Intermediate Valence in Yb Compounds Probed by RIXS and 4f

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8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Intermediate Valence in Yb Compounds

Probed by RIXS and 4f Photoemission

Serguei L. Molodtsov, European XFEL & Freiberg University of Technology

1

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Cooperators

Studies were performed by:

Dresden University :

ESRF (ID16):

Spring-8 (BL25SU):

MPI CPfS Dresden:

K. Kummer (ESRF) , D. Vyalikh,

Yu. Kucherenko, S. Danzenbächer,

M. Holder, C. Laubschat

S. Huotari and L. Simonelli

T. Muro, Y. Kato and T. Kinoshita

C. Krellner and C. Geibel

2

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Correlated f-materials

Periodic table n m 2

[Xe] 4f 5d 6s

Atomic potential

3

Lanthanoide

:

S.L. Molodtsov, European XFEL & TU Freiberg f - electrons

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Correlated f-materials: YbRh

2

Si

2

4

Correlated f-Materials

Periodic table of the elements

Lanthanoide

:

S.L. Molodtsov, European XFEL & TU Freiberg f - electrons

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Correlated f-materials: Mixed-valent Ce and Yb systems

E

DOS f d e

E

F f

1 f d

DOS

E e f

0

E

F f electron promotion energy U fd may be compensated by increase of the system cohesive energy

D

U

C

5

U fd

U fd

>>

D

U

C

– stable configuration f n [f 1 for Ce; f 14 (h 0 ) for Yb]

<<

D

U

C

– stable configuration f n-1 [f 0 for Ce, f 13 (h 1 ) for Yb]

U fd

~ D

U

C

– mixed-valent system f v , (n-1) < v < n

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

From mixed-valent to Kondo behavior (Ce)

E

6

Why exact knowledge of intermediate valency is important ?

e f

2 f states

U ff

Mixed valence: e f

1 and e f

0 are almost equally possible short lifetime efficient hopping broad E

F peak

Kondo e f

0

E

F e f

1

U fd

Kondo: starting from e f

1 , probability to have e f

0 is very low hopping is rear long lifetime sharp Kondo resonance

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Intermediete valency from photoemission

SIAM calculations

Ce:

ε f

= -1.5 eV

Δ = 1.0 eV

Yb:

ε f

= -0.05 eV

Δ = 0.3 eV

U ff

= 7 eV

J.-M. Imer & E. Wuilloud,

Z. Phys. B 66 , 153 (1987).

7

GSP breaks down, since it underestimates experimental intensity at E

F

. Final-state hybridization should be included in consideration!

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Final-state hybridization is included!

SIAM calculations

Ce:

ε f

= -1.5 eV

Δ = 1.0 eV

Yb:

ε f

= -0.05 eV

Δ = 0.3 eV

U ff

= 7 eV

O. Gunnarsson &

K. Schönhammer,

PRB 31 , 4815 (1985)

8

In case final state hybridization and finite valence-band width are considered better agreement between theory and experiments can be achieved

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Intermediete valency of YbRh

2

Si

2 from photoemission

9

Divalent (2 + ) contribution into the ground state is considerably overestimated in photoemission experiments

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

RIXS at L

3 edge

10

2 p 5 4 f 14 configuration energetically preferred due to its better core-hole screening. Because of possible d

→ f electron hopping, the 2 + line thus might enter overemphasized into the spectra

Constant emission energy (CEE) and constant excited energy (CXE) spectra can be calculated

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Intermediarte valency from RIXS

CXE at excitation energy of 2 + resonance is preferable for analysis of almost 3 + system

11 with ζ = 1 for CEE scan and ζ < 1 for CXE scan

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Intermetallic rare-earth materials: YbRh

2

Si

2 12

Typical single-crystalline samples

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Intermetallic rare-earth materials: YbRh

2

Si

2

Yb

Rh

Si

13

Quasi-layered structure, cleave between Yb (blue) and Si (green) layers

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Characterization of cleaved samples: YbRh

2

Si

2

Yb

Rh

Si

14

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Characterization of cleaved samples: YbRh

2

Si

2

Surface

15

Yb

Rh

Si

Bulk

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Evaluation of photoemission spectra

16

Best fit for Δ = 0.26 eV

S.L. Molodtsov, European XFEL & TU Freiberg

Intermediate valency 2.93 for bulk is observed

(2.88 in GSP)

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Evaluation of RIXS spectra

Intensity map of the Yb Lα

1 fluorescence yield for YbRh

2

Si

2

17

CEE and CXE cuts through the 2 + resonance are indicated by white and red circles, respectively

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

CEE cut through the intensity map

XAS measured in total fluorescence yield (TFY) mode and RIXS spectra in

CEE mode of YbRh

2

Si

2

18

Spectral broadening is no longer defined by the lifetime of the deep 2p core hole

(TFY-XAS), but by the much shallower 3d core hole (CEE)

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

CXE cut through the intensity map

Emission intensity curve along the CXE cut (excitation into 2 + resonance) indicated by red circles in fig. below

19

Originally small 2 + intensity is now comparable to that of the

3 + resonance, despite the only small 2 + divalent admixture in the ground state.

But, further normalization is required!

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Absolute intensity normalization

20

ζ = 0 .

13

Information on the absolute intensity ratio between the 2 + and 3 + peaks in their respective resonance maxima can be obtained comparing CEE and CXE cuts crossing maximum of the 2 + signal in the intensity map

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Evaluation of RIXS spectra

Δ = 0.26 eV from photoemission

21

Intermediate valency: 2.93 from CEE scan and 2.92 from CEE scan

(2.89 and 2.88 in GSP)

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Summary

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Valency 2.95 is inferred from low-excitation measurements of the

Kondo temperature (20 K)

Both RIXS and photoemission approaches to determine valency fail if only initial-state properties are accounted for

(2 + contribution is overestimated)

Consideration of final-state hybridization is necessary to obtain correct valency

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

European XFEL (XFEL.EU)

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Superconducting LINAC technology provides 27.000 light pulses/s with duration down to a few fs each. It makes XFEL.EU attractive for photonhungry and time-resolved experiments.

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Heisenberg RIXS (hRIXS) @ XFEL.EU

Spokesperson

: Alexander Föhlisch, Helmholtz-

Zentrum-Berlin, Potsdam University, Germany

Consortium members

: Cooperation of representatives of 20 distinguished research institutions from

7 European countries:

Germany, Italy, Switzerland,

Sweden, the Netherlands,

Finland and France

24

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Experimental hall

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S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Soft X-ray hall (SASE3): Floor plan

42.5 m

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S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Completion of underground construction (06.06.13)

27

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Tunnels: Infrastructure installation

28

S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

European XFEL: Campus

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S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Main building: Architect ’s view

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S.L. Molodtsov, European XFEL & TU Freiberg

8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

Main building: Architect ’s view

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8 th International Conference on Inelastic X-Ray Scattering IXS-2013, May 12-15, Menlo Park

You are very welcome to plan your

IXS/RIXS

experiments at the European XFEL

32

S.L. Molodtsov, European XFEL & TU Freiberg

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