Abstract
The realization of quantum networks and quantum computers relies on the scalable generation of entanglement, for which spinphoton interfaces are strong candidates. Current proposals to produce entangledphoton states with such platforms place stringent requirements on the physical properties of the photon emitters, limiting the range and performance of suitable physical systems. We propose a scalable protocol, which significantly reduces the constraints on the emitter. We use only a single optical transition and an asymmetric polarizing interferometer. This device converts the entanglement from the experimentally robust time basis via a path degree of freedom into a polarization basis, where quantum logic operations can be performed. The fundamental unit of the proposed protocol is realized experimentally in this work, using a nitrogenvacancy center in diamond. This classically assisted protocol greatly widens the set of physical systems suited for scalable entangledphoton generation and enables performance enhancement of existing platforms.
Introduction
The generation of entangledphoton states is of central importance in linear optical quantum computing (LOQC)^{1,2} and optical quantum communication,^{3,4} and has potential applications in quantum sensing and metrology.^{5} Currently, entangledphoton sources rely mostly on spontaneous parametric downconversion, which is robust and offers high purity, but is limited by intrinsically probabilistic entanglement generation.^{6} For most applications in quantum technology, large entangled states are necessary in order to reach performance levels which exceed those of classical devices. The generation of such states therefore remains an outstanding challenge.
Cluster states are particularly desirable resources as they enable measurementbased quantum computation and have an inbuilt resilience to noise and loss.^{7,8,9} Spinbased protocols have been developed for the generation of entangledphoton strings, the most prominent of these being the “clusterstate machine gun” (CSMG) of Lindner and Rudolph.^{10} This protocol is appealingly simple and robust, and can be scaled to higherdimensional cluster states using multiple spins.^{11,12} Its requirements are however quite stringent. Ideally, it necessitates two orthogonally polarized, energydegenerate optical transitions with negligible crossdecay terms (see Fig. 1a). A first demonstration of the CSMG protocol with quantum dots was shown by Schwartz et al.^{13}, where the length of the clusterstate was limited to three photons due to the short lifetime of the qubit.
Here, we employ a nitrogenvacancy (NV) defect in diamond, which is known for its excellent quantum coherence properties, and is therefore a promising candidate for quantum technology.^{14,15,16} As a CSMG source, however, it presents several drawbacks. In particular, the optical transition energies connecting different spin states require careful tuning into resonance while maintaining negligible state mixing, and several of its excitedstate levels can decay to multiple ground states and have a strong decay channel into a longlived metastable state^{17} (see Fig. 1b, c). It is therefore challenging to adhere to the requirements of the original CSMG scheme.^{18}
Instead, in this work we develop and demonstrate an alternative, scalable scheme based on timetopolarization conversion (TPC). Its main advantage is that it requires the use of just one optical transition (Fig. 2). Therefore, the most favorable spin properties of the strongest transition available can be used, and tuning of energy levels is no longer required. With these simplifications, it is applicable to a large variety of emitters.^{19,20}
Results
Scheme
Briefly, our protocol starts with an equal spin superposition between the m_{s }= 0 and m_{s} = −1 optical ground states. Upon excitation, the emitter produces a photon with 50% probability, which is stored in a Hpolarized channel. During the storage time the superposition of the spin is inverted by a πrotation. A second excitation pulse can then launch a photon, again with 50% probability, into a Vpolarized channel. The sequence therefore generates a single photon in a superposition of polarizations. At this stage, it is however not possible to verify entanglement on the spinphoton state as the initial spin state is revealed directly by the photon’s position. The path information, and with it the emission time information, is therefore erased by matching the delay time between excitation pulses to the storage time of the Harm. After the TPC process, the timeseparated wavepackets merge into a single polarization qubit entangled with the NV center spin. The procedure can be iterated to generate a string of entangled photons. Altogether, the single optical transition and the photonic routing elements act as the ideal CSMG fourlevel system.
In more detail, the experimental sequence used to demonstrate the method unfolds in three steps: preparation, entanglement generation, and tomography (Fig. 3).
