1. Magnets without Direction Collin Broholm Johns Hopkins University and NIST Center for Neutron Research  Introduction  Moment Free Magnetism in one dimension  Higher dimensional MFM  Frustrated origins of MFM  Interesting aspects of MFM  Conclusions

2. G. Aeppli P. Bischer Y. Chen J. F. DiTusa D. V. Ferraris C. D. Frost T. Ito T. Lectka K. Oka Acknowledgements R. Paul D. H. Reich J. Rittner M. B. Stone H. Takagi M. Treacy G. Xu H. Yardimci I. Zaliznyak NIST Center for Neutron Research ISIS Facility, Rutherford Appleton Laboratory National Science Foundation DMR 0074571 Civilian Research and Development Foundation

3. Georgetown 9/27/01 Many electrons, few magnetic materials Filled shell in solid: Ti V Cr Mn Fe Co Ni Cu Ce Pr Nd Pm Sm Eu Gd Tb Dy Ho Er Tm U Np Pu Am Cm Partially filled shell in solid:

4. Georgetown 9/27/01 Magnetization of Solid with unfilled Shells Susceptibility data for paramagnetic salt “Brownian” spin dynamics suppresses  as 1/T FeBr(C 44 H 28 N 4 ) Dilute Fe in organic matrix FeBr(C 44 H 28 N 4 ) Dilute Fe in organic matrix

5. Georgetown 9/27/01 S=1/2 Coulomb + Pauli = Heisenberg Coulomb interactions plus Pauli principle split 4-fold spin degeneracy The level scheme is reproduced by Heisenberg Exchange Hamiltonian |J| S=1/2 |J| Singlet gnd. State: J > 0 Triplet gnd. State: J < 0

6. Georgetown 9/27/01 Interactions orient moments Ferromagnetic EuO Antiferromagnetic KNiF 3

7. Georgetown 9/27/01 Unconventional magnetism in NENP  Negative Curie Weiss temperature indicates AFM interactions  No phase transition and  Negative Curie Weiss temperature indicates AFM interactions  No phase transition and

8. Georgetown 9/27/01 A can of magnetic worms Magnetic interactions link spins in chains Magnetic interactions link spins in chains Ensemble of Quasi-one-dimensional Antiferromagnets chains Ensemble of Quasi-one-dimensional Antiferromagnets chains NENP=Ni(C 2 H 8 N 2 ) 2 NO 2 ClO 4

9. Georgetown 9/27/01 “diverges” when dimensionality of Q-space where is When is magnetism unconventional? Conventional: Unconventional: Consider the state of things at T=0 is a measure of how unconventional. We can calculate assuming that it is small for D=1 soft points D=2 soft lines D=3 soft planes

10. Moment Free Magnetism averts infrared catastrophe Y 2 BaNiO 5 Ajiro et al. (1989) 

11. Georgetown 9/27/01 Unconventional magnetism in PHCC  Negative Curie Weiss temperature indicates AFM interactions  No phase transition and  Negative Curie Weiss temperature indicates AFM interactions  No phase transition and

12. Georgetown 9/27/01 b c a c Structure also “consistent” with spin chain C 4 H 12 N 2 Cu 2 Cl 6

13. Georgetown 9/27/01 Magnetic Neutron Scattering The scattering cross section is proportional to the Fourier transformed dynamic spin correlation function Fluctuation dissipation theorem:

14. Georgetown 9/27/01 SPINS Cold neutron triple axis spectrometer at NCNR

15. Georgetown 9/27/01 PHCC is magnetically two dimensional Dispersion to “chains” Not chains but planes

16. Georgetown 9/27/01 Unconventional magnetism in CuHpCl  Negative  CW indicates AFM interactions  No phase transition and  Spin ladder model consistent with  (T)  Negative  CW indicates AFM interactions  No phase transition and  Spin ladder model consistent with  (T) Putative Spin ladder model for CuHpCl

17. Georgetown 9/27/01 CuHpCl hydrogenous single crystals

18. Georgetown 9/27/01 ….But there is dispersion to “ladder” Q // to chainQ to chain  ….and there are two modes when ladder gives only one

19. Georgetown 9/27/01 A frustrated route to Moment Free Magnetism? Magnetic Frustration: All spin pairs cannot simultaneously be in their lowest energy configuration Weak connectivity: Order in one part of lattice does not constrain surrounding spins Frustrated Weakly connected

20. Georgetown 9/27/01 “diverges” when dimensionality of Q-space where is When is magnetism unconventional? Conventional: Unconventional: Consider the state of things at T=0 is a measure of how unconventional. We can calculate assuming that it is small for D=1 soft points D=2 soft lines D=3 soft planes

21. Georgetown 9/27/01 Neutrons can reveal frustration The first  -moment of scattering cross section equals “Fourier transform of bond energies” For a powder sample we know only Q=|Q|  high Qd plateau measures ground state energy  negative terms are “frustrated bonds”  bond energies are small if small   drrd SSand/or J

22. Georgetown 9/27/01 Neutrons reveal frustration in CuHpCl Peak to plateau ratio Mixed signs for bond energies Frustration

23. Georgetown 9/27/01 Structure of CuHpCl CuHpCl is hydrogen bonded crystal of Cu 2 (C 5 H 12 N 2 ) 2 Cl 4 Molecules possess approximate centro symmetry Exchange interaction within molecule |J|<1 meV

24. Two lattices from H-bond exchange b

25. Georgetown 9/27/01 Building an enigma Dispersion throughout a-c plane Spin liquid on 3-dimensional lattice

26. Georgetown 9/27/01 Detailed bond energy distribution a* c* (101) (100) (001) Point size First moment

27. Georgetown 9/27/01 Frustrated three dimensional spin liquid

28. Significance of findings so far  Neutron scattering required to classify quantum spin liquids  Systems thought to be one dimensional may represent a richer class of materials  Experimental realizations of spin liquids were sought, not found, in symmetric frustrated magnets  Perhaps spin liquids are more common in complex geometrically frustrated lattices

29. Georgetown 9/27/01 Impurities in a quantum spin liquid Ca 2+ Y 3+ Mg 2+ on Ni 2+ sites finite length chains Ca 2+ on Y 3+ sites mobile bond defects Mg Ni Kojima et al. (1995) Mg Ca 2+ Pure

30. Georgetown 9/27/01 Holes dressed by spin polarons Y3+Y3+ Ni O FM Ca 2+

31. Georgetown 9/27/01 Transport in Ca doped Y 2 BaNiO 5 T. Ito et al. Submitted to PRL (2001) Charge Transfer excitation Charge polaron 1D conductivity, no Charge ordering

32. Georgetown 9/27/01 Holes in a quantum spin liquid  Experiments in one dimensional spin liquids show holes dressed by spin polaron  However, impurities localize charge in one dimension  Some organic materials can be doped and conduct in Field Effect Transistors [Schon et al. Science (2000)]  If this were possible for organo-metallic spin liquids, could have fascinating correlated metals. PHCC

33. Conclusions  Spin systems with a gap can be mistaken for being quasi-one-dimensional  Two and three dimensional moment free magnetism found in PHCC and CuHpCl  Neutron scattering reveals frustrated bonds in the corner-sharing triangular clusters of these materials  Hypothesis: Moment free magnetism may be a common state of interacting spin systems with triangular motif and weak connectivity  Idea: Interesting transport properties may exist if the materials can be doped