The Seebeck Coefficient: - UCSB MRSEC

The Seebeck Coefficient: - UCSB MRSEC

THE SEEBECK COEFFICIENT Anthony Rice MTRL 286K 12/15/14 Outline The Seebeck coefficient is a property dependent on the electronic structure near the fermi-level and is sensitive to

things including effective mass, carrier concentration, and band shape Seebeck measurements may be used to further elucidate basic electronic properties through a transition NaCo2O4 is a high-Seebeck metal, with possible explanations including configurational entropy and peculiar band shape The Seebeck Effect

= Power Factor [ -Direct Eg, Parabolic bands

J. Solyom. Fundamentals of the Physics of Solids A. Shakouri. Annu. Rev. Mater. Res. 2011. 41:399431 Typical Metallic Values Sign determines whether dominant conduction occurs below or above fermi level J. Solyom. Fundamentals of the Physics of Solids

Mott Formula For a Metal/degenerate-semiconductor: M. Cutler, N.F. Mott. Phys. Rev. 181, 1336 (1969) Generalized For a Semiconductor: -carrier lifetimecarrier lifetime

v-carrier lifetimegroup velocity -carrier lifetimeband dispersion A- material dependent constant J. Solyom. Fundamentals of the Physics of Solids H. Fritzsche,Solid State Commun.9, 1813 (1971) Pisarenko Plots

Seebeck vs. n plot, generally log-log Should be a universal relationship for a given band-structure/material Slope ~200 for a parabolic band insulator B. Jalan, S. Stemmer. Appl. Phys. Lett. 97, 042106 (2010)

PbTe:Tl Solid line-calculated/published to date Dots-Current study J.P. Heremans. V. Jovovic. E.S. Toberer. A. Saramat. K. Kurosaki. A. Charoenphakdee. S. Yamanak, G.J. Snyder. Science 25 July 2008: Vol. 321 no. 5888 pp. 554-557 V1-XWxO2: TMI vs. Ts

T. Katase, K. Endo, and H. Ohta. Phys. Rev. B 90, 161105(R) (2014) V1-XWxO2:Parabolic Bands? T. Katase, K. Endo, and H. Ohta. Phys. Rev. B 90, 161105(R) (2014) Magnetite at the Verwey Transition

Oxidation varied-A least oxidized, E most Above ~120K-independent of oxidation -Provides a probe of carrier type without B-field A.J.M. Kuipers and V.A. Brabers. Phys. Rev. B. 14, 1401 (1976) Thermopower in the Correlated Hoping Regime

Seebeck governed by entropy change due to addition of one more carrier in cases of interacting carriers at high temperatures Heikes formula P.M. Chaikin, G. Beni. Phys. Rev. B. 13, 647 (1975) NaCo2O4

Na/CoO2 Layered Structure At stoichiometry, Co valence +3.5 I. Terasaki, Y. Sasago and K. Uchinokura. Phys. Rev. B 56, R12 685 (1997) Initial explanation- Hopping due to degeneracy g3, g4.-# of configurations for each valence

x-ratio of 3+/4+ states (depends on x na) Degeneracy, plus 3d correlation effects causes large S W. Koshibae, K. Tsutsui, S. Maekawa. Phys. Rev. B. 62, 6869 (2000) ARPES Results Missing crossings near K point

Na0.7CoO2 D.J. Singh. Phys. Rev. B. 13397 (2000) H.-B. Yang et al. Phys. Rev. Lett. 92, 246403 (2004) Na0.6CoO2 M. Z. Hasan et at. Phys. Rev. Lett. 92, 246402 (2004) Pudding mold Bands

K. Kuroki, R. Arita. J. Phys. Soc. Jpn. 76, 083707 (2007) Fe(As1-xSex)2 Pnnm (no. 58) H. Usui, K. Suzuki, K. Kuroki, S. Nakano, K. Kudo, M. Nohara. Phys. Rev. B. 88, 075140 (2013)

Summary The Seebeck coefficient provides useful information beyond resistivity for basic electronic studies Metal-insulator studies may be further enhanced by using thermopower measurements A number of materials with unique band-structure may be potential candidates for further thermoelectric study

CuAlO2-Proposed Hole-doped TE K. Mori, H. Sakakibara, H. Usui, K. Kuroki. Phys. Rev. B. 88, 075141 (2013)

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