毫米波超导超光谱装置

U. Chowdhury, F. Levy-Bertrand, M. Calvo, J. Goupy, A. Monfardini
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引用次数: 0

摘要

毫米波观测是宇宙学研究的重要工具。线强度映射(LIM)技术已经提出在三维空间中映射由于线(例如[C ii], CO)发射的特定强度,例如来自原始星系,作为红移的函数。高光谱集成设备有可能取代目前的傅立叶变换,或计划在毫米和亚毫米波长下工作的基于fabry - perot的仪器。目的是执行高光谱映射,光谱分辨率R = λ/Δλ = 100-1000,对大的,即数千束,天空的瞬时斑块。我们开发的创新集成设备可以避免在低温下操作移动部件,复杂和/或色散光学或可调滤波器。原型高光谱焦平面在75- 90ghz范围内敏感,包含19个角,用于16个光谱成像通道,每个通道选择约0.1 GHz的频段。对于每个通道,一个锥形喇叭天线,连接到一个由薄铝制成的平面超导谐振吸收器,收集辐射。电容耦合的钛铝双层集总元件动态电感检测器(LEKID)负责耗散和感应谐振吸收器中产生的超电流。该原型仅在商业单晶蓝宝石衬底上进行了两步光刻。光谱分辨率R = λ/Δλ≈800。最佳信道的光噪声等效功率在观测相关的$4\cdot 10^{-17} W/\sqrt{Hz}$范围内。所有通道的平均灵敏度约为$1\cdot 10^{-16} W/\sqrt{Hz}$。正如3d模拟所期望的那样,该设备具有偏振敏感性,为在非常大的瞬时视场上进行光谱偏振测量铺平了道路。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A millimetre-wave superconducting hyper-spectral device
Millimetre-wave observations represent an important tool for Cosmology studies. The Line Intensity Mapping (LIM) technique has been proposed to map in three dimensions the specific intensity due to line (e.g. [C ii], CO) emission, for example from the primordial galaxies, as a function of redshift. Hyper-spectral integrated devices have the potential to replace the current Fourier transform, or the planned Fabry-Perot-based instruments operating at millimetre and sub-millimetre wavelengths. The aim is to perform hyper-spectral mapping, with a spectral resolution R = λ/Δλ = 100–1000, over large, i.e. thousands of beams, instantaneous patches of the Sky. The innovative integrated device that we have developed allows avoiding moving parts, complicated and/or dispersive optics or tunable filters to be operated at cryogenic temperatures. The prototype hyper-spectral focal plane is sensitive in the 75-90 GHz range and contains nineteen horns for sixteen spectral-imaging channels, each selecting a frequency band of about 0.1 GHz. For each channel a conical horn antenna, coupled to a planar superconducting resonant absorber made of thin aluminium, collects the radiation. A capacitively coupled titanium-aluminium bilayer Lumped Element Kinetic Inductance Detector (LEKID) is then in charge of dissipating and sensing the super-current established in the resonant absorber. The prototype is fabricated with only two photo-lithography steps over a commercial mono-crystalline sapphire substrate. It exhibits a spectral resolution R = λ/Δλ ≈ 800. The optical noise equivalent power of the best channels is in the observational relevant $4\cdot 10^{-17} W/\sqrt{Hz}$ range. The average sensitivity of all the channels is around $1\cdot 10^{-16} W/\sqrt{Hz}$. The device, as expected from 3-D simulations, is polarisation-sensitive, paving the way to spectro-polarimetry measurements over very large instantaneous field-of-views.
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