2002
DOI: 10.1238/physica.regular.065a00083
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Stark Broadening of In II Spectral Lines

Abstract: Experimental data for antiferromagnetic nanoparticles are often analyzed as if the particles were ferromagnetic. However, due to the volume dependence of the magnetization resulting from uncompensated spins, such analysis will yield erroneous results. This is demonstrated as we analyze ac and dc magnetization data as well as Mössbauer spectra obtained for ferritin. The values of the median energy barrier obtained from the different data are in very close agreement when a distribution of volumes and a volume de… Show more

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Cited by 8 publications
(5 citation statements)
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“…In option 2, we adopted the oscillator strengths from Kurucz & Bell (1995) and the classical line broadening parameter while neglecting pressure shifts. Kurucz & Bell (1995) agreement although the pressure shifts calculated by Dimitrijević & Sahal-Bréchot (1992) are a factor of 3 smaller than measured (Srećković & Djeniže 1993). Because the measured Ca iiλ3933 shift is relatively small (see Vennes, Kawka, & Németh 2010a) it may not be measurable in our spectra and the lack of accuracy in these parameters would not affect the abundance and radial velocity analysis.…”
Section: Si IImentioning
confidence: 76%
See 1 more Smart Citation
“…In option 2, we adopted the oscillator strengths from Kurucz & Bell (1995) and the classical line broadening parameter while neglecting pressure shifts. Kurucz & Bell (1995) agreement although the pressure shifts calculated by Dimitrijević & Sahal-Bréchot (1992) are a factor of 3 smaller than measured (Srećković & Djeniže 1993). Because the measured Ca iiλ3933 shift is relatively small (see Vennes, Kawka, & Németh 2010a) it may not be measurable in our spectra and the lack of accuracy in these parameters would not affect the abundance and radial velocity analysis.…”
Section: Si IImentioning
confidence: 76%
“…As part of option 1, we adopt the theoretical broadening and shift parameters of Dimitrijević & Sahal‐Bréchot (1992), and in option 2, we adopt again the compilation of Kurucz & Bell (1995) without pressure shifts.…”
Section: Analysis and Discussionmentioning
confidence: 99%
“…The theory also predicts that the widths of the hydrogen series in the blue and in the Johnson U -band (λ ≈ 3200 Å−4000 Å) should be much larger than the widths of the nearby resonance lines of Ca II H and K, which are not broadened due to energy level splittings with a linear (hydrogenic) dependence on the perturbing field. The impact broadening of Ca II H and K by ambient electrons have been calculated by Griem (1974), Dimitrijević & Sahal-Bréchot (1992), and Dimitrijevic & Sahal-Brechot (1993). At the highest electron densities in the condensations, the Lorentzian FWHM values 12 are only 1 − 1.5 × 10 −3 Å.…”
Section: Comparisons Of Ca II K Hα Hβ and Hγmentioning
confidence: 98%
“…For example, we adopted log Γ = −7.562 for Ca iλ4226 and log Γ = −7.76 for Ca H&K at T = 10 000 K, and α = 0.238 for Ca iλ4226 and α = 0.223 for Ca H&K. Stark broadening widths for Ca i and Ca ii lines were obtained from Dimitrijević & Sahal-Bréchot (1999) and Dimitrijević & Sahal-Bréchot (1992), respectively. Additional parameters (Stark and collisions with hydrogen) were obtained from the compilation of Kurucz & Bell (1995).…”
Section: Heavy Element Line Profilesmentioning
confidence: 99%