, Z., Hua, Y. et al. Multiplexed storage and realtime manipulation based on a multiple degreeoffreedom quantum memory. Nat Commun 9, 3407 (2018). https://doi.org/10.1038/s41467018056695
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