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Mössbauer Spectroscopy 590B S09 Sergey L. Bud’ko Novel Materials and Ground States Novel Materials and Ground States Novel Materials and Ground States Novel Materials and Ground States Sergey L. Bud’ko (Сергей Леокадьевич Будько)
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Page 1: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Mössbauer Spectroscopy

590B S09

Sergey L. Bud’ko

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

Sergey L. Bud’ko(Сергей Леокадьевич Будько)

Page 2: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

Nobel Prize in 1961 for PhD work of 1958

Page 3: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Mössbauer spectroscopy and its sensitivity

Mössbauer spectroscopy is a technique in which interactionbetween the electromagnetic moment of the nuclear charge andelectromagnetic field produced by the extra-nuclear electrons arestudied. This interaction gives splitting/shifting of the nuclearenergy levels.

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

For the most common Mössbauer isotope, 57Fe, the linewidth is

5x10-9eV. Compared to the Mössbauer gamma-ray energy of

14.4keV this gives a resolution of 1 in 1012 (or the equivalent of a

small speck of dust on the back of an elephant or one sheet of

paper in the distance between the Sun and the Earth).

Page 4: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Emission Absorption

Free emitting and absorbing atoms

Recoil

mc

E=E

2

2

R

2

γEnergy of recoil

γ-ray energy

Mass of atomafter Enver Murad, Workshop on Martian Phyllosilicates, 2008

Page 5: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Emission Absorption

Emitting and absorbing atoms fixed in a lattice

No recoil

Mc

E=E 2

2

R

2

γ

Mass of particle

Mössbauer spectroscopy is the recoil-free emission and absorption of γ-rays

(VERY LARGE)

after Enver Murad, Workshop on Martian Phyllosilicates, 2008

Page 6: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Experimentally:

Page 7: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Experimental

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

Page 8: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Experimental

Mostly in transmission mode

Source (emitted radiation: resonant γ-rays (recoil-free), non-resonant γ-rays (involving recoil), radiation from all other transitions, secondary radiation (mainly X-rays) produced in the matrix)

57Co in Rh matrix: activity: 5 mCi to 150 mCi

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

57Co in Rh matrix: activity: 5 mCi to 150 mCi

119mSn in Ca-stannate matrix: 2-25 mCi

Absorber – your sample (“usually” powder, can use single crystals, thickness is an issue)

Page 9: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Experimental

Drive system (mechanical, electromechanical, piezoelectric, hydraulic, etc.) Constant-velocity and sweep-velocity systems. Usually the source makes the motion.

Up to 300 mm/s (1000 mm/c);

Resonance frequency ~ 25 Hz

Different modes allowed

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

Different modes allowed

~25 mm/s per Volt

---------------------------------------------------

(and if you are really cheap you can try to use old speaker)

Page 10: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Experimental

Detector (scintillation detectors, proportional counters, lithium-drifted germanium or silicon detectors).

Proportional counter – Ar/Kr/Xe filled, ~ 2 kV operating voltage.

Also need a lot of electronics, cryostat/furnace, ME fitting software

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

cryostat/furnace, ME fitting software

Page 11: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

Page 12: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

Page 13: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Hyperfine Parameters

Chemical Isomer Shift (IS) (δδδδ): Arises out of the interactionbetween nuclear charge density and the surrounding ‘s’ electroncharge cloud. IS can give information about the spin state as wellas the co-ordination number.

Quadrupole Splitting (QS) (∆∆∆∆): Arises due to interaction between the

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

Quadrupole Splitting (QS) (∆∆∆∆): Arises due to interaction between the

electric quadrupole moment of the nucleus and Electric Field

Gradient created by the electrons. QS can give information about

the charge symmetry around the nucleus.

Hyperfine field (Hint) It gives the internal magnetic field of a

magnetic material

Page 14: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Isomer Shift

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

Page 15: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Quadrupolar Splitting

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

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Magnetic Hyperfine Field

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

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Magnetic Dipole + Electron Quadrupole Interactions

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

can get some idea about the magnetic moment direction

Page 18: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

“IDEAL” Mössbauer spectra - summary

Depending on the local environments of the Fe atoms and the magnetic properties, Mössbauer spectra of iron oxides can consist of a singlet, a doublet, or a sextet.

