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June 27- July 1, 2005 Trieste, Italy. Numerical study on ESR of V15. IIS, U. Tokyo, Manabu Machida RIKEN, Toshiaki Iitaka Dept. of Phys., Seiji Miyashita. Nanoscale molecular magnet V15. [A. Mueller and J. Doering (1988)]. Vanadiums provide fifteen 1/2 spins.
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June 27- July 1, 2005 Trieste, Italy Numerical study on ESR of V15 IIS, U. Tokyo, Manabu Machida RIKEN, Toshiaki Iitaka Dept. of Phys., Seiji Miyashita
Nanoscale molecular magnet V15 [A. Mueller and J. Doering (1988)] Vanadiums provide fifteen 1/2 spins. (http://lab-neel.grenoble.cnrs.fr/)
The parameter set [H. De Raedt, et al., PRB 70 (2004) 064401] [M. Machida, et al., JPSJ (2005) suppl.]
Difficulty difficult! – Direct diagonalization requires memory of – Its computation time is of (e.g. S. Miyashita et al. (1999))
Two numerical methods • The double Chebyshev expansion method(DCEM) -speed and memory ofO(N) - all states and all temperatures • The subspace iteration method(SIM) - ESR at low temperatures.
ESR absorption curves DCEM Typical calculation time for one absorption curve is about half a day.
Background of DCEM The DCEM = a slight modification of the Boltzmann-weighted time-dependent method (BWTDM). [T. Iitaka and T. Ebisuzaki, PRL (2003)] Making use of the random vector technique and the Chebyshev polynomial expansion
DCEM (1) Random phase vector
>> DCEM (2) Chebyshev expansions of the thermal and time-evolution operators. small w
Temperature dependence of intensity Our calculation Experiment [Y.Ajiro et al. (2003)]
ESR at low temperatures by SIM Intensity ratio We consider the lowest eight levels.
Temperature dependence of R(T) With DM Without DM
Intensity ratio of triangle model At zero temperature
Summary O(N) algorithms for the Kubo formula DCEM ■ Random vector and Chebyshev polynomials ESR of V15 ■ High to low temperatures by DCEM ■Ultra-cold temperature by SIM ■ Triangle model analysis M. Machida, T. Iitaka, and S. Miyashita, JPSJ (2005) suppl. (cond-mat/0501439)