𝔖 Bobbio Scriptorium

✦ LIBER ✦

Wavelengths for n = 4—5 transitions in Cu-like Ta, Au, Pb, and Bi

✍ Scribed by Brown, C. M.; Seely, J. F.; Feldman, U.; Hulburt, E. O.; Cobble, J. A.; Goldstone, P. D.

Book ID: 115393245
Publisher: Optical Society of America
Year: 1989
Tongue: English
Weight: 382 KB
Volume: 6
Category: Article
ISSN: 0740-3224
DOI: 10.1364/JOSAB.6.001433

No coin nor oath required. For personal study only.

📜 SIMILAR VOLUMES

Wavelengths, transition probabilities, a

Wavelengths, transition probabilities, and oscillator strengths for M-shell transitions in Co-, Ni-, Cu-, Zn-, Ga-, Ge-, and Se-like Au ions

✍ Xu, Min; Jiang, Gang; Deng, Banglin; Bian, Guojie 📂 Article 📅 2014 🏛 Elsevier Science 🌐 English ⚖ 482 KB

Paramagnetic resonance of Cu2+ defects i

Paramagnetic resonance of Cu2+ defects in mixed n = 2 and n = 3 phase Bi1.5Pb0.5Sr2Can−1CunO2n+4 superconductor

✍ F.J. Owens; Z. Iqbal; A.A. Zakhidov; I.I. Khairullin 📂 Article 📅 1991 🏛 Elsevier Science 🌐 English ⚖ 722 KB

Debye-Waller factors and magnetism down

Debye-Waller factors and magnetism down to 1.00 K for the high-spin (5T2) ⇌ low-spin (1A1) transition in Bis[2-(2-pyridylamino) -4-(2-pyridyl)thiazolato]iron(II) : E. König, G. Ritter, W. Irler, H.A. Goodwin, Institut fur Physikalische Chemie and Physikalishes Institut, University of Erlangen-Nürnberg, D-8520 Erlangen, W. Germany; and B. Kanellakopulos, Heisse Chemie, Kernforschungszentrum Karlsruhe, D-7500 Karlsruhe, W. Germany

✍ E. König; G. Ritter; W. Irler; H.A. Goodwin; B. Kanellakopulos 📂 Article 📅 1978 🏛 Elsevier Science 🌐 English ⚖ 114 KB

Computational design of benzothiazole-de

Computational design of benzothiazole-derived push?pull dyes with high molecular quadratic hyperpolarizabilitiesElectronic supplementary information (ESI) available: Table S1: Heats of formation and relevant torsional angles (AM1) and ZINDO (gas phase and dioxane solution) dipole moments and ?vec-values for different conformations of compounds 1?51. Table S2: B3LYP/6-31G* energies, zero point energy corrections (au), torsional angles, DRRPA-HF/6-31G* and ZINDO (gas phase) hyperpolarizabilities for different conformations. Table S3: Contributions (two-state model, other configurations) to ZINDO gas phase hyperpolarizabilities (B3LYP/6-31G* lowest energy conformation). Table S4: Orbital energies and coefficients (2pz, 3pz) of the two highest occupied and two lowest virtual orbitals of pertinent model compounds. Table S5: Main configurations (gas phase, ZINDO, B3LYP/6-31G* geometry), wavenumbers ?, oscillator strengths f, and difference ?� of dipole moment for the first two electronic transitions (states). Table S6: Main configurations (gas phase, TDDFT/B3LYP/6-31G*//B3LYP/6-31G*), wavenumbers ? and oscillator strengths f for the first few electronic transitions (states) of compounds 1?4, 16, 42 and 48?50. Table S7: ZINDO SOS results (wavelength ?max of first absorption band (f > 0.1), dipole moment �, and ?vec-values for compounds 1?51 in the gas phase. See http://www.rsc.org/suppdata/cp/b3/b314150k/

✍ Hrobarik, Peter; Zahradnik, Pavol; Fabian, Walter M. F. 📂 Article 📅 2004 🏛 Royal Society of Chemistry 🌐 English ⚖ 410 KB