Abstract
We propose a scheme to probabilistically generate Greenberger–Horne–Zeilinger states encoded on the path degree of freedom of three photons. These photons are totally independent from each other, having no direct interaction during the whole evolution of the protocol, which remarkably requires only linear optical devices to work and two extra ancillary photons to mediate the correlation. The efficacy of the method, which has potential application in distributed quantum computation and multiparty quantum communication, is analyzed in comparison with similar proposals reported in the recent literature. We also discuss the main error sources that limit the efficiency of the protocol in a real experiment and some interesting aspects about the mediator photons in connection with the concept of spatial nonlocality.
Similar content being viewed by others
References
Schrödinger, E.: Discussion of probability relations between separated systems. Math. Proc. Camb. Philos. Soc. (1935). https://doi.org/10.1017/S0305004100013554
Horodecki, R., Horodecki, P., Horodecki, M.: Quantum \(\alpha \)-entropy inequalities: independent condition for local realism? Phys. Lett. Sect. A Gen. Atomic Solid State Phys. (1996). https://doi.org/10.1016/0375-9601(95)00930-2
Calabrese, P., Cardy, J.: Entanglement entropy and quantum field theory. J. Stat. Mech: Theory Exp. (2004). https://doi.org/10.1088/1742-5468/2004/06/P06002
Sarovar, M., Ishizaki, A., Fleming, G.R., Whaley, K.B.: Quantum entanglement in photosynthetic light-harvesting complexes. Nat. Phys. (2010). https://doi.org/10.1038/nphys1652
Maldacena, J., Susskind, L.: Cool horizons for entangled black holes. Fortschr. Phys. (2013). https://doi.org/10.1002/prop.201300020
Laflorencie, N.: Quantum entanglement in condensed matter systems. Quant. Entanglement Condens. Matter Syst. (2016). https://doi.org/10.1016/j.physrep.2016.06.008
Rangarajan, R., Goggin, M., Kwiat, P., Lee, K.F., Chen, J., Liang, C., Li, X., Voss, P.L., Kumar, P., Bennett, C.H., Brassard, G., Crépeau, C., Jozsa, R., Peres, A., Wootters, W.K., Lu, C.Y., Zhou, X.Q., Guhne, O., Gao, W.B., Zhang, J., Yuan, Z.S., Goebel, A., Yang, T., Pan, J.W., Hodelin, J.F., Khoury, G., Bouwmeester, D.: Optimizing type-I polarization-entangled photons “Teleporting an unknown quantum state via dual classical and Einstein–Podolsky–Rosen channels”. Phys. Rev. Lett. Nat. (1993). https://doi.org/10.1364/OE.17.018920
Bennett, C.H., Wiesner, S.J.: Communication via one- and two-particle operators on Einstein–Podolsky–Rosen states. Phys. Rev. Lett. (1992). https://doi.org/10.1103/PhysRevLett.69.2881
Ekert, A.K.: Quantum cryptography based on Bellâs theorem. Phys. Rev. Lett. (1991). https://doi.org/10.1103/PhysRevLett.67.661
Nielsen, M.A., Chuang, I.L.: Quantum Computation and Quantum Information. Cambridge University Press, Cambridge, England (2000)
Dicarlo, L., Chow, J.M., Gambetta, J.M., Bishop, L.S., Johnson, B.R., Schuster, D.I., Majer, J., Blais, A., Frunzio, L., Girvin, S.M., Schoelkopf, R.J.: Demonstration of two-qubit algorithms with a superconducting quantum processor. Nature (2009). https://doi.org/10.1038/nature08121
Blatt, R., Wineland, D.: Entangled states of trapped atomic ions. Nature (2008). https://doi.org/10.1038/nature07125
Nelson, R.J., Cory, D.G., Lloyd, S.: Experimental demonstration of Greenberger–Horne–Zeilinger correlations using nuclear magnetic resonance. Phys. Rev. A (2000). https://doi.org/10.1103/PhysRevA.61.022106
