Fluorescence Yield detection XPS Ground state analysis Fluorescence

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 • Fluorescence Yield detection • XPS • Ground state analysis

• Fluorescence Yield detection • XPS • Ground state analysis

Fluorescence Yield detection • • FY (1. dilute limit) FY (2. state dependent decay)

Fluorescence Yield detection • • FY (1. dilute limit) FY (2. state dependent decay) FY (3. inverse PFY) FY (4. dips and peaks)

Fluorescence Yield detection •

Fluorescence Yield detection •

Fluorescence Yield detection •

Fluorescence Yield detection •

Fluorescence Yield detection •

Fluorescence Yield detection •

FY detection of dilute sample

FY detection of dilute sample

Fluorescence Yield FY detection of non-dilute sample “saturation & self-absorption” De-saturation software (μ(ω) based

Fluorescence Yield FY detection of non-dilute sample “saturation & self-absorption” De-saturation software (μ(ω) based on CRXO)

XAS of radiation sensitive sample Single synchrotron pulselength is too long Mitzner et al,

XAS of radiation sensitive sample Single synchrotron pulselength is too long Mitzner et al, J. Phys. Chem. Lett. 4, 3641 (2013)

FY-XAS of radiation sensitive sample Fluorescence does not measure XAS spectrum • Saturation ?

FY-XAS of radiation sensitive sample Fluorescence does not measure XAS spectrum • Saturation ? Mitzner et al, J. Phys. Chem. Lett. 4, 3641 (2013)

FY-XAS of radiation sensitive sample Fluorescence does not measure XAS spectrum • NO Saturation

FY-XAS of radiation sensitive sample Fluorescence does not measure XAS spectrum • NO Saturation • State-dependent decay Mitzner et al, J. Phys. Chem. Lett. 4, 3641 (2013)

FY detection: State dependent decay • Yield methods assume a constant ratio between radiative

FY detection: State dependent decay • Yield methods assume a constant ratio between radiative and non-radiative decay • If this ratio is state (= energy) dependent then the related yield methods do not measure XAS. • The dominant yield method is not visibly affected, thus for soft X-rays only FY is affected, not electron yield.

FY detection: State dependent decay L 3 FY EY Solid State Comm. 92, 991

FY detection: State dependent decay L 3 FY EY Solid State Comm. 92, 991 (1994) L 2

FY detection (state-dependent, dilute) • Main decay of 2 p core hole is 2

FY detection (state-dependent, dilute) • Main decay of 2 p core hole is 2 p 3 d RIXS • Integrate RIXS spectrum to 2 p 3 d PFY • TFY ~ 2 p 3 d PFY • NOTE: “RIXS” has angular dependence effects

XAS: transmission & FY Mitzner et al, J. Phys. Chem. Lett. 4, 3641 (2013)

XAS: transmission & FY Mitzner et al, J. Phys. Chem. Lett. 4, 3641 (2013)

Fluorescence Yield detection FY-XAS ≠ XAS L 2 edge increases High-energies increase Kurian J.

Fluorescence Yield detection FY-XAS ≠ XAS L 2 edge increases High-energies increase Kurian J. Phys. Cond. Matt. 24, 435602 (2012)

Fluorescence Yield XMCD • XMCD sum rules break down • Ni/Co 20%, Fe 30%,

Fluorescence Yield XMCD • XMCD sum rules break down • Ni/Co 20%, Fe 30%, Mn > 100% error Liu ea, Phys. Rev. B. 96, 054446 (2017)

FY detection: 3 inverse PFY

FY detection: 3 inverse PFY

FY detection: 3 inverse PFY Achkar ea, scientific reports 1, 82 (2011)

FY detection: 3 inverse PFY Achkar ea, scientific reports 1, 82 (2011)

FY detection: 4 dips and peaks • Measure the total fluorescence yield • State-dependent

FY detection: 4 dips and peaks • Measure the total fluorescence yield • State-dependent decay modified metal PFY • + Negative IPFY

FY detection: 4 dips and peaks 766 (2012) & Phys. Rev. Letter discussions (2014)

FY detection: 4 dips and peaks 766 (2012) & Phys. Rev. Letter discussions (2014)

XPS

XPS

X-ray absorption and X-ray XAS and XPS photoemission I( FIXED)

X-ray absorption and X-ray XAS and XPS photoemission I( FIXED)

Charge transfer XAS and XPS Charge transfer effects inin. XAS and XPS • Transition

Charge transfer XAS and XPS Charge transfer effects inin. XAS and XPS • Transition metal oxide: Ground state: 3 d 5 + 3 d 6 L • Energy of 3 d 6 L: Charge transfer energy XPS 3 d 6 L XAS 2 p 53 d 5 -Q Ground State 2 p 53 d 6 L 2 p 53 d 7 L +U-Q 2 p 53 d 6

Charge Transfer Effects XAS Charge transfer effects in in XAS +U-Q

Charge Transfer Effects XAS Charge transfer effects in in XAS +U-Q

Charge transfer effects in XAS = neutral Self screened Small charge transfer satellites

