Mössbauer Effect 200582116 J-H. Kim 2005. 12. 05 1 Contents Motivation - Beginning - Mössbauer Effect(Ir-191) Experiment - Mössbauer Measurements Summary 2 Motivation Applications Summary What is the Mössbauer effect ? Before the Mössbauer theory Yes~! I am a nuclei at ground state. I am a nuclei excited state. I want to go to the excited state. Ok. I will give you a gamma ray for your exciting. You will be unstable. Do you want it? Thank you! This energy is not enough for my exciting. The energy of my gamma should be smaller than excited since I should be recoiled. 3 Motivation Applications Summary What is the Mössbauer effect ? Before the Mössbauer theory. Momentum conservation. Doppler effect. - The nuclei recoil back with velocity v(βc). - The frequency of gamma ray for absorption is lower than at the emission. => Then target nuclei cannot absorb the gamma energy. # For Ir-191 (hν = 129 keV) v = 202 m/s E’ = 128.999912874 keV ΔE= 8.71E-5 keV Γ = 3.22E-8 keV (natural line width) ΔE ≫ Γ 4 Motivation Applications Summary What is the Mössbauer effect ? Beginning - Rudolf Mössbauer.(1929~?, German physicist) - Discovered the recoil-free emission and absorption of gamma rays by nuclei. (in 1958) - Win the Novel prize. (in 1962) Experiment ( Recoil Free Nuclear Radiation ) - Ir-191 How atom can recoil-free emission and absorption? - Atoms are held tightly in crystalline atomic structures 5 Motivation Applications Summary What is the Mössbauer effect ? Beginning with the Mössbauer theory I am a nuclei at ground state. I am a nuclei excited state. I can give you an energy for your exciting. I am K-U.Choi nuclei. K-U.Choi stick me on this space with silicon! so I can have little momentum. Really? but.. I don’t believe you. -_-;; I have a different flavor than yours. Really? I believe you then. 6 Motivation Applications Summary What is the Mössbauer effect ? Beginning with the Mössbauer theory. - We don’t know the share the required momentum. - I calculate the number of nuclei for the condition. ΔE<Γ (ΔE=E_pt-E_pt’) # For Ir-191 (hν = 129 keV) N=2700, v = 7.5 cm/s, E’ = 128.99999999… keV - N ≪ 1 mol(10E23) =>velocity and energy loss is very small. # For Ir-191 (hν = 129 keV), N = 1mol v = 2E-19 cm/s ≒ 0 cm/s 7 Motivation Applications Summary How to measure the Mössbauer effect. Measurement for Mössbauer effect. Data Equipment Source. Intensity 0 ΔE Detector. Absorber. 0 Velocity 8 Motivation Applications Summary Applications. What can we measure with Mössbauer effect? 1. The lifetime determinant for an excited particle. 2. Nuclei energy level. 3. The general relativity theory. - Gravitational red shift. 4. The hyperfine structure. - The nuclear isomer shift. - The nuclear Zeeman effect. - The nuclear quadrupole splitting. 9 Motivation Applications Summary 1. The lifetime determinant for an excited particle. Particle lifetime of an excited state in a nucleus. - τ=Δt : particle lifetime. - ΔE(Γ/2) : can be determined in Mössbauer experiment. The Breit-Wigner distribution : Γ : natural line width. x axis : energy y axis : absorption cross section. 10 Motivation Applications Summary 2. The general relativity theory. Gravitational red shift. - E_0 = hν = 14.4 keV - Gravitational red shift. ν=ν_0(1+(gh/c^2)) ΔE=2*ν_0(gh/c^2) ΔE 11 Motivation Applications Summary 3. The hyperfine structure. The nuclear isomer shift. The nuclear Zeeman effect. The nuclear quadrupole splitting. 12 Motivation Applications Summary 3. The hyperfine structure. 13 Motivation Applications Summary Summary What is the Mössbauer effect? For nuclei in crystalline atomic structures, the gamma radiation emitted from the nuclei are approximately recoil-free. How to measure the Mössbauer effect. 1. Gamma-ray source, an absorber, Gamma Detector. 2. Relative velocity of varying the gamma-ray energy. Applications 1. The lifetime determinant for an excited particle. 2. The general relativity theory. 3. The hyperfine structure. 14 Thank you. 15