{"title":"利用 LHAASO 在高达 300 TeV 的 $γ$ 射线中深入观测复合 SNR CTA1","authors":"LHAASO Collaboration","doi":"arxiv-2409.09499","DOIUrl":null,"url":null,"abstract":"The ultra-high-energy (UHE) gamma-ray source 1LHAASO J0007+7303u is\npositionally associated with the composite SNR CTA1 that is located at high\nGalactic Latitude $b\\approx 10.5^\\circ$. This provides a rare opportunity to\nspatially resolve the component of the pulsar wind nebula (PWN) and supernova\nremnant (SNR) at UHE. This paper conducted a dedicated data analysis of 1LHAASO\nJ0007+7303u using the data collected from December 2019 to July 2023. This\nsource is well detected with significances of 21$\\sigma$ and 17$\\sigma$ at\n8$-$100 TeV and $>$100 TeV, respectively. The corresponding extensions are\ndetermined to be 0.23$^{\\circ}\\pm$0.03$^{\\circ}$ and\n0.17$^{\\circ}\\pm$0.03$^{\\circ}$. The emission is proposed to originate from the\nrelativistic electrons and positrons accelerated within the PWN of PSR\nJ0007+7303. The energy spectrum is well described by a power-law with an\nexponential cutoff function $dN/dE = (42.4\\pm4.1)(\\frac{E}{20\\rm\\\nTeV})^{-2.31\\pm0.11}\\exp(-\\frac{E}{110\\pm25\\rm\\ TeV})$ $\\rm\\ TeV^{-1}\\ cm^{-2}\\\ns^{-1}$in the energy range from 8 TeV to 300 TeV, implying a steady-state\nparent electron spectrum $dN_e/dE_e\\propto (\\frac{E_e}{100\\rm\\\nTeV})^{-3.13\\pm0.16}\\exp[(\\frac{-E_e}{373\\pm70\\rm\\ TeV})^2]$ at energies above\n$\\approx 50 \\rm\\ TeV$. The cutoff energy of the electron spectrum is roughly\nequal to the expected current maximum energy of particles accelerated at the\nPWN terminal shock. Combining the X-ray and gamma-ray emission, the current\nspace-averaged magnetic field can be limited to $\\approx 4.5\\rm\\ \\mu G$. To\nsatisfy the multi-wavelength spectrum and the $\\gamma$-ray extensions, the\ntransport of relativistic particles within the PWN is likely dominated by the\nadvection process under the free-expansion phase assumption.","PeriodicalId":501343,"journal":{"name":"arXiv - PHYS - High Energy Astrophysical Phenomena","volume":"47 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Deep view of Composite SNR CTA1 with LHAASO in $γ$-rays up to 300 TeV\",\"authors\":\"LHAASO Collaboration\",\"doi\":\"arxiv-2409.09499\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The ultra-high-energy (UHE) gamma-ray source 1LHAASO J0007+7303u is\\npositionally associated with the composite SNR CTA1 that is located at high\\nGalactic Latitude $b\\\\approx 10.5^\\\\circ$. This provides a rare opportunity to\\nspatially resolve the component of the pulsar wind nebula (PWN) and supernova\\nremnant (SNR) at UHE. This paper conducted a dedicated data analysis of 1LHAASO\\nJ0007+7303u using the data collected from December 2019 to July 2023. This\\nsource is well detected with significances of 21$\\\\sigma$ and 17$\\\\sigma$ at\\n8$-$100 TeV and $>$100 TeV, respectively. The corresponding extensions are\\ndetermined to be 0.23$^{\\\\circ}\\\\pm$0.03$^{\\\\circ}$ and\\n0.17$^{\\\\circ}\\\\pm$0.03$^{\\\\circ}$. The emission is proposed to originate from the\\nrelativistic electrons and positrons accelerated within the PWN of PSR\\nJ0007+7303. The energy spectrum is well described by a power-law with an\\nexponential cutoff function $dN/dE = (42.4\\\\pm4.1)(\\\\frac{E}{20\\\\rm\\\\\\nTeV})^{-2.31\\\\pm0.11}\\\\exp(-\\\\frac{E}{110\\\\pm25\\\\rm\\\\ TeV})$ $\\\\rm\\\\ TeV^{-1}\\\\ cm^{-2}\\\\\\ns^{-1}$in the energy range from 8 TeV to 300 TeV, implying a steady-state\\nparent electron spectrum $dN_e/dE_e\\\\propto (\\\\frac{E_e}{100\\\\rm\\\\\\nTeV})^{-3.13\\\\pm0.16}\\\\exp[(\\\\frac{-E_e}{373\\\\pm70\\\\rm\\\\ TeV})^2]$ at energies above\\n$\\\\approx 50 \\\\rm\\\\ TeV$. The cutoff energy of the electron spectrum is roughly\\nequal to the expected current maximum energy of particles accelerated at the\\nPWN terminal shock. Combining the X-ray and gamma-ray emission, the current\\nspace-averaged magnetic field can be limited to $\\\\approx 4.5\\\\rm\\\\ \\\\mu G$. To\\nsatisfy the multi-wavelength spectrum and the $\\\\gamma$-ray extensions, the\\ntransport of relativistic particles within the PWN is likely dominated by the\\nadvection process under the free-expansion phase assumption.