Lu, C.Y., Zhou, X.Q., Gühne, O., Gao, W.B., Zhang, J., Yuan, Z.S., Goebel, A., Yang, T., Pan, J.W.: Experimental entanglement of six photons in graph states. Nat. Phys. (2007). https://doi.org/10.1038/nphys507
Gómez, S., Mattar, A., Gómez, E.S., Cavalcanti, D., Farías, O.J., Acín, A., Lima, G.: Experimental nonlocality-based randomness generation with nonprojective measurements. Phys. Rev. A (2018). https://doi.org/10.1103/PhysRevA.97.040102
Dur, W., Vidal, G., Cirac, J.I.: Three qubits can be entangled in two inequivalent ways. Phys. Rev. A—Atomic Mol. Opt. Phys. (2000). https://doi.org/10.1103/PhysRevA.62.062314
Verstraete, F., Dehaene, J., De Moor, B., Verschelde, H.: Four qubits can be entangled in nine different ways. Phys. Rev. A—Atomic Mol. Opt. Phys (2002). https://doi.org/10.1103/PhysRevA.65.052112
Aolita, L., Chaves, R., Cavalcanti, D., Acín, A., Davidovich, L.: Scaling laws for the decay of multiqubit entanglement. Phys. Rev. Lett. (2008). https://doi.org/10.1103/PhysRevLett.100.080501
Chaves, R., Aolita, L., Acín, A.: Robust multipartite quantum correlations without complex encodings. Phys. Rev. A—Atomic Mol. Opt. Phys. (2012). https://doi.org/10.1103/PhysRevA.86.020301
Vivoli, V.C., Ribeiro, J., Wehner, S.: High fidelity GHZ generation within nearby nodes. (2018). http://arxiv.org/abs/1805.10663
Friis, N., Marty, O., Maier, C., Hempel, C., Holzäpfel, M., Jurcevic, P., Plenio, M.B., Huber, M., Roos, C., Blatt, R., Lanyon, B.: Observation of entangled states of a fully controlled 20-qubit system. Phys. Rev. X (2018). https://doi.org/10.1103/PhysRevX.8.021012
Greenberger, D.M., Horne, M.A., Shimony, A., Zeilinger, A.: Bell’s theorem without inequalities. Am. J. Phys. (1990). https://doi.org/10.1119/1.16243
Hao, J.C., Li, C.F., Guo, G.C.: Controlled dense coding using the Greenberger–Horne–Zeilinger state. Phys. Rev. A—Atomic Mol. Opt. Phys. (2001). https://doi.org/10.1103/PhysRevA.63.054301
Giovannetti, V., Lloyd, S., MacCone, L.: Advances in quantum metrology. Nat. Photonics (2011). https://doi.org/10.1038/nphoton.2011.35
Chaves, R., Brask, J.B., Markiewicz, M., Kołodyński, J., Acín, A.: Noisy metrology beyond the standard quantum limit. Phys. Rev. Lett. (2013). https://doi.org/10.1103/PhysRevLett.111.120401
Kómár, P., Kessler, E.M., Bishof, M., Jiang, L., Sørensen, A.S., Ye, J., Lukin, M.D.: A quantum network of clocks. Nat. Phys. (2014). https://doi.org/10.1038/nphys3000
Anders, J., Browne, D.E.: Computational power of correlations. Phys. Rev. Lett. (2009). https://doi.org/10.1103/PhysRevLett.102.050502
Hillery, M., Bužek, V., Berthiaume, A.: Quantum secret sharing. Phys. Rev. A—Atomic Mol. Opt. Phys. (1999). https://doi.org/10.1103/PhysRevA.59.1829
Brunner, N., Cavalcanti, D., Pironio, S., Scarani, V., Wehner, S.: Bell nonlocality. Rev. Mod. Phys. (2014). https://doi.org/10.1103/RevModPhys.86.419
Bouwmeester, D., Pan, J.W., Bongaerts, M., Zeilinger, A.: Observation of three-photon Greenberger–Horne–Zeilinger entanglement. Phys. Rev. Lett. (1999). https://doi.org/10.1103/PhysRevLett.82.1345
de Lima Bernardo, B.: Unified quantum density matrix description of coherence and polarization. Phys. Lett. Sect. A Gen. Atomic Solid State Phys. (2017). https://doi.org/10.1016/j.physleta.2017.05.018
Preskill, J.: Quantum Computation lecture notes for physics 219/computer science 219. http://www.theory.caltech.edu/people/preskill/ph229/
Bergamasco, N., Menotti, M., Sipe, J.E., Liscidini, M.: Generation of path-encoded Greenberger–Horne–Zeilinger states. Phys. Rev. Appl. 8(5), 54014 (2017). https://doi.org/10.1103/PhysRevApplied.8.054014
