The external electric field of a phosphate glass in an electron beam

E. K. Zavadovskaya, V. A. Starodubtsev, B. V. Fedorov, E. S. Kutukova

Research output: Contribution to journalArticle

Abstract

1. The rise in the external electric field of a phosphate glass charged by a fast-electron beam in air is described by a relaxation curve [1] with a time constant of about 2 · 102 sec; the relaxation time is governed by processes at the interface. 2. The direction of the dipole moment in such a glass corresponds to localization of the injected charge nearer the irradiated surface if the extrapolated range is less than the plate thickness. 3. The external field at the saturation level is dependent on the charge distribution and is largest for γ = 0.7. 4. The strength of the external field indicates that the largest charges are accumulated by glasses with high bond energies for materials of the same type.

Original languageEnglish
Pages (from-to)1333-1335
Number of pages3
JournalSoviet Physics Journal
Volume18
Issue number9
DOIs
Publication statusPublished - Sep 1975

Fingerprint

phosphates
electron beams
electric fields
glass
charge distribution
time constant
dipole moments
relaxation time
saturation
air
curves
energy

ASJC Scopus subject areas

  • Physics and Astronomy(all)

Cite this

The external electric field of a phosphate glass in an electron beam. / Zavadovskaya, E. K.; Starodubtsev, V. A.; Fedorov, B. V.; Kutukova, E. S.

In: Soviet Physics Journal, Vol. 18, No. 9, 09.1975, p. 1333-1335.

Research output: Contribution to journalArticle

Zavadovskaya, E. K. ; Starodubtsev, V. A. ; Fedorov, B. V. ; Kutukova, E. S. / The external electric field of a phosphate glass in an electron beam. In: Soviet Physics Journal. 1975 ; Vol. 18, No. 9. pp. 1333-1335.
@article{d0db2a187ec84e7a9e92d762d5ac667a,
title = "The external electric field of a phosphate glass in an electron beam",
abstract = "1. The rise in the external electric field of a phosphate glass charged by a fast-electron beam in air is described by a relaxation curve [1] with a time constant of about 2 · 102 sec; the relaxation time is governed by processes at the interface. 2. The direction of the dipole moment in such a glass corresponds to localization of the injected charge nearer the irradiated surface if the extrapolated range is less than the plate thickness. 3. The external field at the saturation level is dependent on the charge distribution and is largest for γ = 0.7. 4. The strength of the external field indicates that the largest charges are accumulated by glasses with high bond energies for materials of the same type.",
author = "Zavadovskaya, {E. K.} and Starodubtsev, {V. A.} and Fedorov, {B. V.} and Kutukova, {E. S.}",
year = "1975",
month = "9",
doi = "10.1007/BF00892737",
language = "English",
volume = "18",
pages = "1333--1335",
journal = "Russian Physics Journal",
issn = "1064-8887",
publisher = "Consultants Bureau",
number = "9",

}

TY - JOUR

T1 - The external electric field of a phosphate glass in an electron beam

AU - Zavadovskaya, E. K.

AU - Starodubtsev, V. A.

AU - Fedorov, B. V.

AU - Kutukova, E. S.

PY - 1975/9

Y1 - 1975/9

N2 - 1. The rise in the external electric field of a phosphate glass charged by a fast-electron beam in air is described by a relaxation curve [1] with a time constant of about 2 · 102 sec; the relaxation time is governed by processes at the interface. 2. The direction of the dipole moment in such a glass corresponds to localization of the injected charge nearer the irradiated surface if the extrapolated range is less than the plate thickness. 3. The external field at the saturation level is dependent on the charge distribution and is largest for γ = 0.7. 4. The strength of the external field indicates that the largest charges are accumulated by glasses with high bond energies for materials of the same type.

AB - 1. The rise in the external electric field of a phosphate glass charged by a fast-electron beam in air is described by a relaxation curve [1] with a time constant of about 2 · 102 sec; the relaxation time is governed by processes at the interface. 2. The direction of the dipole moment in such a glass corresponds to localization of the injected charge nearer the irradiated surface if the extrapolated range is less than the plate thickness. 3. The external field at the saturation level is dependent on the charge distribution and is largest for γ = 0.7. 4. The strength of the external field indicates that the largest charges are accumulated by glasses with high bond energies for materials of the same type.

UR - http://www.scopus.com/inward/record.url?scp=34250383883&partnerID=8YFLogxK

UR - http://www.scopus.com/inward/citedby.url?scp=34250383883&partnerID=8YFLogxK

U2 - 10.1007/BF00892737

DO - 10.1007/BF00892737

M3 - Article

VL - 18

SP - 1333

EP - 1335

JO - Russian Physics Journal

JF - Russian Physics Journal

SN - 1064-8887

IS - 9

ER -