Ferroelectrics, 447:63–68, 2013
Copyright © Taylor & Francis Group, LLC
ISSN: 0015-0193 print / 1563-5112 online
DOI: 10.1080/00150193.2013.821893
Vibrational Fingerprints of LiNbO
3
-LiTaO
3
Mixed Crystals
S. SANNA,
1
A. RIEFER,
1
S. NEUFELD,
1
W. G. SCHMIDT,
1
G. BERTH,
2
M. R
¨
USING,
2
A. WIDHALM,
2
AND A. ZRENNER
1
1
Lehrstuhl f¨ ur Theoretische Physik, Universit¨ at Paderborn, Warburgestraße 100,
33098 Paderborn, Germany
2
Center for Optoelectronics and Photonics (CeOPP) and Department Physik,
Universit¨ at Paderborn, Warburgestraße 100, 33098 Paderborn, Germany
Atomistic simulations in the framework of the density functional theory have been used
to model morphologic and vibrational properties of lithium niobate–lithium tantalate
mixed crystals as a function of the [Nb]/[Ta] ratio. Structural parameters such as the
crystal volume and the lattice parameters a and c vary roughly linearly from LiTaO
3
to
LiNbO
3
, showing only minor deviations from the Vegard behavior. Our ab initio calcu-
lations demonstrate that the TO
1
, TO
2
and TO
4
vibrational modes become harder with
increasing Nb concentration. TO
3
becomes softer with increasing Nb content, instead.
Furthermore, the investigated zone center A
1
-TO phonon modes are characterized by
a pronounced stoichiometry dependence. Frequency shifts as large as 30 cm
−1
are ex-
pected as the [Nb]/[Ta] ratio grows from 0 to 1. Therefore, spectroscopic techniques
sensitive to the A
1
modes (such as Raman spectroscopy), can be employed for a direct
and non-destructive determination of the crystal composition.
Keywords Ferroelectrics; vibrational properties; LiNbO
3
; LiTaO
3
; mixed crystals
I. Introduction
Both lithium niobate (LiNbO
3
, LN) and lithium tantalate (LiTaO
3
, LT) are optical ma-
terials widely used for a variety of applications ranging from optical modulators over
photo-refractive and acoustic devices to frequency doubling. Thereby mainly the piezo-
and ferroelectric properties of the materials are exploited. In particular, LN is probably the
most important electro-optic material, while LT is mainly employed as a LN replacement
for shorter wavelength applications [1]. Both materials crystallize within the R3c space
group and share several common physical and chemical properties. Commercially available
crystals are usually Czochralsky grown and lithium deficient ([Li] /[Nb], [Ta] < 1), which
results in a highly defective structure of congruent composition. Above the Curie tempera-
ture (607
◦
C for LT and 1142
◦
C for LN) a phase transition to a high-symmetry paraelectric
phase (space group R
¯
3c) occurs.
Mixed crystals have recently attracted the attention of the scientific community, as they
offer the possibility to tune the physical properties by varying the composition. Lithium
niobate-tantalate (LNT, LiNb
1-x
Ta
x
O
3
) is one of the simplest ferroelectric mixed crystals,
Received September 19, 2012; in final form March 13, 2013.
∗
Corresponding author. E-mail: simone.sanna@uni-paderborn.de
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