x-ray emission spectroscopy

12
X-ray Emission Spectroscopy Cormac McGuinness [email protected] Physics Department Trinity College Dublin Soft x-ray emission and resonant inelastic x-ray scattering of transition metal doped semiconductors

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Cormac McGuinness [email protected] Physics Department Trinity College Dublin. X-ray Emission Spectroscopy. Soft x-ray emission and resonant inelastic x-ray scattering of transition metal doped semiconductors. Project Summary. - PowerPoint PPT Presentation

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Page 1: X-ray Emission Spectroscopy

X-ray Emission Spectroscopy

Cormac [email protected]

Physics DepartmentTrinity College Dublin

•Soft x-ray emission and resonant inelastic x-ray scattering of transition metal doped semiconductors

Page 2: X-ray Emission Spectroscopy

Project SummaryProject Summary

• Study of electronic structure of transition metal-doped wide bandgap semiconductor oxide systems – i.e. magnetic semiconductors such as Co-ZnO and Co-SnO2

• Experimental & Theoretical

• Measurements: (approximately 4-5 weeks beamtime per year)– SXE / XAS at:

• O K (1s) edge –> O 2p states

• Co L2,3 (2p) edge -> Co 3d, 4s states

– RIXS measurements at:• O K (1s) edge –> O 2p -> Co 3d excitations

• Co L2,3 (2p) edge -> Co 3d->3d excitations & Co 3d-> O 2p excitations

– SXE/XMCD measurements• Measure element specific spin and orbital moments

• Theoretical:– Modelling of metal 2p RIXS spectra using appropriate multiplet structure codes

• Instrumentation:– Development of instrumentation for SXEXMCD measurements

Page 3: X-ray Emission Spectroscopy

Core Level Spectroscopy

Unoccupied states

Occupied states

Fermi level

Core level

Laser spectroscopy

Excitations ofvalence electrons

Page 4: X-ray Emission Spectroscopy

kinB EhE

Photoelectron Spectroscopy

Page 5: X-ray Emission Spectroscopy

X-ray Absorption Spectroscopy

1lDipole selection rule

ps 21

CrO2:

524 526 528 530 532 534 536 538 540 542 544 546

CrO2 O K SXA

Inte

nsity

Energy (eV)

E || a E || c

Page 6: X-ray Emission Spectroscopy

X-ray Emission Spectroscopy

1lDipole selection rule

sp 12

CrO2:

-12 -10 -8 -6 -4 -2 0 2 4 6

O 2py-x

O 2py+x

+ O 2pz

Energy with respect to EF (eV)

DO

S

515 520 525 530 535

Inte

nsity

Emission energy (eV)

SXE E || a SXE E || c

Page 7: X-ray Emission Spectroscopy

CaCu3Ti4O12: Ti 2p spectra

456 458 460 462 464 466 468

En erg y (eV)

-20 -15 -10 -5 0

-20 -15 -10 -5 0

DCB

A

Energy Loss (eV)

435 440 445 450 455 460 465 470 475 480

435 440 445 450 455 460 465 470 475 480

Energ y (eV)

Ti LTi L

Cu L

Cu L

Resonant Inelastic X-ray Scattering

Radiant resonant processes

Page 8: X-ray Emission Spectroscopy
Page 9: X-ray Emission Spectroscopy

1.0

0.8

0.6

0.4

0.2In

tens

ity

(Arb

itra

ry U

nits

360

0 se

cond

s)

820800780760740720700680660640620

Emission Energy (eV)

Fe L3MValenceEmission

Fe L2MValenceEmission

Soft X-ray spectrometer system

Page 10: X-ray Emission Spectroscopy

Project Summary

• Study of electronic structure of transition metal-doped wide bandgap semiconductor oxide systems – i.e. magnetic semiconductors such as Co-ZnO and Co-SnO2

• Experimental & Theoretical

• Measurements: (approximately 4-5 weeks beamtime per year)– SXE / XAS at:

• O K (1s) edge –> O 2p states

• Co L2,3 (2p) edge -> Co 3d, 4s states

– RIXS measurements at:• O K (1s) edge –> O 2p -> Co 3d excitations

• Co L2,3 (2p) edge -> Co 3d->3d excitations & Co 3d-> O 2p excitations

– SXE/XMCD measurements• Measure element specific spin and orbital moments

• Theoretical:– Modelling of metal 2p RIXS spectra using appropriate multiplet structure codes

• Instrumentation:– Development of instrumentation for SXEXMCD measurements

Page 11: X-ray Emission Spectroscopy

X-ray Emission Spectroscopy

Cormac [email protected]

Physics DepartmentTrinity College Dublin

•Soft x-ray emission and resonant inelastic x-ray scattering of transition metal doped semiconductors

Page 12: X-ray Emission Spectroscopy

Copper Phthalocyanine

Emission from the same excited atom (elemental probe)Dipole selection rules:l = ±1; s = 0; j = ±1, 0; mj = ±1, 0(individual angular momentum resolved states)

•Direct comparison with angular momentum resolved DOS calculations•Determine variations in the occupied states of similar materials

•Localized probe •Photon in/Photon out spectroscopy

•Photon energies ~ 300-900 eV