ÐÏà¡±á>þÿ :<þÿÿÿ9ÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿÿì¥Á'`ð¿v'bjbjLULU <..?.?y ÿÿÿÿÿÿ¤l l l l l l l € 8@D„€ ²Æ¤¤¤¤¤õ÷÷÷÷÷÷$xhà êQl l l ¤¤ÛlZZZÞl ¤l ¤õZõZZ:Ã,l l K¤˜@”ÿ_‡ÌÞšï õ‚0²ùRÊ!xvÊ!KKÊ!l iŒ“Z¡Sîl²€ € € dä$€ € € ä€ € € l l l l l l ÿÿÿÿMagnetic and transport properties of ´-Zn10Fe D. Stani1,2, P. Pop evi1, J. Ivkov1, A. Smontara1, M. Bobnar3, S. Vrtnik3, M. Feuerbacher4, Z. Jagli i5, J. Dolinaek3 1Institute of Physics, Laboratory for the Study of Transport Problems, Zagreb, Croatia 2Department of Physics, J. J. Strossmayer University of Osijek, Osijek, Croatia 3J. Stefan Institute, University of Ljubljana, Ljubljana, Slovenia 4Institut für Festkörperforschung, Forschungszentrum Jülich, Jülich D-52425, Germany 5Institute of Mathematics, Physics and Mechanics, Ljubljana, Slovenia We have studied magnetic susceptibility, electrical resistivity, thermoelectric power, thermal conductivity, specific heat and Hall coefficient of a phase (´) that exists in Zn-rich part of Zn-Fe system. This phase crystallizes in hexagonal space group P63/mmc with unit cell parameters a=12.787(3) Å, c=57.222(7) ú and 556 atoms in unit cell [1]. The sample was a single crystal and magnetic susceptibility measurements reveal that it is a paramagnet without any hysteresis in magnetization curve. The electrical resistivity amount to about 190 mðWðcm at the room temperature. It is a metallic like with relatively large residual resistivity at low temperatures and positive temperature coefficient, but tends to saturate at room temperature. Low-temperature specific heat in C/T versus T2 plot shows an increase in C/T below 8 K, that is frequently observed in heavy fermion systems. The thermoelectric power is small (<4 ¼VDRVZ\nptvxŽ¤¦ÀÂÆÈÚÜòôøíÛÉµÉÛ¡ŒxfTÛ@f@fxf@fxfxf&h3m×h82„5H*OJQJ^JmH sH #h3m×h82„5OJQJ^JmH sH #h3m×haPm5OJQJ^JmH sH &h3m×haPm5H*OJQJ^JmH sH )h3m×haPm5>*H*OJQJ^JmH sH &h3m×haPm5>*OJQJ^JmH sH &h3m×h7–5H*OJQJ^JmH sH #h3m×h7–5OJQJ^JmH sH #h3m×hb4R5OJQJ^JmH sH #h3m×h¡Q*5OJQJ^JmH sH \R T Q ” é /0È%Ê%N&À&ïââÒÂÒÒÒ²¢’‚‚$„Rð„7]„Rð`„7a$gdþ.$„}ð„7]„}ð^„7a$gdb4R$„Rð„]„Rð^„a$gdàL©$„Rð„]„Rð^„a$gd¯0¥$„½ñ„]„½ñ^„a$gdaPm$„½ñ„]„½ñ^„a$gd82„„]ð„]„]ð^„gd82„„^ð„dà]„^ð^„gd7– Z't'þþøú 0 2 4 8 > N P R T V ìÚÆÚ·¨—·…s_N=)&h3m×h]ë6H*OJQJ^JmH sH h3m×h”—OJQJ^JmH sH h82„5H*OJQJ^JmH sH &h3m×haPm5H*OJQJ^JmH sH #h3m×hþ.5OJQJ^JmH sH #h3m×hb4R5OJQJ^JmH sH hUg°5H*OJQJ^JmH sH hUg°5OJQJ^JmH sH hOØ5OJQJ^JmH sH &h3m×hõ»5H*OJQJ^JmH sH #h3m×hõ»5OJQJ^JmH sH &h3m×hb4R5H*OJQJ^JmH sH V Q R f ” • ¡ ¢ è é ê ./0íØÄ°žž{ižiZF4*hàL©OJQJ^J#h3m×hUg°6OJQJ^JmH sH &hUg°hUg°6H*OJQJ^JmH sH hþ.6OJQJ^JmH sH #h3m×hõ»6OJQJ^JmH sH &h3m×h]ë6H*OJQJ^JmH sH hUg°6OJQJ^JmH sH #h3m×hþ.6OJQJ^JmH sH &h3m×haPm6H*OJQJ^JmH sH &h3m×haPm6OJQJ]^JmH sH )h3m×haPm6H*OJQJ]^JmH sH #h3m×h82„6OJQJ^JmH sH 0I›ª«¯ÀÃ`ŒŽÂÄÆÈ $ & € ®âïÞÍÞïÞï¼¯¼¯¢¯”¯†¯”¯yky^QDhÃh÷0POJQJ^JhÃh¥3§OJQJ^JhÃh·LOJQJ^JhÃh”—6OJQJ^JhÃh”—OJQJ^JhÃh3m×H*OJQJ^JhÃh3m×6OJQJ^JhÃh b¶OJQJ^JhÃh3m×OJQJ^J hÃh3m×OJQJ^JmH sH hÃh·LOJQJ^JmH sH hÃh:þOJQJ^JmH sH hÃh¡Q*OJQJ^JmH sH âäDLNTXrt~ Êò”îðD‚°üóæÙÌÙ¿æÙ²Ù²Ù²¥²˜²‡u‡dS‡B hÃh³R?OJQJ^JmH sH hÃh A/OJQJ^JmH sH hÃh»D OJQJ^JmH sH #hÃh›YgH*OJQJ^JmH sH hÃh›YgOJQJ^JmH sH hÃhViÍOJQJ^JhÃh b¶OJQJ^JhÃh÷0POJQJ^JhÃhz/,OJQJ^JhÃhè©OJQJ^JhÃhè©OJQJ^JhÃh»D OJQJ^JhÃh A/OJQJ^Jüþ" ","r"Ô"Ö"Ú"#’#”#–#¸#Ø#ê#%F%Ä%óâàâÏ¾¾âœ‹œziXGX6X hÃhz/,OJQJ^JmH sH hÃh b¶OJQJ^JmH sH hÃhàL©OJQJ^JmH sH hÃhàL©OJQJ^JmH sH hÃhù=WOJQJ^JmH sH hÃh»D OJQJ^JmH sH hÃhÅ¬OJQJ^JmH sH hÃhê ®OJQJ^JmH sH hÃhÈ OJQJ^JmH sH hÃhEOJQJ^JmH sH U hÃh³R?OJQJ^JmH sH hÃh³R?OJQJ^J/K) and negative with complicated temperature behaviour (local minimum around 70 K an maximum around 150 K). The thermal conductivity is anomamalolously low (<10 W/mK) for an alloy of metallic elements. Hall coefficient is positive and increases significantly with temperature at lower temperatures, while exhibiting a tendency to saturate at temperatures above the room temperature. Such temperature behaviour could be attributed to the anisotropy of electron scattering times [2]. [1] C.H.E. Belin, R.C.H. Belin, J. Sol. Stat. Chem. 151 (2000) 85 [2] P. Pop evi et al., Phys. Rev. B 81 (2010) p.184203. 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