1. Quantum information with cold atoms Zheng-Wei Zhou( 周正威） Key Lab of Quantum Information, CAS, USTC October, 2009KITPC

2. Backgrounds on Quantum Computation(QC) Quantum Computation(QC) and Quantum Simulation(QS) with Cold atoms Standard model for QC One-Way QC QS for highly-correlated many body models Quantum Communication Summary and Outlook Outline

3. Backgrounds on Quantum Computation(QC) Father of QC （ 1981 － 1985 ） Elementary Gates for QC （ 1995 ） A. BarencoA. Barenco (Oxford), C. H. Bennett (IBM), R. Cleve (Calgary), D. P. DiVincenzo (IBM), N. Margolus (MIT), P. Shor (AT&T), T. Sleator (NYU), J. Smolin (UCLA), H. Weinfurter (Innsbruck)C. H. BennettR. CleveD. P. DiVincenzoN. Margolus P. ShorT. SleatorJ. Smolin H. Weinfurter R. FeynmanD. Deutsch C. H. Bennett

4. Quantum Algorithms 1994 1997

5. Some Methods to Overcome Decoherence （ 1 ） Quantum Error Correcting Codes （ Shor ， Steane ， Calderbank ， Laflamme ， Preskill ， etc. ）（ 1995 － 2000 ） （ 2 ） Decoherence-Free Subspaces （ Duan, Guo, Zanardi, Whaley ， Bacon, Lidar, etc. ）（ 1997 － 2000 ） （ 3 ） Dynamical Decoupling method （ Lolyd ， Viola ， Duan ， Guo, Zanardi ， etc. ） （ 1998 － 1999 ）

6. Standard Model for QC

7. Beyond Standard model (I) Topological Quantum Computing A. Kitaev (1997)

8. Beyond Standard model (II) One Way Quantum Computing R. RaussendorfH. BriegelH. Briegel (2000)

9. Beyond Standard model (III) Adiabatic Quantum Computation Dorit Aharonov et. al (2004) J. Goldstone et. al (2000) E t...... Adiabatic QCStandard QC

10. P. Zoller D. Jaksch, C. Bruder, C.W. Gardiner, J.I. Cirac and P. Zoller (1998) Intermediate targets of QC——Simulating highly-correlated many body systems D. Jaksch

11. Quantum Computer Standard QC model Quantum Simulation Adiabatic QC Beyond Classical Computer Topological QC Decoherence, Scalability, Energy gap, etc Once Fault-Tolerant QC can be realized…

12. Quantum Computation(QC) and Quantum Simulation(QS) with Cold atoms Standard model for QC One-Way QC QS for highly-correlated many body models

14. Standard Model for QC

15. 1. Register of 2-level systems (qubits) The physical origin of the confinement of cold atoms with laser light is the dipole force: Olaf Mandel, et al., Phys. Rev. Lett. 91, 010407 (2003)

16. 2. Initialization of the qubit register

19. However, nonideal conditions will always result in defects in that phase (i.e., missing atoms and overloaded sites). How to suppress these defects in the lattice? A possible approach is: the coherent filtering scheme. P. Rabl, et al., Phys. Rev. Lett. 91,110403, (2003)

20. 3 、 4. Tools for manipulation: 1- and 2-qubit gates and readout 1-qubit 1: Whether global operations are enough to implement universal quantum computation? 2: How to addressing single qubit in this system? As far as ultracold atoms trapped in an optical lattice is concerned, global operations on atoms are available. However, addressing individual atom becomes very difficult. So, to implement universal quantum computation, we should answer the following questions: OR

21. (S. Lloyd, Science 261, 1569 (1993); S. C. Benjamin, PRA 61, 020301R, 2000, PRL 88, 017904, 2002) Some proposals for QC via global operations Cellular-automata Machine

