arXiv subjects

A. Pashov

Publications and source records attributed to A. Pashov.

9 recordsLinked to original sources

arXiv2025

The double minimum E(3)$^1\Sigma^{+}_{\mathrm{u}}$ state in Cs$_2$

The double minimum E$^1\Sigma^{+}_{\mathrm{u}}$ state in caesium dimer was investigated by analysing spectra of the E$^1\Sigma^{+}_{\mathrm{u}}$ $\leftarrow$ X$^1\Sigma^{+}_{\mathrm{g}}$ band system, simplified by polarisation labelling. A total of 6727 rotationally resolved transitions to levels situated in the inner well and above the internal barrier were identified and a potential energy curve allowing to reproduce their energies was constructed using the Fourier grid Hamiltonian and inverted perturbation approach methods. The unambiguousness of the potential curve in view of lack of data related to levels located in the outer well is discussed.

physics.atom-ph↗

arXiv2022

Intensities of KCs $E(4)^1Σ^+\to (a^3Σ^+,X^1Σ^+)$ band system up to dissociation threshold: an interplay between spin-orbit, hyperfine and rovibronic coupling effects

The relative intensity distribution in the rotationally resolved laser-induced fluorescence spectra belonging to the $E(4)^1Σ^+\to (a^3Σ^+_1,X^1Σ^+)$ band systems of the KCs molecule was analyzed. The experimental intensities in doublet $P$,$R$ progressions assigned to spin-allowed $E\to X$ and spin-forbidden $E\to a$ transitions up to their common ground dissociation limit were described in the framework of a coupled-channels (CC) deperturbation model applied for the interacting \Xstate\ and \astate\ states. The CC intensity simulation was based solely on fixed electronic structure parameters as functions of the internuclear distance $R$, namely: accurate empirical potential energy curves for all three states, \emph{ab initio} estimates for matrix elements $A(R)$ of the hyperfine structure (HFS) , and transition dipole moments $d_{EX}(R)$ and $d_{Ea}(R)$. A comparison between the measured intensities and their theoretical counterparts demonstrates a strong competition between different intramolecular interactions. A weak spin-orbit coupling of the upper \Estate\ state with the remote $^3Π$ states is responsible for appearance of the $E\to a$ vibrational bands for the intermediate $v_a$-values. In turn, the HFS coupling between \Xstate\ and \astate\ states leads to peculiarities in $E\to (X,a)$ intensities, which are pronounced for high $v_{X/a}$-values in the vicinity of K(4$^2S$)+Cs(6$^2S$) dissociation threshold. Both adiabatic ro-vibrational and non-adiabatic electronic-rotational interactions explain the abrupt deviation of some observed $P/R$ intensity ratios from the expected Hönl-London factors.

physics.atom-ph↗

arXiv2022

The $a^3\Sigma^+$ state of KCs revisited: hyperfine structure analysis and potential refinement

Laser-induced fluorescence spectra of the $c^3\Sigma^+(v_{c},J_{c}=N_{c})\rightarrow a^3\Sigma^+(v_{a},N_{a} = J_{c} \pm 1)$ transitions excited from the ground $X^1\Sigma^+$ state of $^{39}$K$^{133}$Cs molecule were recorded with Fourier-transform spectrometer IFS125-HR (Bruker) at the highest achievable spectral resolution of 0.0063 cm${}^{-1}$. Systematic study of the hyperfine structure (HFS) of the $a^3\Sigma^+$ state for levels with $v_{a} \in [0, 27]$ and $N_{a} \in [24, 90]$ shows that the splitting monotonically increases with $v_{a}$. The spectroscopic study was supported by ab initio calculations of the magnetic hyperfine interaction in $X^1\Sigma^+$ and $a^3\Sigma^+$ states. The discovered variation of the electronic matrix elements with the internuclear distance $R$ is in a good agreement with the observed $v_{a}$-dependencies of the HFS. Overall set of available experimental data on the $a^3\Sigma^+$ state was used to improve the potential energy curve particularly near a bottom, providing the refined dissociation energy $D_e$=267.21(1) cm${}^{-1}$. The ab initio HFS matrix elements, combined with the empirical $X^1\Sigma^+$ and $a^3\Sigma^+$ PECs in the framework of the invented coupled-channel deperturbation model, reproduce the experimental term values of both ground states within 0.003 cm${}^{-1}$ accuracy up to their common dissociation limit.

