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  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Physics and chemistry of minerals 18 (1991), S. 117-125 
    ISSN: 1432-2021
    Source: Springer Online Journal Archives 1860-2000
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Abstract Twelve eudialyte specimens from the Khibini alkaline complex (Kola peninsula, USSR) have been studied by optical and Mössbauer spectroscopy methods. It has been found that in optically positive eudialytes Fe is mainly represented by Fe2+ ions in a rare planar four-fold coordination (Mössbauer hyperfine parameters — isomer shift IS=1.08 mm/s and quadrupole splitting QS=0.34 mm/s). It is these ions, not Mn3+ as it was assumed before, that are responsible for the crimson-red colour of eudialyte. In the optically negative red-brown and yellow-brown eudialytes (eucolites) Fe2+ ions are contained also in a tetragonal pyramid based on the above planar quadrangle (IS=1.33 mm/s and QS=2.24 mm/s). Major attention has been paid to an explanation of the colour and crystal-chemical features of optically positive in comparison with optically negative varieties of eudialytes.
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  • 2
    ISSN: 1432-2021
    Source: Springer Online Journal Archives 1860-2000
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Abstract The special properties of spin-allowed transitions of Fe2+, exchanged-coupled in pairs with Fe3+, (ECP-effect) are studied in single crystals of vivianite, phlogopite, biotite, elbaite and schörl under changing temperature and pressure in the ranges 79≤T[K]≤597 and 10-4≤P[GPa]≤8. The two Fe2+ dd-transitions, known to be subject to ECP-effects, occur at 11000 to 14000 (II) and 8400 to 9150 cm-1 (III), depending on the structural matrix. With pressure, band energies shift to higher values, while temperature has the opposite effect. Δv is nearly the same in all cases, decrease on temperature, and increase with pressure. Δα/ΔT or Δα/ΔP have similar values for bands II and III in all minerals studied. These observations are interpreted in terms of geometrical and vibrational changes of the octahedra, involved in the pair effects, on changing P and T. They clearly separate the ECP-bands from ordinary dd-transitions and also from IVCT-bands. A unique pressure effect in the spectral range of 17000 to 26000 cm-1 was found in schörl: a band system that immensly gains intensity on pressure. Two explanations are suggested: (a) traces of Ti3+, exchange-coupled to Fe2+ show the above pressure effect typical of ECP, (b) there occurs pressureinduced reduction of Ti4+ in Y-positions, induced by Fe2+ in connected Y-octahedra, whereby OH in trans-configuration of Y-octahedra promote this process.
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  • 3
    Electronic Resource
    Electronic Resource
    Springer
    Physics and chemistry of minerals 21 (1994), S. 360-372 
    ISSN: 1432-2021
    Source: Springer Online Journal Archives 1860-2000
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Abstract The effect of raising temperature on spin-allowed dd-transitions of octahedral Cr3+ was studied for various point symmetries of the Cr3+-bearing structural sites, i.e. 3 m and 3 with inversion center in spinel and garnets, respectively, or 32, 3, 2 and 1, lacking the inversion centre, in beryl, corundum, diopside and topaz, respectively. For this purpose, crystals of Cr3+-bearing spinel, pyrope, andradite, grossular, uvarovite, emerald, ruby, diopside and topaz were analyzed by microprobe, oriented, and measured in polarized radiation (except for the cubic minerals) in the spectral range 30 000 to 11 100 cm-1 and at temperatures between 77 and 797 K. The evaluation of the intensities, half widths, and energy positions of bands due to Cr3+-transitions derived from 4 A 2g → 4 T 2g (F) and → 4 T 1g (F) as well as of Dq- and B-values derived, had the following results: In all cases, red shift of the above bands and, hence, independent on the site symmetry of Cr3+, decreases in the Dq-values were obtained. The dependcies of Dq on T are nearly linear above room temperature and amount between -1.6% in topaz and -5.1% in pyrope in the temperature range studied. From this, values for the local thermal expansion of the Cr3+-centered octahedra, α loc, were derived on the basis of the R M-0 -5 -proportionality of 10Dq. Such values are consistently higher than those obtained from X-ray refinements, a method averaging rm-o for all the respective octahedral positions. On increasing temperature, the half