研究目的
Investigating the RbSr 2S+ ground state via spectroscopy of hot and ultracold molecules to fit a potential energy curve bridging short-to-long-range domains and benchmark ab initio calculations.
研究成果
The combined spectroscopic approach successfully bridges a significant energy gap in the RbSr ground state PEC, providing high-precision models consistent with experimental data. The fitted PECs enable accurate predictions of molecular properties and Fano-Feshbach resonances, supporting future applications in quantum simulation and controlled chemistry.
研究不足
Thermoluminescence spectra lack rotational resolution, limiting precision to 0.16 cm?1. Equilibrium distances must be taken from theoretical calculations. The method cannot fully characterize hyperfine and spin-rotation couplings without additional experiments.
1:Experimental Design and Method Selection:
Two-colour photoassociation spectroscopy for ultracold molecules (mK temperatures) and thermoluminescence/laser-induced fluorescence spectroscopy for hot molecules (1000 K). Theoretical models include Morse/Long-Range functions and Dunham coefficients for potential energy curves.
2:Sample Selection and Data Sources:
Ultracold mixtures of Rb and Sr isotopes (e.g., 87Rb84Sr, 87Rb87Sr, 87Rb88Sr) prepared in crossed-beam dipole traps. Hot molecules from a heat-pipe oven with Rb and Sr gas mixture.
3:List of Experimental Equipment and Materials:
Crossed-beam dipole trap (1064 nm and 1070 nm lasers), photoassociation lasers (LFB and LBB), Fourier Transform Spectrometer (Bruker Vertex V80), external-cavity diode laser, heat-pipe oven, helium buffer gas.
4:Experimental Procedures and Operational Workflow:
For ultracold samples, perform two-colour photoassociation with magnetic field control; record atom loss and fluorescence. For hot samples, record thermoluminescence and LIF spectra; compare with simulated spectra from ab initio PECs.
5:Data Analysis Methods:
Fit binding energies using semi-classical and MLR models; extract dispersion coefficients (C6, C8); use reduced chi-square for goodness of fit; simulate spectra with Gaussian profiles.
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