Mössbauer spectroscopy

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Mössbauer spectroscopy

References:

J.P. Adloff, R. Guillaumont: Fundamentals of

Radiochemistry, CRC Press, Boca Raton, 1993

Mössbauer effect: recoil free nuclear resonance absorption of g radiation

1,2

Recoil

Recoil

Recoil

EMISSION

E

2

E

1

E photon=(E

2

-E

1

)-R

E photon

E

ABSORPTION

E photon

E

1

E photon=(E2-E1)+R

0

-4 1

Energy

Line width (W) results from: natural width of E

2 level + Doppler widening due to temp.

W ~10 -6 eV (natural width) + 10 -3 eV (temp. effect) → 10 -3 eV (overall effect)

R~100 eV in nuclear processes, R’~10 -7 eV in optical processes

Realization of nuclear resonance:

Source and absorber contain the same element

(same nuclear energy levels).

Reduction of R by embedding the isotope in a solid crystal matrix, cooling the sample (reduced oscillation of the atoms, reduced R ↔reduced W).

The missing part of „2R” energy can be provided by moving the source due to Doppler effect

5/2- 137 keV

9% 91%

57

Co

10

-9

sec

271 days resonance absorption

3/2 14,4 keV 10

-7

sec

1/2- ground

57

Fe emitter

57

Fe absorber

Mössbauer spectrometer:

Source or absorber is moved. (Emission and absorption spectroscopy, respectively.)

Source or absorber should be in ground state, non-magnetic, symmetric environment precluding hyperfine splitting of nuclear level.

S g v

A D

S source emitting weak g radiation

A absorber moving with velocity v (mm/s)

D g radiation detector

The linear motion represents about 10 -8 eV.

The resulting Es energy is derived from the E g source energy:

Es= E g

(1

±v/c)

-10

The Mössbauer spectrum

Resonance absorption spectrum : g radiation intensity vs. velocity

(Energy)

0

0

10

Typical Mössbauer emission spectrum as the superposition of 2 single lines according to magnetic splitting of the nuclear levels in magnetic field:

237

Np

5/2-

5/2+ chemical shift

-1,2 velocíty (mm/s); energy (10 -7

eV)

-10

1,2

Typical Mössbauer emission spectrum as the superposition of 5 single lines according to quadrupole splitting of the nuclear levels in electric field:

237

Np

5/2-

5/2+

0

0

10 20

-1,2 velocíty (mm/s); energy (10-7 eV)

30

Chemical information in Mössbauer spectra

Spectra reveal splittings of nuclear levels, determined by the electronic environment.

• Isomer shift: position of the centroid of the line, oxidation state, covalency of the bondings

• Quadrupole splitting: multiplets asymetry in the electronic environment, chemical spin state, intensity of ligand field

• Magnetic splitting: multiplet due to magnetic field

Mössbauer active atoms

• 75 transitions in isotopes of 44 elements

• Radionuclide: MBq activity alpha, beta, EC or IT

T1/2: hours-hundreds of years

• Conditions to be fulfilled:

- E g

<100 keV,

- emitter should be bound in a lattice

- mean life-time of excited level: 1 ns-100 ns

- solid, cooled absorber (liquid N

2

), m>100mg

E.g.: 57 Co(EC) 57 Fe: 14,4 keV

241 Am(alpha) 237 Np: 60 keV

Tc, Th, Pa, U, Np, Pu, Am

Application examples

• Analysis of steels: oxidation state of iron (+2 or +3) chemical form (oxide, sulfate…) magnetic properties

• Analysis of iron oxide layers magnetite, hematite

• Recoil processes in condensed material

• Oxidation states of Np, Am compounds

Other nuclear related methods providing information on chemical environment

• Positron annihilation spectrometry

• Muon spectrometry

• Nuclear magnetic resonance

• Electron spectroscopies: photoelectron spectroscopy conversion electron spectroscopy

Auger electron spectroscopy

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