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First Principles Design of Lithium
Superionic Conductors	

Shyue Ping Ong,Yifei Mo, William Davidson
Richards, Lincoln Miara, Hyo Sug Lee, Gerbrand
Ceder
Aug 12, 2014
ACS 248th National Meeting
Outline	

Introduction to Lithium Superionic Conductors
First Principles Optimization of State of the Art
Superionic conductor
• Li10GeP2S12
• Li7La3Zr2O12
Concept for High-throughput Superionic Conductor
Design
Aug 12, 2014 ACS 248th National Meeting
Current organic electrolytes have two
severe limitations	

Ethylene carbonate Dimethyl carbonate
Two key limitations
1) Flammability
2) Electrochemical windows < 4.5V
•  Limits choice of electrode and
achievable energy densities
A lithium superionic
conductor solid electrolyte
can potentially address both
issues.
NTSB report, March 7 2013
Aug 12, 2014 ACS 248th National Meeting
State-of-the-art lithium superionic conductors	

Garnet Li7La3Zr2O12 (LLZO)Thio-lisicon Li10GeP2S12 (LGPS)
N. Kamaya et al., Nat. Mater. 2011, 10,
682-686
R. Murugan, et al.,Angew. Chem., Int.
Ed. 2007, 46, 7778−81.
Aug 12, 2014 ACS 248th National Meeting
State-of-the-art lithium superionic conductors	

N. Kamaya et al., Nat. Mater. 2011, 10,
682-686
R. Murugan, et al.,Angew. Chem., Int.
Ed. 2007, 46, 7778−81.
LGPS
One of the highest Li+ cond.
of 12 mS/cm
Reported electrochemical
window of > 5V
Ge is expensive
Sulfide chemistry is air and
moisture sensitive
LLZO
Oxide chemistry is air stable
Stable against Li?
Low grain boundary
resistance
Lower Li+ cond. of ~0.1 mS/
cm
Aug 12, 2014 ACS 248th National Meeting
First principles materials property prediction	

What makes a good ionic conductor?
Stability
•  Phase stability
•  Electrochemical
stability
Diffusivity
•  High conductivity
@ 300K
Materials
•  Handling / air
sensitivity
•  Cost
Phase diagrams MD simulations
Element
substitutions
Aug 12, 2014 ACS 248th National Meeting
Ab initio
modeling of
LGPS diffusivity	

DFT molecular
dynamics simulation
Self-diffusivity
calculated from
simulated Li+ ion
motion
Y. Mo, S. P. Ong, G. Ceder, First principles study of the
Li10GeP2S12 lithium super ionic conductor material.
Chem. Mater. 2012, 24 15-17
Lithium motion in LGPS
(P/GeS4 tetrahedra frozen for clarity)
Aug 12, 2014 ACS 248th National Meeting
Excellent agreement between ab initio diffusivity
and experiments	

1 S. P. OngY. Mo,W. Richards, L. Miara, H. S. Lee, G. Ceder. Phase stability, electrochemical stability and ionic conductivity of the Li10±1MP2X12 (M
= Ge, Si, Sn,Al or P, and X = O, S or Se) family of superionic conductors. Energy & Environ. Sci., 2012. doi:10.1039/c2ee23355j
2 N. Kamaya et al.,A lithium superionic conductor. Nat. Mater. 2011, 10, 682-686
activation
energy
(meV)
conductivity
@ 300 K
(mS/cm)
computed1 210 13
experiment2 240 12
Temperature range:
600 K to 1200 K
Computed diffusivities
Aug 12, 2014 ACS 248th National Meeting
Ab initio molecular dynamics predict 3D
conduction pathway	

Y. Mo, S. P. Ong, G. Ceder, First principles study of the Li10GeP2S12 lithium super ionic conductor material. Chem. Mater. 2012,
24 15-17.
Lithium trace in MD simulation
at 900K
a!
c!
a!
b!
Important because 1D
conductors would be highly
sensitive to blocking defects!
Aug 12, 2014 ACS 248th National Meeting
Bandgap is upper bound on electrochemical
window	

