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Physical Review A

Rotational-hyperfine cooling of TlF 205 in a cryogenic beam

Olivier Grasdijk, David DeMille, Jakob Kastelic, Steve Lamoreaux, Oskari Timgren, Konrad Wenz, Tanya Zelevinsky, D. Kawall

Published Jun 17, 2025• 1 citation
Publisher
DOI
10.1103/vb31-f2c3

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The aim of CeNTREX (Cold Molecule Nuclear Time-Reversal Experiment) is to search for time-reversal symmetry violation in the thallium nucleus, by measuring the Schiff moment of $^{205}$Tl in the polar molecule thallium fluoride (TlF). CeNTREX uses a cryogenic beam of TlF with a rotational temperature of 6.3(2) K. This results in population spread over dozens of rotational and hyperfine sublevels of TlF, while only a single level is useful for the Schiff moment measurement. Here we present a protocol for cooling the rotational and hyperfine degrees of freedom in the CeNTREX beam, transferring the majority of the Boltzmann distribution into a single rotational and hyperfine sublevel by using a single ultraviolet laser and a pair of microwave beams. We achieve a factor of $20.1(4)$ gain in the population of the $J=0$, $F=0$ hyperfine sublevel of the TlF ground state.

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We present a hyperfine-resolved state preparation scheme for thallium fluoride (TlF) molecules based on microwave-driven adiabatic passage (AP) in a spatially varying electric field. This method enables efficient and robust population transfer between selected $\left|J,m_J=0\right\rangle$ hyperfine sublevels of the $X\,^1Σ^+_0$ ground state in a cryogenic molecular beam, a key requirement for the CeNTREX search for nuclear time-reversal symmetry violation. Two sequential stages of AP are implemented. The first transfers population from $J=0$ to $J=1$ at a local field of $173~\mathrm{V/cm}$, and the second transfers from $J=1$ to $J=2$ at $110~\mathrm{V/cm}$. Transfer efficiencies are quantified through laser-induced fluorescence, and accounting for residual population in excited rotational levels after a prior stage of rotational cooling. We achieve state transfer efficiencies of $0.92(6)$ and $1.05(5)$ for the first and second states of AP, respectively. This corresponds to a total efficiency of $0.97(8)$ for population transfer from $J=0$ to $J=2$. These results demonstrate robust and high-fidelity preparation of specific rotational/hyperfine states in TlF.

arXiv:2511.16626•Nov 20, 2025•0 citations
Rotational-hyperfine cooling of 205^{205}205TlF in a cryogenic beam
The aim of CeNTREX (Cold Molecule Nuclear Time-Reversal Experiment) is to search for time-reversal symmetry violation in the thallium nucleus, by measuring the Schiff moment of 205^{205}205Tl in the polar molecule thallium fluoride (TlF). CeNTREX uses a cryogenic beam of TlF with a rotational temperature of 6.3(2) K. This results in population spread over dozens of rotational and hyperfine sublevels of TlF, while only a single level is useful for the Schiff moment measurement. Here we present a protocol for cooling the rotational and hyperfine degrees of freedom in the CeNTREX beam, transferring the majority of the Boltzmann distribution into a single rotational and hyperfine sublevel by using a single ultraviolet laser and a pair of microwave beams. We achieve a factor of 20.1(4)20.1(4)20.1(4) gain in the population of the J=0J=0J=0, F=0F=0F=0 hyperfine sublevel of the TlF ground state.
Adiabatic passage of 205^{205}205TlF with microwaves in a cryogenic beam
We present a hyperfine-resolved state preparation scheme for thallium fluoride (TlF) molecules based on microwave-driven adiabatic passage (AP) in a spatially varying electric field. This method enables efficient and robust population transfer between selected ∣J,mJ=0⟩\left|J,m_J=0\right\rangle∣J,mJ​=0⟩ hyperfine sublevels of the X 1Σ0+X\,^1Σ^+_0X1Σ0+​ ground state in a cryogenic molecular beam, a key requirement for the CeNTREX search for nuclear time-reversal symmetry violation. Two sequential stages of AP are implemented. The first transfers population from J=0J=0J=0 to J=1J=1J=1 at a local field of 173 V/cm173~\mathrm{V/cm}173 V/cm, and the second transfers from J=1J=1J=1 to J=2J=2J=2 at 110 V/cm110~\mathrm{V/cm}110 V/cm. Transfer efficiencies are quantified through laser-induced fluorescence, and accounting for residual population in excited rotational levels after a prior stage of rotational cooling. We achieve state transfer efficiencies of 0.92(6)0.92(6)0.92(6) and 1.05(5)1.05(5)1.05(5) for the first and second states of AP, respectively. This corresponds to a total efficiency of 0.97(8)0.97(8)0.97(8) for population transfer from J=0J=0J=0 to J=2J=2J=2. These results demonstrate robust and high-fidelity preparation of specific rotational/hyperfine states in TlF.