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This article explores resonant photon absorption and the Mossbauer effect, focusing on atomic interactions and the underlying mechanisms of photon attenuation. We delve into the properties of the source and absorber, examining how they affect resonant absorption in nuclear transitions, including kinematic effects and Doppler shifts. The discussion covers the significance of 57Fe isotopes, their nuclear states, and the implications of the nuclear Zeeman effect. Detailed analysis will also be given to the Pound-Rebka experiment, emphasizing its role in demonstrating Mossbauer resonant absorption. ###
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Resonant photon absorption The Mossbauer effect
Source Detector x Absorber Atomic interactions Photon attenuation Radiation attenuation by:-- photoelectric effect-- compton scattering (E << 1.02 MeV)
Source Detector x Absorber E* E* 0.0 0.0 Photon attenuation Consider nuclear resonant absorption Assumesourceandabsorberare identical
emission absorption Source Detector x Absorber for resonant absorption E* E* 0.0 0.0 Kinematics Assumesourceandabsorberare identical
Ignore energy scale Source Absorber
E* E* 0.0 0.0 Natural width of the state Estimates Consider an 57Fe source 57Co 57Co Fe
Enter -- Mr. Mossbauer Place 57Fe source bound in a metal matrix Resonant Absorption! Place 57Fe absorber bound in a metal matrix
+v -v Source Detector x Absorber E* E* 0.0 0.0 move source Kinematics Doppler shift frequency:h’- h = ED move source Assumesourceandabsorberare identical
-v no resonant absorption Source Absorber
-v no resonant absorption Source Absorber
-v small resonant absorption Source Absorber
-v more resonant absorption Source Absorber
v = 0.0 maximum resonant absorption Source Absorber
-v less resonant absorption Source Absorber
-v small resonant absorption Source Absorber
-v no resonant absorption Source Absorber
-v no resonant absorption Source Absorber
Source Detector x Absorber Es* Ea* 0.0 0.0 Kinematics Assume source and absorber are NOT identical
move absorber! +v -v Source Detector x Absorber Es* Ea* when - 0.0 0.0 Doppler kinematics Assume source and absorber are NOT identical Resonant absorption
-v Absorber transition energy shifted no resonant absorption Source
-v Absorber transition energy shifted small resonant absorption Source
-v Absorber transition energy shifted more resonant absorption Source
-v Absorber transition energy shifted more resonant absorption Source
Absorber transition energy shifted v = 0.0 less resonant absorption Source
-v Absorber transition energy shifted smallresonant absorption Source
-v Absorber transition energy shifted no resonant absorption Source
-v Absorber transition energy shifted no resonant absorption Source
-v Absorber transition energy shifted no resonant absorption Source
“Isotope shift” Doppler energy shifted
move absorber! +v -v Source Detector x Absorber Es* Ea* 0.0 0.0 when - Isotope shift Isotope shift:Level shifts due to atomic electronic charge distribution in the nucleus. Resonant absorption Constant velocity data
57Fe What is the J for the ground state and the 14.4 Kev state? ENSDF/NNDS What is the multipolarity of the transition? What is the degeneracy for the-- ground state and the -- 14.4 Kev state? If there is a B field, then we can have a nuclear Zeeman effectthat will remove the degeneracies
move source with constant acceleration -v +v Source Detector x Absorber m-sublevels Es* 0.0 57Fe
= dwell time v = one channel 0 -v +v Source velocity curve t v = 0 maximum +v v = 0 time maximum -v v = 0 Source displacement curve Mossbauer resonant absorption with constant acceleration Use MCS/MCA data
Source Detector x Absorber m-sublevels Es* 0.0 Possible absorption transitions
m-sublevels Possible absorption transitions 6 4 2 5 3 1
Possible absorption transitions Compare these predictions with the measurements… …follow guidelines in Problem. 10.C. and eventually determine
The Pound-Rebecca Experiment Be prepared to explainwhat the experiment discoveredandhow the Mossbauer resonant photon absorption was essential to the measurement.
m-sublevels Possible absorption transitions Case1 6 4 2 5 3 1
m-sublevels Possible absorption transitions Case2 5 3 1 6 4 2
6 5 3 4 2 1 Possible absorption transitions m-sublevels Case3
6 5 4 3 2 1 Possible absorption transitions m-sublevels Case4