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Thermoelectrics : The search for better materials Thermoelectrics : The search for better materials

Thermoelectrics : The search for better materials - PowerPoint Presentation

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Thermoelectrics : The search for better materials - PPT Presentation

Jorge O Sofo Department of Physics Department of Materials Science and Engineering and Materials Research Institute Penn State The basics Abram F Ioffe The devices The performance T 1 ID: 806945

materials phys semiconductors deformation phys materials deformation semiconductors kubo electron transport scattering linear initio method thermoelectric potential sofo applied

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Slide1

Thermoelectrics:The search for better materials

Jorge O. SofoDepartment of Physics,Department of Materials Science and Engineering,andMaterials Research InstitutePenn State

Slide2

The basics

Abram F.

Ioffe

Slide3

The devices

Slide4

The performance

T

1T2

Slide5

The materials

n-typep-type

J.-P. Fleurial, DESIGN AND DISCOVERY OF HIGHLY EFFICIENT THERMOELECTRIC MATERIALS Download Design and Discovery, Jet Propulsion Laboratory/California Institute of Technology, 1993.

Slide6

Conductivity 101

Drude et al.

k-q

q

k

Slide7

k

x

k

y

Conductivity 101

Slide8

Slide9

Slide10

Slide11

Slide12

Slide13

Slide14

Slide15

Slide16

Slide17

Slide18

Slide19

Slide20

Slide21

Slide22

Slide23

Transport distribution

Slide24

“The best thermoelectric,” G. D. Mahan and J. O. Sofo

Proc. Nat. Acad. Sci. USA,

93

, 7436 (1996)

Slide25

The “Best” Thermoelectric

Slide26

Limitations of the Boltzman Equation Method

Also known as the Kinetic Method because of the relation with classical kinetic theoryAccording to Kubo, Toda, and Hashitsume(1) cannot be applied when the mean free path is too short (e.g., amorphous semiconductors) or the frequency of the applied fields is too high.However, it is very powerful and can be applied to non linear problems.(1) R. Kubo, M. Toda, and N. Hashitsume, Statistical Physics II: Non-equilibrium Statistical Mechanics (Springer-Verlag, Berlin, 1991) p. 197

Slide27

Using Boltzman with ab-initio

C. Ambrosch-Draxl and J. O. Sofo

Linear optical properties of solids within the full-potential

linearized

augmented

planewave

method

Comp. Phys. Commun.

175

, 1-14 (2006)

Slide28

First Born Approximation

Defect scattering

Crystal defectsImpuritiesNeutral

IonizedAlloyCarrier-carrier scatteringLattice scattering

Intravalley

Acoustic

Deformation potential

Piezoelectric

Optic

Non-polar

Polar

Intervalley

Acoustic

Optic

Slide29

B. R. Nag - 1980 - Electron Transport in

Compound Semiconductors

Slide30

B. R. Nag - 1980 - Electron Transport in

Compound Semiconductors

Slide31

Slide32

T. J.

Scheidemantel, C. Ambrosch-Draxl, T. Thonhauser, J. V. Badding, and J. O. Sofo. “Transport Coefficients from First-principles Calculations.” Phys. Rev. B 68

, 125210 (2003)Bi2Te3

Slide33

Slide34

Georg Madsen’s

Slide35

Relaxation time from e-p interaction

Slide36

Deformation Potential CalculationsVan de

Walle, Chris G. “Band Lineups and Deformation Potentials in the Model-solid Theory.” Phys. Rev. B 39, 1871–1883 (1989).

Bardeen, J., and W. Shockley. “Deformation Potentials and Mobilities in Non-Polar Crystals.” Phys. Rev. 80, 72–80 (1950).

Wagner, J.-M., and F. Bechstedt. “Electronic and Phonon Deformation Potentials of GaN and AlN: Ab Initio Calculations Versus Experiment.” Phys. Status Solidi (b) 234, 965–969

(2002

)

Lazzeri

, Michele, Claudio

Attaccalite

,

Ludger

Wirtz

, and Francesco

Mauri

. “Impact of the Electron-electron Correlation on Phonon Dispersion: Failure of LDA and GGA DFT

Functionals

in Graphene and Graphite.”

Physical Review B

78, no. 8 (August 26, 2008): 081406.

Slide37

Careful…Doping: rigid bandGap problem

Temperature dependence of the electronic structure.Alloys. Single site approximations do not work.Many k-pointsCorrelated materials?Connection with magnetism and topology?

Slide38

Linear Response Theory (Kubo)Valid only close

to equilibrium HoweverDoes not need well defined energy “bands”It is easy to incorporate most low energy excitations of the solidAmenable to diagrammatic expansions and controlled approximationsEquivalent to the Boltzmann equation when both are valid.

Slide39

Summary

Tool to explore new compounds, pressure, “negative” pressure.Prediction of a new compound by G. Madsen.Easy to expand adding new Scattering MechanismsLimited to applications on “non-correlated” semiconductors.QuestionsShould we start the program of calculating all parameters from ab-initio?What about an implementation based on the Kubo formula?Where the “stochastization” will come from in a small periodic system? Remember that there should be an average somewhere to get irreversibility…