Ground state and excitation of an asymmetric spin ladder model

We perform a systematic investigation on an asymmetric zigzag spin ladder with interleg exchange J 1 and different exchange integrals J 2 ′δ on both legs. In the weak frustration limit, the spin model can be mapped to a revised double frequency sine-Gordon model by using bosonization. Renormalization-group analysis shows that the Heisenberg critical point flows to an intermediate-coupling fixed point with gapless excitations and a vanishing spin velocity. When the frustration is large, a spin gap opens and a dimer ground state is realized. Fixing J 2 =J 1 /2, we find, as a function of δ, a continuous manifold of Hamiltonians with dimer product ground states, interpolating between the Majumdar-Ghosh and sawtooth spin-chain model. While the ground state is independent of the alternating next-nearest-neighbor exchange δ, the gap size of excitations is found to decrease with increasing δ. We also extend our study to a two-dimensional double layer model with an exactly known ground state.

[1]  H. Büttner,et al.  Exact ground state of the generalized three-dimensional Shastry-Sutherland model , 2002, cond-mat/0201003.

[2]  Bangalore,et al.  Field theoretical study of a spin-1/2 ladder with unequal chain exchanges , 2001, cond-mat/0111328.

[3]  H. Büttner,et al.  Phase diagram of an asymmetric spin ladder. , 2001, Physical review letters.

[4]  A. Fledderjohann,et al.  A numerical study of the formation of magnetisation plateaus in quasi one-dimensional spin-1/2 Heisenberg models , 2000, cond-mat/0001442.

[5]  E. Dagotto Experiments on ladders reveal a complex interplay between a spin-gapped normal state and superconductivity , 1999, cond-mat/9908250.

[6]  Yupeng Wang Exact solution of a spin-ladder model , 1999, cond-mat/9901168.

[7]  Rajiv R. P. Singh,et al.  DYNAMICAL TRANSITION FROM TRIPLETS TO SPINON EXCITATIONS : A SERIES EXPANSION STUDY OF THE J1-J2-DELTA SPIN-1/2 CHAIN , 1998, cond-mat/9811028.

[8]  A. Dobry,et al.  From spinons to magnons in explicit and spontaneously dimerized antiferromagnetic chains , 1998, cond-mat/9810073.

[9]  S. Miyahara,et al.  Exact Dimer Ground State of the Two Dimensional Heisenberg Spin System SrCu 2 ( BO 3 ) 2 , 1998, cond-mat/9807075.

[10]  A. Fledderjohann,et al.  Soft modes, Gaps and Magnetization Plateaus in 1D Spin-1/2 Antiferromagnetic Heisenberg Models , 1998, cond-mat/9810272.

[11]  Erik S. Sørensen,et al.  Soliton approach to spin-Peierls antiferromagnets: Large-scale numerical results , 1998, cond-mat/9805386.

[12]  J. von Delft,et al.  Bosonization for beginners — refermionization for experts , 1998, cond-mat/9805275.

[13]  H. Q. Lin,et al.  Exact Ground States and Excited States of Net Spin Models , 1998, cond-mat/9805269.

[14]  F. Schönfeld,et al.  Unified quantum mechanical picture for confined spinons in dimerized and frustrated spin chains , 1998, cond-mat/9805245.

[15]  O. Sushkov,et al.  BOUND STATES OF MAGNONS IN THE S = 1/2 QUANTUM SPIN LADDER , 1998, cond-mat/9803180.

[16]  J. Richter,et al.  The antiferromagnetic spin- chain with competing dimers and plaquettes: numerical versus exact results , 1998, cond-mat/9802147.

[17]  A. Kolezhuk,et al.  Non-Haldane Spin-Liquid Models with Exact Ground States , 1997, cond-mat/9712087.

[18]  A. Tsvelik,et al.  ONE-DIMENSIONAL SPIN-LIQUID WITHOUT MAGNON EXCITATIONS , 1996, cond-mat/9612014.

[19]  Schulz,et al.  Magnetic excitation spectrum of dimerized antiferromagnetic chains. , 1996, Physical review. B, Condensed matter.

[20]  White,et al.  Dimerization and incommensurate spiral spin correlations in the zigzag spin chain: Analogies to the Kondo lattice. , 1996, Physical review. B, Condensed matter.

[21]  T. M. Rice,et al.  Surprises on the Way from One- to Two-Dimensional Quantum Magnets: The Ladder Materials , 1995, Science.

[22]  Sen,et al.  Quantum solitons in the sawtooth lattice. , 1995, Physical review. B, Condensed matter.

[23]  Kubo,et al.  Elementary excitations in the Delta chain. , 1995, Physical review. B, Condensed matter.

[24]  Johannes Voit,et al.  One-dimensional Fermi liquids , 1995, cond-mat/9510014.

[25]  V. J. Emery,et al.  Quantum Magnetism of CuGeO3. , 1995, Physical review letters.

[26]  Allen,et al.  Semiclassical description of the frustrated antiferromagnetic chain. , 1994, Physical review. B, Condensed matter.

[27]  Ishida,et al.  Observation of a spin gap in SrCu2O3 comprising Ssin-12 quasi-1D two-leg ladders. , 1994, Physical review letters.

[28]  K. Nomura,et al.  Fluid-dimer critical point in S=1/2 antiferromagnetic Heisenberg chain with next nearest neighbor interactions , 1992 .

[29]  Tsvelik Am Spectrum of magnetic excitations in the spin-Peierls state. , 1992 .

[30]  Schulz,et al.  Electron-phonon interaction and phonon dynamics in one-dimensional conductors. , 1988, Physical review. B, Condensed matter.

[31]  T. Giamarchi,et al.  Anderson localization and interactions in one-dimensional metals. , 1988, Physical review. B, Condensed matter.

[32]  Schulz,et al.  Electron-phonon interaction and phonon dynamics in one-dimensional conductors: Spinless fermions. , 1987, Physical review. B, Condensed matter.

[33]  T. Bohr Erratum: Dislocations in the commensurate-incommensurate transition , 1982 .

[34]  F. D. M. Haldane,et al.  Erratum: Spontaneous dimerization in theS=12Heisenberg antiferromagnetic chain with competing interactions , 1982 .

[35]  B. Shastry,et al.  Excitation Spectrum of a Dimerized Next-Neighbor Antiferromagnetic Chain , 1981 .

[36]  B. Shastry,et al.  Exact ground state of a quantum mechanical antiferromagnet , 1981 .

[37]  I. Peschel,et al.  Calculation of critical exponents in two dimensions from quantum field theory in one dimension , 1975 .

[38]  Brosl Hasslacher,et al.  Particle spectrum in model field theories from semiclassical functional integral techniques , 1975 .

[39]  B. Hasslacher,et al.  Nonperturbative methods and extended-hadron models in field theory. II. Two-dimensional models and extended hadrons , 1974 .

[40]  J. Kosterlitz,et al.  The critical properties of the two-dimensional xy model , 1974 .

[41]  D. Thouless,et al.  Ordering, metastability and phase transitions in two-dimensional systems , 1973 .

[42]  Chanchal K. Majumdar,et al.  On Next‐Nearest‐Neighbor Interaction in Linear Chain. II , 1969 .

[43]  P. Löwdin Angular Momentum Wavefunctions Constructed by Projector Operators , 1964 .