# Teleportation of entanglement over 143 km

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Contributed by Anton Zeilinger, August 27, 2015 (sent for review July 14, 2015; reviewed by Franco Nori and Gregor Weihs)

## Significance

Teleportation of an entangled state, also known as entanglement swapping, plays a vital role in the vision of a global quantum internet, providing unconditionally secure communication, blind cloud computing, and an exponential speedup in distributed quantum computation. In contrast to the teleportation of a single quantum state from one qubit to another, entanglement swapping generates entanglement between two independent qubits that have never interacted in the past. Therefore this protocol represents a key resource for numerous quantum-information applications that has been implemented in many different systems to date. We experimentally demonstrated entanglement swapping over 143 km between the Canary Islands of La Palma and Tenerife, proving the feasibility of this protocol to be implemented in a future global scenario.

## Abstract

As a direct consequence of the no-cloning theorem, the deterministic amplification as in classical communication is impossible for unknown quantum states. This calls for more advanced techniques in a future global quantum network, e.g., for cloud quantum computing. A unique solution is the teleportation of an entangled state, i.e., entanglement swapping, representing the central resource to relay entanglement between distant nodes. Together with entanglement purification and a quantum memory it constitutes a so-called quantum repeater. Since the aforementioned building blocks have been individually demonstrated in laboratory setups only, the applicability of the required technology in real-world scenarios remained to be proven. Here we present a free-space entanglement-swapping experiment between the Canary Islands of La Palma and Tenerife, verifying the presence of quantum entanglement between two previously independent photons separated by 143 km. We obtained an expectation value for the entanglement-witness operator, more than 6 SDs beyond the classical limit. By consecutive generation of the two required photon pairs and space-like separation of the relevant measurement events, we also showed the feasibility of the swapping protocol in a long-distance scenario, where the independence of the nodes is highly demanded. Because our results already allow for efficient implementation of entanglement purification, we anticipate our research to lay the ground for a fully fledged quantum repeater over a realistic high-loss and even turbulent quantum channel.

Because an unknown single quantum state cannot be cloned or amplified without destroying its essential quantum feature (1), the quantum repeater (2⇓–4) is the main device for faithful entanglement distribution over long distances. The idea is to decompose the total distance into shorter elementary links, over which entanglement is shared, purified, and eventually stored in quantum memories. Once all of the nodes are set the entangled states can be retrieved on demand. Finally the entanglement is swapped between adjacent nodes and faithfully extended over the whole distance. Entanglement purification (5⇓–7) and quantum memories (4, 8) serve solely to enhance the efficiency and the fidelity of the protocol, both of which are limited due to imperfection of the sources of entangled particles, of the involved quantum operations, and of the interconnecting quantum channels. Entanglement swapping (9⇓⇓⇓⇓⇓⇓⇓–17) however provides the underlying nonclassical correlations and constitutes the fundamental process required for the implementation of a quantum repeater. Here we show that we were able to provide this resource via a realistic 143-km long-distance free-space (elementary) link under harsh atmospheric conditions, representing to our knowledge the largest geographical separation for this protocol to date. Furthermore, the simultaneous creation of two randomly generated photon pairs drastically reduces the signal-to-noise ratio, leading to technological requirements on the verge of practicability. Nonetheless, we ensured space-like separation of the remote measurement events, which is important for certain protocols, e.g., quantum key distribution (18, 19).

The entanglement swapping protocol is realized via the generation of two entangled pairs, photons “0” and “1” and photons “2” and “3,” for example the maximally entangled singlet states_{0123} =∣Ψ^{−}〉_{01} ⊗∣Ψ^{−}〉_{23} may be written as^{±}〉_{12} = 1/√2 (|H〉_{1}|V〉_{2} ± |V〉_{1}|H〉_{2}) and ∣Φ^{±}〉_{12} = 1/√2 (|H〉_{1}|H〉_{2} ± |V〉_{1}|V〉_{2}) with an equal probability of 1/4. By that measurement, photons “0” and “3” are projected into the same entangled state as photons “1” and “2.” Thus, the entanglement is swapped from photons “0-1” and “2-3” to the photons “1-2” and “0-3.” This procedure may also be seen as teleportation of the state of photon “1” onto photon “3” or photon “2” onto photon “0.” Although the implementation of this protocol, solely based on linear optics, allows distinguishing between two out of four Bell states only (20), it provides a maximal fidelity of 1 in the successful cases.

