Radioactive Ion Beam (RIB) Facility at VECC : - Saha Institute of ...

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Dispersive PlaneOptics for the analysing section of the LEBT design30X’ [mr]X [mm]-20 20Dipole-30Non-dispersive PlaneConfigurationAcceptanceDrift-Dipole-Drift120 π-mm-mr. (FullTransmission)System Length2.855 m1.07 mDipole30 Φ1 mDispersionMass R. PowerMagnification1.98 m (for 100%rigidity change)43 (3 rd order)-0.95
Optics for the LEBT sectionDispersive Plane125X’ [mr]X [mm]-6 6Transmission 98.8 %Non-dispersive Plane85 Φ30 ΦSolenoid-125125Y’ [mr]Y [mm]-6 61 m1.07 m Dipole1.48 mSolenoid.525 m-125
Page 2: Radioactive Ion Beams : Ions of β-
Page 6 and 7: Physics Motivation • Material Sci
Page 8 and 9: Physics Motivation• Nuclear Physi
Page 12 and 13: Nucleosynthesis in StarsExpandingCo
Page 14 and 15: Nucleosynthesis in StarsCNO CycleZ1
Page 16 and 17: Nucleosynthesis ofelements beyond F
Page 18 and 19: Nuclear Astrophysics• Reactions i
Page 20 and 21: 1.Radioactive Ion Beams will play a
Page 22 and 23: VECC RIBfacility layout1.5 keV/u460
Page 24 and 25: Thick target development :Selection
Page 26 and 27: Thick target R&D : first few target
Page 28 and 29: R&D Initiative on ion source :Integ
Page 30 and 31: R&D Initiative on ion source :Prima
Page 32 and 33: Typical Oxygen spectrum from ECR io
Page 34 and 35: Design & Development of LEBT sectio
Page 38 and 39: Design of Radio Frequency Quadrupol
Page 40 and 41: RADIOFREQUENCY QUADRUPOLE (RFQ) : 1
Page 42 and 43: Beams available from the RIB facili
Page 44 and 45: Design of LINAC cavitiesK=130Cyclot
Page 46 and 47: VECLIN Snap shotε x/y= 0.5 π mm m
Page 48 and 49: IH - LINAC : The design details Str
Page 50 and 51: LINAC-1 : Important ParametersFrequ
Page 53: LINAC-2 : Important ParametersFrequ
Page 56 and 57: Future Plans
Page 58 and 59: e-linace- γUraniumISOL type RIB fa
Page 60 and 61: Thank You!60
Page 62 and 63: 238U photo-fission fragmentsmass di
Page 64: IH - LINAC : The design details Pos

Radioactive Ion Beam (RIB) Facility at VECC : - Saha Institute of ...

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