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1. Berichtskolloquium des SPP 1236, 01.10.07 – 03.10.07, Hünfeld<br />

High pressure-induced pressure induced renormalization phenomena<br />

in lead scandium niobates and tantalates<br />

with relaxor behaviour<br />

Principal investigator: Boriana <strong>Mihailova</strong><br />

Co-investigator: Ulrich Bismayer<br />

(project MI 1127/2-1)<br />

Universität Hamburg<br />

Mineralogisch-Petrographisches Institut


Co-workers Co workers and collaborators<br />

University of Hamburg<br />

Prof Dr Boriana <strong>Mihailova</strong> (JP), Prof Dr Ulrich Bismayer<br />

PhD student Anna-Maria Welsch<br />

Dr Carsten Paulmann, Dr Thomas Malcherek<br />

Virginia Tech<br />

Prof Dr Ross Angel<br />

Dr Jing Zhao, Dr Jens Engel<br />

Bulgarian Academy of Sciences<br />

Prof Dr Marin Gospodinov<br />

PTB Braunschweig<br />

Dr Bernd Güttler, Dr Rainer Stosch


Outline<br />

1. Relaxor ferroelectrics<br />

structural peculiarities and open questions<br />

2. Pressure-induced structural transformations<br />

PbSc 0.5Ta 0.5O 3 and Pb 0.78 Ba 0.22 Sc 0.5 Ta 0.5 O 3<br />

(AP - 9 GPa, RT)<br />

3. Our research plan for next 12 months


Relaxor ferroelectrics vs proper ferroelectrics<br />

proper FE PbTiO3 10 3 ε<br />

8<br />

6<br />

4<br />

2<br />

673<br />

FE<br />

773<br />

Temperature / K<br />

dielectric permittivity ε<br />

PE<br />

873<br />

relaxor FE<br />

10 3 ε<br />

Temperature / K<br />

PbMg 1/3Nb 2/3O 3<br />

high ε in relatively wide T range near RT<br />

→ multifunctionality!


Relaxor ferroelectrics – complex nanoscale structure<br />

Proper ferroelectrics<br />

T c ~ T m<br />

paraelectric<br />

ferroelectric<br />

long-range ferroelectric ordering<br />

(length of coherent atomic shifts >> a 0)<br />

T c ≤ T m<br />

Relaxor ferroelectrics<br />

T B<br />

T m<br />

Δα r ~ 0.1°<br />

pseudo-PE<br />

uncoupled atomic shifts<br />

Burns temperature (non-linearity in n(T))<br />

randomly oriented<br />

polar nanoclusters<br />

dielectric permittivity maximum<br />

coupled polar<br />

nanoclusters<br />

canonical<br />

relaxors


Relaxor ferroelectrics – open questions<br />

Atomistic nature of relaxor behaviour<br />

Can we tune relaxor properties<br />

by tailoring polar nanoclusters?<br />

nanoclusters?<br />

• Which is the driving force for nucleation of polar nanoclusters at HT?<br />

• What is the reason for suppression of ferroelectric long-range ordering at LT?<br />

local electric fields due to charge imbalance<br />

local elastic fields due to local structural distortions<br />

The majority of relaxors :<br />

Pb-based perovskite-type oxides<br />

(Pb,A”)(B’,B”)O 3<br />

performance<br />

structure<br />

properties<br />

processing


Our general goals<br />

Raman scattering and X-ray ray diffraction on single crystals<br />

PbSc0.5Ta0.5O3 (PST)<br />

and<br />

PbSc0.5Nb0.5O3 (PSN)<br />

A-site-doped PST and PSN,<br />

substitution of Ba 2+ , La 3+ , Bi 3+ for Pb 2+<br />

Nb-doped PST, substitution of Nb 5+ for Ta 5+<br />

High-pressure<br />

High pressure studies on relaxors of type PbB’ 0.5B” 0.5O3 :<br />

- atomic clustering under pressure<br />

- pressure-induced phase transitions<br />

AB’ 1/2 B” 1/2 O 3<br />

AB’ 1/3 B” 2/3 O 3<br />

- changes in the compression behaviour upon doping


Relaxors – phonon anomalies at ambient p and T<br />

prototype structure Fm3m<br />

F1u F1u Pb-localised<br />

BO3 translation vs Pb<br />

B-cation localised<br />

Pb-O bond stretching<br />

BO6 bending<br />

p-pol c-pol<br />

F 1u<br />

F 1u<br />

E g<br />

BO 6 stretching<br />

A 1g<br />

F 2g<br />

F 2u<br />

Pb-localised<br />

BO3 translation vs Pb<br />

B-localised<br />

Pb-O bond stretching<br />

BO6 bending<br />

BO6 str.<br />

bold: E i || [100]<br />

thin: E i || [110]<br />

F 2g<br />

PST<br />

PSN<br />

300-350 cm -1 (Pb-O stretching):<br />

correlated ferroic Pb-O species<br />

Raman-activity near 250 cm -1 :<br />

off-centre shifts of B-cations


PbSc 0.5Ta 0.5O 3 (PST) and Pb 0.78 Ba 0.22 Sc 0.5 Ta 0.5 O 3 (PBST) at AP<br />

Why those two compounds?<br />

PST<br />

PBST<br />

relaxor with long-range FE ordering at LT canonical relaxor


PST and PBST at HP<br />

Raman scattering, X-ray X ray diffraction and diffuse scattering<br />

AP - 9 GPa : • enhancement of the anisotropy in the Pb-O system<br />

• suppression of B-cation off-centre shifts<br />

PbSc 0.5Ta 0.5Ta0.5<br />

0.5 O3 new! new!<br />

Pb 0.78Ba 0.78Ba0.22Sc<br />

0.22Sc0.5Ta<br />

0.5Ta0.5<br />

0.5 O3 a sequence of local structural changes between 1.2 - 3.5 GPa<br />

reversible phase transition near 2.0 GPa<br />

(submitted for publication)<br />

new canonical relaxor! relaxor<br />

two types of Pb-O bonds revealed by pressure<br />

stiff octahedral distortions near the incorporated Ba cations<br />

responsible for the suppression of long-range FE ordering<br />

(to be submitted for publication)


Our research plan (next 12 months)<br />

HP Raman spectroscopy on PST and Ba-PST up to 15 GPa<br />

(an attempt to collect polarised spectra < 4 GPa)<br />

Analysis of the XRD data on<br />

PST and Ba-PST collected at DESY<br />

Pressure-induced structural transformations in PSN and Nb-doped PST<br />

(Raman scattering and XRD analysis)<br />

Ba-PSN and Ba-PST-PSN<br />

(Raman scattering)<br />

La-PST and La-PSN<br />

(Raman scattering)


Acknowledgements:<br />

Financial support by the DFG (MI 1127/2-1) 1127/2 1)<br />

Ross Angel, Jing Zhao, Jens Engel, Virginia Tech<br />

Alexandra Friedrich, Uni Frankfurt<br />

Clivia Hejny, Hejny,<br />

Uni Innsbruck<br />

Hans Ahsbahs, Ahsbahs,<br />

Uni Marburg<br />

Karsten Knorr, Knorr,<br />

Uni Kiel<br />

Leonid Dubrovinski,<br />

Dubrovinski,<br />

Uni Bayreuth<br />

Tiziana Boffa Ballaran, Ballaran,<br />

Uni Bayreuth<br />

Organisers and Lecturers of the Workshop in Bayreuth, 24.-26.04.2007<br />

24. 26.04.2007

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