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Sample text
A rather interesting behavior is cxhibited by the specific heat which shows a maximum cv ax at a temperature Tmax that approaches Te in a nOll-mollotollic fashion. ic parabola to the curve Tmax vs. N- 1/3, as indicated in Fig. imate of 1~ if one aSSlIlIJeS Te = 1;,ltIx(N -+ 00). h a behavior Cv = cFit + c;" N- 1/ 3 + N-2/3. o the form y = (t + in;' (x = liN). Of course, the eITect. ic trclld (e,g. y found from the fit. 015(4), and a = 5(2) . -. 00 '. "". (b) ~. ___ .. I _"' ___ """ _ _ 0 ,4 02 ~_"""""" _ A ~_' 0,6 ° 0,0 0,2 N.
Parisi and F. I. PlLys. C. Ciria, C. Parisi, and F. Rit,ort, J. PlLys. A 26, 6731 {1993}. [19J O. DiJlmann, Diploma thesis (Universitat Mainz, 1997), unpublished. [20] O. Dillmltnn, W . Janke, and K. f. Stat. Phys. 92 (July 1998), in press. [21J D. Elderfic1d and D. Sherrington, J. Phys. C 16, L491, L971, LU69 (1983). O. Petcrs, B. Diinweg, K. Binder, M. d'Onorio de Meo, and K. Vollmayr, J. Phys. A 29, 3503 (1996). [23] M. D. Reger, K. P. Young, Pllys. Rev. B 42, 6881 (1990). P. J. f. PILys. A 8, 1495 (1975).
Huse. Phys. Rev. B, 40:10801, (1989). 36 Overlap Barrier Calculations for Spin Glasses Bernd A. Berg Department of Physics, The Florida State University, Tallahassee, FL 32306, USA and Supercomputer Computations Research Institute, Tallahassee, FL 32306, USA Abstract. A novel method for numerical numerical spin glass investigations is described: Simulations of two replica at fixed temperature, weighted such that a broad distribution of the Parisi overlap parameter q is achieved. Canonical expectation values for the entire q-range (multi-overlap) follow by re-weighting and allow a calculation of spin glass tunneling barriers.