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1.
本文介绍了光仪ＰＳＰ０的偏振器设计和实验结果。偏振器设计为旋转半滤片加固定偏振片的系统,但在选用偏振器件方面提出了两种方案。对于低价设计的实验结果表明,偏振器可在４３０－７８０ｎｍ滤长范围内工作,能够实现ＰＳＰ０在其最佳工作波长的偏振测量。 相似文献
2.
分光仪PSP0的光学设计 总被引：1，自引：0，他引：1
本文介绍棱镜分光光度仪ＰＳＰ０的光学设计结果。ＰＳＰ０以ＴＨ７８３２双线ＣＣＤ作为系统探测器，可同时观测０．３６５－１．０微米波长范围内的天体及周转背景的低色散光谱。仪器的入射焦比为Ｆ／１８，平均光谱分辨率约为１０ｎｍ。本文简单介绍了ＰＳＰ０的光学调整，并给出了波长校正实验和配备名古屋大学５０公分望远镜进行试观测的结果。设计和实验结果表明，光学设计很好地满足了天文课题对仪器的设计要求，ＰＳＰ０已可 相似文献
3.
红外相机OASIS的偏振器设计 总被引：5，自引：0，他引：5
介绍为日本冈山天文台１．８８ｍ镜红外相机（ＯＡＳＩＳ）研制的红外偏振器．该偏振器与ＯＡＳＩＳ配备可实现～４．１′视场的近红外成像偏振观测．偏振器包括可旋转的消色差半波片和固定的致冷偏振片,通过旋转半波片对入射光的调制取得线偏振测量．实际观测给出ＪＨＫ波段的偏振效率分别为８６．３％、９７．０％和９７．５％．并给出了ＯＡＳＩＳ偏振观测与前人观测结果的比较 相似文献
4.
本文介绍对分光仪ＰＳＰ０探测器ＴＨ７８３２ＣＣＤ的评估结果。该ＣＣＤ系统工作在－１３０℃￣－１１０℃温度下,具有较好的稳定性和很好的线性。系统的读出噪声约为３００电子,动态范围３５００。在实验结果的基础上,文章对系统性能的改善进行了简单的讨论。 相似文献
5.
介绍恒星形成区Ｓ２５５ ＩＲ 复合体的Ｈ 和Ｋｓ 波段成像偏振和对其中红外源ＩＲＳ１在１ ．２ － ４ ．２ μｍ 上的分光偏振测量．偏振图像揭示了Ｓ２５５ － ２ 核区的两类近红外辐射．以ＩＲＳ１ 双源为中心的一条亮云脊表现出高偏振,而周围延展云却基本上无偏振．偏振图样进一步显示出由ＩＲＳ１ａ 和１ｂ 分别照射的两块反射云．它们都呈双极结构,并且其轴向近于相互垂直．由ＩＲＳ１ｂ 照射的双极云位于方位角ＰＡ～６５°,与Ｈ２ 发射的双极喷流现象很好地符合．两个照射源都是深埋天体．ＩＲＳ１ｂ 和高密度拱星盘成协,其盘平面与双极云垂直．ＩＲＳ１ａ可能也与一未能分辨的盘结构成协,东西方向的盘同样与其成协反射云垂直．从ＩＲＳ１ 的分光偏振测量可辨认出３ μｍ 水冰吸收波段上的偏振超．在此吸收波段上还观测到了反转型的偏振角旋转 相似文献
6.
近红外偏振是研究恒星形成的有效工具.该文介绍了近红外偏振器的工作原理,然后分几个方面介绍了近红外偏振在恒星形成研究中的应用.红外反射云能很好地示踪年轻星天体及分子外流,通过分析偏振矢量的方法确定红外反射云的偏振对称中心,从而确定它的照亮源;偏振波长相关曲线包含了年轻星天体的星周物质的很多信息;年轻星的分子外流导致了红外反射云的形成,因此红外反射云的照亮源通常与年轻星天体成协,并是分子外流的驱动源;一些年轻星天体埋藏得很深,一般在近红外波段无法直接探测到,人们称之为深埋源,通过分析偏振矢量的方法可以找到深埋源;一般认为比较年轻的年轻星天体都是有尘埃盘的,尘埃盘的存在会导致它的偏振形态出现偏振盘,偏振盘町以用来研究尘埃盘;恒星形成区里成员星的偏振主要是由尘埃的二色性消光产生的,这样偏振方向会平行于致使尘埃排列的磁场的方向,从而能够揭示磁场的结构.最后进行了总结,并论述了中远红外偏振研究的优势和意义. 相似文献
7.
