Weak satellite-framed languages

Author(s):  
Víctor Acedo-Matellán
Keyword(s):  
2021 ◽  
Vol 12 (1) ◽  
Author(s):  
Hailing Jia ◽  
Xiaoyan Ma ◽  
Fangqun Yu ◽  
Johannes Quaas

AbstractSatellite-based estimates of radiative forcing by aerosol–cloud interactions (RFaci) are consistently smaller than those from global models, hampering accurate projections of future climate change. Here we show that the discrepancy can be substantially reduced by correcting sampling biases induced by inherent limitations of satellite measurements, which tend to artificially discard the clouds with high cloud fraction. Those missed clouds exert a stronger cooling effect, and are more sensitive to aerosol perturbations. By accounting for the sampling biases, the magnitude of RFaci (from −0.38 to −0.59 W m−2) increases by 55 % globally (133 % over land and 33 % over ocean). Notably, the RFaci further increases to −1.09 W m−2 when switching total aerosol optical depth (AOD) to fine-mode AOD that is a better proxy for CCN than AOD. In contrast to previous weak satellite-based RFaci, the improved one substantially increases (especially over land), resolving a major difference with models.


1975 ◽  
Vol 68 ◽  
pp. 45-64 ◽  
Author(s):  
John H. Parkinson

The last few years have seen great progress in our understanding of X-ray spectra of solar active regions. This paper demonstrates both the usefulness and the limitations of the techniques, both scientific and instrumental, that have recently become available. Improvements in spectral resolution led to the discovery of weak satellite lines to helium-like ions; the quantitative theory for these lines is also discussed. The observed intensities of the Fe XVII lines are also investigated and found to be in agreement with calculations that allow for cascading processes.


1989 ◽  
Vol 156 ◽  
Author(s):  
B. C. Chakoumakos ◽  
J. D. Budai ◽  
B. C. Sales ◽  
Edward Sonder

ABSTRACTSingle crystals of Bi2Sr2−xCuO6−y, (0.1 < x < 0.5, 0 < y < 0.5), were examined using x-ray diffraction techniques. Ditfractometer scans of θ-2θ taken normal to the cleavage planes displayed the even () reflections from = 2 to 26. Weak satellite peaks were observed on either side of each main () reflection, and their intensities relative to the main peak increased as 2θ was increased. With decreasing Sr content, the satellite peaks systematically moved away from the position of the main reflection. In contrast, the positions of the satellite peaks did not change with oxygen content which was varied by up to 0.5 oxygen atoms per formula unit. Since Tc in these crystals is sensitive to oxygen content while the superstructure modulation is not, it is unlikely that superconductivity and the structure modulation are directly related. As shown by a more detailed study of these peaks using a four-circle diffractometer and x-ray precession methods, the satellites that appear in θ-2θ scans are actually the mosaic tails of relatively intense superstructure peaks, positioned off from c* in the b* direction of reciprocal space. Depending on the Sr content of the crystals, generally incommensurate modulations were found with the superstructure periodicity ranging between ˜1/5b* + 0.29c* and ˜1/5b* + 0.65c*. The modulation in Bi2Sr2−xCuO6−y has two components. The component along the b* direction is similar to the superstructure observed in Bi2Sr2CaCu2O7 crystals and thus is probably due to the mismatch between the Bi2O2 layer and the CuO2 layer. The additional component along c* may be due to the ordering of Sr vacancies.


2019 ◽  
Vol 632 ◽  
pp. A71 ◽  
Author(s):  
Tao Chen ◽  
Yi Luo ◽  
Aigen Li

Context. The 3.3 μm aromatic C–H stretching band of polycyclic aromatic hydrocarbon (PAH) molecules seen in a wide variety of astrophysical regions is often accompanied by a series of weak satellite bands at ∼3.4–3.6 μm. One of these sources, IRAS 21282+5050, a planetary nebula, also exhibits a weak band at ∼1.68 μm. While the satellite features at ∼3.4–3.6 μm are often attributed to the anharmonicities of PAHs, it is not clear whether overtones or combination bands dominate the 1.68 μm feature. Aims. In this work, we examine the anharmonic spectra of eight PAH molecules, including anthracene, tetracene, pentacene, phenanthrene, chrysene, benz[a]anthracene, pyrene, and perylene, to explore the origin of the infrared bands in the 1.6–1.7 μm wavelength region. Methods. Density functional theory (DFT) in combination with the vibrational second-order perturbation theory (VPT2) was used to compute the anharmonic spectra of PAHs. To simulate the vibrational excitation process of PAHs, the Wang–Landau random walk technique was employed. Results. All the dominant bands in the 1.6–1.7 μm wavelength range and in the 3.1–3.5 μm C–H stretching region are calculated and tabulated. It is demonstrated that combination bands dominate the 1.6–1.7 μm region, while overtones are rare and weak in this region. We also calculate the intensity ratios of the 3.1–3.5 μm C–H stretching features to the bands in the 1.6–1.7 μm region, I3.1 − 3.5/I1.6 − 1.7, for both ground and vibrationally excited states. On average, we obtain ⟨I3.1 − 3.5/I1.6 − 1.7⟩≈12.6 and ⟨I3.1 − 3.5/I1.6 − 1.7⟩≈17.6 for PAHs at ground states and at vibrationally excited states, respectively.


In continuation of work reported earlier (Kuhn & Series 1950), the weak satellite 2 P 1/2 –3 S 1/2 in the α-line 6561 Å of the Balmer series of heavy hydrogen has been resolved. The light was produced as before in a U-tube cooled by liquid hydrogen, and analyzed by a double Fabry-Perot interferometer with spacings in the ratio 1:2. The satellite was found to be at a distance 0·1326±0·001 cm. -1 from the neighbouring strong component 2 P /2 –3 D 1/2 , in disagreement with the distance 0·1409 cm. -1 predicted by the Dirac relativistic theory of the hydrogen atom. The difference 0-0083 + 0·002 –0·003 cm. ‒1 (where the limits also include possible errors in certain corrections) is interpreted as an upward shift of the 3 S term, and is compared with the value 0·0104 cm. –1 predicted by the radiation theory of Bethe and others (see, for example, Bethe, Brown & Stehn 1950).


1969 ◽  
Vol 47 (18) ◽  
pp. 3429-3434 ◽  
Author(s):  
David G. Cadena Jr. ◽  
Robert E. Linder ◽  
John R. Rowlands

Electron spin resonance measurements of single crystals of α-aminoisobutyric acid, which are both irradiated and measured at 77 °K, give rise to a strong central absorption line at the center of two weak "satellite" peaks. The species largely responsible for the intensity of the central absorption line has been discussed previously and is considered to be the doubly ionized radical anion. In this paper, evidence is presented which shows that some of the intensity of this central line is contributed by the species giving rise to the satellite lines. Furthermore, this evidence, which is based upon saturation studies, variable temperature measurements, deuteration studies, and complete neglect of differential overlap–self consistent field molecular orbital calculations, suggests that the species giving rise to the satellite spectra is a planar conformation of the radical (CH3)2CCO2H.


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