Why is $$}^{208}_{82}\textrm{Pb}$$ 82 208 Pb the heaviest stable nuclide?

zu Verbundenen Objekten

Standort: Deutsche Nationalbibliothek Frankfurt am Main

Umfang: 1 Online-Ressource.

Sprache: Englisch

Erschienen in: Why is $$}^{208}_{82}\textrm{Pb}$$ 82 208 Pb the heaviest stable nuclide? ; volume:84 ; number:8 ; day:13 ; month:8 ; year:2024 ; pages:1-12 ; date:8.2024
The European physical journal / C. C, Particles and fields ; 84, Heft 8 (13.8.2024), 1-12, 8.2024

Urheber: Kosyakov, B. P.
Popov, E. Yu
Vronskiĭ, M. A.

Beteiligte Personen und Organisationen: SpringerLink (Online service)

DOI: 10.1140/epjc/s10052-024-13185-8

URN: urn:nbn:de:101:1-2412092114417.530300888228

Rechteinformation: Open Access; Der Zugriff auf das Objekt ist unbeschränkt möglich.

Letzte Aktualisierung: 15.08.2025, 07:26 MESZ

Datenpartner

Dieses Objekt wird bereitgestellt von:
Deutsche Nationalbibliothek. Bei Fragen zum Objekt wenden Sie sich bitte an den Datenpartner.

Original beim Datenpartner anzeigen

Beteiligte

Kosyakov, B. P.
Popov, E. Yu
Vronskiĭ, M. A.
SpringerLink (Online service)

Ähnliche Objekte (12)

High-precision mass measurement of doubly magic $$^208}$$ 208 Pb

$Predictions for exclusive $$\varUpsilon $$ Υ photoproduction in ultraperipheral $$\textrm{Pb}}+{\textrm{Pb}}$$ Pb + Pb collisions at the LHC at next-to-leading order in perturbative QCD$

Predictions for exclusive $$\varUpsilon $$ Υ photoproduction in ultraperipheral $$\textrm{Pb}}+{\textrm{Pb}}$$ Pb + Pb collisions at the LHC at next-to-leading order in perturbative QCD

$Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV$

Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

Erratum to: High-precision mass measurement of doubly magic $$^208}$$ 208 Pb

Wandmalerei

Raum 208 Ostwand 82

Transverse energy production in 208 Pb + Pb Collisions at 158 GeV per nucleon

$W ± -boson production in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

W ± -boson production in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

$Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

$Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Fusion of 9 Li with 70 Zn and 208 Pb

$Measurement of beauty production via non-prompt D0 mesons in Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV$

Measurement of beauty production via non-prompt D0 mesons in Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

$Low lying particle-hole states in $$^\mathbf206 }$$ 206 Pb and $$^\mathbf208 }$$ 208 Pb and the shell model$

Low lying particle-hole states in $$^\mathbf206 }$$ 206 Pb and $$^\mathbf208 }$$ 208 Pb and the shell model

High-precision mass measurement of doubly magic $$^208}$$ 208 Pb

$Predictions for exclusive $$\varUpsilon $$ Υ photoproduction in ultraperipheral $$\textrm{Pb}}+{\textrm{Pb}}$$ Pb + Pb collisions at the LHC at next-to-leading order in perturbative QCD$

Predictions for exclusive $$\varUpsilon $$ Υ photoproduction in ultraperipheral $$\textrm{Pb}}+{\textrm{Pb}}$$ Pb + Pb collisions at the LHC at next-to-leading order in perturbative QCD

$Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV$

Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

Erratum to: High-precision mass measurement of doubly magic $$^208}$$ 208 Pb

Wandmalerei

Raum 208 Ostwand 82

Transverse energy production in 208 Pb + Pb Collisions at 158 GeV per nucleon

$W ± -boson production in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

W ± -boson production in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

$Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

$Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Fusion of 9 Li with 70 Zn and 208 Pb

$Measurement of beauty production via non-prompt D0 mesons in Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV$

Measurement of beauty production via non-prompt D0 mesons in Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

$Low lying particle-hole states in $$^\mathbf206 }$$ 206 Pb and $$^\mathbf208 }$$ 208 Pb and the shell model$

Low lying particle-hole states in $$^\mathbf206 }$$ 206 Pb and $$^\mathbf208 }$$ 208 Pb and the shell model

High-precision mass measurement of doubly magic $$^208}$$ 208 Pb

$Predictions for exclusive $$\varUpsilon $$ Υ photoproduction in ultraperipheral $$\textrm{Pb}}+{\textrm{Pb}}$$ Pb + Pb collisions at the LHC at next-to-leading order in perturbative QCD$

Predictions for exclusive $$\varUpsilon $$ Υ photoproduction in ultraperipheral $$\textrm{Pb}}+{\textrm{Pb}}$$ Pb + Pb collisions at the LHC at next-to-leading order in perturbative QCD

$Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV$

Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

Erratum to: High-precision mass measurement of doubly magic $$^208}$$ 208 Pb

Wandmalerei

Raum 208 Ostwand 82

Transverse energy production in 208 Pb + Pb Collisions at 158 GeV per nucleon

$W ± -boson production in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV$

W ± -boson production in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

$Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

$Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV$

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Fusion of 9 Li with 70 Zn and 208 Pb

$Measurement of beauty production via non-prompt D0 mesons in Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV$

Measurement of beauty production via non-prompt D0 mesons in Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

$Low lying particle-hole states in $$^\mathbf206 }$$ 206 Pb and $$^\mathbf208 }$$ 208 Pb and the shell model$

Low lying particle-hole states in $$^\mathbf206 }$$ 206 Pb and $$^\mathbf208 }$$ 208 Pb and the shell model

Informationen zur Registrierung von Kultur- und Wissenseinrichtungen finden Sie hier.

