Short-Lived Radioactive Molecules
Precision measurements of molecular systems provide highly sensitive laboratories for exploring the possible violation of fundamental symmetries and search for new physics beyond the standard model physics [Barr14,Demi17,Safr18]. Radioactive molecules compound of heavy and deformed short-lived isotopes are predicted to offer unprecedented sensitivity to investigate parity and time reversal violation effects. However, the experimental knowledge of short-lived radioactive molecules is scarce, and quantum chemistry calculations has constituted the only source of spectroscopy information.
[Barr14] Barry, J. et al. Nature 512, 286 (2014).
[Demi17] DeMille et al. Science 357, 990 (2017).
[Safr18] Safronova et al. Rev Mod Phys 90, 025008 (2018).
RaX Collaboration
We are building a new experiment to laser cool radium-containing molecules, in collaboration with Harvard (Doyle group), Caltech (Hutzler group), and the Facility for Rare Isotope Beams (FRIB). Radium-containing molecules offer unparalleled opportunity to study some of the open questions in our understanding of the universe, such as the root cause of the observed matter/antimatter asymmetry, the long-sought search for CP violation in the strong interaction, and the potential existence of yet-undetected particles and forces [1]. The octuple deformation of radium nuclei [2] is predicted to amplify both parity (P) and time-reversal (T) violating nuclear properties by more than three orders of magnitude compared to stable molecules [3,4]. Recent results in the spectroscopy of radioactive molecules have demonstrated that radium-containing molecules, such as $^{225}$RaF and $^{225}$RaOH, additionally possess a relatively simple structure that is very favorable for laser cooling (see Fig. 1) [4-6]. This combination makes these molecules excellent quantum sensors for fundamental physics, opening the door to searches for P,T violating nuclear effects, such as the nuclear Schiff moment, manifesting as electric dipole moments (EDMs) of molecules [1].
The roadmap to ultra-sensitive measurements with radium-containing molecules begins with the less radioactive isotope $^{226}$Ra ($\tau_{1/2}=1600$~yr), simplifying the experimental apparatus and molecule structure, and enabling rapid prototyping at university laboratories. To demonstrate the first laser cooling and trapping of a radioactive molecule, we will work with the well-characterized diatomic molecule $^{226}$RaF, which has an ideal molecular structure for laser cooling [6]. Concurrently, we will also test optical cycling (the key property that enables laser cooling) in $^{226}$RaOH, where the polyatomic structure generically provides parity doublets, a powerful structural advantage for state-of-the-art precision measurements [7,8]. Fortunately, RaF and RaOH molecules have isoelectronic structure; hence sharing common production methods and similar optical transitions, accessible with common laser technologies. Many of the initial experimental breakthroughs in RaF can pave the way for advances with RaOH, and their similarity enables changing from RaF to RaOH in an experiment with the metaphorical ``flip of a switch''.
Initially, experimental prototyping will be performed in cold ($\sim$~K) molecular beams, an essential tool for measuring, cooling, and trapping molecules. This experiment will overcome challenges in producing and cooling $^{226}$Ra-containing molecules, establishing the path for future work to capture the molecular beam in a long-lived trap at ultracold temperatures ($<$~mK). This work will establish the experimental basis for eventual enhanced hadronic symmetry violation measurements with $^{225}$Ra ($\tau_{1/2}=14.9$~d) containing molecules at the Facility for Rare Isotope Beams (FRIB)
Figure: Laser cooling scheme for $^{226}$RaF, reproduced from [6]. The upwards-pointing arrows represent laser excitations, with the wavelength of each laser shown (energy levels not shown to scale). The wavy, downwards-pointing arrows represent spontaneous emission, labeled by the associated Franck-Condon factors. The vibrational and rotational quantum numbers as well as the parity are shown for the states of interest.
Do not hesitate to contact us if you are interested in this project.
[1] Arrowsmith et al. Prog. Phys. 87 084301 (2024).
[2] Gaffney et al. Nature 497, 199 (2013).
[3] Spevak et al. Phys. Rev. C 56, 1357 (1997).
[4] Garcia Ruiz et al. Nature 581, 396 (2020).
[5] Udrescu et al. Physical Review Letters 127 (3), 033001(2021).
[6] Udrescu et al. Nature Physics 20 (2), 202 (2024).
[7] Andreev et al. Nature 562, 355 (2018).