Observation of the radiative decay of the 229 Th nuclear clock isomer.
Sandro KraemerJanni MoensMichail Athanasakis-KaklamanakisSilvia BaraKjeld BeeksPremaditya ChhetriKaterina ChrysalidisArno ClaessensThomas Elias CocoliosJoão G M CorreiaHilde De WitteRafael FerrerSarina GeldhofReinhard HeinkeNiyusha HosseiniMark HuyseUlli KoesterYuri KudryavtsevMustapha LaatiaouiRazvan LicaGoele MagchielsVladimir ManeaClement MercklingLino M C PereiraSebastian RaederThorsten SchummSimon SelsPeter G ThirolfShandirai Malven TunhumaPaul Van Den BerghPiet Van DuppenAndré VantommeMatthias VerlindeRenan VillarrealUlrich WahlPublished in: Nature (2023)
The radionuclide thorium-229 features an isomer with an exceptionally low excitation energy that enables direct laser manipulation of nuclear states. It constitutes one of the leading candidates for use in next-generation optical clocks 1-3 . This nuclear clock will be a unique tool for precise tests of fundamental physics 4-9 . Whereas indirect experimental evidence for the existence of such an extraordinary nuclear state is substantially older 10 , the proof of existence has been delivered only recently by observing the isomer's electron conversion decay 11 . The isomer's excitation energy, nuclear spin and electromagnetic moments, the electron conversion lifetime and a refined energy of the isomer have been measured 12-16 . In spite of recent progress, the isomer's radiative decay, a key ingredient for the development of a nuclear clock, remained unobserved. Here, we report the detection of the radiative decay of this low-energy isomer in thorium-229 ( 229m Th). By performing vacuum-ultraviolet spectroscopy of 229m Th incorporated into large-bandgap CaF 2 and MgF 2 crystals at the ISOLDE facility at CERN, photons of 8.338(24) eV are measured, in agreement with recent measurements 14-16 and the uncertainty is decreased by a factor of seven. The half-life of 229m Th embedded in MgF 2 is determined to be 670(102) s. The observation of the radiative decay in a large-bandgap crystal has important consequences for the design of a future nuclear clock and the improved uncertainty of the energy eases the search for direct laser excitation of the atomic nucleus.