Abstract
The nocloning theorem states that an unknown quantum state cannot be cloned exactly and deterministically due to the linearity of quantum mechanics. Associated with this theorem is the quantitative nocloning limit that sets an upper bound to the quality of the generated clones. However, this limit can be circumvented by abandoning determinism and using probabilistic methods. Here, we report an experimental demonstration of probabilistic cloning of arbitrary coherent states that clearly surpasses the nocloning limit. Our scheme is based on a hybrid linear amplifier that combines an ideal deterministic linear amplifier with a heralded measurementbased noiseless amplifier. We demonstrate the production of up to five clones with the fidelity of each clone clearly exceeding the corresponding nocloning limit. Moreover, since successful cloning events are heralded, our scheme has the potential to be adopted in quantum repeater, teleportation and computing applications.
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Introduction
The impossibility to perfectly duplicate an unknown quantum state deterministically, known as the nocloning theorem^{1}, lies at the heart of quantum information theory and guarantees the security of quantum cryptography^{2,3}. This nogo theorem, however, does not rule out the possibility of imperfect cloning. The idea of generating approximate copies of an arbitrary quantum state was conceived by Buzek and Hillery in their seminal work^{4} with the proposal of universal quantum cloning machine. This discovery has since sparked intense research in both discrete^{5,6,7,8} and continuous variable^{9,10,11,12,13} systems to explore the fundamental limit of cloning fidelity allowed by quantum mechanics, known as the nocloning limit. Several quantum cloning experiments approaching the optimal fidelity enforced by this limit have since been demonstrated for single photons^{14}, polarization states^{15} and coherent states^{16}.
By forgoing determinism, perfect cloning is not entirely forbidden by the law of quantum physics. In fact, if the quantum states to be cloned are chosen from a discrete, linearly independent set, then the unitarity of quantum evolution does allow probabilistic exact cloning^{17,18,19,20,21}. Nondeterministic highfidelity cloning of linearly dependent input states can also be performed if the cloning operation is only arbitrarily close to the ideal case^{20,22}. Recently, the invention of probabilistic noiseless linear amplifier (NLA)^{23}, and its subsequent theoretical studies^{24,25,26,27,28} and implementations^{29,30,31,32,33} in principle provided a method for cloning arbitrary distributions of coherent states with highfidelity via an amplifyandsplit approach^{29}. In practice, however, implementing NLA for coherent states with amplitude α≥1 remains a technical challenge. This is because the resources required scales exponentially with the coherent state size.
In this article, we follow a different path by adopting a method that interpolates between exactprobabilistic and approximatedeterministic cloning^{34}. We show that a hybrid linear amplifier, comprising of a probabilistic NLA and an optimal deterministic linear amplifier (DLA)^{16,35}, followed by an Nport beam splitter is an effective quantum cloner. Previously, Müller et al.^{36} demonstrated probabilistic cloning of coherent states which outperformed the best deterministic scheme for input alphabet with random phases but fixed mean photon number. Here, we propose a highfidelity heralded cloning for arbitrary distributions of coherent states and experimentally demonstrate the production of N clones with fidelity that surpasses the Gaussian nocloning limit F_{N}=N/(2N−1)^{12,13}.
Results
Hybrid cloning machine
Our heralded hybrid cloning machine (HCM) is depicted conceptually in Fig. 1a, where an Ncopy cloner is parametrized by an NLA amplitude gain (g_{NLA}) and an optimal DLA gain (g_{DLA}). By introducing an arbitrary input coherent state of α〉, and setting the total gain to unity,
HCM will generate N clones with identical complex amplitude α and quadrature variance 1+2(−1)/N (where the quantum noise level is 1). Since the probabilistic amplification incurs no noise at all, the variance is a function of g_{DLA} only. Such setup can be interpreted as two linear amplifiers with distinct features, complementing each other by sharing the burden of amplification. Lower noise can be achieved at the expense of the probability of success by increasing the NLA gain. Conversely, a higher probability of success, although with an increased noise, can be obtained by increasing the DLA gain. Hence, by tailoring both gains appropriately, one can achieve the desired cloning fidelity, with vanishing probability of success as the fidelity approaches unity.
