Mossbauer spectroscopy

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Mossbauer Spectroscopy B. S. VINEETH (Roll# 120121007), B.Tech., IIT Guwahati

Transcript of Mossbauer spectroscopy

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Mossbauer SpectroscopyB. S. VINEETH (Roll# 120121007), B.Tech., IIT Guwahati

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Introduction

• Versatile technique based on Mossbauer Effect that is widely used, even now, from the time it was discovered in 1957, in many areas:

• Physics, Chemistry, Biology, Archaeology,

Geology, Material Science, Metallurgy, …

• Rudolf L. Mossbauer

• NOBEL PRIZE Physics 1961 within 5 years

of its discovery!!

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Nobel Prize, Physics (1961)

• Zeitschrift fur Physik 151, Issue 2 p. 124-143 (1958)

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What is it good for?

• You name it!

• Very precise information on the: chemical, structural, magneticproperties of a material.

• Technique at the interface of Solid State Physics and Nuclear Physics.

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Basic Principle

• Nuclear Energy Levels change (shift or split) because of interaction of the radioactive nucleus with the surrounding solidin which it is embedded.

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Exclusively used by NASA• Mossbauer spectroscopy is used by NASA to study the composition, abundance, magnetic properties of iron-bearing materials in the outer space.

• MARS EXPLORATION ROVERS:

• It is ONE of FOUR facilities mounted

at the end of the ROVER ARM!

Measurements are taken by placing the Rover Arm head directly against a rock or soil sample.

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Used Elements

• Most used: Fe-57

Every Iron containing material has approx. 98% of Fe-56 and 2% of Fe-57.

• I-129, Sn-119, Sb-121 also are used.

• Let us take the example of Fe-57 to demonstrate the concept

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Isolated Fe-57 Nucleus

We expect the Gamma-ray emitted to be of 14.4 keV. (We are only interested till the

first excited state.)

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Fe-57 in ferromagnetic surrounding

• Gamma rays of nearly 14.4 keV but

with differences in the order of

10-8 eV due to splitting+shifting.

Mossbauer spectroscopy exploits this

faint spectrum in the Gamma radiation

to assess the material environment.

Cubic Structure and Ferromagnetic

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Fe 57 in stainless steel solid

• Cubic, No ferromagnetism here

• So, no splitting of levels

• But, due to the interaction of nucleus with the electron density (mainly s-electrons density), the energy levels only SHIFT in the order of 10-8 eV.

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Fe-57 in Olivine solid (FeSiO4)

• Non-cubic crystal arrangement

• Non-ferromagnetic

• Ground level: As it is (no splitting)

• First excited state: mI = -3/2, +3/2 only

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Construction

Source: Co-57 in Rhodium

Rh solid which is cubic and

non-ferromagnetic

So, only shifting of levels in

source.

Absorber: Is the sample to be

analyzed.

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Setup Block Diagram

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Working Theory and Physics

• As the Source is vibrating, the

absorber sees the Gamma rays

with a DOPPLER SHIFT.

So, if Es = E2 – E1, the absorber

sees it as:

E = Es (1 + v/c) (Doppler Shift)

(v lies from –vmax to +vmax)

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Absorber: Simple Case

• Assume, the absorber is

cubic and non-ferromagnetic.

Then for Resonance, we need:

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“Mossbauer Spectrum”

• So, at these particular velocities,

the detector takes a Dip as most

of the Gamma rays get absorbed

and don’t pass through.

Plot velocities versus detector count: “Spectrum”

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If absorber has Olivine type surrounding

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If absorber has ferromagnetic surr.

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Spectrum if ferromagnetic absorber

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A Serious Problem!!!

• Apart from the around 10-8 eV energy shift due to surrounding environment, there is an additional extremely significant (1,00,000 times) correction of around 1 milli-eV which is due to:

• NUCLEAR RECOIL EFFECT

Therefore, energy of emitted

Gamma ray becomes:

(E2 – E1) – ER

Nucleus recoils in the opposite

Direction while emission

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• Similarly, when the absorber nucleus absorbs it, it recoils in the direction of Gamma-ray and therefore for resonance to take place (without Doppler effect) the energy required is:

• (E’2 – E’1) + ER

• Unfortunately, to cover this gap due to recoil, one needs vibrating the source with huge velocities. Then, how can we do Mossbauer spectroscopy??

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Mossbauer Effect to our rescue

• It is a QM-cal phenomena that if you have a Nucleus with energy levels embedded in a Crystal Solid which itself has Crystal Energy levels, both of them couple and so:

• The Crystal has to Recoil whenever the Nucleus absorbs or emits the Gamma rays.

• But, if the Crystal Recoil Energy is less than the first-excited energy of the Nucleus, then the whole Recoil process will NOT occur, and the Gamma rays are emitted with exact energy level difference!!!

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Interpreting Results:

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Limitations

• The material to be analyzed must be composed of Iron or similar materials used in Mossbauer

• Vast majority of rock-forming minerals on Earth contain Fe 2+ in octahedral structure, and all of them have very similar Mossbauer Spectrum. (hard to distinguish)

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References

• [1] R.L. Mossbauer, Zeitschrift fur Physik 151, Issue 2 p. 124-143

• [2] H.C. Verma, Concepts of Physics, Bharati Bhawan (1999)

• [3] E.N. Kaufmann, Characterization of Materials, Wiley (2003)

• [4] Obvious online sources (Wikipedia, etc.)

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Thank You

Term paper submitted to Prof. Giri (Physics, IITG) by

B.S.VINEETH (Roll# 120121007).