首页> 外文会议>Conference on observatory operations: Strategies, processes, and systems, VI >Linear and Angolar Moment of a General Spherical TEM and DEM Beam Radio Wave Detection with a Quadratic Order System Processor in State of Art Technology Implementation: A Three Axis Sensors Array Quadratic Order Correlator for the 21cm Radiation Radio Detection Coming from Early Universe
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Linear and Angolar Moment of a General Spherical TEM and DEM Beam Radio Wave Detection with a Quadratic Order System Processor in State of Art Technology Implementation: A Three Axis Sensors Array Quadratic Order Correlator for the 21cm Radiation Radio Detection Coming from Early Universe

机译:一般球形TEM和DEM光束无线电波检测的线性和Angolar时刻,具有二次订单系统处理器的技术实现:三轴传感器阵列二次订单相关器,用于从早期宇宙的21CM辐射无线电检测

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The paper focuses on an innovative spherical wave beam quadratic order processor, HSCS~(-1). It is an IP, Coulob Gauge based, to directly mesure, At and in any single P AP (along the propagation axis too) the quadratic order Poynting Vector, with both the complex Linear Momentum (LiM) and Angolar Momentum (AnM) contributions, as well as the the mutual quadratic order coherence function of any total or pseudo monochromatic observed beam wave. The focoused spherical quadratic order method, directly mesure the spherical complex OAM (time and propagation axsis invariant) which is composed by the observed beam wave modes. Such solenoidal energy modes, becomes relevant to mesure far distance (as exemple: distance greater than billions of light years away) sources radiations. Furthermore, HSCS~(-1) contemporary and directly mesure the mutual (spatial as well as temporal) complex coherence of any general complex divergent or not strictly TEM (as example: TEM+DEM) observed radiations. Tipically TEM+DEM radiations are characterized by N=LPM+1 complex wave beam modes. N is the number of considered EM fields modes, as great as requested; N and L are integer, which values are internal to a closed interval [0; ∞]; p and M are integer, which values are internal to a closed interval [1;∞]; n=0,l,...,N is the mode or beam channel index; with 1=0, 1,...,L; p= 1,..., P; and m = 1,.. .,M; n=/=0 is the fundamental mode index). Here are considered only the wave beam modes which satisfy the related Helmoltz monochromatic wave equation soluctions. As well known in Physics, only adopting a quadratic order energy processor it is possible Vt to contemporary and directely mesure in P, (A)P(θ; Φ; z) and (A)(P-P_0), both the proper P_0 position and quantity of motion (proper space time variations), or by a Fourier Transformation to contemporary and directely mesure proper phase and frequency spectrum variations, of the observed general radiation source. Effectively a quadratic order energy processor, like HSCS~(-1), directly mesure power spectrum related to both the first and the second observed wave beam time derivatives. Then it exstracts the proper Linear phase (Φ =ω t, with waves beam medium frequency ω in Δt=t) and Quadratic phase (θ depending on the waves beam frequency ω time derivatives in Δt=t)variations values