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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

Extent: 1 Online-Ressource.

Language: Englisch

Bibliographic citation: 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

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

Contributor: SpringerLink (Online service)

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

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

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

Last update: 15.08.2025, 7:26 AM CEST

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

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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

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

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Other Objects (12)

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

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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

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

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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

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

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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

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