Strength of Giant Resonances

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Monopole Enhanced at 0 o .0.30 o Cross Section0.20.1Measure at 0 oThe Monopole!00 10 20 30 40Ex(MeV)0.34 o Cross Seciton0.20.1Measure at 4 oThe Quadrupole!00 10 20 30 40E x (MeV)
At Small anglesBeam would destroy detectors.Use Magnet to separate beam from inelastic scatteringBUT!Beam must be transported without hitting anything!Nobody had done 0 o inelastic scattering.
Page 1 and 2: Giant ResonancesFirst Experiments:G
Page 3 and 4: Shape Oscillations“Giant Resonanc
Page 5: 1970: Only Dipole had been observed
Page 9 and 10: One in particular:Isoscalar Giant M
Page 11: Use an alpha particle beam to excit
Page 16 and 17: Measure over the minimum in the mon
Page 19: Built:New cyclotron - higher energy
Page 24 and 25: E GMR =ħ(K A /m) 1/2: mean square
Page 26: Nuclear Matter Equation of StateA p
Page 29 and 30: Inelastic Scattering to Giant Reson
Page 31 and 32: To study GMR in 27 Si6LiStops in ta
Page 33 and 34: Other Monopole ThingsFraction E0 EW
Page 35: Nuclear equation of state influence

Strength of Giant Resonances

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