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Physics and Chemistry of ABO3
Nanostructures from First Principles
Ghanshyam Pilania
Chemical, Materials & Biomolecular Engineering
Institute of Materials Science
University of Connecticut
Principal Advisor: Prof. R. Ramprasad
Associate Advisor: Prof. P. Gao
Associate Advisor: Prof. G. Rossetti, Jr.
Ph.D. Dissertation Proposal
ABO3-type Perovskite structure
A
B
O
Novel polarization states in ABO3 nanowires
(p,T) surface phase diagrams of ABO3 surfaces
“Vortex” v/s “axial” polarization states
Effect of size, surface termination and axial strain on the
polarization states
Outline
Methodology to construct surface phase diagrams
Calculated (p,T) surface phase diagrams for LaMnO3 and
PbTiO3 (001) surfaces
Remaining work
Impact of work
Novel polarization states in ABO3
nanowires
Ferroelectricity in bulk perovskites
Ferroelectricity: a collective phenomena
A balance between
long range Coulombic force (favor ferroelectric state)
short range repulsive forces (resist ferroelectric state)
Dipole moment per unit volume = Polarization
T
Tc
Ferroelectric
Paraelectric
ABO3 perovskite
Energy
P
Paraelectric state
ABO3 perovskite Ferroelectric Well
Energy
P
Paraelectric state
Energy
P
Ferroelectric state
Energy
P
Ferroelectricity in Nanostructures
Thin film
Depolarizing
Field
+++++++++
- - - - - - - - -
Bulk
Aguado-Puente et al. (PRL, 2008)
Ferroelectricity in Nanostructures
P
Depolarizing
Field
P
No depolarizing
Field
No depolarizing
Field
Closure domain
Prosendeev & Bellaiche (PRB 2007)
PFM results indicate possible presence of non-
rectilinear polarization in PZT nanodots
Rodriguez et al (Nanoletters, 2009)
ABO3 Nanowires – Our DFT Study
2x2-AO-terminated
nanowire
2x2-BO2-terminated
nanowire
AO-plane
BO2-plane
AO-plane
BO2-plane
Construction of ABO3 nanowires
BaTiO3 Nanowires – Our DFT Study
Axial polarization
instability above
1.2 nm
ferroelectric
paraelectric 4x4-TiO2
P
4x4-BaO
τ=rxP
Vortex polarization
instability above
1.6 nm
Geneste et. al, APL 88, 112906 (2006);
Spanier et al, Nano Lett. 6, 735 (2006)
0.8 nm
Off-axis Polarization in BaTiO3 nanowires
BaTiO3 Nanowires – Experimental Study
PbTiO3 Nanowires – Our DFT Study
c (Å)
Fa
Fa
Fa
Fa
P
1x1 to 4x4-PbO
Fv
Shimada et al, PRB 79, 024102 (2009)
c tetragonal Bulk
acubic Bulk
P
P
P
4x4-TiO2
τ=rxP
Unit cell decomposed
dipole moments
PbTiO3 Nanowires vs. Terminations
Strain-induced phase transition: vortex  axial polarization
4x4-TiO2-terminated
nanowire
[001]
Axial compressive Strain
Axial Tensile Strain
4x4-PbO-terminated
nanowire
Four possible switchable polarization states
Vortex (clockwise/counter-clockwise), Axial (positive/negative)
PbTiO3 nanowires display switchable rectilinear (axial)
and non-rectilinear (vortex) polarization configurations
Control of polarization states
axial Strain and surface terminations
(T, p) surface phase diagrams of
ABO3 systems
Flexibility
Versatility
Less expensive
Thermal stability
Excellent oxygen exchange properties
Why are they important?
