A soft X-ray spectroscopic (RIXS) journey into the ... · Kehua Dai Shawn Sallis Qinghao Li...

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A soft X-ray spectroscopic (RIXS) journey into the critical electron states in batteries Wanli Yang Lawrence Berkeley National Laboratory

Transcript of A soft X-ray spectroscopic (RIXS) journey into the ... · Kehua Dai Shawn Sallis Qinghao Li...

Page 1: A soft X-ray spectroscopic (RIXS) journey into the ... · Kehua Dai Shawn Sallis Qinghao Li Zengqing Zhuo Jinpeng Wu Yi-de Chuang Zahid Hussain A LONG List of Materials Collaborators:

A soft X-ray spectroscopic (RIXS) journey into the critical electron states in batteries

Wanli YangLawrence Berkeley National Laboratory

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Tinkering with Batteries: a multidimensional Problem!

Image Source: US DOE

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e.g., “Co-free” electrode? – Sorry, NO good solution

(Only cathodes shown here) Li et al., Chem. Soc. Rev. 46, 3006 (2017)

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What kind of information matters for (practical) battery materials?

o Redox reactions in BULK electrodeso Chemical activities on SURFACE / interfaceo Solvation shells in LIDUID (electrolyte)

Charging Anode: xLi+ + C6 + e- LixC6

Charging Cathode: Li1-xCoO2 xLi+ + CoO2 + e-

• Transportation of Li+

• Reduction/Oxidation ( Redox )

ChargedDischarged

Oxygen? Co? Surface?

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Na0.44+xMnO2: Mn states upon cycling and surface Mn2+ evolution

Qiao et al., Nano Energy 16, 186 (2015)

A known “NO”!

”good” range!

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A rational approach to improve Na0.44+xMnO2 cyclability!

3-4V

2-4V

Qiao et al., Nano Energy 16, 186 (2015)

Improved Cycling Stability from Multiple effects (shallow cycling)!- However, one of the keys is the suppression of surface Mn2+ evolution

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What kind of information matters for (practical) battery materials?

o Redox reactions in BULK electrodeso Chemical activities on SURFACE / interfaceo Solvation shells in LIDUID (electrolyte)

Charging Anode: xLi+ + C6 + e- LixC6

Charging Cathode: Li1-xCoO2 xLi+ + CoO2 + e-

• Transportation of Li+

• Reduction/Oxidation ( Redox )

ChargedDischarged

Oxygen? Co? Surface?

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Two problems of “bulk-sensitive” XAS of oxide electrodes

• Distortions of TM-L in photon-in-photon-out modes !• Lack of chemical sensitivity for O-K !!

Wadati et al., APL 100, 193906 (2012)• Material dependent• Element dependent• “self-absorption correct” -N/A

• Strong 3d character in O-K “pre-edge”• Chemical sensitivity lost due to the

overlapping energy range

Ruimin Qiao et al., unpublished

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Seemingly problem solved: full energy-range mapping of RIXS (mRIXS)

3:1 BIN

Inelastic (lower-energy) Scattering

O-K (XES) iPFY

O-K (XES)

Yang & Devereaux, J. Power Sources 389, 188 (2018)

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The real challenge !

Detection efficiency is NOT a speed/quality issue; it is a FEASIBILITYissue for chemistry and material sciences!

Qiao, Chuang, et al, Plos ONE 7, e49182 (2012)

Lebens-Higgins et al., JPCC 123, 13201 (2019)

LiAlO2 (O-K XAS)

Li(NiMnCo)O2 (RIXS@531 eV)

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A dilemma of resolution vs efficiency for Energy materials

Of course, the true reason is: poor & out of real-estate!

Qiao, et al., RSI 80, 063102 (2017)Chuang, et al., RSI 88, 013110 (2017)

• Grating Ruling Density - Low• Aberration Control - Moderate• Beam focusing - Relaxed• Detector Energy Window - Huge• Angles, etc… …

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2016: full-energy range ultra-high efficiency mRIXS

Qiao et al., RSI 88, 033106 (2017)

LiNi1/3Mn1/3Co1/3O2

Ni 3

d-2p

Ni 3

s-2p

Co 3

d-2p

Co 3

s-2p

Mn

3d-2

p

Mn

3s-2

p

O-K

(2p-

1s)

Li(Ni1/3Mn1/3Co1/3)O2

A 10-second spectrum of a (discharged) NMC electrode

• An ultimate TM 3d probe: mRIXS-iPFY of all TM-L edges

• An alternative: mRIXS 3s-2p decay channels

Time: ~30 minutes for mRIXS-iPFY

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Na2/3Mg1/3Mn2/3O2 : Complex states of evolving Mn & O

• Stoichiometry adjusted to drive (pure) high-valence Mn4+!• Capacity reaches record high with “inactive” Mn?!• Change of Oxygen states is expected to be strong?

