The low- phase diagram of
arXiv:0801.2889 · doi:10.1103/PhysRevB.78.054438
Abstract
The compound is widely considered to be the archetypal dipolar Quantum Ising system, with longitudinal dipolar interactions between spins competing with transverse field-induced tunneling, to give a T=0 quantum phase transition. By varying the concentration x, the typical strength of can be varied over many orders of magnitude; and so can the transverse field . A new effective Hamiltonian is derived, starting from the electronuclear degrees of freedom, and valid at low and intermediate temperatures. For any such dipolar Quantum Ising system, the hyperfine interaction will dominate the physics at low temperatures, even if its strength : one must therefore go beyond an electronic transverse field Quantum Ising model. We derive the full phase diagram of this system, including all nuclear levels, as a function of transverse field , temperature , and dipole concentration x. For we predict a re-entrant critical field as a function of x. We also predict the phase diagram for x, and the behavior of the system in magnetic resonance and SR experiments.
19 pages, 10 figures, predictions regarding magnetic resonance experiments are added, presentation improved
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- Probing strongly hybrid nuclear-electronic states in a model quantum ferromagnet
- Phase diagram of diluted Ising ferromagnet LiHoYF
- Random-field-induced disordering mechanism in a disordered ferromagnet: Between the Imry-Ma and the standard disordering mechanism
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