Metastable and glassy ionic conductors MAGIC Nancy Dudney, ORNL A. - - PowerPoint PPT Presentation

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Metastable and glassy ionic conductors MAGIC Nancy Dudney, ORNL A. - - PowerPoint PPT Presentation

Metastable and glassy ionic conductors MAGIC Nancy Dudney, ORNL A. Westover, A. Kercher, S. Kalnaus, G. Veith, M. Palmer ORNL V. Lacivita, G. Ceder LBNL W. West JPL S. Wang, W. Tenhaeff Univ. Rochester J. Christensen, B.


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SLIDE 1

Nancy Dudney, ORNL

  • A. Westover, A. Kercher, S. Kalnaus, G. Veith, M. Palmer – ORNL
  • V. Lacivita, G. Ceder – LBNL
  • W. West – JPL
  • S. Wang, W. Tenhaeff – Univ. Rochester
  • J. Christensen, B. Kozinsky, M. Kornbluth, J. Mailoa, G. Bucci – Bosch

Find a “MAGIC” glass electrolyte with

  • the stability of Lipon and
  • higher conductivity and
  • practical alternative to sputtering

Total project cost: $3.75M Length 27 mo.

Project Vision

Examine our hypothesis

Do thin-film, glassy, metastable electrolytes inhibit formation of Li filaments that limit performance of ceramic electrolytes?

Metastable and glassy ionic conductors “MAGIC”

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SLIDE 2

20µm

The Concept

  • Synthesize a conductive N-stabilized glassy electrolyte as nanopowders

Conventional sputtered film ~1µm Advanced manufacturing of membranes

Models and films to down select

nucleate gas quench

Support with polymer mesh Li3 P O4  LiSiPON “MAGIC” Si B Nx Sy also LLZO, LATP amorphous * Handle safely.

Plasma torch glassy nano powders

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SLIDE 3

The Team

2

ORNL Make it, test it! Jet Propulsion Lab Engineer one-step to a stable Li interface! LBNL What is the role of N? Bosch (Cambridge) What compositions remain glassy from melt  quench?

  • Univ. of Rochester

Polymer mesh can support thin glass. Bosch (Sunnyvale) How do dendrites form, propagate?

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SLIDE 4
  • 1. MAGIC electrolyte  efficient Li cycling, high rate, high capacity
  • 2. Plasma torch processing  stable, conductive MAGIC powders
  • 3. Mechanical properties of MAGIC  high K1C by indentation
  • 4. Hypothesis test. Will glasses be best at high current?

3 MAGIC metastable and glassy ionic conductors IONICS review 2019 Nancy Dudney June 7, 2019

2.6 2.7 2.8 2.9 3.0 3.1 3.2 3.3 3.4 3.5 10

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Ionic Conductivity (S/cm) 1000/T (K

  • 1)

Li4P2O7

Li4SiO4 Li2Si0.7P0.3O3N0.18 Li2.8Si0.7P0.3O3.2N0.22

5 full cells of 5 cm2, 0.3 mAh/cm2 1 mA/cm2, 100 cycles 30% degrade 2 MPa-m1/2, K1c 200 MPa, flex $10/m2

9th Q end 10th Q

Project Objectives

full cells thin films

10 1.0 0.1

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SLIDE 5

Results (using sputtered MAGIC thin films)

MAGIC thin films by sputtering Theory of glass structure and transport

  • Understand structure, and Li+

mobility

  • Kinetic passivation at Li

4 Insert Presentation Name June 7, 2019

What about Li shorts?

  • No shorts to 10mA/cm2
  • Li dendrites form at artificial

boundary, not through

  • Edges and grain boundaries

 non uniform current

  • New targets,

– long life, – reproducible, – lower cost

JACS 2018 140 11029; Chem Mater, 2018 30, 7077 ACS EnergyLetters, 4 (2019) 651

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SLIDE 6

Results (for Induction Plasma Torch prepared MAGIC nanopowders)

MAGIC nano-powders and membranes – limited to Si rich, need more N Theory of melt/quench of glass

Structure for 200 atoms, 3x to average Mean square displacement (D) for Li motion

  • Ortho Li3PO4 crystallizes with slow quench
  • Pyro and meta phosphate share corners,

form glasses

5 MAGIC metastable and glassy ionic conductors IONICS review 2019 Nancy Dudney e June 7, 2019

With 525-625°C anneal:

  • Partial crystallization
  • No loss of N or Li !

2.6 2.7 2.8 2.9 3.0 3.1 3.2 3.3 3.4 3.5 10-12 10-11 10-10 10-9 10-8 10-7 10-6 10-5 10-4

Ionic Conductivity (S/cm) 1000/T (K-1)

Li2Si0.7P0.3O3N0.18 cold pressed Li2.8Si0.7P0.3O3.2N0.22 cold pressed Li2.8Si0.7P0.3O3.2N0.22 hot pressed

Li2Si0.7P0.3O3N0.18 sintered

800°C 350°C

LiSiPON

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SLIDE 7

Challenges and Potential Technical Partnerships

  • Need more control of gases through induction plasma torch. (tool design Tekna or other)
  • How to consolidate glass powders so no boundaries? (glass processing Saint Gobain)
  • Both sputtering and plasma torch are expensive, but will come down

nucleate gas quench

tuned for Ar

Expense ($$ being 1-10 $/m2) Sputter thin film IPT for powder Precursors / targets $$  $ $ Process – Watt : Watt $$ $$ Yield when optimized 1090% 1585% Direct film on cathode Self-support sheet ($ TBD)  Find MAGIC composition that is ductile.

  • Watt for watt, both processes ≈ rate
  • Material loss needs to be eliminated
  • Then both viable price at scale - if

electrolyte is very thin.

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SLIDE 8

T2M

  • Final goals – by end of project

– Larger cells (with sputtered MAGIC) – Mechanical and thermal properties for full composition range

  • Beyond – Nano-powders* promising, further pre-pilot work needed

– Modified plasma torch  complete range, LiPON to LiSiON – Larger lot of powder  Li+ conductive – Explore advanced manufacturing

  • *provisional patent

7 MAGIC metastable and glassy ionic conductors IONICS review 2019 Nancy Dudney June 7, 2019

5 full cells of 5 cm2, 0.3 mAh/cm2 1 mA/cm2, 100 cycles <30% degrade 2 MPa-m1/2, K1c 200 MPa, flex $10/m2

9th Q end 10th Q

Large scale sputtering is a viable option. Powders of oxynitride glass provide alternative processing. Will a dense, sintered glass membrane effectively resist Li filaments and dendrites?

Images from ORNL brochure