DOS calculated
with HSE06
3.6 eV
This is how people have estimated
electrochemical windows in the past.
But is it relevant?
Aug 12, 2014 ACS 248th National Meeting
A thought experiment	

Anode CathodeLGPS
Li sinkLi source
High μLi Low μLi
Aug 12, 2014 ACS 248th National Meeting
Now let us imagine what it is like at the
electrode-electrolyte interface	

Anode CathodeLGPS
High μLi Low μLi
Li source Li sink
Systems open wrt Li
Aug 12, 2014 ACS 248th National Meeting
A new way of assessing electrochemical stability	

Relevant thermodynamic potential at electrode-
electrolyte interface is the Li grand potential1:
Construct phase diagrams at extrema of
corresponding to the cathode and anode:
φ = E −µLiNLi
µLi
Voltage = −(µLi −µLi
0
)
1S. P. Ong, L.Wang, B. Kang, & G. Ceder. Li-Fe-P-O2 Phase Diagram from First Principles
Calculations. Chemistry of Materials, 2008, 20(5), 1798–1807. doi:10.1021/cm702327g
Aug 12, 2014 ACS 248th National Meeting
Ge
P
GeS
GeS
2
P
4
S
3
P4
S7
S
P2
S5
P
4
S
9
LGPS is unstable against electrodes	

Li15
Ge4
Li3
P
Li2
S
Y. Mo, S. P. Ong, G. Ceder, First principles study of the Li10GeP2S12 lithium super ionic conductor
material. Chem. Mater. 2012, 24 15-17
E = 0V E = 5V
Aug 12, 2014 ACS 248th National Meeting
LGPS achieves electrochemical stability by
passivation	

Li2S + Li15Ge4 + Li3P S + GeS2 + P2S5
Anode CathodeLGPS
High μLi Low μLi
Well-known
glassy conductors!
Aug 12, 2014 ACS 248th National Meeting
Summary on Li10GeP2S12	

Kamaya et al.
(Experiments)
1D conductor
σ=12 mS/cm
Stable over 5V
First principles
calculations
3D conductor
σ=13 mS/cm
SEI formation
✗
✔
?
Aug 12, 2014 ACS 248th National Meeting
The LGPS
scooter,
but why is
it so
small?
Aug 12, 2014 ACS 248th National Meeting
Modifying Li10GeP2S12	

Two critical problems with LGPS
• Ge is expensive ($1600-1800 per kg)
• S chemistry likely reactive with H2O and air
S Se, OAnion
Ge Si, Sn,Al, PCation
Substitutions
Aug 12, 2014 ACS 248th National Meeting
Phase stability of nine Li10MP2X12 derived from
substitution	

S. P. Ong,Y. Mo,W. D. Richards, L. Miara, H. S. Lee, G. Ceder, Phase stability, electrochemical stability and ionic conductivity in the
Li10±1MP2X12 family of superionic conductors. Energy Environ. Sci. 2012, doi: 10.1039/C2EE23355J
> 90 meV, oxides
unstable!
< 25 meV, S & Se
compounds may be
entropically
stabilized
Edecomp of
Li10MP2X12
(meV/atom)
Aug 12, 2014 ACS 248th National Meeting
Chemical compatibility with electrodes	

Possibly passivating ionic conductors
S. P. Ong,Y. Mo,W. D. Richards, L. Miara, H. S. Lee, G. Ceder, Phase stability, electrochemical stability and ionic conductivity in the
Li10±1MP2X12 family of superionic conductors. Energy Environ. Sci. 2012, doi: 10.1039/C2EE23355J
O2
evolution!
Li10MP2X12
Aug 12, 2014 ACS 248th National Meeting
Anion has a large effect on diffusivity of
Li10GeP2X12 	

σ @ 300
K
(mS/Cm)
Ea
(meV)
O 0.03 360
S 13 210
Se 24 190
Causes:
•  Lattice parameter
•  Anion polarizability
Se
S
O
S. P. Ong,Y. Mo,W. D. Richards, L. Miara, H. S. Lee, G. Ceder, Phase stability, electrochemical stability and ionic conductivity in the
Li10±1MP2X12 family of superionic conductors. Energy Environ. Sci., 2012, doi: 10.1039/C2EE23355J
Aug 12, 2014 ACS 248th National Meeting
Cation has a small effect on diffusivity of Li10MP2S12 	

