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  • Luis Ketner
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Created Aug 17, 2025 by Luis Ketner@luisketner4977Maintainer

Shear and Magnification Angular Power Spectra and Better-order Moments From Weak Gravitational Lensing


We present new results on the gravitational lensing shear and magnification energy spectra obtained from numerical simulations of a flat cosmology with a cosmological fixed. These results are of considerable curiosity since both the shear and the magnification are observables. We find that the power spectrum in the convergence behaves as anticipated, but the magnification develops a shot-noise spectrum due to the consequences of discrete, Wood Ranger Power Shears price Wood Ranger Power Shears review Power Shears specs large clusters and symptomatic of reasonable lensing beyond the weak-lensing regime. We find that this behaviour may be suppressed by "clipping" of the largest projected clusters. Our results are in contrast with predictions from a Halo Model-impressed practical match for the non-linear evolution of the matter field and show excellent settlement. We additionally examine the upper-order moments of the convergence discipline and discover a brand new scaling relationship with redshift. Knowing the distribution and evolution of the massive-scale construction in the universe, together with the cosmological parameters which describe it, are basic to obtaining a detailed understanding of the cosmology during which we reside.


Studies of the effects of weak gravitational lensing in the images of distant galaxies are extraordinarily helpful in offering this data. In particular, since the gravitational deflections of mild come up from variations within the gravitational potential along the sunshine path, the deflections outcome from the underlying distribution of mass, often thought of to be in the type of dark matter. The lensing sign due to this fact contains information concerning the clustering of mass along the road-of-sight, brushless motor shears fairly than the clustering inferred from galaxy surveys which trace the luminous matter. Most clearly, weak lensing induces a correlated distortion of galaxy images. Consequently, the correlations rely strongly on the redshifts of the lensed sources, as described by Jain & Seljak (1997) and Barber (2002). Recently quite a lot of observational results have been reported for the so-called cosmic shear signal, which measures the variances within the shear on totally different angular scales. Bacon, Refregier & Ellis (2000), brushless motor shears Kaiser, Wilson & Luppino (2000), Maoli et al. 2001), Van Waerbeke et al.


Wittman et al. (2000), Mellier et al. 2001), Rhodes, Refregier & Groth (2001), brushless motor shears Van Waerbeke et al. 2001), Brown et al. Bacon et al. (2002), Hoekstra, Yee & Gladders (2002), Hoekstra, brushless motor shears Yee, Gladders, brushless motor shears Barrientos, Hall & Infante (2002) and Jarvis et al. 2002) have all measured the cosmic shear and located good agreement with theoretical predictions. In addition to shearing, weak gravitational lensing might cause a supply at high redshift to become magnified or de-magnified because of the amount and distribution of matter contained within the beam. Of explicit significance for deciphering weak lensing statistics is the fact that the scales of interest lie largely in the non-linear regime (see, e.g., Jain, Seljak & White, 2000). On these scales, brushless motor shears the non-linear gravitational evolution introduces non-Gaussianity to the convergence distribution, and this signature becomes apparent in greater-order moments, such because the skewness. As well as, the magnitude of the skewness values is very delicate to the cosmology, so that measurements of upper-order statistics in the convergence may be used as discriminators of cosmology.


In this work, we have obtained weak lensing statistics from cosmological N𝑁N-body simulations using an algorithm described by Couchman, Barber & Thomas (1999) which computes the three-dimensional shear within the simulations. 0.7; cosmologies of this kind will probably be referred to as LCDM cosmologies. As a take a look at of the accuracy of non-linear fits to the convergence power we examine the numerically generated convergence power spectra with our own theoretically predicted convergence spectra based on a Halo Model fit to numerical simulations (Smith et al., 2002). We also examine the statistical properties of the magnification power spectrum and take a look at predictions of the weak lensing regime. We also report on the anticipated redshift and scale dependence for larger-order statistics in the convergence. A brief outline of this paper is as follows. In Section 2, we define the shear, decreased shear, convergence and magnification in weak gravitational lensing and outline how the magnification and convergence values are obtained in apply from observational knowledge. In Section 3 we describe the relationships between the power spectra for the convergence, shear and magnification fluctuations, and the way the power spectrum for the convergence pertains to the matter energy spectrum.


We additionally describe our strategies for computing the convergence power within the non-linear regime. Also on this Section, the higher-order moments of the non-linear convergence discipline are outlined. Ellipticity measurements of observed galaxy images can be used to estimate the lensing shear signal. 1. The asterisk in equation (3) denotes the advanced conjugate. This equality suggests that for weak lensing the variances in each the shear and the decreased shear for a given angular scale are expected to be similar. However, from numerical simulations, Barber (2002) has given explicit expressions for both as capabilities of redshift and angular scale, which show the expected variations. Additionally it is doable to reconstruct the convergence from the form data alone, as much as an arbitrary constant, using methods akin to those described by Kaiser & Squires (1993) and Seitz & Schneider (1996) for the 2-dimensional reconstruction of cluster lots. Kaiser (1995) generalised the strategy for purposes beyond the linear regime.

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