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This study explores Compton scattering to determine the electron mass and cross section. Conducted using a photomultiplier tube, scintillator, and lead shielding, energy spectra were collected with and without a copper cylinder. The data fitting process allows for accurate determination of the electron mass, yielding a value of 503.8 ± 14.6 keV, which closely aligns with the known mass of 510.998910 ± 0.000013 keV. Additionally, the collected data supports the Klein-Nishina model, demonstrating the relationship between theoretical predictions and experimental results.
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Compton Scattering James Durgin Physics 521 March 19, 2009
Background Collecting energies at several points lets one find electron mass and cross section Image from user-review.ca
Photomultiper tube Scintillator Lead shielding Copper cylinder Source inside shielding
Experimental Theory • Calibrate multichannel analyzer • Collect energy spectrums with copper cylinder • Collect energy spectrums without copper cylinder • Fit points to find electron mass and experimental cross section
Calibration Isotope energies v. channel number
Energy Spectrums Counts per channel v. channel number Net counts v. channel number
Net counts v. channel number Fit for Compton Scattered Photons Graphical Compton’s Equation
Cross section comparison Collected data follows Klein-Nishina cross section Thomson cross section Thomson equation Klein-Nishina cross section Klein-Nishina equation
Uncertainty Analysis • Statistical nature of counts • Setup uncertainty • Conversion uncertainty • Negligible events
Conclusion • Experimental electron mass of 503.8 ± 14.6 keV v. actual electron mass of 510.998910±0.000013 keV • Collected data has closer agreement with Klein-Nishina model