Microstructure in Radio Emission of the Pulsar B1133+16 at a Frequency of 111 MHz

IF 1.1 4区 物理与天体物理 Q3 ASTRONOMY & ASTROPHYSICS
M. V. Popov
{"title":"Microstructure in Radio Emission of the Pulsar B1133+16 at a Frequency of 111 MHz","authors":"M. V. Popov","doi":"10.1134/S1063772924700471","DOIUrl":null,"url":null,"abstract":"<p>This study is based on observations of the pulsar B1133+16 conducted on the BSA PRAO antenna array at a frequency of 111 MHz with continuous recording of undetected signal (voltage) in the 2.5 MHz band, providing time resolution 0.2 µs. From 30 observation sessions, 570 strong pulses were selected for the subsequent analysis of microstructure parameters. The analysis was performed by computing autocorrelation functions separately for the three components of the mean profile: two extreme main components <i>I</i> and <i>II</i> and for the central weak component <span>\\(S\\)</span> in the profile saddle. For the component <span>\\(S\\)</span>, microstructure analysis was performed for the first time. Distributions have been constructed by the following parameters: time scales <span>\\({{\\tau }_{\\mu }}\\)</span>, modulation depth <span>\\({{m}_{\\mu }}\\)</span>, and parameter <span>\\(d\\)</span>, which characterizes the shape of the micropulses. Noticeable differences were found in some parameters for different profile components. The discovered features were interpreted in the model of hollow cone with a central component. It was believed that the radio emission of the extreme components (<i>I</i> and <i>II</i>) is generated by ordinary mode O, and the radio emission of the central component is provided by extraordinary mode X. Under this interpretation the radio emission output heights above the polar cap, were estimated to be 45 and 280 km for the X and O modes, respectively. A noticeable deformation of the X mode emission cone relative to the central component <i>S</i> was mentioned. Considerations are presented that point to the spatial structure of the secondary plasma flow, elongated along the meridians of the magnetic field.</p>","PeriodicalId":55440,"journal":{"name":"Astronomy Reports","volume":"68 5","pages":""},"PeriodicalIF":1.1000,"publicationDate":"2024-08-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Astronomy Reports","FirstCategoryId":"101","ListUrlMain":"https://link.springer.com/article/10.1134/S1063772924700471","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"ASTRONOMY & ASTROPHYSICS","Score":null,"Total":0}
引用次数: 0

Abstract

This study is based on observations of the pulsar B1133+16 conducted on the BSA PRAO antenna array at a frequency of 111 MHz with continuous recording of undetected signal (voltage) in the 2.5 MHz band, providing time resolution 0.2 µs. From 30 observation sessions, 570 strong pulses were selected for the subsequent analysis of microstructure parameters. The analysis was performed by computing autocorrelation functions separately for the three components of the mean profile: two extreme main components I and II and for the central weak component \(S\) in the profile saddle. For the component \(S\), microstructure analysis was performed for the first time. Distributions have been constructed by the following parameters: time scales \({{\tau }_{\mu }}\), modulation depth \({{m}_{\mu }}\), and parameter \(d\), which characterizes the shape of the micropulses. Noticeable differences were found in some parameters for different profile components. The discovered features were interpreted in the model of hollow cone with a central component. It was believed that the radio emission of the extreme components (I and II) is generated by ordinary mode O, and the radio emission of the central component is provided by extraordinary mode X. Under this interpretation the radio emission output heights above the polar cap, were estimated to be 45 and 280 km for the X and O modes, respectively. A noticeable deformation of the X mode emission cone relative to the central component S was mentioned. Considerations are presented that point to the spatial structure of the secondary plasma flow, elongated along the meridians of the magnetic field.

Abstract Image

Abstract Image

频率为 111 MHz 的脉冲星 B1133+16 射电发射中的微观结构
摘要 本研究基于在 BSA PRAO 天线阵列上对脉冲星 B1133+16 的观测,观测频率为 111 MHz,在 2.5 MHz 频段上连续记录未检测到的信号(电压),时间分辨率为 0.2 µs。从 30 个观测时段中选择了 570 个强脉冲,用于随后的微观结构参数分析。分析方法是分别计算平均剖面三个分量的自相关函数:两个极端主分量 I 和 II 以及剖面鞍部的中心弱分量 \(S\)。对于分量 \(S\),首次进行了微观结构分析。分布是由以下参数构建的:时间尺度({{\tau }_{\mu }}\)、调制深度({{m}_{\mu }}\)以及描述微脉冲形状的参数(d\)。不同剖面成分的某些参数存在明显差异。所发现的特征被解释为具有中心成分的空心圆锥模型。根据这一解释,X 和 O 模式在极冠上方的无线电发射输出高度估计分别为 45 公里和 280 公里。X模式发射锥相对于中心成分S有明显的变形。考虑指出了次级等离子体流的空间结构,即沿磁场经线拉长的等离子体流。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
Astronomy Reports
Astronomy Reports 地学天文-天文与天体物理
CiteScore
1.40
自引率
20.00%
发文量
57
审稿时长
6-12 weeks
期刊介绍: Astronomy Reports is an international peer reviewed journal that publishes original papers on astronomical topics, including theoretical and observational astrophysics, physics of the Sun, planetary astrophysics, radio astronomy, stellar astronomy, celestial mechanics, and astronomy methods and instrumentation.
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信