Preparation
The experimental cycle (Fig. 3b) starts by initializing the NV charge state, through ionization into NV^{}, with a green laser pulse. The electronic and nuclear (^{14}N nucleus of the NV center) spins are then initialized by iteratively flipping undesired spin populations using resonant optical pumping (see Supplementary Information), preparing them in the m_{s} = −1, m_{I} = 0 state. The electron spin subspace {\(\left0\right\rangle\), \(\left1\right\rangle\)} constitutes the matter qubit of the protocol. Initialization of the nuclear spin is applied to reduce dephasing and to maximize microwave transfer fidelity. We obtain a qubit initialization fidelity of 97.9 ± 1.6% and a nuclear polarization, within the m_{s} = −1 manifold, of 83.8 ± 1.9%.
Entanglement generation
After initialization of the electron spin into \(\left1\right\rangle\), a rotation with a microwave pulse R_{y}(π∕2) brings the electron into a superposition \({\psi }_{0}=(\left1\right\rangle \left0\right\rangle )/\sqrt{2}\). An optical \(\left0\right\rangle\) → \(\left0\right\rangle\)_{e} πpulse (a_{1}) using a resonantly tuned laser then leads to the emission of a photon, conditional upon the state of the electron spin, resulting in the state \(\psi ({a}_{1})=(\left1\right\rangle \left{0}_{a1}\right\rangle \left0\right\rangle \left{H}_{a1}\right\rangle )/\sqrt{2}\). The ket \(\leftH_{a1}\right\rangle\) (\(\left0_{a1}\right\rangle\)) denotes an horizontally polarized photon (no photon) created by the pulse a_{1}. This photon is stored for 262 ns in the long arm of the fiber interferometer (Fig. 3a). Meanwhile, a microwave πpulse rotates the spin to the orthogonal state, \((\left0\right\rangle \left{0}_{a1}\right\rangle +\left1\right\rangle \left{H}_{a1}\right\rangle )/\sqrt{2}\), followed by a second optical excitation (a_{2}), the emission of which is vertically polarized in the TPC apparatus, resulting in the entangled state \(\psi ({a}_{2})=(\left0\right\rangle \left{V}_{a2}\right\rangle +{e}^{i\phi }\left1\right\rangle \left{H}_{a1}\right\rangle )/\sqrt{(2)}\), with the interferometer phase ϕ (see Methods).
We can therefore realize a circuit analogous to the building block of the CSMG protocol by selecting the appropriate phase ϕ of the interferometer: repetition of the entanglement generation step on the existing spin superposition leads to the addition of further photonic qubits to the entangled state (see Supplementary Information). The correct routing of the photons is probabilistic here, and is heralded by the time of arrival, but can be made deterministic with an active switch.
Tomography
On the photonic side, the passive TPC scheme enables direct projection onto both the equatorial basis (D/A and R/L) in the patherasing events, and onto the polar basis (H/V) by selecting pathrevealing events (see Methods and Supplementary Information). The D/A and R/L ports perform a projective measurement on the photon, dependent on the interferometer phase, onto the states: \({\phi }^{\pm}\rangle =\leftH\right\rangle \pm {e}^{i\phi}\leftV\right\rangle\) and \({\phi }_{\pi /4}^{\pm }\rangle =\leftH\right\rangle \pm {e}^{i(\phi +\pi /4)}\leftV\right\rangle\), respectively. The electron spin readout relies on the rotation of the spin state through a R_{y}(θ)pulse and a final 5 μs laser pulse (Fig. 3b).
We experimentally demonstrate the process using a NV center in an artificial diamond created by chemical vapor deposition. A microlens (Fig. 3c) is machined over a preallocated NV center by focusedionbeam milling for improved photon collection efficiency. We manipulate the spin using a microwave field radiated from two bond wires. The diamond is cooled to ~4.5 K in a closedcycle cryostat and photons are collected through a window using a microscope objective.
Experimental realization
The fundamental unit of the proposed protocol is experimentally demonstrated by performing partial tomography on the resulting spinphoton system and quantifying the respective entanglement. The resulting measured correlations in the σ_{z} ⊗ σ_{z} basis are represented in Fig. 4a, with a correlation value of C_{zz} = 〈σ_{z} ⊗ σ_{z}〉 = (83.7 ± 1.6)%.