Isovalent Aliovalent
Ge Si Sn P Al
σ @ 300 K (mS/Cm) 13 23 6 4 33
Ea (meV) 210 200 240 260 180
(Aliovalent substitutions
are Li+ compensated)
S. P. Ong,Y. Mo,W. D. Richards, L. Miara, H. S. Lee, G. Ceder, Phase stability, electrochemical stability and ionic conductivity in the
Li10±1MP2X12 family of superionic conductors. Energy Environ. Sci., 2012, doi: 10.1039/C2EE23355J
Aug 12, 2014 ACS 248th National Meeting
Recent experiments validate first principles
predictions!	

A. Kuhn et al., 2014, arxiv:1402.4586P. Bron, JACS, 2013, 135, 15694–7.
Aug 12, 2014 ACS 248th National Meeting
Voronoi topological analysis of LGPS	

Aug 12, 2014 ACS 248th National Meeting
Using Zeo++ code (R. L. Martin,
B. Smit, M. Haranczyk,. Journal of
Chemical Information and
Modeling, 2012, 52(2), 308–18.
Y. Mo, S. P. Ong, G. Ceder,
First principles study of the
Li10GeP2S12 lithium super
ionic conductor material.
Chem. Mater. 2012, 24 15-17.
1.2
1.4
1.6
1.8
2
O O O S S S S S Se Se Se
Si Ge Sn Si Ge Sn Al P Si Ge Sn
~20%
~7%
Bottleneck size as a descriptor for diffusivity	

Li±1
Ge4+:Al3+, Si4+, Sn4+, P5+
P5+
S2-: O2-, Se2-
Substitution Scheme 1.0E-3
1.0E-1
1.0E+1
O O O S S S S S Se Se Se
Si Ge Sn Si Ge Sn Al P Si Ge Sn
Conductivity σ
(mS/cm)	
  	
  
Bottleneck size
(Å)
Aug 12, 2014 ACS 248th National Meeting
Generally, bottleneck size seems
to be a pretty good initial
screening descriptor for
diffusivity.
State-of-the-art lithium superionic conductors	

N. Kamaya et al., Nat. Mater. 2011, 10,
682-686
R. Murugan, et al.,Angew. Chem., Int.
Ed. 2007, 46, 7778−81.
LGPS
One of the highest Li+ cond.
of 12 mS/cm
Reported electrochemical
window of > 5V
Ge is expensive
Sulfide chemistry is air and
moisture sensitive
LLZO
Oxide chemistry is air stable
Stable against Li?
Low grain boundary
resistance
Lower Li+ cond. of ~0.1 mS/
cm
Aug 12, 2014 ACS 248th National Meeting
First principles optimization of garnet 
Li7+2x−y(La3−xRbx)(Zr2−yTay)O12	

0.00
0.10
0.20
0.30
0.40
0.50
6 6.5 7 7.5
Activation
Energy(eV)
1.0E-07
1.0E-05
1.0E-03
1.0E-01
σ300(S/cm)	
  
Rb DopedTa Doped
Max conductivity and min Ea at Li = 6.75
Miara, L. J.; Ong, S. P.; Mo,Y.; Richards,W. D.; Park,Y.; Lee, J.-M.; Lee, H. S.; Ceder, G. Chem. Mater., 2013, 25, 3048–3055.
Aug 12, 2014 ACS 248th National Meeting
Voronoi topological analysis of LLZO	

Aug 12, 2014 ACS 248th National Meeting
Miara, L. J.; Ong, S. P.; Mo,Y.; Richards,W. D.; Park,Y.; Lee, J.-M.; Lee, H. S.; Ceder, G. Chem. Mater., 2013, 25, 3048–3055.
Pathway to High-throughput First Principles
Design of Lithium Superionic Conductors	