Perovskite Surfaces in Catalysis
R. J. H. Voorhoeve, D. W. Johnson, Jr., J. P. Remeika, P. K. Gallagher
SO4
-2
Dead site Active site
Sulfur poisoning
26 MARCH 2010 VOL 327 SCIENCE
Chang Hwan Kim, Gongshin Qi, Kevin Dahlberg, Wei Li
Perovskite Surfaces in Catalysis
Suprafacial v/s Intrafacial
2
2
1
O
O 
 
Surface-O*↔ Surface + ½ O2 (g)
Cubic LaMnO3 and PbTiO3 surface phase diagrams
+ N/2 O2
Cubic LaMnO3 and PbTiO3 surface phase diagrams
(1x1) AO-terminated (1x1) BO2-terminated
Formation Energies
Cubic LaMnO3 and PbTiO3 surface phase diagrams
A
Relaxed geometries for most favored adsorption sites
Cubic LaMnO3 and PbTiO3 surface phase diagrams
Perovskite surfaces in contact with O2 (g)












 0
0
0 2
2
2
2
ln
)
,
(
)
,
0
(
)
,
(
p
p
T
k
p
T
p
K
T
p
T
O
B
O
O
O 


Assuming ideal gas behavior for O2
2
2
1
O
O 
 
Surface-O*↔ Surface + ½ O2 (g)
Surface phase diagrams for surfaces in contact with O2
PbTiO3 (001) TiO2-terminated
log
P
O2
100% O ad-atom coverage
Partial O vacancy
coverage
Partial coverage of O ad-atom
Clean surface
100% O vacancy
T (K)
LaMnO3 (001) MnO2-terminated
100% O vacancy
Partial coverage of
O ad-atom
100% O ad-atom coverage
log
P
O2
T (K)
Remaining Work
Electric field response of the vortex polarization state in PbTiO3
nanowires
Efield ?
Dielectric tensor of ferroelectric nanowires
4x4-PbO terminated nanowire (axial polarization)
4x4-TiO2 terminated nanowire (vortex polarization)
Effect of surface passivation (by various species such as –OH,
H, -CH3 etc.) on polarization states in PbTiO3 nanowires
Thermodynamics of environment dependent interaction of various
gases on the (001) surface of ABO3 type perovskites
NO, NO2, N2, O2
(gases)
Adsorption site
Equilibrium geometry
Electronic structure
Energetics
Kinetics ??
Remaining Work
Impact of Work
0 1 0 0
Non volatile Ferroelectric memory
Potential to increase present memory storage density by five order of magnitude
How to shrink the
hard drive?!!
Impact of Work
DeNOx processes
NO + CO +
unburned
hydrocarbons
catalytic
converter
CO CO2
NOx
N2 + O2
CnHm CO2+H2O
LaCoO3 (○)
La0.9Sr0.1CoO3 (●)
LaMnO3 (□)
La0.9Sr0.1MnO3 (■)
commercial DOC (▲)
List of Publications
G. Pilania, S. P. Alpay and R. Ramprasad, "Ab initio study of ferroelectricity in
BaTiO3 nanowires", Phys. Rev. B 80, 014113(1)-014113(7)- (2009).
G. Pilania, D. Q. Tan, Y. Cao, V. S. Venkataramani, Q. Chen and R. Ramprasad,
"Ab initio study of antiferroelectric PbZrO3 (001) surfaces", J. Mater. Sci. 44, 5249-
5255 (2009).
G. Pilania, T. Sadowski and R. Ramprasad, "Oxygen adsorption on CdSe
Surfaces: A case study of asymmetric anisotropic growth through Ab initio
computations", J. Phys. Chem. C. 113(5), 1863-1871 (2009).
J. D. Doll, G. Pilania, R. Ramprasad and F. Papadimitrakopoulos, "Oxygen-
Assisted Unidirectional Growth of CdSe Nanorods Using a Low-Temperature
Redox Process", Nano Lett., 10 (2), 680-685 (2010).
G. Pilania and R. Ramprasad “Vortex -Polarization Instability in PbTiO3
nanowires”, under review.
G. Pilania and R. Ramprasad “Thermodynamics of environment dependent
oxygen adsorption and vacancy formation on cubic PbTiO3 and LaMnO3 (001)
surfaces”, In preparation.
Acknowledgments
Group Members :
Ning, Tang, Tom, Hong, Satyesh, Chenchen, Yenny
Committee members:
Profs. Rampi Ramprasad, Puxian Gao and George A. Rossetti, Jr.
Profs. Rainer Hebert and Pamir S. Alpay
Computational resources:
IMS computation clusters; SGI supercomputer in SoE and Teragrid
Funding:
NSF & ONR
Thanks!
