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Abstract
The odd isotopologues of ytterbium monohydroxide, 171,173YbOH, have been identified as promising molecules to measure parity (P) and time reversal (T) violating physics. Here, we characterize the Ã2Π1/2(0,0,0)-X̃2Σ+(0,0,0) band near 577 nm for these odd isotopologues. Both laser-induced fluorescence excitation spectra of a supersonic molecular beam sample and absorption spectra of a cryogenic buffer-gas cooled sample were recorded. In addition, a novel spectroscopic technique based on laser-enhanced chemical reactions is demonstrated and used in absorption measurements. This technique is especially powerful for disentangling congested spectra. An effective Hamiltonian model is used to extract the fine and hyperfine parameters for the Ã2Π1/2(0,0,0) and X̃2Σ+(0,0,0) states. A comparison of the determined X̃2Σ+(0,0,0) hyperfine parameters with recently predicted values [Denis et al., J. Chem. Phys. 152, 084303 (2020); K. Gaul and R. Berger, Phys. Rev. A 101, 012508 (2020); and Liu et al., J. Chem. Phys. 154,064110 (2021)] is made. The measured hyperfine parameters provide experimental confirmation of the computational methods used to compute the P,T-violating coupling constants Wd and WM, which correlate P,T-violating physics to P,T-violating energy shifts in the molecule. The dependence of the fine and hyperfine parameters of the Ã2Π1/2(0,0,0) and X̃2Σ+(0,0,0) states for all isotopologues of YbOH are discussed, and a comparison to isoelectronic YbF is made.
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Affiliation(s)
- Nickolas H Pilgram
- Division of Physics, Mathematics, and Astronomy, California Institute of Technology, Pasadena, California 91125, USA
| | - Arian Jadbabaie
- Division of Physics, Mathematics, and Astronomy, California Institute of Technology, Pasadena, California 91125, USA
| | - Yi Zeng
- Division of Physics, Mathematics, and Astronomy, California Institute of Technology, Pasadena, California 91125, USA
| | - Nicholas R Hutzler
- Division of Physics, Mathematics, and Astronomy, California Institute of Technology, Pasadena, California 91125, USA
| | - Timothy C Steimle
- School of Molecular Science, Arizona State University, Tempe, Arizona 85287, USA
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Butler PA, Gaffney LP, Spagnoletti P, Konki J, Scheck M, Smith JF, Abrahams K, Bowry M, Cederkäll J, Chupp T, de Angelis G, De Witte H, Garrett PE, Goldkuhle A, Henrich C, Illana A, Johnston K, Joss DT, Keatings JM, Kelly NA, Komorowska M, Kröll T, Lozano M, Nara Singh BS, O'Donnell D, Ojala J, Page RD, Pedersen LG, Raison C, Reiter P, Rodriguez JA, Rosiak D, Rothe S, Shneidman TM, Siebeck B, Seidlitz M, Sinclair J, Stryjczyk M, Van Duppen P, Vinals S, Virtanen V, Warr N, Wrzosek-Lipska K, Zielinska M. The observation of vibrating pear-shapes in radon nuclei. Nat Commun 2019; 10:2473. [PMID: 31171788 PMCID: PMC6554308 DOI: 10.1038/s41467-019-10494-5] [Citation(s) in RCA: 18] [Impact Index Per Article: 3.6] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 02/25/2019] [Accepted: 05/15/2019] [Indexed: 11/09/2022] Open
Abstract
There is a large body of evidence that atomic nuclei can undergo octupole distortion and assume the shape of a pear. This phenomenon is important for measurements of electric-dipole moments of atoms, which would indicate CP violation and hence probe physics beyond the Standard Model of particle physics. Isotopes of both radon and radium have been identified as candidates for such measurements. Here, we observed the low-lying quantum states in 224Rn and 226Rn by accelerating beams of these radioactive nuclei. We show that radon isotopes undergo octupole vibrations but do not possess static pear-shapes in their ground states. We conclude that radon atoms provide less favourable conditions for the enhancement of a measurable atomic electric-dipole moment.
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Affiliation(s)
- P A Butler
- Oliver Lodge Laboratory, University of Liverpool, Liverpool, L69 7ZE, UK.