band widths increase. The evaluation for spinel, pyrope and uvarovite showed $$\Delta \tilde v_{{1 \mathord{\left/ {\vphantom {1 2}} \right. \kern-\nulldelimiterspace} 2}}$$ to increase by about 60%, for both types of Cr3+ transitions, in the temperature range studied. The temperature dependence of band intensities is complex, because it depends on the site symmetry and related symmetry selection rules: symmetry forbidden transitions increase strongly on heating. This was observed for Cr3+ in centosymmetric sites $$\bar 3$$ m of spinel and $$\bar 3$$ of garnets as well as for the symmetry-forbidden Cr3+-transitions in the acentric sites 32 in beryl and 3 in ruby. Where no symmetry-related selection rules exist, as in point symmetry 1 in topaz, almost no temperature dependence of band intensities was observed. This holds also for diopside M 1-octahedra with point symmetry 2, although here the U-band should be forbidden at least in one direction. As for the intensity of the U-bands in spinel, pyrope and uvarovite, the observed intensity increase with T, agreed with that calculated on the basis of vibronic coupling with an odd vibration near ω= 450 cm-1. In order to differentiate between the influences of static and dynamic relaxation of the Laporte rule on the intensities, the relative band intensities, subject to static effects only, were calculated for Cr3+ in ruby and emerald. This proved the temperature dependence of the U π and Y π -band, respectively, to be caused by vibronic coupling only.
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  • 4
    Electronic Resource
    Electronic Resource
    Springer
    Physics and chemistry of minerals 16 (1988), S. 304-310 
    ISSN: 1432-2021
    Source: Springer Online Journal Archives 1860-2000
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Abstract Absorption bands are determined in polarized optical spectra of vivianite Fe3(PO4)2·8H2O, recorded at room and low temperatures. These bands are caused by spin-allowed d-d transitions in structurally nonequivalent Fe A 2+ (∼11000 cm-1 (γ-polarization) (and) ∼12000 cm-1 (β-polarization)) (and) Fe B 2+ (∼8400 cm-1 (γ, α-polarization) and ∼11200 cm-1 (α-polarization)) ions. A charge transfer band (CTB) Fe B 2+ +Fe B 3+ →Fe B 2+ +Fe B 2+ (∼15000 cm-1) also determined, has polarizing features giving evidence of a change in the Fe B 2+ -Fe B 3+ bond direction, when compared with Fe B 2+ -Fe B 2+ . Bands of exchange-coupled Fe3+-Fe3+ pairs (∼19400, ∼20400, ∼21300 and ∼21700 cm-1) which appear on oxidation of Fe2+ in paired Fe B octahedra are also characterized.
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  • 5
    Electronic Resource
    Electronic Resource
    Springer
    Physics and chemistry of minerals 24 (1997), S. 109-114 
    ISSN: 1432-2021
    Source: Springer Online Journal Archives 1860-2000
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Abstract  High-pressure electronic absorption spectra at room temperature and at pressures 10−4〈P[GPa]〈8 were measured in the spectral range 380〈λ[nm] 〈780(26218〉ν˜[cm−1]〉12820) on analysed single crystal slabs, about 20 μm thick, of Cr3+-bearing spinel (I), kyanite (II), corundum (III), pyrope (IV) and uvarovite (V) using DAC-cell techniques in combination with single-beam microscopespectrometry. Ligand field theoretical evaluation of the spectra yielded following results: (i) the octahedral crystal field parameter, 10DqCr3+[6], linearly shifts on increasing pressure to higher energies with slopes, (δ10DqCr3+[6]/δP), of 103.1 (I), 99.5 (II), 104.0 (III), 111.7 (IV) and 110.3 [cm−1/GPa] (V) (reliability parameters r≥0.92), (ii) The Racah-parameter BCr3+[6], reflecting the covalency of the Cr–O bonds, does not significantly change with pressure up to 8 GPa, in those cases where it could be evaluated from the spectra (III, IV, V). This result is contrary to the behaviour of BCr3+[6] with increasing temperature (Taran et al. 1994) and shows that P and T are not inversely correlated parameters with respect to BCr3+[6], a decrease of which reflects an increase in covalency. (iii) This result enabled to extract octahedral compression moduli, kCr3+[6], from the pressure slopes of 10DqCr3+[6]: 312+48 (I), 297+70 (II), 298+44 (III), 275+35 (IV), 257+32 GPa (V). Quotients kcr3+[6]/kbulk,phase are nearly the same (ca. 1.6) for I, II, IV and V but significantly lower (ca. 1.1) for III. Deviations between spectroscopically determined kCr3+[6] and published kAl[6], obtained by HP-XRD on ruby and pyrope, are interpreted by lattice strain induced by [Cr3+, Al3+−1][6] substitution.
