论文标题
宇宙网络丝中的磁场强度
Magnetic field strength in cosmic web filaments
论文作者
论文摘要
我们使用了从Lofar两米的天空调查数据释放2(Lots DR2)得出的旋转量度(RM)目录,以低密度环境中源源的红移(RRM:残留RM)和极化分数($ p $)的红移来测量进化。我们还通过与NRAO VLA Sky Survey RM目录进行交叉匹配,在1.4-GHz时测量了相同的测量。我们发现RRM与RedShift的平坦在144 MHz处是平坦的,但是,一旦经过红移校正,它就会显示出很高的意义。 $ p $随着红移的发展,在$ z \ sim2 $下减少了$ \ sim $ 8。比较144-MHz和1.4-GHz数据,我们发现观察到的RRM和$ P $最有可能在1.4-GHz的源局部局部,而宇宙网络丝源起源于144-MHz。如果我们将整个信号归因于细丝,则在RRM_ {0,f} = 0.71 \ pm 0.07 rad m^{ - 2}的情况下,将平均休息帧rrm和每个细丝的磁场B_F = 32 \ pm 3 ng。这与基于同步加速器发射堆叠的互补方法获得的估计值一致,如果天体物理源场播种会放大原始磁场,则与宇宙学模拟相一致。 rrm_ {0,f}的测量支持丝中的弥漫性男气体。我们还估计了σ_{rrm_ {0,f}} = 0.039 \ pm 0.001 rad m^{ - 2}的丝磁湍流的保守上限,得出结论是有序的磁场成分在细丝中占主导地位。
We used the Rotation Measure (RM) catalogue derived from the LOFAR Two-metre Sky Survey Data Release 2 (LoTSS DR2) at 144-MHz to measure the evolution with redshift of the extragalactic RM (RRM: Residual RM) and the polarization fraction ($p$) of sources in low density environments. We also measured the same at 1.4-GHz by cross-matching with the NRAO VLA Sky Survey RM catalogue. We find that RRM versus redshift is flat at 144-MHz, but, once redshift-corrected, it shows evolution at high significance. Also $p$ evolves with redshift with a decrement by a factor of $\sim$8 at $z\sim2$. Comparing the 144-MHz and 1.4-GHz data, we find that the observed RRM and $p$ are most likely to have an origin local to the source at 1.4-GHz, while a cosmic web filament origin is favoured at 144-MHz. If we attribute the entire signal to filaments, we infer a mean rest frame RRM per filament of RRM_{0,f} = 0.71 \pm 0.07 rad m^{-2} and a magnetic field per filament of B_f = 32 \pm 3 nG. This is in agreement with estimates obtained with a complementary method based on synchrotron emission stacking, and with cosmological simulations if primordial magnetic fields are amplified by astrophysical source field seeding. The measurement of an RRM_{0,f} supports the presence of diffuse baryonic gas in filaments. We also estimated a conservative upper limit of the filament magnetic turbulence of σ_{ RRM_{0,f}} =0.039 \pm 0.001 rad m^{-2}, concluding that the ordered magnetic field component dominates in filaments.