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Phonon Dispersion of Perovskite Protonic Conductor SrTiO3

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Phonon Dispersion of Perovskite Protonic Conductor SrTiO3

Phonon Dispersion of Perovskite Protonic Conductor SrTiO3

Anupam Deep Sharma and *M.M. Sinha

Sant Baba Bhag Singh Institute of Engineering and Technology, Padhiana, Jalandhar (Punjab)

*Department of Physics, Sant Longowal Institute of Engineering and Technology Longowal, Sangrur (Punjab) 148106, India

E-mail: dr.anupamdeep@yahoo.com

Abstract

Phonon dispersion relation of cubic Perovskite SrTiO3 is developed on the basis of lattice dynamical simulation method based on de Launey angular force (DAF) constant model. The two types of force constants, central and angular force constants have been considered up to third neighbours. The calculated zone centre frequencies agree well with available existing results. The phonon dispersion curves of SrTiO3 in cubic phase are also drawn. The calculated results are compared and analyzed with available results.

Keywords: – Phonon dispersion; proton conductor; perovskite; SrTiO3;

  1. Introduction

    SrTiO3 is very interesting compound because of the wide applications ranging from superconducting oxide thin films, ferroelectric to proton conducting materials [1, 2]. So it is very important to understand the physical properties of this compound. Lattice dynamics is one of the important properties to understand the proton conducting nature of any material.

    In the present work the phonon dispersion curves of SrTiO3 in cubic phase has been plotted using DAF constant model and compared with available results. The phonon dispersion is helpful to calculate other thermal properties like phonon density of state, specific heat etc.

  2. Crystal Structure

    (three acoustics and twelve optic). The symmetry of these phonons at the point (in terms of the Oh representation) is

    Oh = 41u + 2u

    Where 1u and 2u representing the normal modes with triple degeneracy. One 1u mode is acoustic and the rest are optical modes. The 2u mode is inactive, while 1u modes are only IR active. The compound in cubic phase has no Raman mode.

  3. Methodology

    A de Launey angular force (DAF) constant model [3] has been used to study the phonons in the SrTiO3. In DAF model [3], the relative displacement of the reference atom and one of the neighbors is considered. The forces due to all neighbors are calculated separately and summed up together. The present calculation involves four central force constants 1 , 2, 3, 4 and four angular force constants '1, '2, '3and '4 between Ti-O, Sr-O, Sr-Ti and O-O atoms respectively up to third nearest neighbor. In the present calculation the interatomic force constants are obtained by fitting the calculated results of Zamkova et.al [4] at the ZC for transverse infrared active phonon frequencies. The force constants thus calculated are listed in Table 1. Taking these force constants as input parameters, the dynamical matrix is solved at the zone center (ZC) as well as along three symmetric directions [k00], [kk0] and [kkk]. The ZC phonons and phonon dispersion relations in three symmetric directions are plotted and discussed.

    SrTiO3

    compound shows a cubic perovskite-type

  4. Results and Discussion

crystal structure and belongs to the space group Pm- 3m. The Wyckoff positions of the atoms are Sr 1a (0.0, 0.0, 0.0), Ti 1b (0.5, 0.5, 0.5) and O 3c (0.0, 0.5,

0.5).

From the point of view of lattice dynamics, the unit cell contains five atoms give rise to 15 phonons

Table 1 presents the calculated inter-atomic force constants of SrTiO3. It is observed that

Force constant 1 between (Ti-O) is strongest among all other interatomic interactions. Followed by '1 between (TiO). This suggests that the covalent

bonding between (Ti-O) is strongest than that of others. The larger force constant corresponds to stronger bond give rise to larger value of frequency. One of the central force constant 2 between (SrO)

Table 2. Calculated zone center phonon frequencies in cm-1

is negative. The negative force constant corresponds to motion along modes that lead to energy lowering. The zone centre phonons frequencies are in good agreement with the result of Zamkova et.al [4].

The phonon dispersion relations of SrTiO3, calculated along symmetry directions in the Brillouin zone are shown in Figure 1. Obtained results of SrTiO3 are in agreement with experimental results [4, 7].

Compound:

SrTiO3

1 (Ti-O)

77.90

'1 (TiO)

18.35

2 (SrO)

-11.03

'2 (SrO)

5.0

3 (SrTi)

3.0

'3 (Sr Ti)

1.833

4 (O O)

1.5

'4 (O O)

1.0

Table 1. Values of force constants (in 103 dyne cm-1)

ZC-phonon

Present Work

Zamkova et.al.

T1u(TO1)

26.02

26

T1u(TO2)

254.1

260

T1u(TO3)

501

501

T2u

199

199

References

  1. Conard T, Philippe L, Thiry P.A, Lambin Ph., and Caudano, Surface Science 287/288 (1993) p. 382

  2. Choudhury Narayani, Walter Eric J, Kolesnikov Alexander I, and Loong Chun-Keung, Physical ReviewB, 77 (2008) p.13411

  3. Launey J de, Solid State Physics Series 2 (1956) p.219.

  4. Zamkova N G, Zinenko V I, Ivanoa O V, Maksimov E G & Sofronova S N, Ferroelectrics, 1 (2003) p.283

  5. Moreira M. L, Andres J, at. el, Chemical Physics Letters, 473 (2009) p. 293.

  6. Katsumata Tetsuhiro at, el. Solid State Ionics 108

    (1998) p. 175.

  7. Jr. Barker A.S, and Hopfield J.J, Physical Review 135-

6A (1964) p. 1732.

500

[k00] [kk0]

500

400

400

300

300

200

200

100

100

[kkk]

.

Figure 1: Phonon Dispersion relation of SrTiO3

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