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Magnetization processes in V15
Awaji : 1 Dec. 2002 Magnetization processes in V15 Univ. Tokyo S. Miyashita and K. Saito
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Quantum Dynamics in Nanoscale Molecular Magnets
Resonant Tunneling Phenomena Quantum Dynamics in Discrete Energy Levels L. Thomas, et al. Nature 383 (1996) 167. C. Sangregorio, et al. PRL 78 (1997) 4645 I. Chiorescu, et al. PRL 84 (2000) 3454.
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Resonant Tunneling Discrete Energy level structure
J. M. Hernandez, et al. PRB55(1997) 5858 Discrete Energy level structure J. A.A. J. Perenboom, PRB 58 (1998) 330
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Nonadiabatic Transition
Quantum Dynamics in Discrete Energy Levels Change in Sweeping Field Landau-Zener-Stueckelberg Mechanism C. Zener, Proc. R. Soc. (London) Ser. A137 (1932) 696. Resonant Tunneling SM, JPSJ 64(1995) 3207, 65(1996) 2734. H. De Raedt et al, PRB56 (1997) 2734
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Quantum Dynamics Nonadiabatic Transition: Phase interference LZS, RZ
Nontrivial Resonance SM, JPSJ 64 (1995) 3207, H.De Raedt, SM, K. Saito, D. Garcia-Pablos and N. Garcia, PRB 56 (1997) SM, K. Saito and H. De Raedt, PRL 80 (1998) 1525
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Successive LZS transitions
Magnetization changes only when H(t) crosses 0 SM & K. Saito, JPSJ (2001) 3238
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Dissipation Effect Thernal Bath:Quantum Master equation
Random Noise: Quantum Schroedinger equation
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Adiabatic transition and Relaxation
+ Thermal Bath Pure Quantum K. Saito, SM, H.de Raedt, Phys. Rev. B60 (1999) 14553
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V15 Adiabatic transition Phonon Bottleneck phenomena
I. Chiorescu, et al. PRL 84 (2000) 3454. Adiabatic transition Effective S=3/2 system I. Chiorescu, W. Wernsdorfer, A. Mueller, H. Boegge, B. Barbara, Phys. Rev. Lett. 84 (2000) 3454. K. Saito & SM. JPSJ (2001) 3385. H. Nakano & SM, JPSJ 70(2001) 2151
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Tunneling in half-odd integer spin systems
Tunneling Probability Half-interger、Time Reversal Sym. Kramers doublet Single spin mode Multi-spin model + DM Two avoided cross structures Adiabatic change of M(H) SM, &. N. Nagaosa, Prog. Theor. Phys. 106 (2001) 533
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5spin-model I. Rudra, S. Ramasesha, and D. Sen, J. Phys. Cond. Mat. 13 (2001) 11717 N. P. Konstantinidis and D. Coffey, cond-mat I. Rudra, K. Saito, S. Ramasesha and S. Miyashita, preprint
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Effective interaction
SM, &. N. Nagaosa, Prog. Theor. Phys. 106 (2001) 533
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Energy structure Quasi-degenerate avoided level crossing structures
4 states LZS formula works well
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4-dimensional irreducible space
Overlap of the wave function
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Nonadiabatic Transition in the Field Sweeping
Transition probability of Magnetization
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Adiabatic process in V15 Phonon Bottleneck phenomena
Plateau induced by thermal effect Chiorescu, W. Wernsdorfer, A. Mueller, H. Boegge, B. Barbara, Phys. Rev. Lett. 84 (2000) 3454.
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Reduced Density Matrix
Boson Bath K. Saito, S. Takesue and SM. Phys. Rev. B61 (2000) 2397
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Field sweeping with thermal bath
Fast sweeping Slow sweeping Magnetic FoehnEffect LZS K. Saito & SM. JPSJ (2001) 3385.
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Nonadiabatic Tr. & Heat-inflow
LZ transition Magnetic Foehn Effcet
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Non-monotonic M(H)
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Fe2 Fe-rings Y. Shapira, et al PRB59 (1999) 1046 Y. Ajiro & Y. Inagaki
Y. Narumi & K. Kindo H. Nakano & SM, JPSJ 70(2001) 2151
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Time scales in the simulation
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V15
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Diagonalization of L
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V15-MFE
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V15-magnetization relaxation
I. Chiorescu, W. Wernsdorfer, A. Mueller, S. Miyashita and B. Barbara, preprint
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Relation to the longitudinal relaxation
slow sweeping fast sweeping magnetic Feohn isothermal adiabatic
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Effects of doubly degenerate structure
Transition from 1/ /2
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Transition from 1/2 to 3/2 Symmetry change from A to E Matrix elements
for ESR
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Hidden Conservation Law?
Equilibrium process Adiabatic change SM, &. N. Nagaosa, Prog. Theor. Phys. 106 (2001) 533
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Hysteresis in field sweep
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Resonance on the AC field Non-trivial Resonance
F. Grossman,et al. PRL 67 (1991) 516. Y. Kayamuma, PRB 47 (1993) 9940 S.Miyashita, K. Saito, H. De Daedt, PRL 80 (1998) 1525.
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AC field and `effective ’ gap
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Floquet eigenvalue
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Omega=0.1
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Omega=0.001 <M(t)> 0.02 t
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Quantum Phase Effect Berry phase Control of Energy Gap by
The External Field W.Wernsdorfer & R. Sessoli: Science 284 (1999) 133
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c.f. Spin-rotation pulse
Transverse oscillating filed
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Effective gap due to the AC field
Reduce the too large gap to observe the quantum oscillation of the magnetization in time AC field effect on the sweeping Y. Kayanuma and Y. Mizumoto: PRA 62 (2000)
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Sweep with AC field
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Sweep with AC field2 <M(t)> t
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Sweep with AC field 3 avalanche ?
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Hz resonance
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Classical Switching and Quantum Switching
Switching: 2-values+Metastability Classical: Dissipation Ferromagnetic order+ Hysteresis Quantum : Dynamics Quantum States+ Adiabatic change
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Thank you for your attention
Look for some intrinsic effects due to the real time quantum dynamics Thank you for your attention
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Local magnets due to inhomogeneity
Heisenberg AF chain: Haldane state F. D. M. Haldane,Phys. Lett. 93A (1983) 464. Phys. Rev. Lett. 50(1983) 1153 Edge States Impurity Effects P. Roos and SM, PRB59 (1999) 13782 SM, S. Yamamoto, Phys. Rev. B48(1993) 915
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Inhomogeneity induced magnetization
M. Nishino, H. Onishi, K. Yamaguchi & SM: PRB62 (2000) 9463
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Quantum Langevin Equation
Non-white random field Noise Amplitude >> Gap
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Square-root time dependence
Resonat Tunneling Relaxation C. Sangregorio, T. Ohm, C. Paulsen, R. Sessoli & D. Gatteschi, PRL 78 (1997) 4645. L. Thomas et al. PRL 83 (1999) 2398. Hole digging phenomena Square-root time Initial decay of M(t) W. Wernsdorfer, et al. PRL 82 (1999) 3903
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Phenomenological theory
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SQ-phenomeno
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