To extract the C_{xx} = 〈σ_{x} ⊗ σ_{x}〉 correlations, spin–photon entanglement is generated for two different initial spin superposition states \({\psi }_{}=(\left1\right\rangle \left0\right\rangle )/\sqrt{2}\) and \({\psi }_{+}=(\left1\right\rangle +\left0\right\rangle )/\sqrt{2}\), corresponding to the spin measurement projection states \(\left\pm{x}\right\rangle\). Following established procedure,^{21} we now observe the spinphoton correlations by measuring their dependence on the interferometer phase, ϕ. The measured photon entangling events, on average 25 per hour, in the quadrature ports (D, A, R, and L) are sorted according to ϕ at the time of detection and combined taking into account each port’s phase offset. Figure 4b shows the conditional probability of projecting the spin state onto \(\left+x\right\rangle\) and \(\leftx\right\rangle\), given the projection of a photon onto an equatorial state \(\left{\phi}\right\rangle =\leftH\right\rangle + {e}^{i\phi}\leftV\right\rangle\). The resulting curves correspond to a correlation C_{xx} = (40.7 ± 2.9)%, showing the entanglement signature expected for the ψ^{+} Bellstate (as opposed to C_{xx} = 0 for a statistical mixture). In order to probe the quality of our source directly, the presented results have an accurately calibrated measure of the background light present in our ZPL detection window deducted (see Supplementary Information). The limiting factors contributing to the departure from the ideal state generation are discussed quantitatively in the Supplementary Information, with good agreement between theoretical estimate and measured correlations.
From the retrieved correlations, we estimate a lower bound on the entanglement fidelity with respect to the ideal Bellstate, \(\left\psi^{+}\right\rangle\), of F ≥ 64.7 ± 1.3% and a raw F ≥ (56.0 ± 0.9)%, including background. This value is significantly above the bound for a classical state (F ≤ 50%), thereby demonstrating the entanglement in our spinphoton protocol, by over 11 standard deviations (over six without background subtraction). The fidelity is currently limited by a variety of imperfections (such as spin mixing in the excitedstate manifold and imperfect spin readout), which can be minimized by improvements to the setup and system (see Supplementary Information).
Discussion
The TPC entanglement generation and conversion protocol proposed and demonstrated in this work points at the underlying concept of how the imperfections of a quantum system (NV system) can be counteracted by the role of a classical counterpart (interferometer). Specifically, the TPC technique relaxes many of the requirements placed on the emitter and broadens the range of systems for which such entanglement generation schemes are possible.
The experimental apparatus used in the demonstration of the protocol is currently limited to twoparticle entanglement, owing to the lowphoton collection efficiency, strong decay into the PSB, and long initialization cycles. The fidelity is furthermore limited by undesired transitions from the excited state. These shortcomings have known solutions: the emission and collection of ZPL photons from the optical transition can be drastically improved using an optical resonator,^{22} and fast initialization is achievable with an additional laser and singleshot readout.^{23,24} The spin mixing in the excited state can be removed almost entirely by using an NV in a lowstrain environment.^{17,24} High cooperativity cavity systems may even enable entangling schemes relying on single transitions without excitation of the emitter.^{25,26}
Resolving these imperfections provides an imminent outlook for the scalability of the system. Particularly, seeing that NV centers, single atoms and molecules, or quantum dots are suited to the direct generation of twodimensional cluster states using ancillary spins or remote centers,^{11,12,18,27,28} the TPC scheme offers a robust and adaptable method to realize resource states for quantum communication and universal quantum computation.
Methods
Sample and fabrication
An artificial, singlecrystal diamond of natural isotopic abundance and with a {1, 1, 1} surface orientation hosts the NV center. We surveyed the diamond for shallow defects and created solidimmersion lenses using focussed ionbeam milling over several defects with the desired NV axis orientation (perpendicular to the surface). We then coated the surface with 110 nm of SiO2 in order to reduce Fresnel reflection losses and laser backscatter at the highindex interface.
Experimental details
Our resonant optical pulses at around 637.2 nm are delivered from a narrowband externalcavity diode laser (Toptica DL Pro HP 637) and switched with two electrooptic amplitude modulators (Jenoptik AM635) in series. The fluorescence is split at a laser line filter into the resonant ZPL portion and the far offresonant PSB portion. The latter was used to perform efficient spin readout. Since most (~ 97%) of the photons decay into the PSB^{29} and the system has significant photon losses, the measured ZPL efficiency (pulse to click) is ~ 2 × 10^{−5}. The average probability of detecting a spinreadout click when prepared in m_{s} = 0 is (16.7 ± 0.1)%. We, therefore, observe an average of 25 PSBZPL coincidence events per hour.