A key feature in our implementation is the observation that when the probabilistic gain is less than the deterministic gain, g_{NLA}<g_{DLA}, the hybrid amplifier can be translated to a linear optical setup^{35} with an embedded measurementbased NLA (MBNLA) (Fig. 1b). This equivalence is illustrated in Fig. 2, and discussed in more detail in Supplementary Note 1. The MBNLA is the postselective version of the physical realization of NLA that has been proposed^{37,38}, and experimentally demonstrated recently^{39}. Compared with its physical counterpart, MBNLA offers the ease of implementation and avoids the predicament of demanding experimental resources. By deploying MBNLA as the heralding function in a feedforward control setup^{40}, HCM preserves the amplified quantum state, extending the use of the MBNLA beyond pointtopoint protocols such as quantum key distribution.
To clone an input coherent state, we first tap off part of the light with a beam splitter of transmission
which is then detected on a dualhomodyne detector setup locked to measure the amplitude and phase quadratures (X and P). A probabilistic heralding function, which is the probabilistic quantum filter function of an MBNLA^{37,39}, is then applied to the measurement outcome. By postselecting the dualhomodyne data with higher amplitude, the heralding function gives rise to an output distribution with higher overall mean. Mathematically, this function is given by
Here, α_{m}=(x_{m}+ip_{m})/ is the dualhomodyne outcomes. M=exp[(1−1/)] is the normalization term with α_{c} as the NLA cutoff. The NLA gain is tailored to achieve unity gain, while the cutoff α_{c} is chosen with respect to the gain and maximum input amplitude to emulate noiseless amplification faithfully while retaining a sufficient amount of data points (Supplementary Note 2).
The heralded signal is then scaled with gain g_{x,p}= and used to modulate an auxiliary beam. The auxiliary beam is combined with the transmitted beam using a 98:2 highly transmissive beam splitter, which acts as a displacement operator to the transmitted beam^{41}. Finally, the combined beam passes through an Nport beam splitter to create Nclones, which is then verified by homodyne measurements.
In our experiment, the dualhomodyne measurement heralds successful operation shotbyshot. This is then paired up with the corresponding verifying homodyne measurements to select the successful amplification events. The accumulated accepted data points give the distribution of the conjugate quadratures of the successful clones. The processing of the input coherent state at different stages of the HCM is illustrated by Fig. 3a.
It is instructive to compare our scheme to that of ref. 36, where probabilistic cloning of fixedamplitude coherent states was demonstrated. In ref. 36, the amplification is performed by a phaserandomized displacement and phase insensitive photon counting measurement, which have to be optimized according to input amplitude. In our scheme, the amplitude and the phase of the input state is a priori unknown. Moreover, owing to the phasesensitive dualhomodyne measurement and coherent feedforward control in DLA^{27,42}, the state to be cloned is amplified coherently in the desired quadrature. The integration of MBNLA in HCM, which emulates a phasepreserving noiseless amplification, further enhances the amplitude of the signal, while maintaining its phase.
Two clones
To benchmark the performance of the HCM, Fig. 3b demonstrates the universality of the cloning machine by showing the cloning results of four coherent input states with different complex amplitudes , where (x, p)=(−0.71, 0.72), (−0.01, −1.51), (2.23, 2.19) and (−5.26, −0.02). The figure of merit we use is the fidelity F=〈αρ_{i}α〉, which quantifies the overlap between the input state and the ith clone ρ_{i}. Using a setting of T_{s}≈0.6, our device clones the four input states with average fidelities of 0.695±0.001, 0.676±0.005, 0.697±0.001 and 0.681±0.007, respectively. All of the experimental fidelities are significantly higher than that of a classical measureandprepare (M&P) cloner (F_{M&P}=0.5), where the clones are prepared from a dualhomodyne measurement of an input state^{43}. More importantly, all the clones also surpass the nocloning limit of F_{2}=2/3, which is impossible even with a perfect deterministic cloning machine.
