scholarly journals Recovering the real-space correlation function from photometric redshift surveys

2009 ◽  
Vol 394 (3) ◽  
pp. 1631-1639 ◽  
Author(s):  
Pablo Arnalte-Mur ◽  
Alberto Fernández-Soto ◽  
Vicent J. Martínez ◽  
Enn Saar ◽  
Pekka Heinämäki ◽  
...  
2017 ◽  
Vol 600 ◽  
pp. A32 ◽  
Author(s):  
Srivatsan Sridhar ◽  
Sophie Maurogordato ◽  
Christophe Benoist ◽  
Alberto Cappi ◽  
Federico Marulli

1997 ◽  
Vol 479 (1) ◽  
pp. 82-89 ◽  
Author(s):  
C. W. Shepherd ◽  
R. G. Carlberg ◽  
H. K. C. Yee ◽  
E. Ellingson

2012 ◽  
Vol 68 (4) ◽  
pp. 454-467 ◽  
Author(s):  
Ian J. Tickle

The commonly used validation metrics for the local agreement of a structure model with the observed electron density, namely the real-space R (RSR) and the real-space correlation coefficient (RSCC), are reviewed. It is argued that the primary goal of all validation techniques is to verify the accuracy of the model, since precision is an inherent property of the crystal and the data. It is demonstrated that the principal weakness of both of the above metrics is their inability to distinguish the accuracy of the model from its precision. Furthermore, neither of these metrics in their usual implementation indicate the statistical significance of the result. The statistical properties of electron-density maps are reviewed and an improved alternative likelihood-based metric is suggested. This leads naturally to a χ2 significance test of the difference density using the real-space difference density Z score (RSZD). This is a metric purely of the local model accuracy, as required for effective model validation and structure optimization by practising crystallographers prior to submission of a structure model to the PDB. A new real-space observed density Z score (RSZO) is also proposed; this is a metric purely of the model precision, as a substitute for other precision metrics such as the B factor.


2007 ◽  
Vol 40 (4) ◽  
pp. 756-760 ◽  
Author(s):  
Victor-O. de Haan ◽  
Jeroen Plomp ◽  
Ad A. van Well

The phase-object approximation for neutron scattering is applied to determine the real-space sample correlation function for a sphere for kinematic and dynamic scattering. The sample correlation function determined in this way corresponds to the kinematic and refraction limits.


1985 ◽  
Vol 29 ◽  
pp. 143-152 ◽  
Author(s):  
James W. Richardson ◽  
John Faber

AbstractRietveld profile refinements using high-resolution pulsed neutron povder diffraction data, collected at IPNS, often reveal broad intensity contributions from sources other than the crystalline materials being studied. Such non-crystalline intensity hampers standard Rietveld refinement, and its removal and/or identification is imperative for successful refinement of the crystalline structure. A Fourier-filtering technique allows removal of the non-crystalline scattering contributions to the overall scattering pattern and yields information about the noncrystalline material. In particular, Fourier transformation of residual intensities not accounted for by the Rietveld procedure results in a real-space correlation function similar to a radial distribution function (RDF). From the inverse Fourier transform of the correlation function a Fourier-filtered fit to the diffuse scattering is obtained. This mathematical technique was applied to data for crystalline quartz, amorphous silica, and to a simulated diffraction pattern for a mixture of the two phases.


2020 ◽  
Vol 493 (4) ◽  
pp. 5506-5519 ◽  
Author(s):  
Boryana Hadzhiyska ◽  
Sownak Bose ◽  
Daniel Eisenstein ◽  
Lars Hernquist ◽  
David N Spergel

ABSTRACT We use the IllustrisTNG cosmological, hydrodynamical simulations to test fundamental assumptions of the mass-based halo occupation distribution (HOD) approach to modelling the galaxy–halo connection. By comparing the clustering of galaxies measured in the 300 Mpc TNG box (TNG300) with that predicted by the standard (basic) HOD model, we find that, on average, the ‘basic’ HOD model underpredicts the real-space correlation function in the TNG300 box by ∼15 per cent on scales of $1 \,\,\lt\,\, r \,\,\lt\,\, 20 \ {\rm Mpc}\, h^{-1}$, which is well beyond the target precision demanded of next-generation galaxy redshift surveys. We perform several tests to establish the robustness of our findings to systematic effects, including the effect of finite box size and the choice of halo finder. In our exploration of ‘secondary’ parameters with which to augment the ‘basic’ HOD, we find that the local environment of the halo, the velocity dispersion anisotropy, β, and the product of the half-mass radius and the velocity dispersion, σ2Rhalfmass, are the three most effective measures of assembly bias that help reconcile the ‘basic’ HOD-predicted clustering with that in TNG300. In addition, we test other halo properties such as halo spin, formation epoch, and halo concentration. We also find that at fixed halo mass, galaxies in one type of environment cluster differently from galaxies in another. We demonstrate that a more complete model of the galaxy–halo connection can be constructed if we combine both mass and local environment information about the halo.


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