Su, X., Tian, C., Deng, X., Li, Q., Xie, C., Peng, K.: Quantum entanglement swapping between two multipartite entangled states. Phys. Rev. Lett. (2016). https://doi.org/10.1103/PhysRevLett.117.240503
Jin, X.R., Ji, X., Zhang, Y.Q., Zhang, S., Hong, S.K., Yeon, K.H., Um, C.I.: Three-party quantum secure direct communication based on GHZ states. Phys. Lett. Sect. A Gen. Atomic Solid State Phys. (2006). https://doi.org/10.1016/j.physleta.2006.01.035
Zukowski, M., Zeilinger, A., Horne, M.A., Ekert, A.K.: “Event-ready-detectors” Bell experiment via entanglement swapping. Phys. Rev. Lett. (1993). https://doi.org/10.1103/PhysRevLett.71.4287
de Lima Bernardo, B.: How a single photon can mediate entanglement between two others. Ann. Phys. (2016). https://doi.org/10.1016/j.aop.2016.06.018
De Lima Bernardo, B., Canabarro, A., Azevedo, S.: How a single particle simultaneously modifies the physical reality of two distant others: a quantum nonlocality and weak value study. Sci. Rep. (2017). https://doi.org/10.1038/srep39767
Hong, C.K., Ou, Z.Y., Mandel, L.: Measurement of subpicosecond time intervals between two photons by interference. Phys. Rev. Lett. (1987). https://doi.org/10.1103/PhysRevLett.59.2044
Eltschka, C., Osterlohe, A., Siewert, J., Uhlmann, A.: Three-tangle for mixtures of generalized GHZ and generalized W states. New J. Phys. (2008). https://doi.org/10.1088/1367-2630/10/4/043014
Bose, S., Vedral, V., Knight, P.L.: Multiparticle generalization of entanglement swapping. Phys. Rev. A—Atomic Mol. Opt. Phys. (1998). https://doi.org/10.1103/PhysRevA.57.822
Lu, C.Y., Yang, T., Pan, J.W.: Experimental multiparticle entanglement swapping for quantum networking. Phys. Rev. Lett. (2009). https://doi.org/10.1103/PhysRevLett.103.020501
Srivastava, A., Sidler, M., Allain, A.V., Lembke, D.S., Kis, A., Imamoglu, A.: Optically active quantum dots in monolayer WSe2. Nat. Nanotechnol. 10, 491 EP (2015). https://doi.org/10.1038/nnano.2015.60
Chakraborty, C., Kinnischtzke, L., Goodfellow, K.M., Beams, R., Vamivakas, A.N.: Voltage-controlled quantum light from an atomically thin semiconductor. Nat. Nanotechnol. 10, 507 EP (2015). https://doi.org/10.1038/nnano.2015.79
He, Y.M., Clark, G., Schaibley, J.R., He, Y., Chen, M.C., Wei, Y.J., Ding, X., Zhang, Q., Yao, W., Xu, X., Lu, C.Y., Pan, J.W.: Single quantum emitters in monolayer semiconductors. Nat. Nanotechnol. 10, 497 EP (2015). https://doi.org/10.1038/nnano.2015.75
Tran, T.T., Bray, K., Ford, M.J., Toth, M., Aharonovich, I.: Quantum emission from hexagonal boron nitride monolayers. Nat. Nanotechnol. 11, 37 EP (2015). https://doi.org/10.1038/nnano.2015.242
Aharonovich, I., Englund, D., Toth, M.: Solid-state single-photon emitters. Nat. Photonics 10, 631 (2016). https://doi.org/10.1038/nphoton.2016.186
Pan, J.W., Chen, Z.B., Lu, C.Y., Weinfurter, H., Zeilinger, A., Zukowski, M.: Multiphoton entanglement and interferometry. Rev. Mod. Phys. (2012). https://doi.org/10.1103/RevModPhys.84.777
Lopes, R., Imanaliev, A., Aspect, A., Cheneau, M., Boiron, D., Westbrook, C.I.: Atomic Hong–Ou–Mandel experiment. Nature (2015). https://doi.org/10.1038/nature14331
Kaufman, A.M., Tichy, M.C., Mintert, F., Rey, A.M., Regal, C.A.: The Hong–Ou–Mandel effect with atoms. Nature (2018). https://doi.org/10.1016/bs.aamop.2018.03.003
Acknowledgements
The authors acknowledge the Brazilian funding agency CNPq (AC’s Universal Grant No. 423713/2016-7, BLB’s PQ Grant No. 309292/2016-6), UFAL (AC’s paid license for scientific cooperation at UFRN), MEC/UFRN (postdoctoral fellowships at IIP). We also thank Rafael Chaves for fruitful discussions.