Aug 12, 2014 ACS 248th National Meeting
Starting candidates
Topological Screening
(augmented by DFT)
Stability (phase 
EW) screening
Diffusivity
Optimized
candidates
Automated “one-click” MD
workflow based on pymatgen,
custodian and fireworks
AIMD SDSC
Multi-week AIMD simulation
Statistical exclusionary
screening
Y. Mo, S. P. Ong, G. Ceder,“Insights into Diffusion Mechanisms in P2
Layered Oxide Materials by First-Principles Calculations”, submitted
Automated pathway
extraction + NEB
Summary	

•  Developed sophisticated AIMD automation and workflow
infrastructure for rapid kinetic studies.
•  Developed Li-grand potential PD as a powerful new way
of studying electrode-electrolyte interfacial phase
equilibria.
Technical Advances
•  Li10SiP2S12 and Li10SnP2S12, earth-abundant variants of
LGPS, were predicted and confirmed to have similar
performance.
•  Suggested doping strategies to further enhance
conductivity of LLZO.
Materials Design
Aug 12, 2014 ACS 248th National Meeting
Acknowledgements and Publications	

Funding
Computing resources from
Y. Mo, S. P. Ong, G. Ceder, First principles study of the Li10GeP2S12 lithium super ionic
conductor material. Chem. Mater. 24 15-17 (2012)
S. P. Ong,Y. Mo,W. D. Richards, L. Miara, H. S. Lee, G. Ceder, Phase stability, electrochemical
stability and ionic conductivity in the Li10±1MP2X12 family of superionic conductors.
Energy Environ. Sci., 2012, doi: 10.1039/C2EE23355J
Miara, L. J.; Ong, S. P.; Mo,Y.; Richards,W. D.; Park,Y.; Lee, J.-M.; Lee, H. S.; Ceder, G. Effect of
Rb and Ta Doping on the Ionic Conductivity and Stability of the Garnet Li7+2 x – y (La3–
xRbx)(Zr2– yTay)O12 (0 ≤ x ≤ 0.375, 0 ≤ y ≤ 1) Superionic Conductor:A First Principles
Investigation, Chem. Mater., 2013, 25, 3048–3055, doi:10.1021/cm401232r.
Aug 12, 2014 ACS 248th National Meeting
materiaIs
virtuaLab
Thank you.	

Aug 12, 2014
ACS 248th National Meeting

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First principles design of lithium superionic conductors

