论文标题

部分可观测时空混沌系统的无模型预测

Pulse Profiles and Polarization of Terzan 5 Pulsars

论文作者

Martsen, Ashley R., Ransom, Scott M., DeCesar, Megan E., Freire, Paulo C. C., Hessels, Jason W. T., Ho, Anna Y. Q., Lynch, Ryan S., Stairs, Ingrid H., Wang, Yuankun

论文摘要

Terzan 5是银河凸起中丰富的球状簇,其中包含39个已知的毫秒脉冲星,这是任何球状簇中最大的已知种群。 Terzan 5脉冲星是微弱的,因此对大多数脉冲星的单个观察值太少,无法测量可靠的通量密度或极化信息。在过去的11年中,我们合并了超过5.2 \,在1.5 \,GHz和2.0 \,GHz中的每个日子中,与绿色银行望远镜一起使用。我们为32个脉冲星创建了高S/N轮廓,并确定了其中28个曲线的精确旋转措施(RMS)。我们使用RMS,已知的脉冲星位置和分散度量(DMS),将银河磁场的投影平行分量绘制为群集。 The $\langle B_{||}\rangle$ shows a rough gradient of $\sim$6\,nG/arcsec ($\sim$160\,nG/parsec), or fractionally, a change of $\sim$20$\%$ in the right ascension direction across the cluster, implying Galactic magnetic field variability at sub-parsec scales.我们还测量了脉冲星的平均通量密度$s_ν$,范围从$ \ sim $ 10 \,$μ$ jy到$ \ sim $ 2 \,mjy,以及平均光谱索引$α= -1.35 $,其中$s_ν\ propt \ propto f proptotte n propto n^α)$。该频谱指数比大多数已知的脉冲星更平坦,由于脉冲星搜索中使用的高频以减轻分散和散射,因此可能会产生选择效果。推断的脉冲星光度函数是大致的,斜率$(d \ log n)/(d \ log l)= -1 $在高亮度末端。在低亮度端,存在不完整的效果,这意味着Terzan 5包含更多的脉冲星。

Terzan 5 is a rich globular cluster within the galactic bulge that contains 39 known millisecond pulsars, the largest known population of any globular cluster. The Terzan 5 pulsars are faint, so that individual observations of most of the pulsars have too little signal-to-noise (S/N) to measure reliable flux density or polarization information. We combined over 5.2\,days of archival data, at each of 1.5\,GHz and 2.0\,GHz, taken with the Green Bank Telescope over the past 11\,years. We created high S/N profiles for 32 of the pulsars and determined precise rotation measures (RMs) for 28 of them. We used the RMs, and the known pulsar positions and dispersion measures (DMs), to map the projected parallel component of the Galactic magnetic field toward the cluster. The $\langle B_{||}\rangle$ shows a rough gradient of $\sim$6\,nG/arcsec ($\sim$160\,nG/parsec), or fractionally, a change of $\sim$20$\%$ in the right ascension direction across the cluster, implying Galactic magnetic field variability at sub-parsec scales. We also measured average flux densities $S_ν$ for the pulsars, ranging from $\sim$10\,$μ$Jy to $\sim$2\,mJy, and an average spectral index $α= -1.35$, where $S_ν\propto ν^α)$. This spectral index is flatter than most known pulsars, likely a selection effect due to the high frequencies used in pulsar searches to mitigate dispersion and scattering. The inferred pulsar luminosity function is roughly power-law, with slope $(d\log N)/(d\log L) = -1$ at the high-luminosity end. At the low-luminosity end, there are incompleteness effects implying that Terzan 5 contains many more pulsars to be found.

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