New Arrivals/Restock

Introduction Generalremarks Thisreportisthecompilationofexperimentalandtheoreticaldataonatomicmasses, nuclear bindingenergies, nucleonseparationenergies, Q-valuesofsomenuclearreactionsandpar- etersof nucleonresidualinteractionsderivedfromdifferencesof nuclearbindingenergies.It consistsoftwoparts, volumesI/22AandI/22B, inwhichdatafornucleiwithatomicnumbers Z = 1?54andZ ? 55arepresented.EarlierQ-valuesofnuclearreactionswereconsideredin volume1/5AoftheNewSeriesLandoldt-Bornsteinlibrary[73Sc0A].Thedatainourcompi- tionarepresentedintableswhoseformatisanalogoustothatofothercompilationsofatomic masses (AM), nuclear binding energies (E ), atomic mass excesses of nuclei (ME, ME = 0 B 12 for Cbyde?nition), Q-valuesandseparationenergiesofasinglenucleonorapairofnuc- ons(S, S, S, S )[05Au0A,05Wa35,03Au03,03AuZZ,03Wa32,02Wa27,01Au10,95Au04, n p 2n 2p 85Wa02,85Bo10,37Li0A]. AtomicmassesM areconnectedwithnuclearmassesM bytheformula: A N M (A, Z) =M (A, Z)+Z xm ?B (Z) (1) A N e el ?4 wherem = 510.99892(4)keV = 5.485799094(2)x10 uistheelectronrestmass(inatomic e massunitu)[06Ya08].ThetotalbindingenergyofallremovedelectronsB (Z)canbefound el in [76Hu0A] or approximated with the expression given by Lunney, Pearson and Thibault [03Lu10]: 2.39 ?6 5.35 B (Z) = (14.4381xZ +1.55468x10 Z )eV (2) el The mass excess, M (A, Z) ?Au, and the nuclear binding energy E calculated by the A B formula: E =Z xM(p)+N xM(n)?M (A, Z) (3) B N areusuallygiveninunitkeV.HerevaluesM(p)andM(n)arethemassesofthenucleons.There isanassumptionthattheuncertaintyincalculatedvalueB (about150eVfortheatomswith el Z