1985
DOI: 10.7567/jjaps.24s4.225
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TSEE from Ion-Implanted LiF Crystals

Abstract: TSEE glow curves were studied for ion-implanted LiF single-crystals and for crystals irradiated by X-rays as well as those thermally annealed and irradiated by X-rays (afterward). It was found that the TSEE glow curve for Mg+ implanted LiF is influenced by the implantation energy and dose. Also, the annealed Mg+ implanted LiF (100 kV ×1012 Mg+/cm2) showed a greater response upon X-rays irradiation (compared with non-implanted LiF). Variations in the TSEE glow curves are qualitatively discussed.

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“…OSEE electrons, which are released from local defect centers, are usually characterized by an energy distribution with the mean energy of ~1 eV and a maximum energy of a few eV. For this reason, released electrons are not lost by ionization and their escape depth can be considerably larger than the free path length and reach ~0.1 µm [18,19]. At this depth optical properties of defects do not differ from those in the bulk.…”
Section: Originalmentioning
confidence: 99%
See 1 more Smart Citation
“…OSEE electrons, which are released from local defect centers, are usually characterized by an energy distribution with the mean energy of ~1 eV and a maximum energy of a few eV. For this reason, released electrons are not lost by ionization and their escape depth can be considerably larger than the free path length and reach ~0.1 µm [18,19]. At this depth optical properties of defects do not differ from those in the bulk.…”
Section: Originalmentioning
confidence: 99%
“…where n is the refraction coefficient, f is the optical transition oscillator strength, h is the maximum electron escape depth (~0.1 µm) [18,19], and K 1 (s/pulse) is the coefficient of proportionality between the OSEE intensity and the OA coefficient. The parameter K 1 represents an apparatus calibration constant, which can be found from Eq.…”
Section: Originalmentioning
confidence: 99%
“…The PSEE electrons released from the local defective centers are usually characterized by an energy distribution with a mean energy of ,1 eV and a maximum energy not exceeding a few eV. Because of this, the ionization losses of released electrons are absent and their escape depth considerably exceeds the mean free path and reaches ,1 µm [12,13]. At such a depth, the optical properties of defects do not differ from those in the bulk.…”
mentioning
confidence: 99%
“…where h is the escape depth of electrons (,0.1 µm [11,12]); K 2 is the second apparatus constant 1 (2.53⋅10 7 pulse −1 ⋅cm −2 for our experimental facility). The parameter K 2 was determined by us from (21) with the use of a set of standard samples of SiO 2 glass and α−Al 2 O 3 crystal with a known concentration of defects by the kinetic curves of the OSEE of the radiation E 1 ′ -and F-centers, respectively.…”
mentioning
confidence: 99%