Masses of 130Te and 130Xe and double-beta-decay Q value of 130Te
- PMID:19519099
- DOI: 10.1103/PhysRevLett.102.212502
Masses of 130Te and 130Xe and double-beta-decay Q value of 130Te
Abstract
The atomic masses of 130Te and 130Xe have been obtained by measuring cyclotron frequency ratios of pairs of triply charged ions simultaneously trapped in a Penning trap. The results, with 1 standard deviation uncertainty, are M(130Te)=129.906 222 744(16) u and M(130Xe)=129.903 509 351(15) u. From the mass difference the double-beta-decay Q value of 130Te is determined to be Qbetabeta(130Te)=2527.518(13) keV. This is a factor of 150 more precise than the result of the AME2003 [G. Audi, Nucl. Phys. A729, 337 (2003)10.1016/j.nuclphysa.2003.11.003].
Similar articles
- Mass and double-beta-decay Q value of 136Xe.Redshaw M, Wingfield E, McDaniel J, Myers EG.Redshaw M, et al.Phys Rev Lett. 2007 Feb 2;98(5):053003. doi: 10.1103/PhysRevLett.98.053003. Epub 2007 Feb 2.Phys Rev Lett. 2007.PMID:17358854
- Q value of ;{115}In --> ;{115}sn(3/2;{+}): the lowest known energy beta decay.Mount BJ, Redshaw M, Myers EG.Mount BJ, et al.Phys Rev Lett. 2009 Sep 18;103(12):122502. doi: 10.1103/PhysRevLett.103.122502. Epub 2009 Sep 16.Phys Rev Lett. 2009.PMID:19792427
- Determination of the (76)Ge double beta decay Q value.Douysset G, Fritioff T, Carlberg C, Bergström I, Björkhage M.Douysset G, et al.Phys Rev Lett. 2001 May 7;86(19):4259-62. doi: 10.1103/PhysRevLett.86.4259.Phys Rev Lett. 2001.PMID:11328149
- High Precision Determination of the β Decay Q(EC) Value of (11)C and Implications on the Tests of the Standard Model.Gulyuz K, Bollen G, Brodeur M, Bryce RA, Cooper K, Eibach M, Izzo C, Kwan E, Manukyan K, Morrissey DJ, Naviliat-Cuncic O, Redshaw M, Ringle R, Sandler R, Schwarz S, Sumithrarachchi CS, Valverde AA, Villari AC.Gulyuz K, et al.Phys Rev Lett. 2016 Jan 8;116(1):012501. doi: 10.1103/PhysRevLett.116.012501. Epub 2016 Jan 6.Phys Rev Lett. 2016.PMID:26799013
- Mass and lifetime measurements of exotic nuclei in storage rings.Franzke B, Geissel H, Münzenberg G.Franzke B, et al.Mass Spectrom Rev. 2008 Sep-Oct;27(5):428-69. doi: 10.1002/mas.20173.Mass Spectrom Rev. 2008.PMID:18636527Review.
Cited by
- TeO[Formula: see text] bolometers with Cherenkov signal tagging: towards next-generation neutrinoless double-beta decay experiments.Casali N, Vignati M, Beeman JW, Bellini F, Cardani L, Dafinei I, Di Domizio S, Ferroni F, Gironi L, Nagorny S, Orio F, Pattavina L, Pessina G, Piperno G, Pirro S, Rusconi C, Schäffner K, Tomei C.Casali N, et al.Eur Phys J C Part Fields. 2015;75(1):12. doi: 10.1140/epjc/s10052-014-3225-4. Epub 2015 Jan 14.Eur Phys J C Part Fields. 2015.PMID:25983645Free PMC article.
- CALDER: neutrinoless double-beta decay identification in TeO[Formula: see text] bolometers with kinetic inductance detectors.Battistelli ES, Bellini F, Bucci C, Calvo M, Cardani L, Casali N, Castellano MG, Colantoni I, Coppolecchia A, Cosmelli C, Cruciani A, de Bernardis P, Di Domizio S, D'Addabbo A, Martinez M, Masi S, Pagnanini L, Tomei C, Vignati M.Battistelli ES, et al.Eur Phys J C Part Fields. 2015;75(8):353. doi: 10.1140/epjc/s10052-015-3575-6. Epub 2015 Jul 31.Eur Phys J C Part Fields. 2015.PMID:26269692Free PMC article.
- Nuclear physics: Weighing up the superheavies.Bollen G.Bollen G.Nature. 2010 Feb 11;463(7282):740-1. doi: 10.1038/463740a.Nature. 2010.PMID:20148021No abstract available.
LinkOut - more resources
Full Text Sources