Nuclei with Z=1....54 (Landolt-Börnstein: Numerical Data and Functional Relationships in Science and Technology - New Series, 22A) - Hardcover
Synopsis
Themassexcessisrepresentedusuallysimultaneouslywiththetotalnuclearbindingenergy (E )orthebindingenergypernucleonE /A.Thelattervalueisconnectedwiththestabilityof B B nucleiandshowsamaximumaroundthe“iron-peak”importantinastrophysics[03Au03].As inothermasscompilationswegivenucleonandtwo-nucleonseparationenergies.Clustering effectsinnucleardataarepresentedbyseparationenergiesofdifferentnucleoncombinations (S ,S ,etc.).Forneutronseparationenergiesonlythemostprecisevaluesfromtherecent 2p2n 2p4n neutroncaptureexperimentsarepresented.Inseveralcasesonlynucleonseparationenergies areknownaccuratelywhiletotalbindingenergiesremainuncertain(insuchcasesweinclude newseparationenergy). The experimental study of atomic masses started nearly hundred years ago. In the p- neeringworkofAston[27As0A]nuclearbindingenergieswereobtainedformanynucleiand Landolt-Börnstein DOI:10.1007/978-3-540-69945-3_1 NewSeriesI/22A ©Springer2009 21 Introduction nearconstancyof theaveragebindingenergypernucleonsuggestedtheindependenceof the nucleardensitywiththeatomicweightAandthesaturationof thenuclearforces.Thesetwo nuclear features were represented by the ?rst mass formula byWeizsäcker in 1935 [35Vo0A] inspired by the liquid-drop model (DM) of the nucleus by Nils Bohr. The Bethe-Weizsäcker formula is extended recently in [08Me01, 08Ki01]. Some methodical aspects of earlier mass measurementswerediscussedbyWapstraandAudi[01Wa49,06Au0A].
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Nuclei with Z=1.54
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Condition: Sehr gut. Zustand: Sehr gut | Seiten: 505 | Sprache: Englisch | Produktart: Bücher | Keine Beschreibung verfügbar. Seller Inventory # 5172311/12
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Nuclei with Z=1.54 (Hardcover)
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Springer-Verlag Berlin and Heidelberg GmbH & Co. KG, Berlin, 2009
ISBN 10: 3540699449
ISBN 13: 9783540699446
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Hardcover. Condition: new. Hardcover. Introduction Generalremarks Thisreportisthecompilationofexperimentalandtheoreticaldataonatomicmasses,nuclear bindingenergies,nucleonseparationenergies,Q-valuesofsomenucl earreactionsandpar- etersof nucleonresidualinteractionsderivedfromdifferencesof nuclearbindingenergies.It consistsoftwoparts,volumesI/22AandI/22B,inwhichdatafornucleiwithatomicnumb ers 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.Ther e isanassumptionthattheuncertaintyincalculatedvalueB (about150eVfortheatomswith el Z < 100 [03Lu10]) is smaller than the experimental error. If ionized atoms are involved in massmeasurementsthiscorrectionisappliedforthedeterminationoftheato micmass. Themassexcessisrepresentedusuallysimultaneouslywiththetotalnuclearbindingenergy (E )orthebindingenergypernucleonE /A.Thelattervalueisconnectedwiththestabilityof B B nucleiandshowsamaximumaroundthe"iron-peak"importantinastrophysics[ 03Au03].As inothermasscompilationswegivenucleonandtwo-nucleonseparationenergies.Clustering effectsinnucleardataarepresentedbyseparationenergiesofdifferentnucleoncombinations (S ,S ,etc.).Forneutronseparationenergiesonlythemostprecisevaluesf romtherecent 2p2n 2p4n neutroncaptureexperimentsarepresented.Inseveralcasesonlynucleonseparationenergies areknownaccuratelywhiletotalbindingenergiesremainuncertain(insuchcasesweinc lude newseparationenergy).The experimental study of atomic masses started nearly hundred years ago. In the p- neeringworkofAston[27As0A]nuclearbindingenergieswereobtainedformanynuc leiand Landolt-Bornstein DOI:10.1007/978-3-540-69945-3_1 NewSeriesI/22A (c)Springer2009 21 Introduction nearconstancyof theaveragebindingenergypernucleonsuggestedtheindependenceof the nucleardensitywiththeatomicweightAandthesaturationof thenuclearforces.Thesetwo nuclear