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首页> 外文期刊>Astronomy and astrophysics >The UVES Large Program for testing fundamental physics I. Bounds on a change in α towards quasar HE?2217?2818
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The UVES Large Program for testing fundamental physics I. Bounds on a change in α towards quasar HE?2217?2818

机译:测试基本物理的UVES大型计划I.限制α向类星体HE?2217?2818的变化

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Context. Absorption-line systems detected in quasar spectra can be used to compare the value of the fine-structure constant, α, measured today on Earth with its value in distant galaxies. In recent years, some evidence has emerged of small temporal and also spatial variations in α on cosmological scales. These variations may reach a fractional level of ?≈?10?ppm (parts per million). Aims. To test these claims we are conducting a Large Program of observations with the Very Large Telescope’s Ultraviolet and Visual Echelle Spectrograph (UVES), and are obtaining high-resolution (R?≈?60?000) and high signal-to-noise ratio (S/N?≈?100) UVES spectra calibrated specifically for this purpose. Here we analyse the first complete quasar spectrum from this programme, that of HE?2217?2818. Methods. We applied the many multiplet method to measure α in five absorption systems towards this quasar: zabs?=?0.7866, 0.9424, 1.5558, 1.6279 , and 1.6919. Results. The most precise result is obtained for the absorber at zabs?=?1.6919 where 3 Fe?ii transitions and Al?ii λ1670 have high S/N and provide a wide range of sensitivities to α. The absorption profile is complex with several very narrow features, and it requires?32 velocity components to be fitted to the data. We also conducted a range of tests to estimate the systematic error budget. Our final result for the relative variation in α in this system is Δα/α?=?+1.3?±?2.4stat?±?1.0sys?ppm. This is one of the tightest current bounds on α-variation from an individual absorber. A second, separate approach to the data reduction, calibration, and analysis of this system yielded a slightly different result of ?3.8?ppm, possibly suggesting a larger systematic error component than our tests indicated. This approach used an additional 3 Fe?ii transitions, parts of which were masked due to contamination by telluric features. Restricting this analysis to the Fe?ii transitions alone and using a modified absorption profile model gave a result that is consistent with the first approach, Δα/α?=?+1.1?±?2.6stat?ppm. The four other absorbers have simpler absorption profiles, with fewer and broader features, and offer transitions with a narrower range of sensitivities to α. They therefore provide looser bounds on Δα/α at the ??10?ppm precision level. Conclusions. The absorbers towards quasar HE?2217?2818 reveal no evidence of any variation in α at the 3-ppm precision level (1σ confidence). If the recently reported 10-ppm dipolar variation in α across the sky is correct, the expectation at this sky position is (3.2?5.4)?±?1.7?ppm depending on dipole model used. Our constraint of Δα/α?=?+1.3?±?2.4stat?±?1.0sys?ppm is not inconsistent with this expectation.
机译:上下文。在类星体光谱中检测到的吸收线系统可用于比较当今在地球上测得的精细结构常数α的值与在遥远星系中的值。近年来,一些证据表明宇宙尺度上α的时空变化很小。这些变化可能达到≈≈10≤ppm(百万分之一)的分数水平。目的为了检验这些说法,我们正在使用超大型望远镜的紫外线和视觉埃歇尔光谱仪(UVES)进行大型观察,并获得了高分辨率(R≈≈60≤000)和高信噪比( S /N≈≈100)UVES光谱是专门为此校准的。在这里,我们分析了该程序的第一个完整的类星光谱,即HE?2217?2818。方法。我们针对该类星体采用了多重多重法来测量五个吸收系统中的α:zabs?=?0.7866、0.9424、1.5558、1.6279和1.6919。结果。对于吸收体,在z abs =α1.6919处获得最精确的结果,其中3 Fe 3 ii跃迁和Al 2 iiλ1670具有高的S / N并提供对α的宽泛灵敏度。吸收曲线很复杂,具有几个非常狭窄的特征,需要32个速度分量才能拟合到数据中。我们还进行了一系列测试以估计系统误差预算。在该系统中,α的相对变化的最终结果是Δα/α?=?+ 1.3?±?2.4stat?±?1.0sys?ppm。这是来自单个吸收器的α变化最严格的电流范围之一。采用另一种单独的方法对系统进行数据减少,校准和分析的结果略有不同,约为3.8ppm,这可能表明系统误差分量要比我们的测试所示的大。这种方法使用了另外3个Fe?ii过渡,由于碲元素的污染,部分过渡被掩盖了。仅将这种分析限制在Fe 2+跃迁上,并使用改进的吸收曲线模型,得出的结果与第一种方法相符,即Δα/αβ=α+1.1β±β2.6statαppm。其他四种吸收剂具有更简单的吸收曲线,具有更少和更广泛的特征,并提供对α的灵敏度范围更窄的跃迁。因此,它们在Δα/α的精度为Δ10/ ppm时提供了较宽松的边界。结论。朝向类星体HE?2217?2818的吸收剂没有显示出在3 ppm精度水平(1σ置信度)下α发生任何变化的迹象。如果最近报告的整个天空中α的10 ppm偶极变化是正确的,则根据所使用的偶极子模型,该天空位置的期望值为(3.2?5.4)?±?1.7?ppm。我们对Δα/α?=?+ 1.3?±?2.4stat?±?1.0sys?ppm的约束与这一预期并不矛盾。

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