| | - L P Gaffney
- Oliver Lodge Laboratory, University of Liverpool, Liverpool, L69 7ZE, UK.,CERN, Geneva 23, CH-1211, Switzerland
| | - P Spagnoletti
- School of Computing, Engineering and Physical Sciences, University of the West of Scotland, Paisley, PA1 2BE, UK
| | - J Konki
- CERN, Geneva 23, CH-1211, Switzerland
| | - M Scheck
- School of Computing, Engineering and Physical Sciences, University of the West of Scotland, Paisley, PA1 2BE, UK
| | - J F Smith
- School of Computing, Engineering and Physical Sciences, University of the West of Scotland, Paisley, PA1 2BE, UK
| | - K Abrahams
- Department of Physics & Astronomy, University of the Western Cape, Private Bag X17, Bellville, 7535, South Africa
| | - M Bowry
- TRIUMF, Vancouver, V6T 2A3, BC, Canada
| | - J Cederkäll
- Physics Department, Lund University, Box 118, Lund, SE-221 00, Sweden
| | - T Chupp
- Department of Physics, University of Michigan, Ann Arbor, 48104, MI, USA
| | - G de Angelis
- INFN Laboratori Nazionali di Legnaro, Legnaro, 35020, PD, Italy
| | - H De Witte
- Instituut voor Kern- en Stralingsfysica, KU Leuven, Leuven, B-3001, Belgium
| | - P E Garrett
- Department of Physics, University of Guelph, Guelph, N1G 2W1, Ontario, Canada
| | - A Goldkuhle
- Institute for Nuclear Physics, University of Cologne, Cologne, 50937, Germany
| | - C Henrich
- Institut für Kernphysik, Technische Universität Darmstadt, Darmstadt, 64289, Germany
| | - A Illana
- INFN Laboratori Nazionali di Legnaro, Legnaro, 35020, PD, Italy
| | | | - D T Joss
- Oliver Lodge Laboratory, University of Liverpool, Liverpool, L69 7ZE, UK
| | - J M Keatings
- School of Computing, Engineering and Physical Sciences, University of the West of Scotland, Paisley, PA1 2BE, UK
| | - N A Kelly
- School of Computing, Engineering and Physical Sciences, University of the West of Scotland, Paisley, PA1 2BE, UK
| | - M Komorowska
- Heavy Ion Laboratory, University of Warsaw, Warsaw, PL-02-093, Poland
| | - T Kröll
- Institut für Kernphysik, Technische Universität Darmstadt, Darmstadt, 64289, Germany
| | - M Lozano
- CERN, Geneva 23, CH-1211, Switzerland
| | - B S Nara Singh
- School of Computing, Engineering and Physical Sciences, University of the West of Scotland, Paisley, PA1 2BE, UK
| | - D O'Donnell
- School of Computing, Engineering and Physical Sciences, University of the West of Scotland, Paisley, PA1 2BE, UK
| | - J Ojala
- Department of Physics, University of Jyvaskyla, P.O. Box 35, Jyvaskyla, FIN-40014, Finland.,Helsinki Institute of Physics, P.O. Box 64, Helsinki, FIN-00014, Finland
| | - R D Page
- Oliver Lodge Laboratory, University of Liverpool, Liverpool, L69 7ZE, UK
| | - L G Pedersen
- Department of Physics, University of Oslo, P.O. Box 1048, Oslo, N-0316, Norway
| | - C Raison
- Department of Physics, University of York, York, YO10 5DD, UK
| | - P Reiter
- Institute for Nuclear Physics, University of Cologne, Cologne, 50937, Germany
| | | | - D Rosiak
- Institute for Nuclear Physics, University of Cologne, Cologne, 50937, Germany
| | - S Rothe
- CERN, Geneva 23, CH-1211, Switzerland
| | | | - B Siebeck
- Institute for Nuclear Physics, University of Cologne, Cologne, 50937, Germany
| | - M Seidlitz
- Institute for Nuclear Physics, University of Cologne, Cologne, 50937, Germany
| | - J Sinclair
- School of Computing, Engineering and Physical Sciences, University of the West of Scotland, Paisley, PA1 2BE, UK
| | - M Stryjczyk
- Instituut voor Kern- en Stralingsfysica, KU Leuven, Leuven, B-3001, Belgium
| | - P Van Duppen
- Instituut voor Kern- en Stralingsfysica, KU Leuven, Leuven, B-3001, Belgium
| | - S Vinals
- Consejo Superior De Investigaciones Científicas, Madrid, S 28040, Spain
| | - V Virtanen
- Department of Physics, University of Jyvaskyla, P.O. Box 35, Jyvaskyla, FIN-40014, Finland.,Helsinki Institute of Physics, P.O. Box 64, Helsinki, FIN-00014, Finland
| | - N Warr
- Institute for Nuclear Physics, University of Cologne, Cologne, 50937, Germany
| | - K Wrzosek-Lipska
- Heavy Ion Laboratory, University of Warsaw, Warsaw, PL-02-093, Poland
| | - M Zielinska
- IRFU CEA, Université Paris-Saclay, Gif-sur-Yvette, F-91191, France
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5
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Butler P, Gaffney L, Spagnoletti P, Konki J, Scheck M, Smith J, Abrahams K, Bowry M, Cederkäll J, Chupp T, de Angelis G, De Witte H, Garrett P, Goldkuhle A, Henrich C, Illana A, Johnston K, Joss D, Keatings J, Kelly N, Komorowska M, Kröll T, Lozano M, Nara Singh B, O'Donnell D, Ojala J, Page R, Pedersen L, Raison C, Reiter P, Rodriguez JA, Rosiak D, Rothe S, Shneidman T, Siebeck B, Seidlitz M, Sinclair J, Stryjczyk M, Van Duppen P, Vinals S, Virtanen V, Warr N, Wrzosek-Lipska K, Zielinska M. Coulomb excitation of pear-shaped nuclei. EPJ Web Conf 2019. [DOI: 10.1051/epjconf/201922301007] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/14/2022] Open
Abstract
There is a large body of evidence that atomic nuclei can undergo octupole distortion and assume the shape of a pear. This phenomenon is important for measurements of electric-dipole moments of atoms, which would indicate CP violation and hence probe physics beyond the Standard Model of particle physics. Isotopes of both radon and radium have been identified as candidates for such measurements. Here, we have observed the low-lying quantum states in 224Rn and 226Rn by accelerating beams of these radioactive nuclei. We show that radon isotopes undergo octupole vibrations but do not possess static pear-shapes in their ground states. We conclude that radon atoms provide less favourable conditions for the enhancement of a measurable atomic electric-dipole moment.
