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, 2020
The emission spectrum of the platinum(II) bipyridine complex [Pt(CN)2(bpy)] (bpy = 2,2′-bipyridine) interestingly exhibits blue shift and peak broadening in crystal as temperature increases from 15...
M. Nakagaki +3 more
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The emission spectrum of the platinum(II) bipyridine complex [Pt(CN)2(bpy)] (bpy = 2,2′-bipyridine) interestingly exhibits blue shift and peak broadening in crystal as temperature increases from 15...
M. Nakagaki +3 more
semanticscholar +1 more source
Photon emission spectrum of ion pumps
Review of Scientific Instruments, 2023As the sensitivity of gravitational-wave detectors increases, new sources of noise appear. A potential source of noise may arise from charge accumulating on the mirrors of the experiment, the origin of which can be related to UV photons from the surroundings.
Antonios Kontos, Rainer Weiss
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Emission spectrum of Cs2AgEuCl6
Journal of Alloys and Compounds, 1995Abstract The emission spectrum of Cs2AgEuCl6, which has the elpasolite structure, has been measured at 77 K in the wavelength range 460–700 nm. Transitions were found from 5D0, 5D1 and 5D2 to the 7F0, 7F1, 7F2, and 7F3 components of the ground state.
S.C. Kuo, L.C. Thompson, H.-D. Amberger
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Proceedings of the Indian Academy of Sciences - Section A, 1972
The bands of PrO at 8488.95 A and 7986.44 A of system I and at 7662.85 A of system III have been photographed on 6.6 meter concave grating spectrograph at a dispersion of 1.2 A/mm and their rotational structure analysed. They are assigned transitions fromv′ = 0 and 1 levels of A2 Δ5/2 andv′ = 0 level of B2 Δ5/2 to a commonv′’ = 0 level of the ground ...
T. V. Venkitachalam +2 more
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The bands of PrO at 8488.95 A and 7986.44 A of system I and at 7662.85 A of system III have been photographed on 6.6 meter concave grating spectrograph at a dispersion of 1.2 A/mm and their rotational structure analysed. They are assigned transitions fromv′ = 0 and 1 levels of A2 Δ5/2 andv′ = 0 level of B2 Δ5/2 to a commonv′’ = 0 level of the ground ...
T. V. Venkitachalam +2 more
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Advanced Optical Materials, 2020
Thermally activated delayed fluorescence (TADF) materials that are able to realize electroluminescence showing simultaneously narrow emission band, high color purity, and high efficiency are highly demanded for display applications. Up to now, a few blue
Yincai Xu +7 more
semanticscholar +1 more source
Thermally activated delayed fluorescence (TADF) materials that are able to realize electroluminescence showing simultaneously narrow emission band, high color purity, and high efficiency are highly demanded for display applications. Up to now, a few blue
Yincai Xu +7 more
semanticscholar +1 more source
Chemical Physics Letters, 1991
Abstract Laser excitation at 206–232 nm of a supersonic free jet of Cd(CH3)2 produced an emission due to one-photon absorption from vibrationally cold A CdCH3. The 0—0 line was at 444.1 nm and ground-state vibrational frequencies of 345 cm−1 (CdCH3 stretch) and 998 cm−1 (CH3 umbrella mode) were measured. Much stronger emissions caused by multiphoton
Abraham Penner +2 more
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Abstract Laser excitation at 206–232 nm of a supersonic free jet of Cd(CH3)2 produced an emission due to one-photon absorption from vibrationally cold A CdCH3. The 0—0 line was at 444.1 nm and ground-state vibrational frequencies of 345 cm−1 (CdCH3 stretch) and 998 cm−1 (CH3 umbrella mode) were measured. Much stronger emissions caused by multiphoton
Abraham Penner +2 more
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Chemical Physics Letters, 1969
Abstract The analysis of high resolution emission spectra of isotopic enriched 130Te2 gave the rotational constants suggesting the transition as a σ - σ type. Heat of dissociation of Te2 is evaluated from the computed dissociation limit in the excited state.
B.L. Jha, D. Ramachandra Rao
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Abstract The analysis of high resolution emission spectra of isotopic enriched 130Te2 gave the rotational constants suggesting the transition as a σ - σ type. Heat of dissociation of Te2 is evaluated from the computed dissociation limit in the excited state.
B.L. Jha, D. Ramachandra Rao
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Physical Review, 1964
The spectrum of ZnIn shows bands which can be analyzed into four systems. Two narrow systems at $\ensuremath{\lambda}4102$ and $\ensuremath{\lambda}4511$ appeared continuous. Systems at $\ensuremath{\lambda}5308$ ($B\ensuremath{-}A$) and $\ensuremath{\lambda}5625$ ($D\ensuremath{-}C$) were photographed with a dispersion of 5 \AA{}/mm.
C. Santaram, J. G. Winans
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The spectrum of ZnIn shows bands which can be analyzed into four systems. Two narrow systems at $\ensuremath{\lambda}4102$ and $\ensuremath{\lambda}4511$ appeared continuous. Systems at $\ensuremath{\lambda}5308$ ($B\ensuremath{-}A$) and $\ensuremath{\lambda}5625$ ($D\ensuremath{-}C$) were photographed with a dispersion of 5 \AA{}/mm.
C. Santaram, J. G. Winans
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Journal of Molecular Spectroscopy, 1973
Abstract Bands in the region 2100–2600 A observed in emission by passing silicon tetrafluoride through an electrodeless discharge have been investigated and assigned to SiF3 insteadd of SiF2.
J. Ling-Fai Wang +2 more
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Abstract Bands in the region 2100–2600 A observed in emission by passing silicon tetrafluoride through an electrodeless discharge have been investigated and assigned to SiF3 insteadd of SiF2.
J. Ling-Fai Wang +2 more
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