Absorption spectrum of the (2,1) band in the A2Пi–X2Σ+ system of CS+ cation

Enhancement-Mode LaLuO3–AlGaN/GaN Metal–Insulator–Semiconductor High-Electron-Mobility Transistors Using Fluorine Plasma Ion Implantation

“…For the ground state X 2 Σ + , the calculated values of ω e , ω e x e , and B e accord well with experimental data, each with an error of 5.883, 0.0195, and 0.0068 cm −1 , respectively; the difference between the latest experimental values [8] and our calculated ones of R e is about 0.0059Å. For A 2 Π and B 2 Σ + states, the calculated spectroscopic constants T e , ω e , ω e x e , B e , and R e are suitably consistent with the experimental results, [2,8,12] each with an error of 377.3 cm −1 , 1.173 cm −1 , 1.135 cm −1 , 0.0158 cm −1 , and 0.005Å, respectively. Compared with previously calculated results, [3,9,10] the differences between experimental values and our calculated ones of the spectroscopic parameters of X 2 Σ + , A 2 Π, and B 2 Σ + states are evidently small.…”

“…Horani and Vervloet [18] measured the electronic spectrum of the A 2 Π-X 2 Σ + transition for CS + by employing Fourier transform spectroscopy. The (1, 0) absorption band, [6] (5, 0) and (6, 0) absorption bands, [8] and (2, 1) absorption band [12] of the A 2 Π-X 2 Σ + transition for CS + were observed through velocity modulation detection. Bailleux et al [11] measured the submillimeter-wave spectrum of the ground state (X 2 Σ + ) of CS + by employing positive column discharge in a CS 2 -Ar mixture partially cooled by a limited flow of liquid nitrogen.…”

“…Carbon monosulfide (CS) and its ion (CS + ) are an important molecule and molecular ion in astronomy, and have received much attention in spectroscopy [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15] and astrophysics. [16][17][18] CS and CS + are usually formed in plasmas of sulfur and carbon using ultraviolet photolysis and the collisional dissociation of CS 2 .…”

Ab initioMRCI + Q study on potential energy curves and spectroscopic parameters of low-lying electronic states of CS+

“…For the ground state X 2 Σ + , the calculated values of ω e , ω e x e , and B e accord well with experimental data, each with an error of 5.883, 0.0195, and 0.0068 cm −1 , respectively; the difference between the latest experimental values [8] and our calculated ones of R e is about 0.0059 Å. For A 2 Π and B 2 Σ + states, the calculated spectroscopic constants T e , ω e , ω e x e , B e , and R e are suitably consistent with the experimental results, [2,8,12] each with an error of 377.3 cm −1 , 1.173 cm −1 , 1.135 cm −1 , 0.0158 cm −1 , and 0.005 Å, respectively. Compared with previously calculated results, [3,9,10] the differences between experimental values and our calculated ones of the spectroscopic parameters of X 2 Σ + , A 2 Π, and B 2 Σ + states are evidently small.…”

“…Carbon monosulfide (CS) and its ion (CS + ) are an important molecule and molecular ion in astronomy, and have received much attention in spectroscopy [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15] and astrophysics. [16][17][18] CS and CS + are usually formed in plasmas of sulfur and carbon using ultraviolet photolysis and the collisional dissociation of CS 2 .…”