Phyllosilicates, 2008

Symmetric charge

No magnetic field

Asymmetric charge

No magnetic fieldSymmetric or asymmetric charge

Magnetic field (internal or external)

∆ Bhfδ Isom

er

shift

Quadru

pole

split

ting

Magnetic h

yperf

ine f

ield

after EnverMurad, Workshop on Martian Phyllosilicates

Page 19: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

e T

ran

sm

issio

n

Fe3+

-4 -2 0 2 4

Velocity (mm/s)

Rela

tive

δFe2+

-4 -2 0 2 4

Velocity (mm/s)

after Enver Murad, Workshop on Martian Phyllosilicates, 2008

Page 20: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Use of Mössbauer spectroscopy as a “fingerprinting” technique

3

4

[6]Fe2+

[8]Fe2+

[5]Fe3+

Isomer shifts and quadrupole splittings of Fe-bearing phases vary systematically as a function of Fe

1.0 1.5

1

-0.5 0.5

Isomer shift (mm/s)

0

2

0.0

[6]Fe(II)

[6]Fe(III)[6]Fe3+

[4]Fe3+

[4]Fe2+

[sq]Fe2+

[5]Fe3+

[5]Fe2+

as a function of Fe oxidation, Fe spin states, and Fe coordination.

Knowledge of the Mössbauer parameters can therefore be used to “fingerprint” an unknown phase.

after Enver Murad, Workshop on Martian Phyllosilicates, 2008

Page 21: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

ME applications: Fe – containing minerals on Mars

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

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Mars

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

Mars surface geology

Page 23: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Examples

Pressure-induced magnetic order

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

J.P.Sanchez et al., Hyperfine Interactions…

Page 24: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Examples

TbNi2B2C (actually, Tb(Ni0.9957Fe0.01)2B2C)

TWFM

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

TN

D. Sanchez et al, PRB

Page 25: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Examples

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

RNi2B2C

Fe replaces Ni, both are non-magnetic in these materials

No HF field on 57Fe

Possibly collinear AFM (consistent with earlier neutron data)

Page 26: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Examples

CeFeAs(O/F)

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

neutron scattering

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Examples

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

D.Sanchez et al. + Ames Laboratory

unpublished

Page 28: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Mössbauer Spectroscopy

“cheap”

“fast”

sensitive to magnetic transitions, phase purity

can give some information about the nature of the magnetic phase

local probe

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

local probe

reasonably easy to use T, P, H as variables

limited number of isotopes

interpretation somewhat model/fit dependent

NEED TO USE IN CONJUNCTION WITH OTHER MEASUREMENTS

Page 29: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

timescales associated with some spectroscopic techniques

Energy of excited state Typical relaxation Typical

Technique (Hz) time (seconds) linewidth (Hz)

NMR (solution) 108 10 10-1

ESR (solution) 1010 10-5 105

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

rotationalspectroscopy (gas) 1011 10-4 104

vibrationalspectroscopy (gas) 1014 10-8 108

electronicspectroscopy (solution) 1016 10-15 1015

Mössbauerspectroscopy (solid) 1019 10-8 108

Page 30: Sergey L. Bud’ko - Condensed Matter Physics | …cmp.physics.iastate.edu/canfield/course/EM2_35.pdfProportional counter –Ar/Kr/Xe filled, ~ 2 kV operating voltage. Also need a

Reading materials

Mössbauer Spectroscopy and its Applications, T E Cranshaw, B W Dale, G O Longworth and C E Johnson, (Cambridge Univ. Press: Cambridge) 1985

Mössbauer Spectroscopy, D P E Dickson and F J Berry, (Cambridge Univ. Press: Cambridge) 1986

The Mössbauer Effect, H Frauenfelder, (Benjamin: New York) 1962Principles of Mössbauer Spectroscopy, T C Gibb, (Chapman and Hall: London) 1977

Mössbauer Spectroscopy, N N Greenwood and T C Gibb, (Chapman and Hall:

Novel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground StatesNovel Materials and Ground States

Mössbauer Spectroscopy, N N Greenwood and T C Gibb, (Chapman and Hall: London) 1971

Chemical Applications of Mössbauer Spectroscopy, V I Goldanskii and R H Herber ed., (Academic Press Inc: London) 1968

Mössbauer Spectroscopy Applied to Inorganic Chemistry Vols. 1-3, G J Long, ed., (Plenum: New York) 1984-1989

Mössbauer Spectroscopy Applied to Magnetism and Materials Science Vol. 1, G J Long and F Grandjean, eds., (Plenum: New York) 1993


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