STUDY OF EXCITED VIBRATIONAL LEVELS OF THE $Na_{2} A^{1}\Sigma^{+}_{u}$ STATE USING MODULATED GAIN
Gunjit K. Chawla, H. J. Vedder, Robert W. Field, Roger Bacis, Serge Churassy
Abstract
Gunjit K. Chawla, H. J. Vedder, Robert W. Field, Roger Bacis, Serge Churassy
Abstract
Highly excited vibrational levels of the $Na_{2} A^{1}\\Sigma^{+}_{u}$ state are observed from $v=62$ to $v=131$. The highest level of excitation corresponds to a binding energy of 0.65\\% of the potential well depth, a classical outer turning point $R_{+}\\sim 19.1{AA}$ in contrast with $R_{+}(v=0)\\sim 3.8{\\AA}$, and a vibrational frequency of $\\omega \\sim 4.6 cm^{-1}$ in contrast with $\\omega_{e} \\sim 117 cm^{-1}$ These excited levels have poor Franck-Condon factors with thermally populated levels of the ground $X^{1}\\Sigma^{+}_{g}$ electronic state. Therefore, modulated gain spectroscopy (MGS) is based upon a triple resonance excitation scheme where $Na_{2}$ is used as a gain medium in an optically-pumped-laser (OPL) to transfer thermal population, state-selectively, to high v of the ground state. Transitions from these high v levels of the X-state to high v levels of the A-state have good vibrational overlaps and are excited with a third laser. These absorption resonances are monitored by detecting increases in the saturated gain of the OPL. The three cw lasers are each independently frequency stabilized, resulting in a frequency accuracy of $\\pm 0.005 cm^{-1}$. A ``long range'' analysis of the vibrational and rotational levels determines the Van der Waals coefficients $C_{3}, C_{6}$, and $C_{8}$. These reflect the atomic properties of $Na (3^{2}S_{1/2})$ and $Na(3^{2}P_{3/2})$ states into which the A-state dissociates, such as the transition dipole moments, dipole polarizabilities, and quadrupole polarizabilities. From the $C_{n}$-values, we have determined the most accurate value to date of the oscillator strength for the $Na ({^{2}}S\\rightarrow {^{2}}P)$ D lines as well as the dipole polarizability of the $Na({^{2}}P)$ state.
A significance statement is not available in the OpenAlex record.
A contribution statement is not available in the OpenAlex record.
Method details are not available in the OpenAlex metadata.
Findings are not separately available in the OpenAlex metadata.
Limitations are not available in the OpenAlex metadata.
Application details are not available in the OpenAlex metadata.
Highly excited vibrational levels of the $Na_{2} A^{1}\\Sigma^{+}_{u}$ state are observed from $v=62$ to $v=131$. The highest level of excitation corresponds to a binding energy of 0.65\\% of the potential well depth, a classical outer turning point $R_{+}\\sim 19.1{AA}$ in contrast with $R_{+}(v=0)\\sim 3.8{\\AA}$, and a vibrational frequency of $\\omega \\sim 4.6 cm^{-1}$ in contrast with $\\omega_{e} \\sim 117 cm^{-1}$ These excited levels have poor Franck-Condon factors with thermally populated levels of the ground $X^{1}\\Sigma^{+}_{g}$ electronic state. Therefore, modulated gain spectroscopy (MGS) is based upon a triple resonance excitation scheme where $Na_{2}$ is used as a gain medium in an optically-pumped-laser (OPL) to transfer thermal population, state-selectively, to high v of the ground state. Transitions from these high v levels of the X-state to high v levels of the A-state have good vibrational overlaps and are excited with a third laser. These absorption resonances are monitored by detecting increases in the saturated gain of the OPL. The three cw lasers are each independently frequency stabilized, resulting in a frequency accuracy of $\\pm 0.005 cm^{-1}$. A ``long range'' analysis of the vibrational and rotational levels determines the Van der Waals coefficients $C_{3}, C_{6}$, and $C_{8}$. These reflect the atomic properties of $Na (3^{2}S_{1/2})$ and $Na(3^{2}P_{3/2})$ states into which the A-state dissociates, such as the transition dipole moments, dipole polarizabilities, and quadrupole polarizabilities. From the $C_{n}$-values, we have determined the most accurate value to date of the oscillator strength for the $Na ({^{2}}S\\rightarrow {^{2}}P)$ D lines as well as the dipole polarizability of the $Na({^{2}}P)$ state.
Key concepts: Sigma, Excited state, State (computer science), Physics, Chemistry, Atomic physics, Computer science, Algorithm