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Skripnikov LV, Petrov AN, Titov AV, Flambaum VV. CP-violating effect of the Th nuclear magnetic quadrupole moment: accurate many-body study of ThO. Phys Rev Lett 2014; 113:263006. [PMID: 25615324 DOI: 10.1103/physrevlett.113.263006] [Citation(s) in RCA: 9] [Impact Index Per Article: 0.9] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 08/22/2014] [Indexed: 06/04/2023]
Abstract
Investigations of CP violation in the hadron sector may be done using measurements in the ThO molecule. Recent measurements in this molecule improved the limit on the electron electric dipole moment (EDM) by an order of magnitude. Another time-reversal (T) and parity (P)-violating effect in 229ThO is induced by the nuclear magnetic quadrupole moment. We perform nuclear and molecular calculations to express this effect in terms of the strength constants of T, P-odd nuclear forces, neutron EDM, QCD vacuum angle θ, quark EDM, and chromo-EDM.
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Affiliation(s)
- L V Skripnikov
- B.P. Konstantinov Petersburg Nuclear Physics Institute, Gatchina, Leningrad District 188300, Russia and Department of Physics, Saint Petersburg State University, Saint Petersburg, Petrodvoretz 198504, Russia
| | - A N Petrov
- B.P. Konstantinov Petersburg Nuclear Physics Institute, Gatchina, Leningrad District 188300, Russia and Department of Physics, Saint Petersburg State University, Saint Petersburg, Petrodvoretz 198504, Russia
| | - A V Titov
- B.P. Konstantinov Petersburg Nuclear Physics Institute, Gatchina, Leningrad District 188300, Russia and Department of Physics, Saint Petersburg State University, Saint Petersburg, Petrodvoretz 198504, Russia
| | - V V Flambaum
- School of Physics, The University of New South Wales, Sydney, New South Wales 2052, Australia
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7
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Flambaum VV, DeMille D, Kozlov MG. Time-reversal symmetry violation in molecules induced by nuclear magnetic quadrupole moments. Phys Rev Lett 2014; 113:103003. [PMID: 25238355 DOI: 10.1103/physrevlett.113.103003] [Citation(s) in RCA: 17] [Impact Index Per Article: 1.7] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/25/2014] [Indexed: 06/03/2023]
Abstract
Recent measurements in paramagnetic molecules improved the limit on the electron electric dipole moment (EDM) by an order of magnitude. Time-reversal (T) and parity (P) symmetry violation in molecules may also come from their nuclei. We point out that nuclear T, P-odd effects are amplified in paramagnetic molecules containing deformed nuclei, where the primary effects arise from the T, P-odd nuclear magnetic quadrupole moment (MQM). We perform calculations of T, P-odd effects in the molecules TaN, ThO, ThF+, HfF+, YbF, HgF, and BaF induced by MQMs. We compare our results with those for the diamagnetic TlF molecule, where the T, P-odd effects are produced by the nuclear Schiff moment. We argue that measurements in molecules with MQMs may provide improved limits on the strength of T, P-odd nuclear forces, on the proton, neutron, and quark EDMs, on quark chromo-EDMs, and on the QCD θ term and CP-violating quark interactions.
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Affiliation(s)
- V V Flambaum
- School of Physics, The University of New South Wales, Sydney, New South Wales 2052, Australia
| | - D DeMille
- Department of Physics, Post Office Box 208120, Yale University, New Haven, Connecticut 06520, USA
| | - M G Kozlov
- Petersburg Nuclear Physics Institute, Gatchina 188300, Russia and St. Petersburg Electrotechnical University "LETI," Professor Popov Street 5, St. Petersburg 197376, Russia
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