Author information
Authors and Affiliations
Corresponding author
Additional information
Publisher's Note
Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Appendix: Calculating the error influence in the protocol of GHZ state generation
Appendix: Calculating the error influence in the protocol of GHZ state generation
Here we show how to obtain the most general outcome in our protocol of GHZ state generation, as shown in Fig. 1 of the main article. First, one needs to consider all possible paths taken by the photons. At this point, we shall treat each photon independently. For the sake of notation, we divide the interferometer of Fig. 1 into 10 regions (channels), which represents the upper and lower halves of the five circuits. The upper halves of the original circuits of photons 1 to 5 will be labeled as 1, 3, 5, 7, and 9, respectively. On the other hand, the lower halves of these circuits will be labeled as 2, 4, 6, 8, and 10, respectively. For example, the history reflection–reflection–transmission (r,r,t) of photon 1 can be denoted as \((i)^2 R_1|1,1,2\rangle _1\). The parameter \(R_{1}\) represents the reflection amplitude of BS\(_{1}\), and \(i^{2}\) is the phase acquired due to the two reflections.
Note that photons 1 and 5 can have four different histories, whereas photons 2, 3, and 4 can take six different paths before detection. Therefore, the general outcome has \(4^2 6^3=3456\) terms. For example, there is a term
with coefficient
representing the path (r,r,t); (r,r,r), (t,r,t); (t,r,t) and (t,r,t) of photons 1 to 5, respectively. Again, we put a factor i whenever a reflection takes place, and \(R_{j}\) (\(T_{j}\)) is the reflection (transmission) amplitude of BS\(_{j}\). This particular path provides single photons in the channels 2, 3, 5, 7, 9. We denote such outcome as (2, 3, 5, 7, 9), which has the information that photon 1 ends up in channel 2, photon 2 in channel 3, etc. If an experiment had this history, detectors \(D_1\) and \(D_3\) would click.
Let us consider the following two histories
with coefficient
and
with coefficient
The beam splitters in our proposal have \(R=T=1/\sqrt{2}\). If the photons are indistinguishable, the above two histories are equivalent. Due to the opposite sign in the linear combination, this term does not have any contribution at the end (the HOM effect at BS\(_6\) with the simultaneously arrivals of photons 1 and 2). One can handle the failure of the HOM effect at the second layer by keeping the photons distinguishable, but changing \(R_i^2=T_i^2=\delta \) for \(i=6\dots 9\) in the coefficients, and then setting the remaining factors \(R_i\) and \(T_i\) to \(1/\sqrt{2}\) (50:50 beam splitters and allowed failure of the HOM effect with probability \(\delta \)). When \(\delta =0\), we have the ideal case considered in the main text.
Having the above substitutions been carried out, one can apply detector projections. Here we suppose that the detectors can count the number of incoming photons. To get the GHZ state (\(|\psi \rangle _1\)), for example, one needs exactly one click on the detectors \(D_1\) and \(D_3\) and no click on the other two detectors (postselection). Therefore, from the general linear combination of the outgoing state, one can select only the ones which have exactly one photon in channels 3 and 7 and no photons in channels 4 and 8.
As a matter of fact, we can restore the indistinguishability of the photons by checking the last parts of the history and identifying the indistinguishable outcomes. For example, one identifies (1, 3, 8, 10, 9) with (3, 1, 8, 10, 9). See the HOM failure example above. Then, one has to sum up over all the possible histories generating the same outcome. With \(\delta =0\), the \(D_1D_3\) postselection leads to the following general outcome:
If \(\delta \ne 0\), one has even more terms. One can easily see that there are many outcomes with multiple photons in the same channel.
Let us suppose that one can make an extra postselection step, namely selecting outcomes with single photons in each channel (for example, by using at the end an apparatus which works only with single-photon input states). In this case, the general (\(\delta \ne 0\)) outcome is the following
It is easy to see that the GHZ state is obtained when \(\delta =0\)
or restoring the notation of Sect. 2 in the main text
Rights and permissions
About this article
Cite this article
de Lima Bernardo, B., Lencses, M., Brito, S. et al. Greenberger–Horne–Zeilinger state generation with linear optical elements. Quantum Inf Process 18, 331 (2019). https://doi.org/10.1007/s11128-019-2442-z
Received:
Accepted:
Published:
DOI: https://doi.org/10.1007/s11128-019-2442-z