## Dataset referencing 2016HO05

Phys.Rev. C 93, 044611 (2016)

W.Horiuchi, S.Hatakeyama, S.Ebata, Y.Suzuki

*Extracting nuclear sizes of medium to heavy nuclei from total reaction cross sections*

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140}Sn; calculated neutron and proton rms radii. ^{40,42,44,46,48,50,52,54,56,58,60}Ca, ^{56,58,60,62,64,66,68,70,72,74,76,78,80,82,84}Ni, ^{80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118,120,122}Zr, ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140}Sn, ^{156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196}Yb, ^{190,192,194,196,198,200,202,204,206,208,210,212,214}Pb; calculated matter radius of even-even nuclei using SkM*, SLy4, and SkI3 interactions. HF+BCS and HF theory with different interactions.

NUCLEAR REACTIONS ^{1,2}H, ^{4}He, ^{12}C(^{40}Ca, X), (^{42}Ca, X), (^{44}Ca, X), (^{46}Ca, X), (^{48}Ca, X), (^{50}Ca, X), (^{52}Ca, X), (^{54}Ca, X), (^{56}Ca, X), (^{58}Ca, X), (^{60}Ca, X), (^{56}Ni, X), (^{58}Ni, X), (^{60}Ni, X), (^{62}Ni, X), (^{64}Ni, X), (^{66}Ni, X), (^{68}Ni, X), (^{70}Ni, X), (^{72}Ni, X), (^{74}Ni, X), (^{76}Ni, X), (^{78}Ni, X), (^{80}Ni, X), (^{82}Ni, X), (^{84}Ni, X), (^{80}Zr, X), (^{82}Zr, X), (^{84}Zr, X), (^{86}Zr, X), (^{88}Zr, X), (^{90}Zr, X), (^{92}Zr, X), (^{94}Zr, X), (^{96}Zr, X), (^{98}Zr, X), (^{100}Zr, X), (^{102}Zr, X), (^{104}Zr, X), (^{106}Zr, X), (^{108}Zr, X), (^{110}Zr, X), (^{112}Zr, X), (^{114}Zr, X), (^{116}Zr, X), (^{118}Zr, X), (^{120}Zr, X), (^{122}Zr, X), (^{100}Sn, X), (^{102}Sn, X), (^{104}Sn, X), (^{106}Sn, X), (^{108}Sn, X), (^{110}Sn, X), (^{112}Sn, X), (^{114}Sn, X), (^{116}Sn, X), (^{118}Sn, X), (^{120}Sn, X), (^{122}Sn, X), (^{124}Sn, X), (^{126}Sn, X), (^{128}Sn, X), (^{130}Sn, X), (^{132}Sn, X), (^{134}Sn, X), (^{136}Sn, X), (^{138}Sn, X), (^{140}Sn, X), (^{156}Yb, X), (^{158}Yb, X), (^{160}Yb, X), (^{162}Yb, X), (^{164}Yb, X), (^{166}Yb, X), (^{168}Yb, X), (^{170}Yb, X), (^{172}Yb, X), (^{174}Yb, X), (^{176}Yb, X), (^{178}Yb, X), (^{180}Yb, X), (^{182}Yb, X), (^{184}Yb, X), (^{186}Yb, X), (^{188}Yb, X), (^{190}Yb, X), (^{192}Yb, X), (^{194}Yb, X), (^{196}Yb, X), (^{190}Pb, X), (^{192}Pb, X), (^{194}Pb, X), (^{196}Pb, X), (^{198}Pb, X), (^{200}Pb, X), (^{202}Pb, X), (^{204}Pb, X), (^{206}Pb, X), (^{208}Pb, X), (^{210}Pb, X), (^{212}Pb, X), (^{214}Pb, X), E=1000 MeV, also 200 MeV for proton target; calculated Coulomb breakup cross sections by equivalent-photon method (EPM) with projectile density from SkM*, SLy4, and SkI3 Skyrme interactions, total reaction and Coulomb breakup probabilities, reaction radii versus point matter rms radii. Glauber model with densities from Skyrme-Hartree-Fock+BCS model. ^{12}C(^{208}Pb, ^{12}C), E=200, 1000 MeV; ^{1}H(^{208}Pb, p), E=45-1000 MeV; calculated elastic σ(θ, E) using SkM* interaction, and compared with experimental data. ^{1}H(^{40}Ca, X), (^{58}Ni, X), (^{90}Zr, X), (^{120}Sn, X), (^{208}Pb, X), E=40-1000 MeV; calculated total reaction σ(E) and compared with experimental data.

doi: 10.1103/PhysRevC.93.044611

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