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It is shown by rneaiis of investigation of both optical absorption spectra and Roentgen Kal-lines of chroiiiiuni doped in LiKSO,, LiNaSO,, and Li,SO,. H,O crystals, t h a t Xirradiation results in change of the impurity charge state in a following way : Cr3+ + h+Cr4, Cr4+ + h + Cr5+.Earlier we have studied the EYR and optical absorption spectra of LizSO,. H,O, LiKSO, and LiNaSO, crystals doped with Cr3+ (ALYBAKOV et al. 1979(ALYBAKOV et al. , 1982 and the change of spectra of chromium-doped lithium and lithium-potassium sulphates under the X-irradiation (ALYBAKOV et al. 1980(ALYBAKOV et al. , 1983. It was shown, that X-irradiation results in weakening of Cr3+ ion absorption bands; at the same time a new band appears at about 350 nm in Li,SO, : Cr and about 355 nni in LiKSO, : Cr. A new group of lines appears also in a highfield side of EPR spectrum of the irradiated crystal; spectrum is described by spin-Hamiltonian with 8 = 1/2. This spectrum is absent in irradiated undoped crystals, therefore its appearance was supposed to be connected with a chromium valence change. The spectruin is stable a t a room temperature, consequently, it may not be due t o either divalent or tetravalent chromium. We supposed, that Cr3+ converts in Cr+ by means of a successive capture of two electrons, Cr+ being in a low-spin state (X = l / 2 ) in the assumption of a strong crystalline field.A subsequent investigation has shown, that the intensity of a irradiation-induced absorption band in anhydrous sulphates increases when heating and becomes maximal after the annealing a t 200 'C; at LNT this band has a clearly pronounced fine structure (Fig. 1). The separation between the fine structure components is -830 cm-' in LiKSO, : Cr spectrum and -806 cm-l in LiNaSO, : Cr spectrum. It is difficult t o explain the appearance of a fine structure, if one connects the irradiation-induced absorption band with Cr+. On the other hand, absorption bands in the region of 350 t o 360nm with a fine structure were observed earlier in the crystals, containing Cr5+ ions in the oxygen environment (BAKKS et al.; SIMO et al.); the fine structure was interpreted, as electronic-vibrational one due t o interaction with a v,-mode of chromate ion.I n principle, during the irradiation chroniium ions may trap either electrons or holes. To elucidate a question about a valent state of chromium in the irradiated crystals of alkali sulphates, we have studied Roentgen K,>-lines of chromium in these crystals. Such an investigation is a direct way of studying of a valence change, as the displacement of K,,-lime maximum is completely caused by the change of the number of valent electrons. Figure 2 shows Kal-lines of chroinium in different valent states. The positions of chromium lines in standard samples were used t o construct the dependence of a line
It is shown by rneaiis of investigation of both optical absorption spectra and Roentgen Kal-lines of chroiiiiuni doped in LiKSO,, LiNaSO,, and Li,SO,. H,O crystals, t h a t Xirradiation results in change of the impurity charge state in a following way : Cr3+ + h+Cr4, Cr4+ + h + Cr5+.Earlier we have studied the EYR and optical absorption spectra of LizSO,. H,O, LiKSO, and LiNaSO, crystals doped with Cr3+ (ALYBAKOV et al. 1979(ALYBAKOV et al. , 1982 and the change of spectra of chromium-doped lithium and lithium-potassium sulphates under the X-irradiation (ALYBAKOV et al. 1980(ALYBAKOV et al. , 1983. It was shown, that X-irradiation results in weakening of Cr3+ ion absorption bands; at the same time a new band appears at about 350 nm in Li,SO, : Cr and about 355 nni in LiKSO, : Cr. A new group of lines appears also in a highfield side of EPR spectrum of the irradiated crystal; spectrum is described by spin-Hamiltonian with 8 = 1/2. This spectrum is absent in irradiated undoped crystals, therefore its appearance was supposed to be connected with a chromium valence change. The spectruin is stable a t a room temperature, consequently, it may not be due t o either divalent or tetravalent chromium. We supposed, that Cr3+ converts in Cr+ by means of a successive capture of two