\",\"PeriodicalId\":501343,\"journal\":{\"name\":\"arXiv - PHYS - High Energy Astrophysical Phenomena\",\"volume\":\"47 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-14\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - High Energy Astrophysical Phenomena\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2409.09499\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - High Energy Astrophysical Phenomena","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.09499","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
超高能(UHE)伽马射线源1LHAASO J0007+7303u与位于银河系高纬度$b\approx 10.5^\circ$的复合SNR CTA1位置相关。这为空间解析UHE上的脉冲星风星云(PWN)和超新星(SNR)的成分提供了一个难得的机会。本文利用2019年12月至2023年7月收集的数据对1LHAASOJ0007+7303u进行了专门的数据分析。该源被很好地探测到,在8$-$100 TeV和$>$100 TeV的显著性分别为21$\sigma$和17$\sigma$。相应的扩展值分别为0.23$^{circ}/pm$0.03$^{circ}$和0.17$^{circ}/pm$0.03$^{circ}$。据推测,这些发射源于在PSRJ0007+7303的PWN内加速的相对论电子和正电子。能谱可以用一个幂律来描述,其指数截止函数为 $dN/dE = (42.4\pm4.1)(\frac{E}{20\rm\TeV})^{-2.31\pm0.11}\exp(-\frac{E}{110\pm25\rm\TeV})$ $\rm\TeV^{-1}\cm^{-2}s^{-1}$ in the energy range from 8 TeV to 300 TeV, implying a steady-stateparent electron spectrum $dN_e/dE_e\propto (\frac{E_e}{100\rm\TeV})^{-3.13pm0.16}exp[(\frac{E_e}{373\pm70\rm\TeV})^2]$ 在能量超过$\approx 50 \rm\TeV$ 时。电子能谱的截止能量大致等于目前在PWN末端冲击加速的粒子的预期最大能量。结合X射线和伽马射线发射,当前空间平均磁场可以限制在大约4.5\rm\mu G$。为了满足多波长频谱和伽马射线的扩展,在自由膨胀阶段假设下,相对论粒子在PWN内的传输可能是由对流过程主导的。
Deep view of Composite SNR CTA1 with LHAASO in $γ$-rays up to 300 TeV
The ultra-high-energy (UHE) gamma-ray source 1LHAASO J0007+7303u is
positionally associated with the composite SNR CTA1 that is located at high
Galactic Latitude $b\approx 10.5^\circ$. This provides a rare opportunity to
spatially resolve the component of the pulsar wind nebula (PWN) and supernova
remnant (SNR) at UHE. This paper conducted a dedicated data analysis of 1LHAASO
J0007+7303u using the data collected from December 2019 to July 2023. This
source is well detected with significances of 21$\sigma$ and 17$\sigma$ at
8$-$100 TeV and $>$100 TeV, respectively. The corresponding extensions are
determined to be 0.23$^{\circ}\pm$0.03$^{\circ}$ and
0.17$^{\circ}\pm$0.03$^{\circ}$. The emission is proposed to originate from the
relativistic electrons and positrons accelerated within the PWN of PSR
J0007+7303. The energy spectrum is well described by a power-law with an
exponential cutoff function $dN/dE = (42.4\pm4.1)(\frac{E}{20\rm\
TeV})^{-2.31\pm0.11}\exp(-\frac{E}{110\pm25\rm\ TeV})$ $\rm\ TeV^{-1}\ cm^{-2}\
s^{-1}$in the energy range from 8 TeV to 300 TeV, implying a steady-state
parent electron spectrum $dN_e/dE_e\propto (\frac{E_e}{100\rm\
TeV})^{-3.13\pm0.16}\exp[(\frac{-E_e}{373\pm70\rm\ TeV})^2]$ at energies above
$\approx 50 \rm\ TeV$. The cutoff energy of the electron spectrum is roughly
equal to the expected current maximum energy of particles accelerated at the
PWN terminal shock. Combining the X-ray and gamma-ray emission, the current
space-averaged magnetic field can be limited to $\approx 4.5\rm\ \mu G$. To
satisfy the multi-wavelength spectrum and the $\gamma$-ray extensions, the
transport of relativistic particles within the PWN is likely dominated by the
advection process under the free-expansion phase assumption.