22. QC via translation-invariant operations R. Raussendorf, Phys. Rev. A 72, 052301 (2005). K. G. H. Vollbrecht et al., Phys. Rev. A 73, 012324 (2006). G. Ivanyos, et al., Phys. Rev. A 72, 022339 (2005). Z. W. Zhou, et al., Phys. Rev. A 74, 052334 (2006). In the above proposals, only translationally invariant global operations are required! Redundant qubits (space and time overhead) Initialization Physical implementation Shortcomings:

23. Bose Hubbard model Ising Model Type I Type II PRL 91,090402 (2003) PRL 81, 3108 (1998); 90, 100401(2003); 91,090402 (2003) Z. W. Zhou, et al., Phys. Rev. A 74, 052334 (2006). (Effective periodic magnetic field induced by left and right circularly polarized light)

24. 1D 2D Addressing single qubit Two-qubit operation Z. W. Zhou, et al., Phys. Rev. A 74, 052334 (2006).

25. (Phys. Rev. A 70, 012306 (2004); Phys. Rev. Lett. 93, 220502 (2004)) Some proposals for QC via addressing single atom Marked Qubit as Data-bus

27. Phys. Rev. A 70, 012306 (2004)

28. single-qubit rotation via multiqubit addressing J. Joo, et al., PHYSICAL REVIEW A 74, 042344 (2006)

29. single-qubit rotation via Position-dependent hyperfine splittings C. Zhang, et al., PHYSICAL REVIEW A 74, 042316 (2006)

30. the progress of experiments Imaging of single atoms in an optical lattice Nelson, K. D., Li, X. & Weiss, D. S. Nature Phys. 3, 556–560 (2007).

32. effective magnetic field results from the atom‘s vector light shift ：

34. Novel quantum gates via exchange interactions

35. Anderlini, M. et al. Controlled exchange interaction between pairs of neutral atoms in an optical lattice. Nature 448, 452–456 (2007).

36. Science 319, 295–299 (2008).

37. Trotzky, S. et al. Time-resolved observation and control of superexchange interactions with ultracold atoms in optical lattices. Science 319, 295–299 (2008).

38. 5. Long decoherence times How many gate operations could be carried out within a fixed decoherence time? “ For the atoms of ultracold gases in optical lattices, Feshbach resonances can be used to increase the collisional interactions and thereby speed up gate operations. However, the ‘unitarity limit’ in scattering theory does not allow the collisional interaction energy to be increased beyond the on-site vibrational oscillation frequency, so the lower timescale for a gate operation is typically a few tens of microseconds.” “ Much larger interaction energies, and hence faster gate times, could be achieved by using the electric dipole–dipole interactions between polar molecules, for example, or Rydberg atoms; in the latter case, gate times well below the microsecond range are possible.” I. Bloch, NATURE|Vol 453|19 June 2008|doi:10.1038.

39. Quantum Computation(QC) and Quantum Simulation(QS) with Cold atoms Standard model for QC One-Way QC QS for highly-correlated many body models

40. R. RaussendorfH. Briegel R. Raussendorf and H. J. Briegel, Phys. Rev. Lett. 86, 5188, (2001)

41. Graph states Graph States Stabilizer code For Example: 132 Given a graph, the corresponding graph state is

42. A Controlled Phase Gate D. Jaksch, et. al., Entanglement of atoms via cold controlled collisions, Phys. Rev. Lett. 82, 1975 (1999).

43. Nature 425, 937 (2003)

45. New Journal of Physics 10 (2008) 023005

47. Preparation of decoherence-free cluster states with optical superlattices Liang Jiang, et. Al., Phys. Rev. A 79, 022309 (2009)

48. Logical qubit in decoherence-free subspace Here, Logical qubit: Implementing a C-Phase Gate

49. Quantum Computation(QC) and Quantum Simulation(QS) with Cold atoms Standard model for QC One-Way QC QS for highly-correlated many body models

50. Cold Atoms Trapped in Optical Lattices to Simulate condensed matter physics D. Jaksch, C. Bruder, C.W. Gardiner, J.I. Cirac and P. Zoller (1998)

51. Advantages as one of promising candidates of quantum simulations Neutral atoms couple only weakly to the environment, allowing long storage and coherence times. So far, cold atoms trapped in optical lattices is the only system in which a large number of particles can be initialized simultaneously. Highly controllability Control of interaction strength with magnetic field (Feshbach Resonance) Various geometry of optical lattices Controllable tunneling rates Bosons, Fermions, or mixture

52. Bose-Hubbard Model Effective highly-correlated many body models

53. Two-component Bose-Hubbard Model

54. Feshbach resonance -- magnitude Optical lattice -- diversity Experiments: Ketterle, Esslinger etc. Weakly interacting fermions in an optical lattice -- single-band Hubbard model ( Hofstetter et al, PRL 2003 ) Strongly (resonantly) interacting fermions in optical lattice -- Boson-fermion Hubbard model ?? Stoof, Holland, Zhou, etc., 2005 Inadequate! Fermions in an Optical Lattice

55. Multi-band populations (T.-L. Ho, cond-mat/0507253; 0507255, PRL 2006) Why is it inadequate? Band gap On-site coupling rate Off-site collision couplings (L.-M. Duan, PRL 95, 243202, 2005) Off-site coupling rate Tunneling rate Off-site coupling Different bands Strong interaction effects

56. Starting point: the field Hamiltonian Keep all the bands Keep the off-site couplings L.-M. Duan, PRL 95, 243202,2005

57. Limiting case2: molecule limit Limiting case 1: atom limit

58. Quantum simulation with polar molecules A. Micheli, G. K. Brennen and P. Zoller, A toolbox for lattice-spinmodels with polar molecules, Nature Physics, 2, 341 (2006)

59. Time-of-flight imaging expansion density condensate Diagonal correlation in momentum space Detection of ultracold atoms One can also utilize density-density correlations in the image of an expanding gas cloud to probe complex many-body states.

60. Nature Physics, 4, 50 (2008)

62. Quantum Simulation Quantum Computer Limits from classical world Starting point

63. Quantum Communication  Why long-distance quantum communication is so difficult?  Transmission loss/fidelity of entanglement—decreasing exponentially with the length of the connecting channel  Solution: Quantum repeater combining entanglement swapping and purification [H. Briegel et al., Phys. Rev. Lett. 81, 5932 (1998)]

64. Atomic-ensemble-based quantum memory is used to transfer the photonic states to the excitation in atomic internal states so that it can be stored, and after the storage of a programmable time, it should be possible to read out the excitation to photons without change of its quantum state. M.D. Lukin et al., Phys. Rev. Lett. 84, 4232 (2000); M. Fleischhauer and M.D. Lukin, Phys. Rev. Lett. 84, 5094 (2000). Atomic-ensemble-based quantum memory

65.  Physical implementation of Quantum Repeater: A Scheme based on atomic ensembles, the DLCZ scheme [L.-M. Duan et al., Nature 414, 413 (2001)]

66. The phase stability problem in the DLCZ scheme  In the DLCZ protocol, two entangled pairs are generated in parallel. The relative phase between the two entangled states has to be stabilized during the entanglement generation process. As entanglement generation process is probabilistic. The experiment has to be repeated many times to ensure that there is a click at the detectors. The two phases achieved at different runs of the experiments are usually different due to the path length fluctuations in this time interval.

67. A robust, fault-tolerant quantum repeater a) Local preparation of entanglement (at adjacent nodes) by a linear-optical polarization entangler and then entanglement swapping (b) Entanglement connection (c) Linear-optical entanglement purification B. Zhao, Z.-B.Chen. et al., Phys. Rev. Lett, 98, 240502 (2007); Z.-B.Chen. et al., Phys. Rev. A 76, 022329 (2007).

70. Summary and Outlook Quantum Computation(QC) and Quantum Simulation(QS) with Cold atoms Standard model for QC One-Way QC QS for highly-correlated many body models Quantum Communication Lowering the temperature Achieving single-site addressing