从ＲＯＳＡＴ ＰＳＰＣ观测数据中我国发现了与ＰＳＲ０３５５＋５４相关联的脉冲星Ｘ射线喷流存在的证据。这是一个与脉冲星自行方向相反的长度为１２′的近似线性的辐射特征。假设喷流具有ＰＳＲ０３５５＋５４相同的距离和星际吸收,而其能谱是谱指数为－０．５的幂律谱,可导出喷流的光度为２．４８±０．８３×１０＾２４Ｊ／Ｓ。喷流中的平均磁场约为７．９×１０＾－９Ｔ,典型的电子能量为２．１×１０＾７ＭｅＶ。 相似文献
8.
本文利用Ｂｅｒｔｅｌｉ等人新算出的等龄线，以及Ｇｕｎｎ和Ｓｔｒｙｋｅｒ观测的恒星光谱（３１３０－１０８００）构造了一个星族综合模型．该模型能预计金属丰度在Ｚ＝０．０００４－０．０５，年龄在１０７－２×１０１０年范围内的简单星族（ＳＳＰ）的光谱能量分布（ＳＥＤ）．利用ＳＳＰ，通过对不同时刻恒星形成率的卷积能够得到星系的ＳＥＤ的演化．我们计算出ＳＳＰ以及星系在ＵＢＶＲＩ系统和ＢＡＴＣ１５色中带测光系统中的颜色．计算出的从Ｅ／ＳＯ到Ｓｄｍ各类星系的ＵＢＶＲＩ颜色在年龄为１２Ｇｙｒ时都和观测符合较好．因此，我们的模型为正在进行的关于星系ＳＥＤ的多色测光研究提供了理论上的探索． 相似文献
9.
介绍恒星形成区ＮＧＣ７５３８的Ｈ和Ｋｓ波段偏振成像的观测结果．近５′视场的偏振图像揭示了与亮红外源ＩＲＳ１１１成协的年轻星团和红外星云的复杂结构．ＩＲＳ１３星云的偏振图像表明星云的近红外辐射主要来自对深埋红外源ＩＲＳ１的反射;其形态可解释为颜色很红的高偏振的壳层包围着的低消光气泡．ＩＲＳ１周围的近红外的偏振强度在ＩＲＳ１双极分子外流方向上呈现出一较小的壳结构．ＩＲＳ４在近红外表现为双源,其中较红的源ＩＳＲ４ｂ周围观测到中心对称的偏振图像．ＩＲＳ５与亮星云成协,ＩＲＳ６则处于一组星的中心．在ＩＲＳ５和ＩＲＳ６周围的星云中没有观测到偏振．ＩＫＳ９照亮着两块星云,ＩＲＮ１和ＩＲＮ２．ＩＲＮ１星云有很好的锥形并包含一高偏振的喷流成分．云中较高偏振的部分对应较蓝的颜色,显示着其较大的视向张角的外流腔结构．与复杂的ＩＲＳ９区分子外流相比较,ＩＲＮ１星云与在ＮＥＳＷ方向的外流相符合．首次证认了ＩＲＳ１１近红外点源,并观测到其周围有一组星和很暗的星云物质 相似文献
10.
利用简单的ｔｏｒｕｓ束流模型定量计算Ｓｅｙｆｅｒｔ２型星系的偏振度和散射流量和角分布,在“一次电子散射”的假定下,得到偏振度约为１０％￣８０％,而偏振流量的角分布与ｔｏｒｕｓ半张角θｃ和观测角φ０都有关。 相似文献
11.
