Nuclear laser spectroscopy at the 10−12 precision level (Nature 633.8028 (2024): 63–70) determined the fractional change in the nuclear quadrupole
moment of 229Th upon excitation, ΔQ0/Q0 = 1.791(2)%. Such high-accuracy nuclear parameters enable stringent tests and refinement of 229Th nuclear
models. Using a semi-classical prolate-spheroid model, we quantify the transition frequency’s sensitivity to fine-structure constant variations as
K = 5900(2300), with uncertainty dominated by the measured charge-radius change Δ〈r2〉. This supports the predicted higher α-sensitivity of nuclear clocks
over atomic clocks, important for new-physics searches.We find ΔQ0 strongly dependent on nuclear volume, challenging the constant-volume approximation. The deviation between measured and predicted ΔQ0/Q0 underlines the need for improved modeling and measurement of additional nuclear parameters. We explicitly assess the octupole contribution to α-sensitivity.
Nuclear laser spectroscopy at the 10−12 precision level (Nature 633.8028 (2024): 63–70) determined the fractional change in the nuclear quadrupole
moment of 229Th upon excitation, ΔQ0/Q0 = 1.791(2)%. Such high-accuracy nuclear parameters enable stringent tests and refinement of 229Th nuclear
models. Using a semi-classical prolate-spheroid model, we quantify the transition frequency’s sensitivity to fine-structure constant variations as
K = 5900(2300), with uncertainty dominated by the measured charge-radius change Δ〈r2〉. This supports the predicted higher α-sensitivity of nuclear clocks
over atomic clocks, important for new-physics searches.We find ΔQ0 strongly dependent on nuclear volume, challenging the constant-volume approximation. The deviation between measured and predicted ΔQ0/Q0 underlines the need for improved modeling and measurement of additional nuclear parameters. We explicitly assess the octupole contribution to α-sensitivity.