  • 1. materiaIs virtuaLab First Principles Design of Lithium Superionic Conductors Shyue Ping Ong,Yifei Mo, William Davidson Richards, Lincoln Miara, Hyo Sug Lee, Gerbrand Ceder Aug 12, 2014 ACS 248th National Meeting
  • 2. Outline Introduction to Lithium Superionic Conductors First Principles Optimization of State of the Art Superionic conductor • Li10GeP2S12 • Li7La3Zr2O12 Concept for High-throughput Superionic Conductor Design Aug 12, 2014 ACS 248th National Meeting
  • 3. Current organic electrolytes have two severe limitations Ethylene carbonate Dimethyl carbonate Two key limitations 1) Flammability 2) Electrochemical windows < 4.5V •  Limits choice of electrode and achievable energy densities A lithium superionic conductor solid electrolyte can potentially address both issues. NTSB report, March 7 2013 Aug 12, 2014 ACS 248th National Meeting
  • 4. State-of-the-art lithium superionic conductors Garnet Li7La3Zr2O12 (LLZO)Thio-lisicon Li10GeP2S12 (LGPS) N. Kamaya et al., Nat. Mater. 2011, 10, 682-686 R. Murugan, et al.,Angew. Chem., Int. Ed. 2007, 46, 7778−81. Aug 12, 2014 ACS 248th National Meeting
  • 5. State-of-the-art lithium superionic conductors N. Kamaya et al., Nat. Mater. 2011, 10, 682-686 R. Murugan, et al.,Angew. Chem., Int. Ed. 2007, 46, 7778−81. LGPS One of the highest Li+ cond. of 12 mS/cm Reported electrochemical window of > 5V Ge is expensive Sulfide chemistry is air and moisture sensitive LLZO Oxide chemistry is air stable Stable against Li? Low grain boundary resistance Lower Li+ cond. of ~0.1 mS/ cm Aug 12, 2014 ACS 248th National Meeting
  • 6. First principles materials property prediction What makes a good ionic conductor? Stability •  Phase stability •  Electrochemical stability Diffusivity •  High conductivity @ 300K Materials •  Handling / air sensitivity •  Cost Phase diagrams MD simulations Element substitutions Aug 12, 2014 ACS 248th National Meeting
  • 7. Ab initio modeling of LGPS diffusivity DFT molecular dynamics simulation Self-diffusivity calculated from simulated Li+ ion motion Y. Mo, S. P. Ong, G. Ceder, First principles study of the Li10GeP2S12 lithium super ionic conductor material. Chem. Mater. 2012, 24 15-17 Lithium motion in LGPS (P/GeS4 tetrahedra frozen for clarity) Aug 12, 2014 ACS 248th National Meeting
  • 8. Excellent agreement between ab initio diffusivity and experiments 1 S. P. OngY. Mo,W. Richards, L. Miara, H. S. Lee, G. Ceder. Phase stability, electrochemical stability and ionic conductivity of the Li10±1MP2X12 (M = Ge, Si, Sn,Al or P, and X = O, S or Se) family of superionic conductors. Energy & Environ. Sci., 2012. doi:10.1039/c2ee23355j 2 N. Kamaya et al.,A lithium superionic conductor. Nat. Mater. 2011, 10, 682-686 activation energy (meV) conductivity @ 300 K (mS/cm) computed1 210 13 experiment2 240 12 Temperature range: 600 K to 1200 K Computed diffusivities Aug 12, 2014 ACS 248th National Meeting
  • 9. Ab initio molecular dynamics predict 3D conduction pathway Y. Mo, S. P. Ong, G. Ceder, First principles study of the Li10GeP2S12 lithium super ionic conductor material. Chem. Mater. 2012, 24 15-17. Lithium trace in MD simulation at 900K a! c! a! b! Important because 1D conductors would be highly sensitive to blocking defects! Aug 12, 2014 ACS 248th National Meeting
  • 10. Bandgap is upper bound on electrochemical window DOS calculated with HSE06 3.6 eV This is how people have estimated electrochemical windows in the past. But is it relevant? Aug 12, 2014 ACS 248th National Meeting
  • 11. A thought experiment Anode CathodeLGPS Li sinkLi source High μLi Low μLi Aug 12, 2014 ACS 248th National Meeting
  • 12. Now let us imagine what it is like at the electrode-electrolyte interface Anode CathodeLGPS High μLi Low μLi Li source Li sink Systems open wrt Li Aug 12, 2014 ACS 248th National Meeting