physics.atom-ph↗

arXiv2007

Spectroscopy of the a^3Σ_u^+ state and the coupling to the X^1Σ_g^+ state of K_2

We report on high resolution Fourier-transform spectroscopy of fluorescence to the a^3Σ_u^+ state excited by two-photon or two-step excitation from the X^1Σ_g^+ state to the 2^3Π_g state in the molecule K_2. These spectroscopic data are combined with recent results of Feshbach resonances and two-color photoassociation spectra for deriving the potential curves of X^1Σ_g^+ and a^3Σ_u^+ up to the asymptote. The precise relative position of the triplet levels with respect of the singlet levels was achieved by including the excitation energies from the X^1Σ_g^+ state to the 2^3Π_g state and down to the a^3Σ_u^+ state in the simultaneous fit of both potentials. The derived precise potential curves allow for reliable modeling of cold collisions of pairs of potassium atoms in their ^2S ground state.

physics.atom-ph↗

arXiv2007

The coupling of the X$^{1}Σ^{+}$ and a$^{3}Σ^{+}$ states of KRb

A comprehensive study of the electronic states at the 4s+5s asymptote in KRb is presented. Abundant spectroscopic data on the \astate state were collected by Fourier-transform spectroscopy which allow to determine an accurate experimental potential energy curve up to 14.8 Å. The existing data set (C. Amiot et al. J. Chem. Phys. 112, 7068 (2000)) on the ground state \Xstate was extended by several additional levels lying close to the atomic asymptote. In a coupled channels fitting routine complete molecular potentials for both electronic states were fitted. Along with the line frequencies of the molecular transitions, recently published positions of Feshbach resonances in $^{40}$K and $^{87}$Rb mixtures (F. Ferlaino et al. Phys. Rev. A 74, 039903 (2006)) were included in the fit. This makes the derived potential curves capable for an accurate description of observed cold collision features so far. Predictions of scattering lengths and Feshbach resonances in other isotopic combinations are reported.

physics.atom-ph↗

arXiv2005

Study of coupled states for the (4s^{2})^{1}S + (4s4p)^{3}P asymptote of Ca_{2}

The coupled states A^{1}Σ_{u}^{+} (^{1}D +}1}S), c^{3}Π_{u} (^{3}P + ^{1}S) and a^{3}Σ_{u}^{+} (^{3}P +}1}S) of the calcium dimer are investigated in a laser induced fluorescence experiment combined with high-resolution Fourier-transform spectroscopy. A global deperturbation analysis of the observed levels, considering a model, which is complete within the subspace of relevant neighboring states, is performed using the Fourier Grid Hamiltonian method. We determine the potential energy curve of the A^{1}Σ_{u}^{+} and c^{3}Π_{u} states and the strengths of the couplings between them. The c^{3}Π_{u} and \as states are of particular importance for the description of collisional processes between calcium atoms in the ground state ^{1}S_{0} and excited state ^{3}P_{1} applied in studies for establishing an optical frequency standard with Ca.

physics.atm-clus↗

arXiv2004

A regularized inverted perturbation approach method: potential energy curve of the $4^1Σ^+_u$ state in $Na_2$

We describe a modification of the inverted perturbation approach method allowing to construct physically sensible potential energy curves for electronic states of diatomic molecules even when some parts of the potential are not adequately characterized by the experimental data. The method is based on a simple regularization procedure, imposing an additional constraint on the constructed potential curve. In the present work it is applied to the double minimum 4$^1Σ^{+}_{\mathrm u}$ state of Na$_2$, observed experimentally by polarization labeling spectroscopy technique.

physics.atom-ph↗

arXiv2003

The potential of the ground state of NaRb

The X$^{1}Σ^{+}$ state of NaRb was studied by Fourier transform spectroscopy. An accurate potential energy curve was derived from more than 8800 transitions in isotopomers $^{23}$Na$^{85}$Rb and $^{23}$Na$^{87}$Rb. This potential reproduces the experimental observations within their uncertainties of 0.003 \rcm to 0.007 \rcm. The outer classical turning point of the last observed energy level ($v''=76$, $J''=27$) lies at $\approx 12.4$ Å, leading to a energy of 4.5 \rcm below the ground state asymptote.

physics.atom-ph↗

arXiv2002

Experimental study of the Ca2 1S+1S asymptote

The filtered laser excitation technique was applied for measuring transition frequencies of the Ca$_2$ B-X system from asymptotic levels of the X$^1Σ_{\mathrm g}^{+}$ ground state reaching $v''=38$. That level has an outer classical turning point of about 20~Åwhich is only 0.2 \rcm below the molecular $^1$S$+^1$S asymptote. Extensive analysis of the spectroscopic data, involving Monte Carlo simulation, allowed for a purely experimental determination of the long range parameters of the potential energy curve. The possible values of the s-wave scattering length could be limited to be between 250$a_0$ and 1000$a_0$.

physics.atom-ph↗