The theoretical design of the polarimeter used for the Fibre Arrayed Solar Optical Telescope (FASOT) is described. It has the following characteris- tics: (1) It is provided with the function of optical polarization switching, which makes the high-effciency polarimetry possible; (2) In the waveband of 750 nm, the polarimetric effciency is higher than 50% for the every Stokes parameter, and higher than 86.6% for the total polarization, thus an observer can make the simultaneous polarization measurements on multiple magnetosensitive lines in such a broad range of wavelength; (3) According to the selected photospheric and chromospheric lines, the measurement can be focused on either linear polarization or circular polarization; (4) The polarimeter has a loose tolerance on the manufacturing technology of polarimetric elements and installation errors. All this makes this polarimeter become a high-performance polarimetric device. 相似文献
12.
Variations on short time-scales have been found in solar flares at different wavelengths. Millisecond scale radio spikes are a quickly developing area of solar radio astronomy. The solar radio astronomy group of Beijing Astronomical Observatory (BAO) has found fine structures of microwave bursts with millisecond time-scale at 2840 MHz. In this paper, we briefly summarize the observations. A joint-observation network for observing solar radio bursts with high time resolution has also been established. The equipment in the network covers a frequency domain of more than 10:1, including 1.3, 2.0, 6, 10, 15, 20 cm, and meter wavelengths. In particular, a multi-channel polarimeter with super-fast sampling (10 s) at 2600 MHz, an intensity interferometer with 1 ms sampling rate at 6 cm wavelength, and an auto-correlation radio spectrograph with 8 ms time constant at 21 cm wavelength are being established. We pay close attention to research on the spike emission features over wide bands, and their relationship to special characteristics in other spectral ranges. 相似文献
13.
The Haleakala Stokes polarimeter 总被引：1，自引：0，他引：1
D. L. Mickey 《Solar physics》1985,97(2):223-238
A versatile Stokes polarimeter for solar observations has been developed at the University of Hawaii. Recent improvements to the instrument include a high-resolution echelle spectrometer coupled to the telescope by optical fibers, and 128-element diode array detectors. The on-axis design of the telescope and polarimeter limit instrumental polarization to 10–4, and the spectrometer detector combination provides spectral resolving power of 160000 for any wavelength between 4000 and 11000 Å. This paper describes the Haleakala polarimeter and in particular the spectrometer with its fiber-optic coupling. Examples of Stokes line profiles observed in a sunspot are presented, together with derived vector magnetic field maps. 相似文献
14.
B. R. Johnson M. E. Abroe P. Ade J. Bock J. Borrill J. S. Collins P. Ferreira S. Hanany A. H. Jaffe T. Jones A. T. Lee L. Levinson T. Matsumura B. Rabii T. Renbarger P. L. Richards G. F. Smoot R. Stompor H. T. Tran C. D. Winant 《New Astronomy Reviews》2003,47(11-12):1067
We discuss MAXIPOL, a bolometric balloon-borne experiment designed to measure the E-mode polarization anisotropy of the cosmic microwave background radiation (CMB) on angular scales of 10′ to 2°. MAXIPOL is the first CMB experiment to collect data with a polarimeter that utilizes a rotating half-wave plate and fixed wire-grid polarizer. We present the instrument design, elaborate on the polarimeter strategy and show the instrument performance during flight with some time domain data. Our primary dataset was collected during a 26 h turnaround flight that was launched from the National Scientific Ballooning Facility in Ft. Sumner, New Mexico in May 2003. During this flight five regions of the sky were mapped. Data analysis is in progress. 相似文献
15.
E. Wiehr 《Solar physics》1969,9(1):225-234
The miscentering by the Doppler compensator of the Locarno polarimeter is investigated in detail. It is shown that the linear polarization is strongly falsified by this effect which also occurs at the Crimean and Izmiran polarimeters.The new design for the exit slits of the Locarno polarimeter is described. It avoids the ambiguities in the determination of the magnetic field vector that always occur when using two exit slits.A new simple electronic setup avoids most of the difficulties which are usually involved in eliminating instrumental polarization and compensating intensity fluctuations.The observational techniques for solar polarimetry at the Locarno observatory are described.To avoid mutual influences of V and U, the line centre 0 (corresponding to V = 0 and U = max.) must coincide with the centre of slit II. Only in this case we have 234-01 相似文献
16.
