Electrooptic Vector Sampling--Measurement of Vector Components of Electric Field by the Polarization Control of Probe Light--
Summary :
We measured the longitudinal electric field of the electrical pulses with a rise time less than 1 ps on a coplanar transmission line by electrooptic sampling. The longitudinal component is a sharp pulse and is only observed at the wavefront. The transverse component has no overshoot or undershoot. The mixing of longitudinal component to the transverse component is discussed for C3v crystals whose electrooptic coefficient is large. We developed the method to estimate the longitudinal and the transverse component of the electric field by the polarization control of a probe light without changing the probe configuration which affects sensitivity severely. The waveform and the rise time of the transverse electric field were eatimated, for the first time, by subtracting the influence of the longitudinal component.
- Publication
- IEICE TRANSACTIONS on Electronics Vol.E78-C No.1 pp.73-80
- Publication Date
- 1995/01/25
- Publicized
- Online ISSN
- DOI
- Type of Manuscript
- Special Section PAPER (Special Issue on Ultrafast Optoelectronics)
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Taro ITATANI, Tadashi NAKAGAWA, Fumihisa KANO, Kimihiro OHTA, Yoshinobu SUGIYAMA, "Electrooptic Vector Sampling--Measurement of Vector Components of Electric Field by the Polarization Control of Probe Light--" in IEICE TRANSACTIONS on Electronics,
vol. E78-C, no. 1, pp. 73-80, January 1995, doi: .
Abstract: We measured the longitudinal electric field of the electrical pulses with a rise time less than 1 ps on a coplanar transmission line by electrooptic sampling. The longitudinal component is a sharp pulse and is only observed at the wavefront. The transverse component has no overshoot or undershoot. The mixing of longitudinal component to the transverse component is discussed for C3v crystals whose electrooptic coefficient is large. We developed the method to estimate the longitudinal and the transverse component of the electric field by the polarization control of a probe light without changing the probe configuration which affects sensitivity severely. The waveform and the rise time of the transverse electric field were eatimated, for the first time, by subtracting the influence of the longitudinal component.
URL: https://global.ieice.org/en_transactions/electronics/10.1587/e78-c_1_73/_p
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@ARTICLE{e78-c_1_73,
author={Taro ITATANI, Tadashi NAKAGAWA, Fumihisa KANO, Kimihiro OHTA, Yoshinobu SUGIYAMA, },
journal={IEICE TRANSACTIONS on Electronics},
title={Electrooptic Vector Sampling--Measurement of Vector Components of Electric Field by the Polarization Control of Probe Light--},
year={1995},
volume={E78-C},
number={1},
pages={73-80},
abstract={We measured the longitudinal electric field of the electrical pulses with a rise time less than 1 ps on a coplanar transmission line by electrooptic sampling. The longitudinal component is a sharp pulse and is only observed at the wavefront. The transverse component has no overshoot or undershoot. The mixing of longitudinal component to the transverse component is discussed for C3v crystals whose electrooptic coefficient is large. We developed the method to estimate the longitudinal and the transverse component of the electric field by the polarization control of a probe light without changing the probe configuration which affects sensitivity severely. The waveform and the rise time of the transverse electric field were eatimated, for the first time, by subtracting the influence of the longitudinal component.},
keywords={},
doi={},
ISSN={},
month={January},}
Copy
TY - JOUR
TI - Electrooptic Vector Sampling--Measurement of Vector Components of Electric Field by the Polarization Control of Probe Light--
T2 - IEICE TRANSACTIONS on Electronics
SP - 73
EP - 80
AU - Taro ITATANI
AU - Tadashi NAKAGAWA
AU - Fumihisa KANO
AU - Kimihiro OHTA
AU - Yoshinobu SUGIYAMA
PY - 1995
DO -
JO - IEICE TRANSACTIONS on Electronics
SN -
VL - E78-C
IS - 1
JA - IEICE TRANSACTIONS on Electronics
Y1 - January 1995
AB - We measured the longitudinal electric field of the electrical pulses with a rise time less than 1 ps on a coplanar transmission line by electrooptic sampling. The longitudinal component is a sharp pulse and is only observed at the wavefront. The transverse component has no overshoot or undershoot. The mixing of longitudinal component to the transverse component is discussed for C3v crystals whose electrooptic coefficient is large. We developed the method to estimate the longitudinal and the transverse component of the electric field by the polarization control of a probe light without changing the probe configuration which affects sensitivity severely. The waveform and the rise time of the transverse electric field were eatimated, for the first time, by subtracting the influence of the longitudinal component.
ER -
English