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mRIXS-iPFY & TEY Mn-L: bulk and surface Mn redox quantification

iPFY (bulk)

TEY (surface)

TFY

PFYMn-L

Mn-L Excitation energy (eV)

Mn-

Led

ge in

tens

ity (A

rb. U

nit)

O-K

& M

n-L

RIX

SEm

issi

onen

ergy

(eV)

Dai et al., Joule 3, 518 (2019)

Quantify the Mn states on surface (10nm) and in bulk (150 nm)

Quantitative probes of both the surface and bulk oxidation states of TMs

Absolute quantification of the cycling capacity from Mn redox reactions

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Mn-L mRIXS reveals Mn1+: a 90-year speculation!

Firouzi, Qiao et al., Nat Comm 9, 861 (2018)- Dr. Maxon’s congressional testimony for U.S. National Labs (2018)

(- Theory: Prof. Andrew Wray at NYU)

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Fingerprint non-divalent oxygen states through mRIXS

σu*𝝅𝝅𝒈𝒈∗

πuσg

Excitonse-

Zhuo, Pemmaraju et al., JPCL 9, 6378 (2018)

Li2O2 experiment Theory

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mRIXS: a reliable probe of unusual bulk Oxygen states

• TM-O hybridization is dissociated from oxygen redox reactions• A full energy range mRIXS is necessary (signals buried in XAS)• Theoretical calculations in process …

Yang & Devereaux, J Power Sources 389, 188 (2018)

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mRIXS fingerprints the evolving oxygen state upon battery cycling

Excitation energy (eV)

Emis

sion

ene

rgy

(eV)

Charge

Discharge

0 20 40 60 80 100 120 140 160 180

2.0

2.5

3.0

3.5

4.0

4.5

D-140D-100Pot

entia

l vs

Na/

Na+ (

V)

Specific capacity (mAh g-1)

C-8 C-70

D-50Pristine

1Ch

1D

0.1 C

(b)

(a)

• O-K mRIXS feature follows tightly with electrochemical cycling!• O-K mRIXS feature fingerprints the oxygen redox quantitatively!

Na2/3Mg1/3Mn2/3O2

Dai et al., Joule 3, 518 (2019)

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Na2/3Mg1/3Mn2/3O2: Independent probe of Mn/O states in battery

Dai et al., Joule 3, 518 (2019)

mRIXS quantifications precisely match the electrochemical capacity/profile!

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Quantify the reversibility of Oxygen redox through mRIXS

A strong O.R. system could also be highly reversible! Assessment of the reversibility of Oxygen redox

reactions upon extended cycles!NOTE: NOT all systems show such a perfect match between mRIXS quantification and electrochemistry

Dai et al., Joule 3, 518 (2019)

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“After the discovery of “antimatter” and “dark Matter”, we have just confirmed the existence of “doesn’t matter”, which does not have any influence whatsoever!”

- the 5th wave

Always #1 question: what matters for batteries?

Conclusions• High-efficiency mRIXS is truly needed and provides unique information on battery

material performance, especially the novel chemical states of TMs & O.• Instrumentational and especially theoretical developments are still needed.• Improvements on detection efficiency has opened RIXS technique as almost the

only “tool-of-choice” for a wide range of topics in energy materials!

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AcknowledgementsALS staff: Ruimin Qiao Kehua Dai Shawn Sallis Qinghao Li Zengqing Zhuo Jinpeng Wu

Yi-de Chuang Zahid Hussain

A LONG List of Materials Collaborators: Gao Liu (LBNL) Ning Li, Wei Tong (LBNL) Yuhao Lu (previously, Sharp USA) & many many others …

Theory : Andrew Wray (NYU) Tom Devereaux (Stanford)

Industry: Colin D. Wessells (Natron Energy)

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BACKUP SLIDES

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Quantitative analysis of various TM-redox in battery cathodes

0 20 40 60 80 100 120

2.0

2.5

3.0

3.5

4.0

Pote

ntia

l (V

vs. N

a+ /Na)

Specific Capacity/mAh g-1

1st cycle 2nd cycle Po

tent

ial (

V vs

Li+ /

Li)

State of Charge (%)

Mn-

L3sX

AS In

tens

ity (A

rb. U

nit)

Fe-L

3sX

AS In

tens

ity (A

rb. U

nit)

Ni-L

3sX

AS In

tens

ity (A

rb. U

nit)

NaxMnO2LixFePO4 LixNi0.5Mn1.5O4

(Review) QH Li et al., J. Phys. D 49, 413003 (2016)Nano Energy 16, 186 (2015) JACS 134, 13708 (2012) JPCC 119, 27228 (2015)

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5 different XAS channels through full mRIXS

Yang & Devereaux, J Power Sources 389, 188 (2018)