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Photoinduced chesorluminescence from radical processes on ZrO2 surfaces. / Andreev, N. S.; Emeline, A. V.; Khudnev, V. A.; Polikhova, S. A.; Ryabchuk, V. K.; Serpone, N.

в: Chemical Physics Letters, Том 325, № 1-3, 21.07.2000, стр. 288-292.

Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование

Harvard

Andreev, NS, Emeline, AV, Khudnev, VA, Polikhova, SA, Ryabchuk, VK & Serpone, N 2000, 'Photoinduced chesorluminescence from radical processes on ZrO2 surfaces', Chemical Physics Letters, Том. 325, № 1-3, стр. 288-292. https://doi.org/10.1016/S0009-2614(00)00648-5

APA

Andreev, N. S., Emeline, A. V., Khudnev, V. A., Polikhova, S. A., Ryabchuk, V. K., & Serpone, N. (2000). Photoinduced chesorluminescence from radical processes on ZrO2 surfaces. Chemical Physics Letters, 325(1-3), 288-292. https://doi.org/10.1016/S0009-2614(00)00648-5

Vancouver

Andreev NS, Emeline AV, Khudnev VA, Polikhova SA, Ryabchuk VK, Serpone N. Photoinduced chesorluminescence from radical processes on ZrO2 surfaces. Chemical Physics Letters. 2000 Июль 21;325(1-3):288-292. https://doi.org/10.1016/S0009-2614(00)00648-5

Author

Andreev, N. S. ; Emeline, A. V. ; Khudnev, V. A. ; Polikhova, S. A. ; Ryabchuk, V. K. ; Serpone, N. / Photoinduced chesorluminescence from radical processes on ZrO2 surfaces. в: Chemical Physics Letters. 2000 ; Том 325, № 1-3. стр. 288-292.

BibTeX

@article{a3e1901b62934ab4bf3973d6109b0b86,
title = "Photoinduced chesorluminescence from radical processes on ZrO2 surfaces",
abstract = "Photoexcitation of ZrO2 particles causes luminescence (τ~15.0 s) which, after its termination, on addition of H2 causes emission of a light pulse that displays biphasic decay kinetics (τ1~0.9 s and τ2~15.5 s). The latter emission is referred to as a photoinduced chesorluminescence (PhICL). At 77 K, the longer-lived emission is thermally quenched. The shorter-lived emission is caused by electron trapping by the Va (anion vacancies) low energy traps; the longer-lived emission involves electron trapping by shallow traps, followed by detrapping and subsequent retrapping by the Va traps. Formation of highly energetic radical species is a necessary condition to observe PhICL emission.",
author = "Andreev, {N. S.} and Emeline, {A. V.} and Khudnev, {V. A.} and Polikhova, {S. A.} and Ryabchuk, {V. K.} and N. Serpone",
year = "2000",
month = jul,
day = "21",
doi = "10.1016/S0009-2614(00)00648-5",
language = "English",
volume = "325",
pages = "288--292",
journal = "Chemical Physics Letters",
issn = "0009-2614",
publisher = "Elsevier",
number = "1-3",

}

RIS

TY - JOUR

T1 - Photoinduced chesorluminescence from radical processes on ZrO2 surfaces

AU - Andreev, N. S.

AU - Emeline, A. V.

AU - Khudnev, V. A.

AU - Polikhova, S. A.

AU - Ryabchuk, V. K.

AU - Serpone, N.

PY - 2000/7/21

Y1 - 2000/7/21

N2 - Photoexcitation of ZrO2 particles causes luminescence (τ~15.0 s) which, after its termination, on addition of H2 causes emission of a light pulse that displays biphasic decay kinetics (τ1~0.9 s and τ2~15.5 s). The latter emission is referred to as a photoinduced chesorluminescence (PhICL). At 77 K, the longer-lived emission is thermally quenched. The shorter-lived emission is caused by electron trapping by the Va (anion vacancies) low energy traps; the longer-lived emission involves electron trapping by shallow traps, followed by detrapping and subsequent retrapping by the Va traps. Formation of highly energetic radical species is a necessary condition to observe PhICL emission.

AB - Photoexcitation of ZrO2 particles causes luminescence (τ~15.0 s) which, after its termination, on addition of H2 causes emission of a light pulse that displays biphasic decay kinetics (τ1~0.9 s and τ2~15.5 s). The latter emission is referred to as a photoinduced chesorluminescence (PhICL). At 77 K, the longer-lived emission is thermally quenched. The shorter-lived emission is caused by electron trapping by the Va (anion vacancies) low energy traps; the longer-lived emission involves electron trapping by shallow traps, followed by detrapping and subsequent retrapping by the Va traps. Formation of highly energetic radical species is a necessary condition to observe PhICL emission.

UR - http://www.scopus.com/inward/record.url?scp=0000726018&partnerID=8YFLogxK

U2 - 10.1016/S0009-2614(00)00648-5

DO - 10.1016/S0009-2614(00)00648-5

M3 - Article

AN - SCOPUS:0000726018

VL - 325

SP - 288

EP - 292

JO - Chemical Physics Letters

JF - Chemical Physics Letters

SN - 0009-2614

IS - 1-3

ER -

ID: 35144037