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Sources of γ - radiation: CATE

Sources of γ - radiation: CATE. γ - detection system: BaF 2 detectors HECTOR array. distance HECTOR-target: 35cm distance HECTOR-CATE: 175cm ratio of solid angles: factor 25 distance target-CATE: 140cm. CATE CsI ρ =4.51g/cm 3 1-2.5cm thick. Be-target (0.7g/cm 2 ).

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Sources of γ - radiation: CATE

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  1. Sources of γ-radiation: CATE γ-detection system: BaF2 detectors HECTOR array distance HECTOR-target: 35cm distance HECTOR-CATE: 175cm ratio of solid angles: factor 25 distance target-CATE: 140cm CATE CsI ρ=4.51g/cm3 1-2.5cm thick Be-target (0.7g/cm2)

  2. target atoms [cm-2]= (nuclear range in CsI= 1cm) CsI atoms [cm-2]= Sources of γ-radiation: CATE Ca→Be:σreac=1227[mb] σ1n=10[mb]Ca→CsI:σreac=4807[mb] Ca→Be: rate=57.5[s-1] rate=0.5[s-1]Ca→CsI:rate=100.4[s-1](for 103 fragments/s) target CATE target 15ns 37Ca→36,37Ca 37Ca→36K BaF2-time BaF2-time ratio of solid angles: 25

  3. Sources of γ-radiation: elastic channel target CATE 37Ca→36,37Ca 15ns BaF2-time solid angle ratio: 25

  4. Sources of γ-radiation: elastic channel target CATE 1420 1420 1420 1420 1420 900 37Ca→36,37Ca 900 1420 BaF2-time

  5. Sources of γ-radiation: 1p fragmentation target 37Ca→36K BaF2-time

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