which satisfy the observed source motion equation. Furthermore, HSCS~(-1) quadratic Poynting Vector and complex spherical Visibility processor is immune by planar interpherometric Phase error and mesurement ambiguity. Contrary, because any 1st order planar interferometry TEM system mesures only the TEM linear power density spectrum (LiM) contributions, it is impossible directly and without ambiguity mesure or assigne both spherical spazial position and quantity of motion of a general TEM+DEM wave beam source, At and (A)P(θ;Φ; z) and (A)(P-Po). Because 1st order TEM Systems are insensitive to longitudinal quadratic orders Fields modes, then a lot of energy related to the transverse AnM of observed wave beam is definitively lost. Morever 1storder measurement systems are affected by planar interpherometric distructive phase error and measurement ambiguity, because the measurement is sensitive to trasversal wave field modes (TEM, TE, TM) only. Effectively, HSCS~(-1) is sensitive to the quadratic spatial fast beam spherical phase variation [△ψ_(HSCS)-_LPM = ± (Δθ_(LPM) - ΔΦ_(LPM))] as well as to the linear temporal beam phase variation [coot] of the observed field. It extracts both transverse and longitudinal components of the observed solenoidal and/or irrotational fields (elecromagnetic, termodinamic, etc). The complex TEM+DEM wave mutual quadratic order coherence function γ, and the "Quadratic order fringes Visibility" as well as the related mutual quadratic order coherence degree may be directly computed by the innovative depositated IP, the synthetic spherical quadratic order system HSCS~(-1). The HSCS~(-1) direct measure of the mu
机译:本文关注的创新的球面波光束二次顺序处理器上,HSCS〜(-1)。据的IP,Coulob计基础,以直接MESURE,At和在任何单P AP(沿着传播轴太)二次顺序坡印亭矢量,同时与复杂的线性动量(LIM)和Angolar动量(ANM)的贡献,以及任何总的的相互二次阶相关函数或伪单色光束观测波。所述focoused球形二次顺序的方法,直接MESURE这是由观察到的光束的波模组成的球形复杂OAM(时间和传播axsis不变)。这种螺线管能量模式,成为相关MESURE远的距离(如为例:距离大于十亿光年)源辐射。此外,HSCS〜(-1)和当代直接MESURE相互(空间以及时间)络合物任何一般复杂的发散的相干性或不严格TEM(如实施例:TEM + DEM)观察到辐射。 Tipically TEM + DEM辐射由N = LPM + 1种复合波光束模式为特征。 N是考虑电磁场模式的数量,那么大的要求; N和L是整数,其值是内部的闭区间[0; ∞]; P和M是整数,其值是内部的闭区间[1;∞]; n = 0时,L,...,N是模式或波束信道索引;与1 = 0,1,...,L; P = 1,...,P;且m = 1,...,M。; N = / = 0是基本模式索引)。这里被认为是仅满足相关亥姆霍兹单色波方程soluctions波束模式。正如在物理公知的,只采用一个二次顺序能量处理器是可能的Vt到P中当代和directely MESURE,(A)P(θ;Φ; z)和(A)(P-P_0),两者都正确P_0位置和运动的量(适当的空间时间的变化),或通过进行傅立叶变换,当代和directely MESURE适当的相位和频谱的变化所观察到的一般辐射源。有效地二次顺序能量处理器,像HSCS〜(-1),直接MESURE与第一和第二观测波束时间衍生物既功率谱。然后,它exstracts适当线性相位(Φ=ωt,其中波光束中频ω在ΔT= t)和二次相位(θ取决于波光束频率ω的时间导数在ΔT= T2)满足下观察到的源的变化值运动方程。此外,HSCS〜(-1)二次坡印亭矢量和复杂的球形能见度处理器是通过免疫平面interpherometric相位误差和测宽歧义。相反,因为任何一阶平面干涉TEM系统mesures仅TEM线性功率密度谱(LIM)的贡献,这是不可能直接且毫不含糊MESURE或assigne一般TEM + DEM波束源的运动的两个球形spazial位置和数量,在与(A)P(θ;Φ; z)和(A)(P-PO)。因为第一顺序TEM系统是不敏感的纵向二次订单字段模式,那么很多有关观测波束的横向ANM能量被明确丢失。 Morever 1storder测量系统由平面interpherometric distructive相位误差和测量模糊性的影响,因为测量是trasversal波场模式(TEM,TE,TM)只有敏感。有效地,HSCS〜(-1)是二次空间快速光束球面相位变化敏感[△ψ_(HSCS)-_ LPM =±(Δθ_(LPM) - ΔΦ_(LPM))]以及对线性时序光束相变化所观察到的场的[口子。它提取横向和所观察到的螺线管和/或不旋转的字段(elecromagnetic,termodinamic等)的纵向分量。复杂的TEM + DEM波相互二次阶相关函数γ,和“二次顺序条纹可见性”以及相关的相互二次为了一致性程度可以通过创新depositated IP,合成球形二次顺序系统HSCS〜(直接计算-1)。在HSCS〜(-1)的亩的直接测量

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