The timetopolarization conversion was performed by directing the ZPL part of the NV emission into a polarizationmaintaining, fiberbased MachZehnder interferometer. We matched the time between the two optical πpulses in our sequence to the propagation delay between the arms of the interferometer. The interferometer was passively stabilized to minimize path length changes occurring during each entanglement cycle. The phase was furthermore tracked during each entanglement cycle by sending resonant laser pulses through the TPC between entanglement sequences and measuring the intensity on four quadrature detectors corresponding to the photon states D, A, R, and L.
Passive routing of photons
The emitted photons are diagonally polarized with respect to the unbalanced interferometer’s arms and therefore split in two possible propagation paths (50% take the H(V)polarized long (short) arm) and two corresponding propagation times. Therefore, two excitation/emission cycles result in four arrival times at the output of the interferometer:

1.
Early emission takes the short (V) path;

2.
Early emission, long (H) path;

3.
Late emission, short (V) path;

4.
Late emission, long (H) path.
If the separation between the two emissions matches the time difference in the propagation, then events of type 2 and 3 have the same arrival time. Detection within this time window erases the path information and heralds the intended function of the passive switch (50% success probability). Events outside this window, 1 and 4, are pathrevealing and are not conducive to the creation of the photonic polarization qubit.
Electron and nuclear spin initialization
The initialization sequence relies on electron and nuclear spin flips in the optically excited state of the NV center. A lowpower laser pulse (5 μs long), resonant with the 0 ↔ 0_{e} transition, results in an electron (nuclear) spin flip with high (low) probability. Subsequently, nuclear spin selective microwave pulses are applied to the ground state, which drive the population in the undesired states back to 0. This sequence is repeated several times in order to enhance the probability of initializing the electron (nuclear) spin in state \(\leftm_{s}\,=\,1\right\rangle\) (\(\leftm_{I}\,=\,0\right\rangle\)).
Fidelity estimation
Following a wellestablished method^{21,28} we calculate the lower bound on the fidelity as:
where ρ_{ii} denotes the diagonal entries of ρ and C_{xx} denotes the xx basis correlations C_{xx} = 〈σ_{x} ⊗ σ_{x}〉 of ρ. The diagonal elements ρ_{11}, ..., ρ_{44} are directly extracted from the data in Fig. 4a, whereas the equatorial correlations C_{xx} are calculated from the contrast of the curves in Fig. 4b.
Further details of all methods are provided in the Supplementary Information.
Note: During preparation of the manuscript, we became aware of preliminary efforts towards the results achieved in this work using a quantum dot.^{30} During the review process of this article, an implementation of the scheme combined with photon frequency conversion was published.^{31}
Data availability
The data supporting the findings of this work are available from the corresponding author, upon reasonable request.
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Acknowledgements
We are grateful to the WWTF (project ICT12041 PhoCluDi), the Austrian Science Fund (FWF): projects M 1852N36 Lise Meitner Program, W1210 DKCOQUS, I 3167N27 SiCEiC, and W1243 DKSolids4Fun; the TU Innovative Projekte, and the EU Marie Curie Actions project 628802. The focussed ionbeam milling for this project was carried out using facilities at the University Service Center for Transmission Electron Microscopy, Vienna University of Technology, Austria.
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R.V., S.R., and C.S. contributed equally to this work. R.V., S.R., and C.S. performed the experiments. R.V., S.R., C.S., and M.T. analyzed the data. G.W. and D.W. contributed to the experimental apparatus. J.S., P.W., and M.T. provided support for the work. M.T. devised the scheme, supervised the work, and drafted the manuscript. All authors contributed to the interpretation of the data and the writing of the manuscript.
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Vasconcelos, R., Reisenbauer, S., Salter, C. et al. Scalable spin–photon entanglement by timetopolarization conversion. npj Quantum Inf 6, 9 (2020). https://doi.org/10.1038/s415340190236x
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DOI: https://doi.org/10.1038/s415340190236x
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