electrons, Cr+ being in a low-spin state (X = l / 2 ) in the assumption of a strong crystalline field.A subsequent investigation has shown, that the intensity of a irradiation-induced absorption band in anhydrous sulphates increases when heating and becomes maximal after the annealing a t 200 'C; at LNT this band has a clearly pronounced fine structure (Fig. 1). The separation between the fine structure components is -830 cm-' in LiKSO, : Cr spectrum and -806 cm-l in LiNaSO, : Cr spectrum. It is difficult t o explain the appearance of a fine structure, if one connects the irradiation-induced absorption band with Cr+. On the other hand, absorption bands in the region of 350 t o 360nm with a fine structure were observed earlier in the crystals, containing Cr5+ ions in the oxygen environment (BAKKS et al.; SIMO et al.); the fine structure was interpreted, as electronic-vibrational one due t o interaction with a v,-mode of chromate ion.I n principle, during the irradiation chroniium ions may trap either electrons or holes. To elucidate a question about a valent state of chromium in the irradiated crystals of alkali sulphates, we have studied Roentgen K,>-lines of chromium in these crystals. Such an investigation is a direct way of studying of a valence change, as the displacement of K,,-lime maximum is completely caused by the change of the number of valent electrons. Figure 2 shows Kal-lines of chroinium in different valent states. The positions of chromium lines in standard samples were used t o construct the dependence of a line
The optical absorption spectra of 3 CdSO, -8 H,O single crystals doped with Cr3+ is recorded a t 300 and 80 K ; the crystal field transitions are assigned and the B, C, Dq parameters evaluated. Polarisation investigations are undertaken t o establish the exact electric dipole transitions and the exact magnetic dipole transitions. Splitting of the bands (differences between the parallel and perpendicular polarised spectra) due to the non-cubic fields acting on the chromium(II1) ion are not observed though two inequivalent cadmium atoms exist in the lattice. Also no lowering of symmetry is observed either from the low temperature spectra or the polarised spectra. Radiation damage studies are undertaken to study the mechanism of the formation of Cr3+ to Crf and the valence state effect on the electronic transitions. The effect of space charge compensating vacancies on the electronic transitions and its effect on the crystal field strength is studied using the radiation damage spectra. The formation of Cr+ from Cr3+ through Cr*+ is well explained. The theoretically calculated values coincide well with t,he experimentally observed values for the octahedral symmetry for both, Cr3+ and Cr+ ions in 3 CdSO, -8 H,O lattice.Die optischen Absorptionsspektren von Cr3+-dotierten 3 CdSO, . 8 H,O-Einkristallen werden bei 300 und 80 K aufgenommen, die Kristallfeld-ubergange zugeordnet und die B-, C-, Dp-Parameter berechnet. Um die exakten elektrischen und exakten magnetischen Dipoliibergiinge festzustellen, werden Polarisationsuntersuchungen unternommen. Aufspaltung der Banden (Unterschiede zwischen den parallel und senkrecht polarisierten Spektren) infolge der nicht-kubischen Felder, die auf das Chrom(II1)-Ion wirken, werden nicht beobachtet, obwohl zwei nichtaquivalente Kadmiumatome im Gitter vorhanden sind. Auch eine Erniedrigung der Symmetrie wird weder in den Niedertemperaturspektren noch in den polarisierten Spektren beobachtet. Untersuchungen des Strahlungsdamage werden durchgefuhrt, um den Mechanismus der Bildung von Cr3+ zu Cr+ sowie den EinfluD des Valenzzustandes auf den elektronischen ubergang zu untersuchen. Der EinfluB von raumladungskompensierenden Leerstellen auf die elektronischen n e r g a n g e und deren Ein-flu13 auf die Starke des Kristallfeldes werden mittels Strahlungsdamagespektren untersucht. Die Cr+-Bildung aus Cr3+ uber Cr2+ wird gut erkllrt. Die theoretisch berechneten Werte stimmen gut mit den experimentell beobachteten Werten fur die Oktaedersymmetrie sowohl fur Cr3+-als auch fur Cr+-Ionen in 3 CdSO, . 8 H,O-Gittern uberein.
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