17.
J. R. Lemen G. A. Chanan J. P. Hughes M. R. Laser R. Novick I. T. Rochwarger M. Sackson L. J. Tramiel 《Solar physics》1982,80(2):333-349
We have recently built and tested an instrument designed to measure the polarization of the hard (5–30 keV) X-ray emission from solar flares, and thereby to investigate the energy release mechanism and constrain flare models. In particular, these measurements will help to determine whether hard X-ray bursts are produced by nonthermal or by thermal electrons. The polarimeter makes use of the angular dependence of Thomson scattering from targets of metallic lithium. It has an energy resolution of a few keV, a time resolution of 5 s, and sufficient sensitivity to measure polarization levels (3) of a few percent in about 10 s for a moderate strength solar flare. The instrumental polarization has been directly measured and found to be within the design goal of 1%. This polarimeter is scheduled to be flown as part of the OSS-1 pallet on an early Space Shuttle mission. 相似文献
18.
The Ku-band polarization identifier (KUPID) will integrate a very low noise 12–18 GHz, correlation polarimeter onto the Crawford Hill seven meter, millimeter-wave antenna. The primary components of the polarimeter will be built at the University of Miami and other key components, including the microwave horn and data acquisition system will be built at the University of Chicago and Princeton University. This project will measure the Q and U Stokes parameters in regions near the north celestial pole, in regions of low galactic contamination, and in regions near the galactic plane. The KUPID survey experiment makes use of many of the techniques employed in the Princeton IQU experiment (PIQUE) that was developed by the members of this collaboration to detect CMB polarization at shorter wavelengths. The KUPID experiment will be constructed in parallel and on the same timescale as the CAPMAP experiment (see Barkats, this volume) which is the follow-on experiment to PIQUE. KUPID will observe on the Crawford Hill antenna from late spring until early autumn, while CAPMAP will observe during the lower water vapor months of late autumn until early spring. 相似文献
19.
We developed a polarimeter with ferroelectric liquid crystals (FLCs) to observe polarization of flare kernels in the H line. Polarization is one of the important diagnostics of the high-energy particles in solar flares, and high-cadence imaging polarimetry with the precision of the order of 0.1% is required to observe the polarization of flare kernels. However, to achieve such high precision is difficult mainly due to the seeing-induced polarization error, which particularly appears around the flare kernels, because the brightness gradient is steep there. To reduce the seeing-induced error, a high modulation frequency is required, and our new polarimeter based on the combination of a high-speed CCD camera and FLCs realized high-frequency polarization modulation nearly 250 Hz. We evaluated the polarization error, and confirmed that the error was significantly reduced with the new polarimeter. We concluded that the polarimeter with FLCs meets the requirement of solar flare polarimetry. 相似文献
20.
The speckle polarimeter is a facility instrument of the 2.5-mSAIMSU telescope that combines the features of a speckle interferometer and a polarimeter. The speckle polarimeter is designed for observations in several visible bands in the following modes: speckle interferometry, polarimetry, speckle polarimetry, and polaroastrometry. In this paper we describe the instrument design and the procedures for determining the angular scale of the camera and the position angle of the camera and the polarimeter. Our measurements of the parameters for the binary star HD 9165 are used as an example to demonstrate the technique of speckle interferometry. For bright objects the accuracy of astrometry is limited by the error of the correction for the distortion caused by the atmospheric dispersion compensator. At zenith distances less than 45? the additional relative measurement error of the separation is 0.7%, while the additional error of the position angle is 0.3°. In the absence of a dispersion compensator the accuracy of astrometry is limited by the uncertainty in the scale and position angle of the camera, which are 0.15% and 0.06°, respectively. We have performed polarimetric measurements of unpolarized stars and polarization standards. The instrumental polarization at the Cassegrain focus in the V band does not exceed 0.01%. The instrumental polarization for the Nasmyth focus varies between 2 and 4% within the visible range; we have constructed its model and give a method for its elimination from the measurements. For stars with an intrinsic polarization of less than 0.2% during observations at the Cassegrain focus the error is determined mainly by the photon and readout noises and can reach 5 × 10?5. 相似文献