## Experiment

Here we report successful entanglement swapping in an experiment performed on the Canary Islands, using a 143-km horizontal free-space link between the Jacobus Kapteyn Telescope (JKT) building of the Isaac Newton Group of Telescopes (ING) on La Palma and the Optical Ground Station (OGS) of the European Space Agency (ESA) on Tenerife. Both buildings are located at an elevation of 2,400 m above sea level. The JKT served as the base station for the production of the two entangled photon pairs, for the BSM between photons “1” and ”2” and for the polarization detection of photon “0” at Alice. The transmitter telescope, sending photon “3” to the receiving station on Tenerife, was installed on the rooftop of the JKT building. At the receiver the photons were collected by the 1-m-diameter OGS reflector telescope and guided through the optical Coudé path to the setup for polarization analysis and the final measurement by Bob.

In our experimental setup (Fig. 1) a mode-locked femtosecond pulsed Ti:Saph laser emitted light with a central wavelength of 808 nm at a repetition rate of 80 MHz. Those near-infrared pulses were then frequency doubled to a central wavelength of 404 nm using second-harmonic generation in a type-I nonlinear β-barium borate (BBO) crystal. The individual polarization-entangled photon pairs used in the protocol were generated via spontaneous parametric down-conversion (SPDC) in two subsequent type-II phase-matched BBOs (21) and coupled into single-mode (SM) optical fibers for spatial mode selection. Eliminating the spectral distinguishability, which is inherent to pulsed SPDC schemes, optimized the quality of entanglement. We therefore decoupled the photon pairs’ spectral degree of freedom from the polarization degree of freedom using the scheme as outlined in refs. 22⇓–24. The first SPDC source provided the entangled state∣Ψ^{−}〉_{23}, with photon “2” as one input photon for the BSM and photon “3” being guided through a 50-m-long SM fiber to the transmitter telescope. The subsequent SPDC source prepared the state ∣Ψ^{−}〉_{01}, where photon “1” was the second input photon for the BSM. Photon “0” was locally delayed in a 100-m fiber (∼500 ns) and subsequently measured by Alice, thus ensuring space-like separation between Alice’s and Bob’s measurement events (19).

In La Palma, the BSM was implemented using a tunable fiber beam splitter (FBS) set to a 50:50 splitting ratio. Whereas the spatial overlap of photons “1” and “2” is inherent to the FBS, a perfect temporal overlap is accomplished in the minimum of the Hong–Ou–Mandel (25) interference dip. The latter was achieved by adjusting the optical path length for photon “2” by linearly moving the SM fiber coupler in the first SPDC source. Both output arms of the FBS were equipped with a quarter- and a half-wave plate followed by a polarizing beam splitter (PBS) in order to project on any desired polarization measurement basis. Intrinsic polarization rotations in the SM fibers were compensated for with in-fiber polarization controllers. The avalanche photodiodes (APDs) a, b, c, and d, placed at the four outputs of the two PBSs, were connected to a home-made coincidence logic, providing the two valid outcomes of our BSM: simultaneous clicks of APDs (a and d) ∨ (b and c) or (a and b) ∨ (c and d) (where ∨ denotes the logical OR operator) indicated that photons “1” and “2” were projected onto the maximally entangled ∣Ψ^{−}〉_{12} singlet or ∣Ψ^{+}〉_{12} triplet Bell state, respectively. As can be seen from Eq. **2**, conditioned on these BSM results, photons “0” and “3” were thus simultaneously projected onto the very same states ∣Ψ^{−}〉_{03} and ∣Ψ^{+}〉_{03}, respectively. The projection onto the other Bell states ∣Φ^{±}〉_{12} does not result in a coincidence detection event by the BSM and thus cannot be resolved with a linear-optics scheme. Furthermore, the two valid BSM outcomes together with Alice’s detection events of photon “0” (APDs e and f) were fed into a logic AND gate, providing four possible combinations. These local threefold coincidence events on La Palma as well as the remote detection events of photon “3” on Tenerife (APDs g and h) were then recorded by two separate time-tagging units (TTUs) with a temporal resolution of 156 ps. To retrieve the final fourfolds between Alice’s events and those measured on Bob’s side we calculated the cross-correlation between the remotely recorded individual measurement data—both synchronized to the Global Positioning System (GPS) standard time. To compensate for residual relative clock drifts between the distant TTU clocks we harnessed the temporal correlations of our entangled photon pairs. This clock synchronization (26) between consecutive 30-s measurements allowed for a coincidence-time window of down to 5 ns.

The strong average attenuation of −32 dB over the 143-km free-space quantum channel calls for high production rates of the SPDC sources to operate well above the noise level of the single-photon detectors on Tenerife. However, pumping the SPDC sources with high pump intensities reduces the achievable entanglement-swapping visibility (i.e., the average visibility of states ∣Ψ^{−}〉_{03} and ∣Ψ^{+}〉_{03}) due to increased multipair emissions. Hence, a reasonable trade-off between count rates and this visibility was required. To find the optimal operating point, we locally characterized our setup for various pump powers of the SPDC sources (Fig. 2). The entanglement-swapping visibilities of our setup varied between 0.87 at lowest average pump power of 60 mW and 0.49 at 950 mW full pump power. At lowest pump power we locally detected a twofold rate of 15,000 counts per second (cps) and a fourfold rate of about 1 cps. Full pump power yielded 240,000 cps twofolds and 370 cps fourfolds.