Back-up slides
[001]
4x4-TiO2-terminated
nanowire
4x4-TiO2 terminated Nanowire
Atomic relaxations in the vortex state
Cubic LaMnO3 and PbTiO3 surface phase diagrams
∆γ=
Effect of vibrational free energy
(1x1)-MnO2-terminated (001) LaMnO3 surface
O ad-atoms
% change in ∆γ
T (k)
O vacancies
% change in ∆γ
T (k)

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7633426.ppt

  • 1. Physics and Chemistry of ABO3 Nanostructures from First Principles Ghanshyam Pilania Chemical, Materials & Biomolecular Engineering Institute of Materials Science University of Connecticut Principal Advisor: Prof. R. Ramprasad Associate Advisor: Prof. P. Gao Associate Advisor: Prof. G. Rossetti, Jr. Ph.D. Dissertation Proposal
  • 3. Novel polarization states in ABO3 nanowires (p,T) surface phase diagrams of ABO3 surfaces “Vortex” v/s “axial” polarization states Effect of size, surface termination and axial strain on the polarization states Outline Methodology to construct surface phase diagrams Calculated (p,T) surface phase diagrams for LaMnO3 and PbTiO3 (001) surfaces Remaining work Impact of work
  • 4. Novel polarization states in ABO3 nanowires
  • 5. Ferroelectricity in bulk perovskites Ferroelectricity: a collective phenomena A balance between long range Coulombic force (favor ferroelectric state) short range repulsive forces (resist ferroelectric state) Dipole moment per unit volume = Polarization T Tc Ferroelectric Paraelectric ABO3 perovskite Energy P Paraelectric state ABO3 perovskite Ferroelectric Well Energy P Paraelectric state Energy P Ferroelectric state Energy P
  • 6. Ferroelectricity in Nanostructures Thin film Depolarizing Field +++++++++ - - - - - - - - - Bulk Aguado-Puente et al. (PRL, 2008)
  • 7. Ferroelectricity in Nanostructures P Depolarizing Field P No depolarizing Field No depolarizing Field Closure domain Prosendeev & Bellaiche (PRB 2007) PFM results indicate possible presence of non- rectilinear polarization in PZT nanodots Rodriguez et al (Nanoletters, 2009)
  • 8. ABO3 Nanowires – Our DFT Study 2x2-AO-terminated nanowire 2x2-BO2-terminated nanowire AO-plane BO2-plane AO-plane BO2-plane Construction of ABO3 nanowires
  • 9. BaTiO3 Nanowires – Our DFT Study Axial polarization instability above 1.2 nm ferroelectric paraelectric 4x4-TiO2 P 4x4-BaO τ=rxP Vortex polarization instability above 1.6 nm Geneste et. al, APL 88, 112906 (2006);
  • 10. Spanier et al, Nano Lett. 6, 735 (2006) 0.8 nm Off-axis Polarization in BaTiO3 nanowires BaTiO3 Nanowires – Experimental Study
  • 11. PbTiO3 Nanowires – Our DFT Study c (Å) Fa Fa Fa Fa P 1x1 to 4x4-PbO Fv Shimada et al, PRB 79, 024102 (2009) c tetragonal Bulk acubic Bulk P P P 4x4-TiO2 τ=rxP Unit cell decomposed dipole moments
  • 12. PbTiO3 Nanowires vs. Terminations Strain-induced phase transition: vortex  axial polarization 4x4-TiO2-terminated nanowire [001] Axial compressive Strain Axial Tensile Strain 4x4-PbO-terminated nanowire Four possible switchable polarization states Vortex (clockwise/counter-clockwise), Axial (positive/negative)
  • 13. PbTiO3 nanowires display switchable rectilinear (axial) and non-rectilinear (vortex) polarization configurations Control of polarization states axial Strain and surface terminations
  • 14. (T, p) surface phase diagrams of ABO3 systems
  • 15. Flexibility Versatility Less expensive Thermal stability Excellent oxygen exchange properties Why are they important? Perovskite Surfaces in Catalysis
  • 16. R. J. H. Voorhoeve, D. W. Johnson, Jr., J. P. Remeika, P. K. Gallagher SO4 -2 Dead site Active site Sulfur poisoning 26 MARCH 2010 VOL 327 SCIENCE Chang Hwan Kim, Gongshin Qi, Kevin Dahlberg, Wei Li Perovskite Surfaces in Catalysis