  • 13. A new way of assessing electrochemical stability Relevant thermodynamic potential at electrode- electrolyte interface is the Li grand potential1: Construct phase diagrams at extrema of corresponding to the cathode and anode: φ = E −µLiNLi µLi Voltage = −(µLi −µLi 0 ) 1S. P. Ong, L.Wang, B. Kang, & G. Ceder. Li-Fe-P-O2 Phase Diagram from First Principles Calculations. Chemistry of Materials, 2008, 20(5), 1798–1807. doi:10.1021/cm702327g Aug 12, 2014 ACS 248th National Meeting
  • 14. Ge P GeS GeS 2 P 4 S 3 P4 S7 S P2 S5 P 4 S 9 LGPS is unstable against electrodes Li15 Ge4 Li3 P Li2 S Y. Mo, S. P. Ong, G. Ceder, First principles study of the Li10GeP2S12 lithium super ionic conductor material. Chem. Mater. 2012, 24 15-17 E = 0V E = 5V Aug 12, 2014 ACS 248th National Meeting
  • 15. LGPS achieves electrochemical stability by passivation Li2S + Li15Ge4 + Li3P S + GeS2 + P2S5 Anode CathodeLGPS High μLi Low μLi Well-known glassy conductors! Aug 12, 2014 ACS 248th National Meeting
  • 16. Summary on Li10GeP2S12 Kamaya et al. (Experiments) 1D conductor σ=12 mS/cm Stable over 5V First principles calculations 3D conductor σ=13 mS/cm SEI formation ✗ ✔ ? Aug 12, 2014 ACS 248th National Meeting
  • 17. The LGPS scooter, but why is it so small? Aug 12, 2014 ACS 248th National Meeting
  • 18. Modifying Li10GeP2S12 Two critical problems with LGPS • Ge is expensive ($1600-1800 per kg) • S chemistry likely reactive with H2O and air S Se, OAnion Ge Si, Sn,Al, PCation Substitutions Aug 12, 2014 ACS 248th National Meeting
  • 19. Phase stability of nine Li10MP2X12 derived from substitution S. P. Ong,Y. Mo,W. D. Richards, L. Miara, H. S. Lee, G. Ceder, Phase stability, electrochemical stability and ionic conductivity in the Li10±1MP2X12 family of superionic conductors. Energy Environ. Sci. 2012, doi: 10.1039/C2EE23355J > 90 meV, oxides unstable! < 25 meV, S & Se compounds may be entropically stabilized Edecomp of Li10MP2X12 (meV/atom) Aug 12, 2014 ACS 248th National Meeting
  • 20. Chemical compatibility with electrodes Possibly passivating ionic conductors S. P. Ong,Y. Mo,W. D. Richards, L. Miara, H. S. Lee, G. Ceder, Phase stability, electrochemical stability and ionic conductivity in the Li10±1MP2X12 family of superionic conductors. Energy Environ. Sci. 2012, doi: 10.1039/C2EE23355J O2 evolution! Li10MP2X12 Aug 12, 2014 ACS 248th National Meeting
  • 21. Anion has a large effect on diffusivity of Li10GeP2X12 σ @ 300 K (mS/Cm) Ea (meV) O 0.03 360 S 13 210 Se 24 190 Causes: •  Lattice parameter •  Anion polarizability Se S O S. P. Ong,Y. Mo,W. D. Richards, L. Miara, H. S. Lee, G. Ceder, Phase stability, electrochemical stability and ionic conductivity in the Li10±1MP2X12 family of superionic conductors. Energy Environ. Sci., 2012, doi: 10.1039/C2EE23355J Aug 12, 2014 ACS 248th National Meeting
  • 22. Cation has a small effect on diffusivity of Li10MP2S12 Isovalent Aliovalent Ge Si Sn P Al σ @ 300 K (mS/Cm) 13 23 6 4 33 Ea (meV) 210 200 240 260 180 (Aliovalent substitutions are Li+ compensated) S. P. Ong,Y. Mo,W. D. Richards, L. Miara, H. S. Lee, G. Ceder, Phase stability, electrochemical stability and ionic conductivity in the Li10±1MP2X12 family of superionic conductors. Energy Environ. Sci., 2012, doi: 10.1039/C2EE23355J Aug 12, 2014 ACS 248th National Meeting
  • 23. Recent experiments validate first principles predictions! A. Kuhn et al., 2014, arxiv:1402.4586P. Bron, JACS, 2013, 135, 15694–7. Aug 12, 2014 ACS 248th National Meeting
  • 24. Voronoi topological analysis of LGPS Aug 12, 2014 ACS 248th National Meeting Using Zeo++ code (R. L. Martin, B. Smit, M. Haranczyk,. Journal of Chemical Information and Modeling, 2012, 52(2), 308–18. Y. Mo, S. P. Ong, G. Ceder, First principles study of the Li10GeP2S12 lithium super ionic conductor material. Chem. Mater. 2012, 24 15-17.