A traditional measure of entanglement is constituted by violation of a Clauser–Horne–Shimony–Holt (27) (CHSH)-type Bell inequality. To accomplish this, a CHSH S value above the classical bound of S ≤ 2 needs to be experimentally obtained, being equivalent to an entanglement visibility of 1/√2 ∼ 0.71. This was only achievable when operating at low pump powers and, given the resulting low count rates, therefore only feasible in the course of a measurement performed locally on La Palma. Nevertheless, such a local measurement serves to indicate the quality of the setup and to estimate the functionality over the long distance. We accumulated data over 8,000 s and measured the required S value for both the singlet ∣Ψ^{−}〉_{03} and triplet ∣Ψ^{+}〉_{03} state. In total we detected 5,647 singlet and 5,618 triplet swapping events and violated the inequality with S_{singlet} = 2.487 ± 0.287 and S_{triplet} = 2.469 ± 0.287 at an average pump power of 60 mW, respectively (Table 1). This result clearly proves that photons “0” and “3” were projected into an entangled state.

To reduce the accumulation time in the remote measurement scenario, we increased the average pump power to 520 mW, corresponding to a locally detected fourfold count rate of 100 cps and an average entanglement visibility of the swapped state of ∼0.60. We measured the expectation value of an entanglement-witness operator W, with W < 0 representing a sufficient condition for the presence of entanglement (28). Our entanglement-witness operator is given as_{H/V}, V_{P/M}, V_{R/L} being the correlation visibilities of state ∣Ψ〉_{03} in the three mutually unbiased bases horizontal/vertical (H/V), plus/minus (P/M) and right/left (R/L), respectively. The visibility is given by V = (CC_{max} − CC_{min})/(CC_{max} + CC_{min}) with the max (min) coincidence counts CC_{max} (CC_{min}). Inserting the measured visibilities into Eq. **3** yields a negative expectation value for the entanglement-witness operator W_{singlet}= −0.212 ± 0.027 and W_{triplet}= −0.177 ± 0.028 with statistical significances of 7.99 and 6.37 SDs, respectively (assuming Poissonian photon statistics). Hence, we unambiguously demonstrated that the experimentally obtained states between photon “0” and “3” became entangled over 143 km (Table 1). These results were obtained from subsequent 30-s data files, accumulated over a measurement time of 271 min during four consecutive nights. In total, 506 and 492 entanglement-swapping events have been recorded for the singlet and triplet state, respectively.

Our data demonstrate successful entanglement swapping via a long-distance free-space link under the influence of highly demanding environmental conditions, in fact more challenging than expected for a satellite-to-ground link. This proves the feasibility of a crucial element for realizing a quantum repeater in a future space- and ground-based worldwide quantum internet (29, 30) and for distributed quantum computation (31⇓⇓–34). In particular, in a quantum repeater scheme assuming perfect quantum memories, a single step of the purification method realized in ref. 7 would increase our obtained visibilities beyond the bound for the violation of a CHSH-type Bell inequality even in the remote scenario. Together with a reliable quantum memory, our results set the benchmark for an efficient quantum repeater at the heart of a global quantum-communication network.

## Acknowledgments

The authors thank X.-S. Ma for fruitful discussions. The authors thank the staff of the Instituto de Astrofísica de Canarias: F. Sanchez-Martinez, A. Alonso, C. Warden, M. Serra, J. Carlos; and the staff of ING: M. Balcells, C. Benn, J. Rey, O. Vaduvescu, A. Chopping, D. González, S. Rodríguez, M. Abreu, L. González; as well as J. Kuusela, E. Wille, and Z. Sodnik from the European Space Agency (ESA), for their support. This work was made possible by grants from the ESA (Contract 4000105798/12/NL/CBi), the Austrian Science Foundation under Projects SFB F4008 and CoQuS, the Austrian Research Promotion Agency within the ASAP 7 (828316) program, and the Federal Ministry of Science, Research and Economy of Austria.

## Footnotes

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^{1}To whom correspondence may be addressed. Email: thomas.herbst{at}univie.ac.at or anton.zeilinger{at}univie.ac.at.

Author contributions: T.H., T.S., R.U., and A.Z. designed research; T.H., T.S., M.F., J.H., B.W., R.U., and A.Z. performed research; T.H., T.S., M.F., J.H., R.U., and A.Z. analyzed data; and T.H., T.S., R.U., and A.Z. wrote the paper.

Reviewers: F.N., RIKEN; and G.W., University of Innsbruck.

The authors declare no conflict of interest.

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