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  • 6
    Electronic Resource
    Electronic Resource
    Springer
    Physics and chemistry of minerals 20 (1993), S. 209-220 
    ISSN: 1432-2021
    Source: Springer Online Journal Archives 1860-2000
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Abstract Tourmaline solid solutions containing Fe, Fe+ Ti, Cr, Ni, Cu, Co, Mn chromophoric centers have been grown hydrothermally at 650° C and 1,5 kbar on natural seeding plates close to the elbaite composition. The newly grown tourmalines were characterized by chemical analyses and optical absorption spectroscopy in the range 26316-5000 cm-1 at 297 K and in the range 26316-9090 cm-1 at 77 K. Most characteristic of Fe2+, Fe3+-bearing specimens is the presence of intensive σpolarized absorption bands caused by exchange-coupled Fe2+-Fe3+ pairs in Y- and Z-sites of the tourmaline structure. An additional intensive absorption band 12500 cm-1 (σ-polarisation) appears in some specimens but is not yet found in spectra of natural tourmalines. The colour and spectroscopic properties of the Fe3+, Mn3+ and Cu2+ containing tourmalines are significantly affected by the presence of even the smallest Li-contents. The results suggest that Fe2+, Cu2+, Co2+, Ni2+-ions occupy, predominantly, Y-sites of the tourmaline structure, whereas the Cr3+-ions seem to enter the smaller Z-octachedra.
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  • 7
    Electronic Resource
    Electronic Resource
    Springer
    Physics and chemistry of minerals 27 (1999), S. 59-69 
    ISSN: 1432-2021
    Keywords: Key words Amphiboles ; Charge transfer bands ; Optical spectroscopy ; Mössbauer spectroscopy
    Source: Springer Online Journal Archives 1860-2000
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Abstract Over thirty samples of natural Ti-bearing amphiboles with Ti- and Fe-contents ranging from 0.111 to 0.729 atom per formula unit (a.p.f.u.) and from 0.479 to 2.045 a.p.f.u., respectively, were studied by means of optical absorption spectroscopy and microprobe analysis. Thirteen samples were also studied by Mössbauer spectroscopy. A strong pleochroic absorption edge, causing the dark brown colours of Ti-bearing amphiboles, is attributed to ligand-metal and metal-metal charge transfer transitions involving both iron and titanium ions (O2−→ Fe3+, Fe2+, O2−→ Ti4+ and Fe2+ + Ti4+→ Fe3+ + Ti3+). A broad intense Y-polarized band ∼22 000 cm−1 (ν1/2 ≈ 3700 cm−1) in spectra of two low iron amphiboles with a relatively low Fe3+/Fetotal ratio, both from eclogite-like rocks in kimberlite xenoliths, was attributed to electronic Fe2+(M3) + Ti4+(M2)→Fe3+(M3)+Ti3+(M2) IVCT transitions. The IVCT bands of other possible ion pairs, involving Ti4+ and Fe2+ in M2 and M1, M4 sites, respectively, are presumed to be at higher energies, being obscured by the absorption edge.
