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Effect of Native Defects on Transport Properties in Non-Stoichiometric CoSb(3)

The effect of native defects originated by a non-stoichiometric variation of composition in CoSb(3) on I-V curves and Hall effect was investigated. Hysteretic and a non-linear behavior of the  I-V curves at cryogenic temperatures were observed; the non-linear behavior originated from the Poole-Frenk...

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Detalles Bibliográficos
Autores principales: Realyvázquez-Guevara, Paula R., Rivera-Gómez, Francisco J., Faudoa-Arzate, Alejandro, Botello-Zubiate,  María E., Sáenz-Hernández, Renee J., Santillán-Rodríguez, Carlos R., Matutes-Aquino, José A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2017
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5503341/
https://www.ncbi.nlm.nih.gov/pubmed/28772648
http://dx.doi.org/10.3390/ma10030287
Descripción
Sumario:The effect of native defects originated by a non-stoichiometric variation of composition in CoSb(3) on I-V curves and Hall effect was investigated. Hysteretic and a non-linear behavior of the  I-V curves at cryogenic temperatures were observed; the non-linear behavior originated from the Poole-Frenkel effect, a field-dependent ionization mechanism that lowers Coulomb barriers and increases emission of charge carriers, and the hysteresis was attributed to the drastic decrease of specific heat which produces Joule heating at cryogenic temperatures. CoSb(3) is a narrow gap semiconductor and slight variation in the synthesis process can lead to either n- or p-type conduction. The Sb-deficient CoSb(3) presented an n-type conduction. Using a single parabolic model and assuming only acoustic-phonon scattering the charge transport properties were calculated at 300 K. From this model, a carrier concentration of 1.18 × 10(18) cm(−3) and a Hall factor of 1.18 were calculated. The low mobility of charge carriers, 19.11 cm(2)/V·s, and the high effective mass of the electrons, 0.66 m(0), caused a high resistivity value of 2.75 × 10(−3) Ω·m. The calculated Lorenz factor was 1.50 × 10(−8) V(2)/K(2), which represents a decrease of 38% over the degenerate limit value (2.44 × 10(−8) V(2)/K(2)).