Designing spin-1 lattice models using polar molecules

We describe how to design a large class of always on spin-1 interactions between polar molecules trapped in an optical lattice. The spin degrees of freedom correspond to the hyperfine levels of a ro-vibrational ground state molecule. Interactions are induced using a microwave field to mix ground states in one hyperfine manifold with the spin entangled dipole–dipole coupled excited states. Using multiple fields, anistropic models in one, two, or three dimensions can be built with tunable spatial range. An illustrative example in one-dimension is the generalized Haldane model, which at a specific parameter has a gapped valence bond solid ground state. The interaction strengths are large compared to decoherence rates and should allow for probing the rich phase structure of strongly correlated systems, including dimerized and gapped phases.

[1]  S. A. Dodds,et al.  Chemical Physics , 1877, Nature.

[2]  G. G. Stokes "J." , 1890, The New Yale Book of Quotations.

[3]  H. Radford Hyperfine Structure of theBΣ+2State of CN , 1964 .

[4]  C. Lai Lattice gas with nearest‐neighbor interaction in one dimension with arbitrary statistics , 1974 .

[5]  B. Sutherland Model for a multicomponent quantum system , 1975 .

[6]  J. Hoeft,et al.  Effects of unresolved hyperfine structure in the microwave rotational spectra of the 2Σ-radicals CaBr and CaCl , 1982 .

[7]  J. Hoeft,et al.  Rotational spectrum and hyperfine structure of the 2Σ radicals BaF and BaCl , 1982 .

[8]  W. Ernst,et al.  Determination of the ground-state dipole moment of CaCl from molecular-beam laser-microwave double-resonance measurements , 1984 .

[9]  E. Lieb,et al.  Valence bond ground states in isotropic quantum antiferromagnets , 1988 .

[10]  A. Auerbach Interacting electrons and quantum magnetism , 1994 .

[11]  Dudley R. Herschbach,et al.  Polarization of Molecules Induced by Intense Nonresonant Laser Fields , 1995 .

[12]  Garel,et al.  Onset of incommensurability at the valence-bond-solid point in the S=1 quantum spin chain. , 1996, Physical review. B, Condensed matter.

[13]  Seth Lloyd,et al.  Universal Quantum Simulators , 1996, Science.

[14]  G. Müller,et al.  Static and Dynamic Structure Factors in the Haldane Phase of the Bilinear-Biquadratic Spin-1 Chain , 1998 .

[15]  P. Alsing,et al.  Spatial correlation diagnostics for atoms in optical lattices. , 1999, Optics express.

[16]  G. K. Brennen,et al.  Quantum logic for trapped atoms via molecular hyperfine interactions , 2002 .

[17]  D DeMille Quantum computation with trapped polar molecules. , 2002, Physical review letters.

[18]  Andrew M. Childs,et al.  Universal simulation of Hamiltonian dynamics for quantum systems with finite-dimensional state spaces , 2002 .

[19]  G. Ortiz,et al.  Unveiling order behind complexity: Coexistence of ferromagnetism and Bose-Einstein condensation , 2002, cond-mat/0207073.

[20]  Artificial light and quantum order in systems of screened dipoles , 2002, cond-mat/0210040.

[21]  G. Vidal Efficient classical simulation of slightly entangled quantum computations. , 2003, Physical review letters.

[22]  M. Lukin,et al.  Spin-exchange interactions of spin-one bosons in optical lattices: Singlet, nematic, and dimerized phases , 2003, cond-mat/0306204.

[23]  M. Lukin,et al.  Controlling spin exchange interactions of ultracold atoms in optical lattices. , 2002, Physical review letters.

[24]  Quantum state control via trap-induced shape resonance in ultracold atomic collisions. , 2003, Physical review letters.

[25]  R. Krems,et al.  Topical issue on Ultracold polar molecules: Formation and collisions , 2004 .

[26]  J I Cirac,et al.  Diverging entanglement length in gapped quantum spin systems. , 2004, Physical review letters.

[27]  M. Lukin,et al.  Probing many-body states of ultracold atoms via noise correlations (4 pages) , 2003, cond-mat/0306226.

[28]  Guifré Vidal Efficient simulation of one-dimensional quantum many-body systems. , 2004, Physical review letters.

[29]  J J García-Ripoll,et al.  Implementation of spin Hamiltonians in optical lattices. , 2004, Physical review letters.

[30]  X. Wen Quantum Field Theory of Many-body Systems: From the Origin of Sound to an Origin of Light and Electrons , 2004 .

[31]  M. Rosa Laser-cooling molecules , 2004 .

[32]  P Zoller,et al.  Atomic quantum simulator for lattice gauge theories and ring exchange models. , 2005, Physical review letters.

[33]  I. Bloch Ultracold quantum gases in optical lattices , 2005 .

[34]  Department of Physics,et al.  Optical production of ultracold polar molecules. , 2005 .

[35]  G J Milburn,et al.  Measurement-based teleportation along quantum spin chains. , 2005, Physical review letters.

[36]  D. Porras,et al.  Renormalization algorithm for the calculation of spectra of interacting quantum systems , 2006 .

[37]  F. Verstraete,et al.  Matrix product states represent ground states faithfully , 2005, cond-mat/0505140.

[38]  T. Osborne Efficient approximation of the dynamics of one-dimensional quantum spin systems. , 2006, Physical review letters.

[39]  I. Chuang,et al.  Limitations of quantum simulation examined by simulating a pairing Hamiltonian using nuclear magnetic resonance. , 2006, Physical review letters.

[40]  R. Ciuryło,et al.  Stationary phase approximation for the strength of optical Feshbach resonances , 2006 .

[41]  P. Zoller,et al.  A toolbox for lattice-spin models with polar molecules , 2006 .

[42]  Jun Ye,et al.  Cold molecule spectroscopy for constraining the evolution of the fine structure constant. , 2006, Physical review letters.