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  • 8
    Electronic Resource
    Electronic Resource
    Springer
    Journal of applied spectroscopy 53 (1990), S. 1167-1169 
    ISSN: 1573-8647
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
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  • 9
    Publication Date: 2012-09-01
    Description: Guyanaite, β-CrOOH, is a structural analogue of the high-pressure oxyhydroxide phases -AlOOH and -FeOOH. Here, it was synthesized in piston-cylinder and multi-anvil press experiments at 4–13.5 GPa and 900–1100 °C. The deuterated phase β-CrOOD was synthesized at 4 GPa and 600 °C. The samples were characterized at ambient conditions by X-ray diffraction, diffuse optical reflectance spectroscopy and infrared absorption (IR) spectroscopy. In addition, the structural evolution of β-CrOOH and β-CrOOD with increasing pressure up to about 20 GPa was studied by in situ IR spectroscopy in a diamond anvil cell (DAC). This investigation was complemented by first-principles calculations in the framework of the density-functional theory (DFT). A pronounced geometric isotope effect and very short O-H. . .O bond lengths of 2.497(3) Å for β-CrOOH and 2.541(3) Å for β-CrOOD are observed at ambient pressure. In the IR spectra, no bands show up above 2000 cm –1 , which indicates strong hydrogen bonding. The evolution of OH- and OD-related vibrational bands with pressure studied by IR spectroscopy shows a discontinuity at about 5 GPa. The DFT calculations suggest that this change in compression mechanism is related to a second-order phase transition from the low-pressure phase with asymmetric hydrogen positions (space group P 2 1 nm or Pnnm ) to a high-pressure phase with space group Pnnm that is characterized by symmetric hydrogen bonds with two identical OH bond lengths of 1.20(1) Å. Using density functional perturbation theory, the most prominent high-frequency modes observed in the IR spectra are assigned to O-H-O bending vibrations. The transition pressure for hydrogen bond symmetrisation in β-CrOOH is considerably lower than in other hydrous phases of recent interest, such as -AlOOH or phase D.
    Print ISSN: 0935-1221
    Electronic ISSN: 1617-4011
    Topics: Geosciences
    Published by Schweizerbart
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  • 10
    Publication Date: 2012-09-01
    Description: Optical absorption spectra of synthetic clinopyroxenes of NaVSi 2 O 6 , LiVSi 2 O 6 and CaVAlSiO 6 composition consist of a high-energy absorption edge and two broad absorption bands 1 and 2 at around 15,000 cm –1 and 22,000 cm –1 caused by spin-allowed electronic transitions 3 T 1 g ( 3 F ) -〉 3 T 2 g ( 3 F ) and 3 T 1 g ( 3 F ) -〉 3 T 1 g ( 3 P ) of V 3+ in octahedral M1-site of the clinopyroxene structure. In polarized spectra of NaVSi 2 O 6 and LiVSi 2 O 6 pyroxenes the relative intensities of the polarized components of 1 - and 2 -bands are rather different, revealing differences in the distortion of VO 6 -octahedra in the two structures. In spite of a formal similarity to the absorption spectra of Cr 3+ in Cr-bearing clinopyroxenes, the pressure-induced behaviour of the spin-allowed bands of V 3+ in NaVSi 2 O 6 -pyroxene is noticeably different: although they also shift to higher energies as do the bands of Cr 3+ , the integral intensity of the 1 -band remains nearly constant within uncertainty whereas that of the 2 -band somewhat decreases, in contrast to Cr 3+ for which the spin-allowed bands significantly decrease. Comparing with k oct loc -value of CrO 6 -octahedron in NaCrSi 2 O 6 kosmochlor, ~196 GPa, the VO 6 -octahedron in NaVSi 2 O 6 clinopyroxene structure is considerably softer, with k oct loc 163 GPa. The 〈V – O〉distances derived from the optical absorption spectra can fairly well be approximated by a linear dependence. The Racah parameter B of V 3+ evidently decreases with increasing pressure from ~554 cm –1 at 10 –4 GPa to 508 cm –1 at 10.7 GPa, thus indicating that V – O bonds in the VO 6 -octahedra become more covalent.
    Print ISSN: 0935-1221
    Electronic ISSN: 1617-4011
    Topics: Geosciences
    Published by Schweizerbart
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