features were represented by the ?rst mass formula byWeizsacker in 1935 [35Vo0A] inspired by the liquid-drop model (DM) of the nucleus by Nils Bohr. The Bethe-Weizsacker formula is extended recently in [08Me01, 08Ki01]. Some methodical aspects of earlier mass measurementswerediscussedbyWapstraandAudi[01Wa49,06Au0A]. First of two volumes dedicated to nuclear binding energies and atomic masses of all nuclei, this work considers related properties like the separation energies of single nucleons, or groups of nucleons, Q-values of alpha and beta nuclear reactions, and parameters of the residual interaction between nucleons. Shipping may be from multiple locations in the US or from the UK, depending on stock availability. Seller Inventory # 9783540699446
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Nuclei with Z=1.54
Published by
Springer, Berlin, Springer Berlin Heidelberg, Springer, 2009
ISBN 10: 3540699449
ISBN 13: 9783540699446
New
Hardcover
Seller: AHA-BUCH GmbH, Einbeck, Germany
Seller rating 5 out of 5 stars
Buch. Condition: Neu. Neuware - Introduction Generalremarks Thisreportisthecompilationofexperimentalandtheoreticaldataonatomicmasses,nuclear bindingenergies,nucleonseparationenergies,Q-valuesofsomenucle arreactionsandpar- etersof nucleonresidualinteractionsderivedfromdifferencesof nuclearbindingenergies.It consistsoftwoparts,volumesI/22AandI/22B,inwhichdatafornucleiwithatomicnumbe rs Z = 1 54andZ 55arepresented.EarlierQ-valuesofnuclearreactionswereconsideredin volume1/5AoftheNewSeriesLandoldt-Börnsteinlibrary[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 ×m B (Z) (1) A N e el 4 wherem = 510.99892(4)keV = 5.485799094(2)×10 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) = (14.4381×Z +1.55468×10 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 ×M(p)+N ×M(n) M (A,Z) (3) B N areusuallygiveninunitkeV.HerevaluesM(p)andM(n)arethemassesofthenucleons.There isanassumptionthattheuncertaintyincalculatedvalueB (about150eVfortheatomswith el Z 100 [03Lu10]) is smaller than the experimental error. If ionized atoms are involved in massmeasurementsthiscorrectionisappliedforthedeterminationoftheatomicmass. Themassexcessisrepresentedusuallysimultaneouslywiththetotaln uclearbindingenergy (E )orthebindingenergypernucleonE /A.Thelattervalueisconnectedwiththestabilityof B B nucleiandshowsamaximumaroundthe iron-peak importantinastrophysics[03Au03].As inothermasscompilationswegivenucleonandtwo-nucleonseparationenergies.Clustering effectsinnucleardataarepresentedbyseparationenergiesofdifferentnucleoncombinations (S ,S ,etc.).Forneutronseparationenergiesonlythemostprecisevaluesfromtherec ent 2p2n 2p4n neutroncaptureexperimentsarepresented.Inseveralcasesonlynucleonseparationenergies areknownaccuratelywhiletotalbindingenergiesremainuncertain(insuchcasesweinclude newseparationenergy). The experimental study of atomic masses started nearly hundred years ago. In the p- neeringworkofAston[27As0A]nuclearbindingenergieswereobtainedformanynucleiand Landolt-Börnstein DOI:10.1007/978-3-540-69945-3_1 NewSeriesI/22A Springer2009 21 Introduction nearconstancyof theaveragebindingenergypernucleonsuggestedtheindependenceof the nucleardensitywiththeatomicweightAandthesaturationof thenuclearforces.Thesetwo nuclear features were represented by the rst mass formula byWeizsäcker in 1935 [35Vo0A] inspired by the liquid-drop model (DM) of the nucleus by Nils Bohr. The Bethe-Weizsäcker formula is extended recently in [08Me01, 08Ki01]. Some methodical aspects of earlier mass measurementswerediscussedbyWapstraandAudi[01Wa49,06Au0A]. Seller Inventory # 9783540699446
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Nuclear Binding Energies and Atomic Masses: Nuclei With Z=1-54: Vol A
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Hardcover. Condition: Brand New. 2009 edition. 505 pages. 11.00x8.00x1.75 inches. In Stock. Seller Inventory # x-3540699449
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