To further analyse the HCM, we examine the cloning of an input state (x, p)=(2.23, 2.19) (α=1.56) in greater detail. This experiment is repeated 5 × 10^{7} times, from which about 5.9 × 10^{5} runs produced successfully heralded clones. The electronic gain g_{x,p} and the splitting ratio of the beam splitter are carefully tuned to ensure that the two clones produced are nearly identical. The probabilistic heralding function was chosen to ensure that the output clones have exactly unity gain on average. This is done to prevent any overestimation of the fidelity (Supplementary Note 3 and Supplementary Fig. 1). As can be seen in Fig. 3c, the produced clones have noise significantly lower than the M&P cloning protocol. Since the noise variance is only affected by the deterministic amplification, setting g_{NLA}>1 will reduce the required DLA gain, while still achieving unity gain. As a result, the clones produced by our HCM will have less noise compared with its deterministic counterpart. The data points also show that the heralded events (purple region of Fig. 3c right) have Gaussian distributions with mean equal to that of the input state. We experimentally obtained a fidelity of 0.698±0.002 and 0.697±0.002 for the two clones. The fidelity plot in Fig. 3d clearly demonstrates that the fidelities of both clones exceed not only the M&P limit but also lie beyond the nocloning limit by more than 15 s.d.
Multiple clones
We operate our HCM at higher gains to enable the production of more than two clones. To have g_{NLA}>1, from equations (1) and (2), we require g_{DLA}<, which leads to T_{s}>1/N. Hence, by tailoring T_{s} for each N, HCM can produce N clones with fidelity beating the deterministic bound F_{N} with the desired probability of success. Figure 4a shows the fidelity of the multiple clones with an input of α≈0.5. The average fidelities of the clones for N=2, 3, 4 and 5 are 0.695±0.002, 0.634±0.012, 0.600±0.009 and 0.618±0.007, respectively, clearly surpassing the corresponding nocloning limit. In Fig. 4b, we plot the theoretical prediction of the fidelity as a function of the probability of success with the experimental data. The theoretical fidelity is modelled on the dualhomodyne detection efficiency of 90±5%, which is the main source of imperfection (see Supplementary Note 3 for details). We find that our results lie well within the expected fidelities, with the probability of success ranging between 5 and 15%. Remarkably, by keeping 5% of the data points, the average cloning fidelity for N=5 can be enhanced by >15%, and hence exceeding the nocloning limit F_{5} by 11.2%.
For deterministic unity gain cloners, as long as N clones are produced each with fidelity F>F_{N+1} (refs 12, 13), one may conclude that there are no other clones with equal or higher fidelity. Here we show that this is not necessarily the case for probabilistic cloning. By further increasing NLA gain, we successfully produce three clones, each with fidelity F>F_{2} (Fig. 4c), and the average fidelity is 0.684±0.009. Given only fidelity, it is impossible for a receiver with only two clones to determine whether the clones originate from a twoclone or threeclone probabilistic protocol (Fig. 4a,c). The resulting probability distribution from 7.2 × 10^{6} successful threeclone states out of 5 × 10^{8} inputs, and the corresponding experimental reconstructed Wigner function are shown in Fig. 4d together with the input state.
The theoretical fidelity for the HCM’s clones at unity gain can be shown to be F_{HCM}=1/(1+(−1)/N), which is only a function of the deterministic gain and the number of clones. We note that maximum fidelity for a given N can be achieved in the limit of T_{s}→1, giving F_{max}(N)=1/(1+(−1)/N) (Supplementary Note 3). F_{max}(N) converges to 1 in the limit of an infinite number of clones. However, since this also requires an infinitely large nondeterministic gain, and thus an unbounded truncation in postselection, the probability of success will be essentially zero.
Discussion
In summary, we have proposed and demonstrated a hybrid cloning machine that combines a deterministic and a probabilistic amplifier to clone unknown coherent states with fidelity beyond the nocloning limit. Although an ideal NLA implementation is not possible with our setup, as this would require zero deterministic gain, our hybrid approach does allow the integration of measurementbased NLA in the optimal deterministic amplifier. We showed that our device is capable of highfidelity cloning of large coherent states and generation of multiple clones beyond the nocloning limit, limited only by the amount of data collected and the desired probability of success. Our cloner, while only working probabilistically, provides a clear heralding signal for all successful cloning events.
