Abstract
1. The variation dynamics of the external electric field above the irradiated surface of alumophosphate glasses is described by a function of the type (1), where x is the length of irradiation, and y is the field intensity. 2. The relaxation process of the decay of the external field intensity is characterized by a time constant of the order of 10 sec. 3. The mentioned magnitude of the time constant may be due to radiation conductivity of the glasses investigated having a magnitude of ρirr = 1013 Ω ·m.
| Original language | English |
|---|---|
| Pages (from-to) | 1331-1332 |
| Number of pages | 2 |
| Journal | Soviet Physics Journal |
| Volume | 18 |
| Issue number | 9 |
| DOIs | |
| Publication status | Published - Sep 1975 |
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ASJC Scopus subject areas
- Physics and Astronomy(all)
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Variation of the external electric field intensity of phosphate glasses charged by a stream of electrons. / Starodubtsev, V. A.; Fedorov, B. V.
In: Soviet Physics Journal, Vol. 18, No. 9, 09.1975, p. 1331-1332.Research output: Contribution to journal › Article
}
TY - JOUR
T1 - Variation of the external electric field intensity of phosphate glasses charged by a stream of electrons
AU - Starodubtsev, V. A.
AU - Fedorov, B. V.
PY - 1975/9
Y1 - 1975/9
N2 - 1. The variation dynamics of the external electric field above the irradiated surface of alumophosphate glasses is described by a function of the type (1), where x is the length of irradiation, and y is the field intensity. 2. The relaxation process of the decay of the external field intensity is characterized by a time constant of the order of 10 sec. 3. The mentioned magnitude of the time constant may be due to radiation conductivity of the glasses investigated having a magnitude of ρirr = 1013 Ω ·m.
AB - 1. The variation dynamics of the external electric field above the irradiated surface of alumophosphate glasses is described by a function of the type (1), where x is the length of irradiation, and y is the field intensity. 2. The relaxation process of the decay of the external field intensity is characterized by a time constant of the order of 10 sec. 3. The mentioned magnitude of the time constant may be due to radiation conductivity of the glasses investigated having a magnitude of ρirr = 1013 Ω ·m.
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U2 - 10.1007/BF00892736
DO - 10.1007/BF00892736
M3 - Article
VL - 18
SP - 1331
EP - 1332
JO - Russian Physics Journal
JF - Russian Physics Journal
SN - 1064-8887
IS - 9
ER -