  • 18. 2 2 1 O O    Surface-O*↔ Surface + ½ O2 (g) Cubic LaMnO3 and PbTiO3 surface phase diagrams
  • 19. + N/2 O2 Cubic LaMnO3 and PbTiO3 surface phase diagrams
  • 20. (1x1) AO-terminated (1x1) BO2-terminated Formation Energies Cubic LaMnO3 and PbTiO3 surface phase diagrams A
  • 21. Relaxed geometries for most favored adsorption sites Cubic LaMnO3 and PbTiO3 surface phase diagrams
  • 22. Perovskite surfaces in contact with O2 (g)              0 0 0 2 2 2 2 ln ) , ( ) , 0 ( ) , ( p p T k p T p K T p T O B O O O    Assuming ideal gas behavior for O2 2 2 1 O O    Surface-O*↔ Surface + ½ O2 (g)
  • 23. Surface phase diagrams for surfaces in contact with O2 PbTiO3 (001) TiO2-terminated log P O2 100% O ad-atom coverage Partial O vacancy coverage Partial coverage of O ad-atom Clean surface 100% O vacancy T (K) LaMnO3 (001) MnO2-terminated 100% O vacancy Partial coverage of O ad-atom 100% O ad-atom coverage log P O2 T (K)
  • 24. Remaining Work Electric field response of the vortex polarization state in PbTiO3 nanowires Efield ? Dielectric tensor of ferroelectric nanowires 4x4-PbO terminated nanowire (axial polarization) 4x4-TiO2 terminated nanowire (vortex polarization) Effect of surface passivation (by various species such as –OH, H, -CH3 etc.) on polarization states in PbTiO3 nanowires
  • 25. Thermodynamics of environment dependent interaction of various gases on the (001) surface of ABO3 type perovskites NO, NO2, N2, O2 (gases) Adsorption site Equilibrium geometry Electronic structure Energetics Kinetics ?? Remaining Work
  • 26. Impact of Work 0 1 0 0 Non volatile Ferroelectric memory Potential to increase present memory storage density by five order of magnitude How to shrink the hard drive?!!
  • 27. Impact of Work DeNOx processes NO + CO + unburned hydrocarbons catalytic converter CO CO2 NOx N2 + O2 CnHm CO2+H2O LaCoO3 (○) La0.9Sr0.1CoO3 (●) LaMnO3 (□) La0.9Sr0.1MnO3 (■) commercial DOC (▲)
  • 28. List of Publications G. Pilania, S. P. Alpay and R. Ramprasad, "Ab initio study of ferroelectricity in BaTiO3 nanowires", Phys. Rev. B 80, 014113(1)-014113(7)- (2009). G. Pilania, D. Q. Tan, Y. Cao, V. S. Venkataramani, Q. Chen and R. Ramprasad, "Ab initio study of antiferroelectric PbZrO3 (001) surfaces", J. Mater. Sci. 44, 5249- 5255 (2009). G. Pilania, T. Sadowski and R. Ramprasad, "Oxygen adsorption on CdSe Surfaces: A case study of asymmetric anisotropic growth through Ab initio computations", J. Phys. Chem. C. 113(5), 1863-1871 (2009). J. D. Doll, G. Pilania, R. Ramprasad and F. Papadimitrakopoulos, "Oxygen- Assisted Unidirectional Growth of CdSe Nanorods Using a Low-Temperature Redox Process", Nano Lett., 10 (2), 680-685 (2010). G. Pilania and R. Ramprasad “Vortex -Polarization Instability in PbTiO3 nanowires”, under review. G. Pilania and R. Ramprasad “Thermodynamics of environment dependent oxygen adsorption and vacancy formation on cubic PbTiO3 and LaMnO3 (001) surfaces”, In preparation.
  • 29. Acknowledgments Group Members : Ning, Tang, Tom, Hong, Satyesh, Chenchen, Yenny Committee members: Profs. Rampi Ramprasad, Puxian Gao and George A. Rossetti, Jr. Profs. Rainer Hebert and Pamir S. Alpay Computational resources: IMS computation clusters; SGI supercomputer in SoE and Teragrid Funding: NSF & ONR
  • 32.
  • 34. Cubic LaMnO3 and PbTiO3 surface phase diagrams ∆γ=
  • 35. Effect of vibrational free energy (1x1)-MnO2-terminated (001) LaMnO3 surface O ad-atoms % change in ∆γ T (k) O vacancies % change in ∆γ T (k)