JPS6474434A - Measuring instrument for electrooptic effect - Google Patents

Measuring instrument for electrooptic effect

Info

Publication number
JPS6474434A
JPS6474434A JP23302487A JP23302487A JPS6474434A JP S6474434 A JPS6474434 A JP S6474434A JP 23302487 A JP23302487 A JP 23302487A JP 23302487 A JP23302487 A JP 23302487A JP S6474434 A JPS6474434 A JP S6474434A
Authority
JP
Japan
Prior art keywords
polarized light
linear polarized
polarization
plane
signal
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP23302487A
Other languages
Japanese (ja)
Inventor
Masahiro Nakada
Keiji Shono
Hiroshi Kano
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Fujitsu Ltd
Original Assignee
Fujitsu Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP23302487A priority Critical patent/JPS6474434A/en
Publication of JPS6474434A publication Critical patent/JPS6474434A/en
Pending legal-status Critical Current

Links

Landscapes

  • Measuring Magnetic Variables (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)
  • Liquid Crystal (AREA)

Abstract

PURPOSE:To find the angle of rotation of a plane of polarization by inputting a signal which is reconverted into linear polarized light by a Senarmont optical system to a Faraday cell and vibrating the plane of polarization of the polarized light, and then providing an analyzer. CONSTITUTION:The Senarmont optical system polarizes light from a laser light source 1 into linear polarized light by a polarizer 3 and the linear polarized light from the polarizer 3 is projected on a sample 5 to be measured and made into elliptic polarized light, which is reconverted into the linear polarized light through a 1/4-wavelength plate 7. The Faraday cell 13 applies an alternating magnetic field to the linear polarized light from an oscillator 16 to rotate and also vibrate the plane of polarization of the linear polarized light. A detector 15 detects the output of the signal passed through the Faraday cell 13 through the analyzer 14. A lock-in amplifier 11 extracts only a signal component synchronized with the frequency and phase of the oscillator from the detection signal of the detector 15. A recorder 12 records the extracted signal. Consequently, the angle of rotation of the plane of polarization is found.
JP23302487A 1987-09-17 1987-09-17 Measuring instrument for electrooptic effect Pending JPS6474434A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP23302487A JPS6474434A (en) 1987-09-17 1987-09-17 Measuring instrument for electrooptic effect

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP23302487A JPS6474434A (en) 1987-09-17 1987-09-17 Measuring instrument for electrooptic effect

Publications (1)

Publication Number Publication Date
JPS6474434A true JPS6474434A (en) 1989-03-20

Family

ID=16948608

Family Applications (1)

Application Number Title Priority Date Filing Date
JP23302487A Pending JPS6474434A (en) 1987-09-17 1987-09-17 Measuring instrument for electrooptic effect

Country Status (1)

Country Link
JP (1) JPS6474434A (en)

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