Felder mit * müssen ausgefüllt werden.

Benutzername*

Bitte geben Sie Ihren Benutzernamen ein

E-Mail*

Bitte geben Sie Ihre E-Mail ein

Bitte füllen Sie dieses Feld nicht aus

Vorname

Nachname

Passwort*

Bitte geben Sie Ihr Passwort ein

Passwort bestätigen*

Bitte geben Sie das gleiche Passwort ein

Ich habe die Nutzungsbedingungen und die Datenschutzerklärung zur Erhebung persönlicher Daten gelesen und stimme ihnen zu. *

Dieses Feld ist ein Pflichtfeld.

Ich möchte den Newsletter der Deutschen Digitalen Bibliothek abonnieren. Siehe Informationen zum Newsletter-Abonnement.

Benutzerkonto angelegt

Ihr „Meine DDB“-Konto wurde erfolgreich angelegt. Bevor Sie sich in Ihrem Konto anmelden können, müssen Sie auf den Bestätigungslink in der Nachricht klicken, die wir gerade an die von Ihnen angegebene E-Mail-Adresse geschickt haben

Why is $$}^{208}_{82}\textrm{Pb}$$ 82 208 Pb the heaviest stable nuclide?

Angaben zum Objekt

Verweise und Beziehungen

Beteiligte, Orts- und Zeitangaben

Weitere Informationen

Datenpartner

Beteiligte

Ähnliche Objekte (12)

High-precision mass measurement of doubly magic $$^208}$$ 208 Pb

Predictions for exclusive $$\varUpsilon $$ Υ photoproduction in ultraperipheral $$\textrm{Pb}}+{\textrm{Pb}}$$ Pb + Pb collisions at the LHC at next-to-leading order in perturbative QCD

Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

Erratum to: High-precision mass measurement of doubly magic $$^208}$$ 208 Pb

Raum 208 Ostwand 82

Transverse energy production in 208 Pb + Pb Collisions at 158 GeV per nucleon

W ± -boson production in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Fusion of 9 Li with 70 Zn and 208 Pb

Measurement of beauty production via non-prompt D0 mesons in Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

Low lying particle-hole states in $$^\mathbf206 }$$ 206 Pb and $$^\mathbf208 }$$ 208 Pb and the shell model

High-precision mass measurement of doubly magic $$^208}$$ 208 Pb

Predictions for exclusive $$\varUpsilon $$ Υ photoproduction in ultraperipheral $$\textrm{Pb}}+{\textrm{Pb}}$$ Pb + Pb collisions at the LHC at next-to-leading order in perturbative QCD

Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

Erratum to: High-precision mass measurement of doubly magic $$^208}$$ 208 Pb

Raum 208 Ostwand 82

Transverse energy production in 208 Pb + Pb Collisions at 158 GeV per nucleon

W ± -boson production in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Fusion of 9 Li with 70 Zn and 208 Pb

Measurement of beauty production via non-prompt D0 mesons in Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

Low lying particle-hole states in $$^\mathbf206 }$$ 206 Pb and $$^\mathbf208 }$$ 208 Pb and the shell model

High-precision mass measurement of doubly magic $$^208}$$ 208 Pb

Predictions for exclusive $$\varUpsilon $$ Υ photoproduction in ultraperipheral $$\textrm{Pb}}+{\textrm{Pb}}$$ Pb + Pb collisions at the LHC at next-to-leading order in perturbative QCD

Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

Erratum to: High-precision mass measurement of doubly magic $$^208}$$ 208 Pb

Raum 208 Ostwand 82

Transverse energy production in 208 Pb + Pb Collisions at 158 GeV per nucleon

W ± -boson production in p–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 8.16 TeV and Pb–Pb collisions at s NN $$ \sqrts_{\textrm{NN}}} $$ = 5.02 TeV

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Azimuthal anisotropy of dijet events in PbPb collisions at $ \sqrts_{\textrm{NN}}} $ = 5.02 TeV

Fusion of 9 Li with 70 Zn and 208 Pb

Measurement of beauty production via non-prompt D0 mesons in Pb-Pb collisions at s NN $$ \sqrt{\textrm{s}}_{\textrm{NN}}} $$ = 5.02 TeV

Low lying particle-hole states in $$^\mathbf206 }$$ 206 Pb and $$^\mathbf208 }$$ 208 Pb and the shell model

Verbundene Objekte

Passwort zurücksetzen