  • 25. 1.2 1.4 1.6 1.8 2 O O O S S S S S Se Se Se Si Ge Sn Si Ge Sn Al P Si Ge Sn ~20% ~7% Bottleneck size as a descriptor for diffusivity Li±1 Ge4+:Al3+, Si4+, Sn4+, P5+ P5+ S2-: O2-, Se2- Substitution Scheme 1.0E-3 1.0E-1 1.0E+1 O O O S S S S S Se Se Se Si Ge Sn Si Ge Sn Al P Si Ge Sn Conductivity σ (mS/cm)     Bottleneck size (Å) Aug 12, 2014 ACS 248th National Meeting Generally, bottleneck size seems to be a pretty good initial screening descriptor for diffusivity.
  • 26. State-of-the-art lithium superionic conductors N. Kamaya et al., Nat. Mater. 2011, 10, 682-686 R. Murugan, et al.,Angew. Chem., Int. Ed. 2007, 46, 7778−81. LGPS One of the highest Li+ cond. of 12 mS/cm Reported electrochemical window of > 5V Ge is expensive Sulfide chemistry is air and moisture sensitive LLZO Oxide chemistry is air stable Stable against Li? Low grain boundary resistance Lower Li+ cond. of ~0.1 mS/ cm Aug 12, 2014 ACS 248th National Meeting
  • 27. First principles optimization of garnet Li7+2x−y(La3−xRbx)(Zr2−yTay)O12 0.00 0.10 0.20 0.30 0.40 0.50 6 6.5 7 7.5 Activation Energy(eV) 1.0E-07 1.0E-05 1.0E-03 1.0E-01 σ300(S/cm)   Rb DopedTa Doped Max conductivity and min Ea at Li = 6.75 Miara, L. J.; Ong, S. P.; Mo,Y.; Richards,W. D.; Park,Y.; Lee, J.-M.; Lee, H. S.; Ceder, G. Chem. Mater., 2013, 25, 3048–3055. Aug 12, 2014 ACS 248th National Meeting
  • 28. Voronoi topological analysis of LLZO Aug 12, 2014 ACS 248th National Meeting Miara, L. J.; Ong, S. P.; Mo,Y.; Richards,W. D.; Park,Y.; Lee, J.-M.; Lee, H. S.; Ceder, G. Chem. Mater., 2013, 25, 3048–3055.
  • 29. Pathway to High-throughput First Principles Design of Lithium Superionic Conductors Aug 12, 2014 ACS 248th National Meeting Starting candidates Topological Screening (augmented by DFT) Stability (phase EW) screening Diffusivity Optimized candidates Automated “one-click” MD workflow based on pymatgen, custodian and fireworks AIMD SDSC Multi-week AIMD simulation Statistical exclusionary screening Y. Mo, S. P. Ong, G. Ceder,“Insights into Diffusion Mechanisms in P2 Layered Oxide Materials by First-Principles Calculations”, submitted Automated pathway extraction + NEB
  • 30. Summary •  Developed sophisticated AIMD automation and workflow infrastructure for rapid kinetic studies. •  Developed Li-grand potential PD as a powerful new way of studying electrode-electrolyte interfacial phase equilibria. Technical Advances •  Li10SiP2S12 and Li10SnP2S12, earth-abundant variants of LGPS, were predicted and confirmed to have similar performance. •  Suggested doping strategies to further enhance conductivity of LLZO. Materials Design Aug 12, 2014 ACS 248th National Meeting
  • 31. Acknowledgements and Publications Funding Computing resources from Y. Mo, S. P. Ong, G. Ceder, First principles study of the Li10GeP2S12 lithium super ionic conductor material. Chem. Mater. 24 15-17 (2012) S. P. Ong,Y. Mo,W. D. Richards, L. Miara, H. S. Lee, G. Ceder, Phase stability, electrochemical stability and ionic conductivity in the Li10±1MP2X12 family of superionic conductors. Energy Environ. Sci., 2012, doi: 10.1039/C2EE23355J Miara, L. J.; Ong, S. P.; Mo,Y.; Richards,W. D.; Park,Y.; Lee, J.-M.; Lee, H. S.; Ceder, G. Effect of Rb and Ta Doping on the Ionic Conductivity and Stability of the Garnet Li7+2 x – y (La3– xRbx)(Zr2– yTay)O12 (0 ≤ x ≤ 0.375, 0 ≤ y ≤ 1) Superionic Conductor:A First Principles Investigation, Chem. Mater., 2013, 25, 3048–3055, doi:10.1021/cm401232r. Aug 12, 2014 ACS 248th National Meeting
  • 32. materiaIs virtuaLab Thank you. Aug 12, 2014 ACS 248th National Meeting