• Title/Summary/Keyword: Polarimeter

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The Penn Polarimeters

  • Koch, Robert H.;Wolf, George W.;Hull, Anthony B.;Elias, Nicholas M. II;Holenstein, Bruce D.;Mitchell, Richard J.
    • Journal of Astronomy and Space Sciences
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    • v.29 no.1
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    • pp.69-77
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    • 2012
  • This report describes the inception, development and extensive use over 30 years of elliptical polarimeters at the University of Pennsylvania. The initial Mark I polarimeter design utilized oriented retarder plates and a calcite Foster-Clarke prism as the analyzer. The Mark I polarimeter was used on the Kitt Peak 0.9 m in 1969-70 to accomplish a survey of approximately 70 objects before the device was relocated to the 0.72 m reflector at the Flower and Cook Observatory. Successive generations of automation and improvements included the early-80's optical redesign to utilize a photoelastic modulated wave plate and an Ithaco lock-in amplifier-the photoelastic modulating polarimeter. The final design in 2000 concluded with a fully remote operable device. The legacy of the polarimetric programs includes studies of close binaries, pulsating hot stars, and luminous late-type variables.

Simulation of a Polarimeter for a Spin-Polarized Positron Beam

  • Kim, J.H.;Saito, F.;Suzuki, N.;Wei, L.;Nagashima, Y.;Kurihara, T.;Goto, A.;Itoh, Y.;Lee, Y.S.;Hyodo, T.
    • Journal of Korean Vacuum Science & Technology
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    • v.6 no.3
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    • pp.116-119
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    • 2002
  • A performance of a new positron polarimeter is investigated by simulation using a charged-particle trajectory program. The results of the ray tracing are presented along with the details of the design parameters and projected system performance. A ray tracing analysis indicates that this design is capable of effectively transmitting positrons at beam energies varying from 0.1 to 30 keV within the beam diameter of 2-6mm. However, the observed reflection of the positrons(lower than 2 keV) at 12 kGauss indicated that further refinement of beam design is needed to produce a better positron polarimeter.

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A Study on the Optical Characteristics of Biaxial Film by using Dual Rotating Retarder Polarimeter and a Novel Simulation Model

  • Yun, C.H.;Jeon, B.K.;Park, M.S.;Yu, J.S.
    • 한국정보디스플레이학회:학술대회논문집
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    • 2006.08a
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    • pp.809-813
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    • 2006
  • We have studied the optical properties of the biaxial film such as fast axis, retardance and the change of polarization state between crossed polarizer using dual rotating retarder polarimeter. We have developed a novel simulation model, which could explain well the experimental results, and found that it could be used to optimize the compensation film in LCD for improving wide-viewing property.

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An Undergraduate Level Polarimeter and Specific Rotation at 543 nm of Sucrose (학부용 편광계와 543 nm에서 설탕의 비회전 측정)

  • Jung, Semin
    • Korean Journal of Optics and Photonics
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    • v.23 no.6
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    • pp.241-245
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    • 2012
  • Measurements of the optical activity become very important issues in fields related to polymers, optical communications, astronomy, physics and many more. Hence it need to introduce this subject in our regular curriculum. In this experiment, an inexpensive, reliable, motorized polarimeter system which is suitable for undergraduate courses is constructed with PASCO's well-known Science Workshop 750 and a rotational motion sensor and light sensor, and the system is presented along with its experimental formulas. After responsivity of this system was checked by a half wave plate, and some repetitive experiments with 30% sucrose solution at 543.8 nm were performed. Comparing the experimental result with two calculated values from CRC data[1] showed that the specific rotation of the sucrose sample could be strongly suggested to be around +76 deg.cc/g.dm and it was an amply acceptable result for most undergraduate level courses.

