z-logo
open-access-imgOpen Access
Two-layer Hall effect model for intermediate band Ti-implanted silicon
Author(s) -
J. Olea,
G. González-Dı́az,
David Pastor,
I. Mártil,
Antonio Martı́,
E. Antolín,
A. Ĺuque
Publication year - 2011
Publication title -
journal of applied physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.699
H-Index - 319
eISSN - 1089-7550
pISSN - 0021-8979
DOI - 10.1063/1.3561374
Subject(s) - materials science , silicon , band gap , condensed matter physics , substrate (aquarium) , semiconductor , hall effect , layer (electronics) , electron mobility , sheet resistance , metal , optoelectronics , electrical resistivity and conductivity , nanotechnology , physics , metallurgy , oceanography , quantum mechanics , geology
Si samples have been implanted with very high Ti doses (over the theoretical Mott limit) to obtain an intermediate band (IB) in the host semiconductor. The electronic transport properties of this material have been analyzed by temperature-dependent sheet resistance and Hall effect measurements in the 7-400 K range. The experimental results are successfully explained by means of an analytical two-layer model, in which the implanted layer and the substrate behave as an IB/n-Si type junction. We deduce that the IB is located at 0.38 eV below the conduction band, which is around one third of the Si bandgap, i.e., theoretically close to the optimum location for an IB. Finally, we obtain that carriers at the IB behave as holes with a mobility of 0.4-0.6 cm(2) V(-1) s(-1). This extremely low mobility is the one expected for a semifilled, metallic band, being this metallic condition of the IB a requirement for IB solar cells

The content you want is available to Zendy users.

Already have an account? Click here to sign in.
Having issues? You can contact us here
Accelerating Research

Address

John Eccles House
Robert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom