Relativistic Models of Quasielastic Electron and Neutrino-Nucleus Scattering Carlotta Giusti
Relativistic Electron Mass Experiment John Klumpp.
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Transcript of Relativistic Electron Mass Experiment John Klumpp.
![Page 1: Relativistic Electron Mass Experiment John Klumpp.](https://reader036.fdocuments.in/reader036/viewer/2022082611/56649e7b5503460f94b7b8d0/html5/thumbnails/1.jpg)
Relativistic Electron Mass Experiment
John Klumpp
![Page 2: Relativistic Electron Mass Experiment John Klumpp.](https://reader036.fdocuments.in/reader036/viewer/2022082611/56649e7b5503460f94b7b8d0/html5/thumbnails/2.jpg)
Testing Velocity Dependence of the Electron Mass
• Special relativity: A body’s mass increases with velocity according to the equation:
m = m0*[1-(v/c)2]-1/2
• Test by curving electron beam with B field, straightening with E field.
![Page 3: Relativistic Electron Mass Experiment John Klumpp.](https://reader036.fdocuments.in/reader036/viewer/2022082611/56649e7b5503460f94b7b8d0/html5/thumbnails/3.jpg)
Setup
-Electron beam from 90Sr source is curved by a B field
-A series of narrow apertures only allow electrons curving with R=15cm to pass by
-Beam then travels through a capacitor. Electrons whose path is not straightened by the E field collide with capacitor plates.
-Scintillator counts electrons which make it through
-Vary E field to find out which one best balances B
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What Does This Tell Us?
• We know E, B, and R• We know the forces from the B field and E
field match• Knowing this, we find:
v = E/Bm= = eRB2/E
• By determining which E field matches a series of B fields, we can find out how mass varies with velocity
![Page 5: Relativistic Electron Mass Experiment John Klumpp.](https://reader036.fdocuments.in/reader036/viewer/2022082611/56649e7b5503460f94b7b8d0/html5/thumbnails/5.jpg)
Calibration• To prevent arcing in the capacitor, we put the
whole apparatus in a vacuum chamber• This means we can’t measure B directly while
doing the experiment• Solution: Use Hall probe to find out in advance
what currents lead to what fields:
I (Amps) Average B (Gauss) Uncertainty
0.744 80.04 0.16
0.943 99.98 0.22
1.140 120.36 0.20
1.334 139.93 0.24
1.533 159.73 1.54
1.731 180.36 0.38
1.822 189.69 0.41
![Page 6: Relativistic Electron Mass Experiment John Klumpp.](https://reader036.fdocuments.in/reader036/viewer/2022082611/56649e7b5503460f94b7b8d0/html5/thumbnails/6.jpg)
Calibration Results
Magnetic field vs current with linear polynomial overlay.
-Calibration Equation: B = 101.7A + 4.3
-χ2 is 1.79 with 5 degrees of freedom.
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The Experiment
• Remove Hall probe, insert experimental apparatus• Take measurements at 80, 100, 120, 140, 160, 180, and
190 Gauss.• For each B field, Take 13 measurements for 100
seconds each• Measurements are in 50V intervals about theoretical
value• Plot each set of measurements, fit a Gaussian to
determine peak position• This peak is the E field which should perfectly balance
the B field
![Page 8: Relativistic Electron Mass Experiment John Klumpp.](https://reader036.fdocuments.in/reader036/viewer/2022082611/56649e7b5503460f94b7b8d0/html5/thumbnails/8.jpg)
Finding the Peak
• E field vs. counts for B = 80.6T with Gaussian overlay• Peak is 2.78kVm-1, in agreement with theory
![Page 9: Relativistic Electron Mass Experiment John Klumpp.](https://reader036.fdocuments.in/reader036/viewer/2022082611/56649e7b5503460f94b7b8d0/html5/thumbnails/9.jpg)
• Using this method, we found the electric fields which corresponded to each B field.
• From there we calculated mass and velocity
I (Amps) B(Tessla) Peak (KV) m (kg) dm beta dbeta
0.75 0.0081 2.784 1.14E-30 6.531E-33 0.567 0.017
0.95 0.0101 3.99 1.24E-30 2.3E-32 0.650 0.019
1.14 0.0120 5.17 1.36E-30 8.129E-33 0.708 0.015
1.35 0.0141 6.579 1.48E-30 6.292E-33 0.765 0.013
1.53 0.0160 7.897 1.59E-30 1.105E-32 0.809 0.013
1.73 0.0180 9.117 1.73E-30 3.988E-33 0.832 0.011
1.83 0.0190 9.785 1.8E-30 5.895E-33 0.844 0.011
-Clearly mass varies with velocity, but how?
![Page 10: Relativistic Electron Mass Experiment John Klumpp.](https://reader036.fdocuments.in/reader036/viewer/2022082611/56649e7b5503460f94b7b8d0/html5/thumbnails/10.jpg)
Mass vs. Velocity• Relativity predicts mass will vary with velocity as such:
m = mo(1- β2)-1/2
• We plotted m vs β and m vs (1- β2)-1/2 to find out if our results match this shape, and to find the rest mass.
-As expected, these fit lines match the data quite well. The m vs β fit gives m0 = 9.572*10-31. The m vs (1- β2)-1/2 fit gives m0 = 9.48*10-31. The χ2 on the two graphs are 32.6 and 16.5 respectively. Each has 5 degrees of freedom.
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Charge to Mass Ratio• The charge-to-mass ratio of the electron can be
determined by the equatione/mo = e/[m(1- β2)1/2] = U/[RB(D2B2 – U2/e2)1/2]
• Results:
B(Tessla) U (kV) e/mo (C/kg) de/mo
0.00806 2784 1.71E+11 1.24E+10
0.01008 3990 1.7E+11 1.11E+10
0.01199 5170 1.67E+11 9.99E+09
0.01413 6579 1.68E+11 9.74E+09
0.01604 7897 1.71E+11 1.03E+10
0.01800 9117 1.66E+11 9.58E+09
0.01903 9785 1.66E+11 9.64E+09
-Conclusion: e/m0 = (1.68 +/- .04)*1011 C/kg
![Page 12: Relativistic Electron Mass Experiment John Klumpp.](https://reader036.fdocuments.in/reader036/viewer/2022082611/56649e7b5503460f94b7b8d0/html5/thumbnails/12.jpg)
Sources of Uncertainty• Tiny uncertainty on E, big uncertainty on B:
-σE/E ≈ .001-σB/B ≈ .025
• B varies within the magnet• Some, but not much, statistical uncertainty from calibration equation• Does the calibration remain stable throughout the experiment?• e/m0 results consistently below accepted value – suggests
systematic uncertainty• On plots to determine E, most points had uncertainty of 5% or
higher (√N statistics) -Could be reduced by taking longer measurements-Uncertainty on location of peak only 0.5%, so not worth it.
• Different results on mo for different plots. Reason?-The uncertainties on the x-values of these fits are different-MatLab does not consider uncertainty on x values when making the plot
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Conclusion
• Mass varies with velocity in accordance with special relativity
• We have two values for m0. Choose the one from the plot with the better fit: m0 = (9.48 +/- 0.506)*10-31kg
• e/m0 = (1.68 +/- .04)*1011 C/kg• Most significant source of uncertainty: B• Uncertainty can be minimized by
-Taking extreme care in calibrating the magnet-Ensuring calibration conditions hold throughout experiment