Strength of Giant Resonances

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Multipole Distributions116 SnFraction E0 EWSR/MeV0.30.20.16 LiE0Fraction E2 EWSR/MeV0.250.20.150.10.05E2005 15 25 35 5 15 25 35E x (MeV)E x (MeV)28 Si GMR0.1628 Si E0 EWSR/MeVFraction E0 EWSR/MeV0.120.080.046Li scatteringalpha scattering05 15 25E x (MeV)6 Li, agree for GR’s 116 Sn, 28 Si, 24 Mg.35
To study GMR in 27 Si6LiStops in targetto decay detector27Si6Li4.12sTarget27Si*10 -20 s23Mg11.32sto magneticspectrometer
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 14 and 15: Monopole Enhanced at 0 o .0.30 o Cr
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: Inelastic Scattering to Giant Reson
Page 33 and 34: Other Monopole ThingsFraction E0 EW
Page 35: Nuclear equation of state influence

Strength of Giant Resonances

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