Several comments on the prospects and avenues for future work are in order. An immediate extension is the implementation of HCM in various feedforward based cloning protocols, such as phase conjugate cloning^{44}, cloning of Gaussian states^{45,46}, telecloning^{47} and cloning with prior information^{36,48,49}. Our tunable probabilistic cloner could further elucidate fundamental concepts of quantum mechanics and quantum measurement, for instance, quantum deleting^{50} and quantum state identification^{34,51}. This probabilistic coherent protocol might also play a role in the security analysis of eavesdropping attacks in continuous variable quantum cryptography as well^{52,53}. The implication of HCM in the context of quantum information distributor^{54} and quantum computation^{55} also demands further investigation.
Beyond probabilistic cloning, owing to the robustness and ease of implementation of this heralded hybrid amplification, we envisage numerous applications in quantum communication^{39,56,57}, quantum teleportation^{40,58,59} and quantum error correction^{60}. As such, we believe our scheme will be a useful tool in the quest to realize largescale quantum networks.
Methods
Experimental details
Our hybrid cloning machine is shown in Fig. 1b. The coherent state is created by modulating the sidebands of a 1,064 nm laser at 4 MHz with a pair of phase and amplitude modulators. In the cloning stage, the input mode is split by a variable beam splitter consisting of a halfwave plate and polarizing beam splitter with transmissivity T_{s}=(g_{NLA}/g_{DLA})^{2}. An optical dualhomodyne measurement is performed on the reflected beam, where the measurement outcome is further split into two parts. The first part is used to extract the 4 MHz modulation by mixing it with an electronic local oscillator, before being low pass filtered at 100 kHz and oversampled on a 12bit analoguetodigital converter at 625 k samples per second. The data are used to provide the heralding signal. The second part of the output is amplified electronically with a gain g_{x,p} and sent to another pair of phase and amplitude modulators, modulating a bright auxiliary beam. This beam is used to provide the displacement operation by interfering it in phase with the delayed transmitted beam on a 98:2 beam splitter. The delay on the transmitted beam ensures that it is synchronised to the auxiliary beam at the beam splitter. The combined beam is then split by an Nport splitter to generate clones. The clones are then verified individually by the same homodyne detector. Two conjugate quadratures X and P are recorded and used to characterize the Gaussian output. For each separate homodyne detection at least 5 × 10^{7} data points are saved. We note that in evaluating the fidelities, we take into account the detection efficiency and losses to avoid an overestimation of the fidelity (Supplementary Note 3).
Data availability
The data that support the findings of this study are available from the corresponding author on request.
Additional information
How to cite this article: Haw, J. Y. et al. Surpassing the nocloning limit with a heralded hybrid linear amplifier for coherent states. Nat. Commun. 7, 13222 doi: 10.1038/ncomms13222 (2016).
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Acknowledgements
We thank S. Armstrong for helpful discussions. The research is supported by the Australian Research Council (ARC) under the Centre of Excellence for Quantum Computation and Communication Technology (CE110001027). P.K.L. is an ARC Laureate Fellow.
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J.D., R.B., S.M.A. and T.C.R. developed the theory. J.Y.H., J.Z., S.M.A., M.B., T.S. and P.K.L. conceived and conducted the experiment. J.Y.H., J.Z. and S.M.A. analysed the data. J.Y.H., J.Z., M.B. and S.M.A. drafted the initial manuscript. T.S., T.C.R. and P.K.L. supervised the project. All authors discussed the results and commented on the manuscript.
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Supplementary Figure 1, Supplementary Notes 13 and Supplementary References. (PDF 214 kb)
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Haw, J., Zhao, J., Dias, J. et al. Surpassing the nocloning limit with a heralded hybrid linear amplifier for coherent states. Nat Commun 7, 13222 (2016). https://doi.org/10.1038/ncomms13222
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DOI: https://doi.org/10.1038/ncomms13222
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