Search arXivSearch

arXiv · 2312.17005

Fourier-transform spectroscopy and global deperturbation treatment of the $A^1Σ^+_u$ and $b^3Π_u$ states of K$_2$ in the entire bound energy range

Abstract

Rotationally-resolved Fourier-transform spectra of laser-induced fluorescence (LIF) $A^1Σ^+_u\sim b^3Π_u \rightarrow X^1Σ^+_g$ of K$_2$ molecules were recorded and analyzed yielding 4053 term values of spin-orbit (SO) coupled $A \sim b$ complex of $^{39}$K$_2$ isotopologue with ca 0.01 cm$^{-1}$ accuracy. Their compilation with 1739 term values from previously published sources allowed to cover the energy range [9955, 17436] cm$^{-1}$ from the bottom of the lower-lying $b^3Π_u$ state up to the vicinity of the atomic asymptote $4s\;^2{\rm S}_{1/2}$ + $4p\;^2{\rm P}_{1/2}$, with rotational quantum number $J\in[0,149]$. The experimental data were processed by a direct 6$\times$6 coupled-channel (CC) deperturbation treatment, which accounted explicitly for both SO and electronic-rotational interactions between six states: $A^1Σ^+_u$($0$), $b^3Π_u$(0,1,2), $c^3Σ_u$(1), and $B^1Π_u$(1). The initial parameters of the global deperturbation model have been estimated in the framework of {\it ab initio} electronic structure calculations applying multi-referenced configuration-interaction and coupled-clusters methods. The interatomic potentials analytically defined for $A$ and $b$ states, as well as SO-splitting of the triplet $b$ state and $A\sim b$ SO-coupling functions have been refined to fit 5792 term values of the $^{39}$K$_2$ isotopologue, whereas the rest parameters were fixed on their {\it ab initio} values. The resulting mass-invariant parameters of the CC model reproduced the overall rovibronic term energies of the $A \sim b$ complex of $^{39}$K$_2$ with the accuracy, which is well within the experimental errors. This deperturbation analysis provided the refined dissociation energy $T_{dis}$=17474.569(5) cm$^{-1}$ and the long-range coefficient $C_3^Σ$ = 5.501(4) $\times10^5$cm$^{-1}$ A$^3$ relevant to the non-relativistic atomic limit $4s$+$4p$.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

I. Klincare, A. Lapins, M. Tamanis, R. Ferber, A. Zaitsevskii, E. A. Pazyuk, A. V. Stolyarov. 2023-12-28. Fourier-transform spectroscopy and global deperturbation treatment of the $A^1Σ^+_u$ and $b^3Π_u$ states of K$_2$ in the entire bound energy range. https://arxiv.org/abs/2312.17005

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Effective Conservation and Bistability of Atomic Alignment under Strong Spin~Exchange

We present a phenomenological model of anomalous alignment signals in dense cesium vapor under linearly polarized pumping and fast spin exchange near zero magnetic field. Despite the absence of a conservation law for rank-2 angular momentum, our recent experiments reveal anisotropic narrow resonances, hysteresis, and bistability. We attribute these effects to a stretched state forming a collective mode in which orientation and alignment are bidirectionally coupled. This mode acts as a reservoir, preserving the essential properties of alignment despite rapid spin exchange.

physics.atom-ph

$LS/LSJ$ Hybrid Coupling Framework for Auger Angular Distributions of Experimentally Unresolved Multiplets with Isolated Fine-Structure

We present a hybrid $LS/LSJ$ coupling framework for treating state multiplets in the regime $ΔE_\text{int}\sim\hbar/τ_\text{int} \ggΔE_\text{FS}\ggΓ$, where $τ_\text{int}$ is the collision interaction time, $ΔE_\text{FS}$ the fine-structure splitting, and $Γ$ the natural width. In this regime, the collision interaction is fast compared with fine-structure evolution, whereas the individual $J$ levels are well isolated on the scale of their natural widths. The produced multiplet's alignment is therefore described in $LS$ coupling and then projected onto the individual fine-structure $J$ levels before their subsequent decay, described by $LSJ$ coupling. Applied to the multi-open-shell $1s2s2p\,^4\!P_J$ manifold, which closely satisfies these conditions, the hybrid treatment reveals strong suppression and inversion of the Auger angular-distribution anisotropy relative to the traditional pure-$LS$ treatment. It substantially improves agreement with absolute experimental data while using the same $LS$ production cross sections. This hybrid $LS/LSJ$ framework thus provides the appropriate treatment of state multiplets with isolated fine-structure levels, as it retains the $J$-dependent decay dynamics missing from the traditional pure-$LS$ treatment.

physics.atom-ph

Optical Ion Clock with Engineered Immunity to Motion-Induced Frequency Shifts

Spectroscopic frequency shifts due to residual motion of the probed atoms significantly contribute to the uncertainty budgets of state-of-the-art optical ion clocks. For clock transitions with second-order Doppler and quadratic Stark shifts of opposite signs, it is possible to configure electrodynamic ion confinement such that these two shift effects become anticorrelated causing zero net shift. Here, we introduce a spectroscopic interrogation protocol which leads, for systems with unknown and varying motional energy gain rates, to first-order auto-suppression of corresponding frequency shifts without requiring the opposite-sign configuration. We experimentally demonstrate the proposed method on a new ytterbium ion optical clock probing the 467 nm electric octupole (E3) transition, where the combined fractional uncertainty contribution from motion-induced frequency shifts is reduced from $1.3\times10^{-18}$ to $0.3\times10^{-18}$. An interleaved optical frequency ratio measurement against ytterbium's electric quadrupole transition (E2) at 435 nm delivers an E3/E2 frequency ratio of $0.932 \,829 \,404 \,530 \,965 \, 340 (39)$. Combined with previously published ratio data this leads to a limit for a potential fractional temporal variation of the fine-structure constant of $2.4 (2.7) \times 10^{-19}/$yr, in agreement with existing bounds.

physics.atom-ph