A Study on Fabrication and Performance Evaluation of Ti:LiNbO3 Polarization Mode Controllers (Ti:LiNbO3 편광모드 조절기 제작 및 성능 평가에 관한 연구)

  • Moon, Je-Young;Jung, Hong-Sik
    • Korean Journal of Optics and Photonics
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    • v.15 no.6
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    • pp.547-554
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    • 2004
  • We investigated a LiNbO$_3$ based integrated-optic polarization controller with the Ti-indiffused waveguide along the z-axis utilizing the electro-optic effect. The device consists of a first quarter-wave (λ / 4) followed by a half-wave (λ / 2) and a second quarter-wave (λ / 4) wave-plate. We analyzed the amount of phase change and the transformation of the polarized mode as a function of the combination of wave-plates and of their applied voltages. The operation has been systematically measured utilizing a polarimeter and Poincare sphere. We confirmed that the fabricated device controls the transformations from any arbitrary input state of polarization (SOP) into any general output SOP.

Developments of the Wide Wavelength Range Polarimeter of the Domeless Solar Telescope at the Hida Observatory

  • Anan, Tetsu;Ichimoto, Kiyoshi;Oi, Akihito;Ueno, Satoru;Kimura, Goichi;Nakatani, Yoshikazu
    • The Bulletin of The Korean Astronomical Society
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    • v.36 no.2
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    • pp.86.1-86.1
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    • 2011
  • We are developing a new universal spectropolarimeter on the Domeless Solar Telescope (DST) at the Hida Observatory to realize precise spectropolarimetric observations in a wide range of wavelength in visible and near infrared. The system aims to open a new window of plasma diagnostics by using Zeeman effect, Hanle effect, Stark effect, impact polarization, and atomic polarization for measuring the external magnetic field, electric field, or an anisotropy in the excitation of the atoms. The polarimeter is a successor of formerly developed polarimeter on DST, which make possible to observe a polarization in a photospheric spectral line with polarimetric accuracy of 10-2 (Kiyohara et al. 2004). The new system consists of a 60cm aperture vacuum telescope, a high dispersion vacuum spectrograph, polarization modulator / analyzer composed of a rotating waveplate whose retardation is constant for a wide range of wavelength and Wallaston prism, and a fast and large format CCD camera or IR camera. Spectral images in both orthogonal polarizations are taken simultaneously with a frame rate of ~20Hz while the waveplate rotates continuously in a rate of 1rev./sec. Thus It takes 5 ~ 60 sec to observe polarization with accuracy of 10-3 in a wide wavelength range (400 - 1100nm). We also examined a polarimetric model of the telescope with accuracy of 10-3 to calibrate instrumental polarization on some wavelengths. In this talk, I will focus on the performance of the instrument.

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Infrared Spectro-Polarimeter of the Solar Flare Telescope at NAOJ

  • Hagino, Masaoki;Sakurai, Takashi;Hanaoka, Yoichiro;Shinoda, Kazuya;Noguchi, Motokazu;Miyashita, Masakuni;Fukuda, Takeo;Suzuki, Isao;Arai, Takehiko;Takeyama, Norihide
    • The Bulletin of The Korean Astronomical Society
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    • v.36 no.2
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    • pp.85.2-85.2
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    • 2011
  • A new infrared spectro-polarimeter was installed in 2008 onto the Solar Flare Telescope of NAOJ in the Mitaka headquarters. The Solar Flare Telescope had been operated previously as a filter-based magnetograph and obtained vector magnetograms of active regions with the Fe I 630.3nm line during 1992 - 2005. The aim of this new instrument is to measure the distribution of magnetic helicity over the whole Sun and for an extended period with high magnetic sensitivity in the infrared wavelengths. This spectro-polarimter is able to obtain polarizations in both photospheric and chromospheric layers. In order to take full Stokes profiles, we observe Fe I 1564.8 nm and He I 1083.0 nm lines (with the neighboring photospheric Si line) for the photospheric and chromospheric magnetic field vectors, respectively. The infrared detector of this instrument is a $640{\times}512$-pixel InGaAs camera produced by a Belgian company Xenics. The frame rate of the camera is 90 frames/sec. The 640-pixel row of this camera is set along the spectrograph slit of the polarimeter. Since the slit only covers the solar hemisphere, a full disk map is obtained by raster scanning the solar disk twice. A magnetic map is made of about $1200{\times}1200$ pixels with a pixel size of 1.8 arcsec. It generally takes 1.5 hours to scan the whole Sun. Although some issues on the instrument calibration still remain, a few maps of the whole Sun at the two wavelengths are now taken daily. In this presentation, we will introduce the instrument and present some observational results.

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