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Hall effect in superconducting Fe(Se0.5Te0.5) thin films

Source: Phys. Rev. B 81, 054515 (2010); doi:10.1103/PhysRevB.81.054515

Published 22 February 2010

ERRATUM
  1. Publisher's Note: Hall effect in superconducting Fe(Se0.5Te0.5) thin films [Phys. Rev. B 81, 054515 (2010)]
    I. Tsukada, M. Hanawa, Seiki Komiya et al.
    Phys. Rev. B 81, 099903 (2010)
PACS
  • 74.78.-w
    Superconducting films and low-dimensional structures
  • 74.25.F-
    Transport properties
  • 74.62.Dh
    Effects of crystal defects, doping and substitution on superconducting transition temperature
  • 74.70.Dd
    Superconducting ternary, quaternary and multinary compounds
  • YEAR: 2010
PUBLICATION DATA
Publisher:
AIP is a member of CrossRef APS
I. Tsukada,1,3 M. Hanawa,1,3 Seiki Komiya,1,3 T. Akiike,2,3 R. Tanaka,2,3 Y. Imai,2,3 and A. Maeda2,3
1Central Research Institute of Electric Power Industry, 2-6-1 Nagasaka, Yokosuka, Kanagawa 240-0196, Japan
2Department of Basic Science, The University of Tokyo, 3-8-1 Komaba, Meguro-ku, Tokyo 153-8902, Japan
3JST, TRIP, Sanbancho, Chiyoda-ku, Tokyo 102-0075, Japan

The Hall effect is investigated for eight superconducting Fe(Se0.5Te0.5) thin films grown on MgO and LaSrAlO4 substrates with different transition temperatures (Tc). The normal Hall coefficients (RH) have positive values with magnitude of 1~1.5×10−3  cm3/C at room temperature for the all samples. With decreasing temperature, we find two characteristic types of behavior in RH(T) depending on Tc. For thin films with lower Tc (typically Tc<5  K), RH start decreasing approximately below T=250  K toward a negative side, some of which shows sign reversal at T=50~60  K, but turns positive toward T=0  K. On the other hand, for the films with higher Tc (typically Tc>9  K), RH leaves almost unchanged down to T[approximate]100  K, and then starts decreasing toward a negative side. Around the temperatures when RH changes its sign from positive to negative, obvious nonlinearity is observed in the field-dependence of Hall resistance as to keep the low-field RH positive while the high-field RH negative. Thus, the electronic state just above Tc is characterized by ne (electron density) >nh (hole density) with keeping µe<µh. These results suggest the dominance of electron density to the hole density is an essential factor for the occurrence of superconductivity in Fe-chalcogenide superconductors. ©2010 The American Physical Society
History: Received 28 October 2009; revised 5 January 2010; published 22 February 2010
Permalink: http://link.aps.org/abstract/PRB/v81/e054515
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