Charge transfer effects in XAS = neutral Self screened Small charge transfer satellites

Charge Transfer Effects XPS Charge transfer effects in in XPS -Q

Charge Transfer Effects XPS Charge transfer effects in in XPS -Q

Charge effectsin in XPS Chargetransfer effects XPS XAS = neutral XPS = ionising Self

Charge effectsin in XPS Chargetransfer effects XPS XAS = neutral XPS = ionising Self screened Large screening Small charge transfer satellites Large charge transfer satellites

Charge transfer effects in XPS 1 s and 2 p XPS of Fe 2

Charge transfer effects in XPS 1 s and 2 p XPS of Fe 2 O 3

Charge transfer effects in XPS 1 s and 2 p XPS of Fe 2

Charge transfer effects in XPS 1 s and 2 p XPS of Fe 2 O 3

Charge transfer effects in XPS 1 s and 2 p XPS of Fe 2

Charge transfer effects in XPS 1 s and 2 p XPS of Fe 2 O 3

Charge transfer effects in XPS 1 s and 2 p XPS of Fe 2

Charge transfer effects in XPS 1 s and 2 p XPS of Fe 2 O 3

Resonant Auger of Ni. O

Resonant Auger of Ni. O

Resonant Auger of Ni. O Phys. Rev. B. 59, 9933 (1999)

Resonant Auger of Ni. O Phys. Rev. B. 59, 9933 (1999)

Resonant Auger of Ni. O 3 d 8 → 2 p 53 d 9

Resonant Auger of Ni. O 3 d 8 → 2 p 53 d 9 → 3 s 03 d 9ε Phys. Rev. B. 59, 9933 (1999)

Resonant Auger of Ni. O 3 d 8 → 2 p 53 d 9

Resonant Auger of Ni. O 3 d 8 → 2 p 53 d 9 L→ 2 p 53 d 10 L 2 p 53 d 9 → 3 s 03 d 9ε 2 p 53 d 10 L → 3 s 03 d 10ε ONLY 2 PEAKS Phys. Rev. B. 59, 9933 (1999)

Resonant Auger of Ni. O Phys. Rev. B. 59, 9933 (1999)

Resonant Auger of Ni. O Phys. Rev. B. 59, 9933 (1999)

Resonant Auger of Ni. O Phys. Rev. B. 59, 9933 (1999)

Resonant Auger of Ni. O Phys. Rev. B. 59, 9933 (1999)

Resonant Auger of Ni. O

Resonant Auger of Ni. O

Ground state analysis

Ground state analysis

Hunds rules • Term symbols with maximum spin S are lowest in energy, •

Hunds rules • Term symbols with maximum spin S are lowest in energy, • Among these terms: Term symbols with maximum L are lowest in energy • In the presence of spin-orbit coupling, the lowest term has • J = |L-S| if the shell is less than half full • J = L+S if the shell is more than half full

Hunds rules max S > max L > max J (if more than half

Hunds rules max S > max L > max J (if more than half full) What is the Hund’s rule ground states for 3 d 2 ? 2 2 1 1 0 0 -1 -2

Hunds rules max S > max L > max J (if more than half

Hunds rules max S > max L > max J (if more than half full) What is the Hund’s rule ground states for 3 d 2 ? 2 2 1 1 0 0 L=3, S=1 J=2 Term symbol = 3 F 2 -1 -2

Hunds rules max S > max L > max J (if more than half

Hunds rules max S > max L > max J (if more than half full) What is the Hund’s rule ground states for 3 d 2 ? 2 2 1 1 0 0 -1 -2

Hunds rules What is the Hund’s rule ground states for 3 d 2 ?

Hunds rules What is the Hund’s rule ground states for 3 d 2 ?

Crystal Field Effects on 3 d 8 states Energy Symmetries Oh 1 S 4.

Crystal Field Effects on 3 d 8 states Energy Symmetries Oh 1 S 4. 6 e. V 1 A 3 P 0. 2 e. V 3 T 1 D -0. 1 e. V 3 F -1. 8 e. V 1 G 0. 8 e. V 1 E 3 A 1 A 2 1 1 + 1 T 2 + 3 T 1 + 3 T 2 1 T +1 E + 1 1 2 Total symmetry

Crystal Field Effects: Tanabe-Sugano

Crystal Field Effects: Tanabe-Sugano

Tanabe-Sugano with Charge transfer α 3 d 8 + β 3 d 9 L

Tanabe-Sugano with Charge transfer α 3 d 8 + β 3 d 9 L

CTM 4 DOC 48 [Delgado et al. J. Synchrot. Rad 23, 1264 (2016)] 48

CTM 4 DOC 48 [Delgado et al. J. Synchrot. Rad 23, 1264 (2016)] 48

CTM 4 DOC + charge transfer + translation symmetry 49 [Delgado et al. J.

CTM 4 DOC + charge transfer + translation symmetry 49 [Delgado et al. J. Synchrot. Rad 23, 1264 (2016)] 49

CTM 4 DOC 50 50

CTM 4 DOC 50 50

CTM 4 DOC 51 51

CTM 4 DOC 51 51