Lopsided and Bulging Distribution of Satellites around Paired Halos. II. 3D Analysis and Dependence on Projection and Selection Effects

Abstract We use the Illustris-TNG300 simulation to investigate the anisotropic distribution of subhalos in/around dark matter halo pairs. We measure the position angle ( θ ) of each subhalo by the angle between the line connecting it to the nearest host halo and the line connecting the paired halos, and examine <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>P</mml:mi> <mml:mo stretchy="false">(</mml:mo> <mml:mi>cos</mml:mi> <mml:mi>θ</mml:mi> <mml:mo stretchy="false">)</mml:mo> </mml:math> (the distribution of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>cos</mml:mi> <mml:mi>θ</mml:mi> </mml:math> of all subhalos) for halo pairs with various separations ( d sep ), primary halo masses ( M p ), and secondary-to-primary halo mass ratios ( M s / M p ). We find that <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>P</mml:mi> <mml:mo stretchy="false">(</mml:mo> <mml:mi>cos</mml:mi> <mml:mi>θ</mml:mi> <mml:mo stretchy="false">)</mml:mo> </mml:math> generally exhibits a combined result of two distinct features: the “bulging” distribution characterized by an overabundance along the pairwise direction, and the “lopsided” distribution showing an overabundance in the region between the paired halos. The bulging signal is stronger for halo pairs with larger d sep and smaller M p , while the lopsidedness strengthens as M p increases. Both signals depend weakly on M s / M p , and are primarily contributed by subhalos that are relatively distant from the host halos. Remarkably, these measurements can be broadly reproduced by the overlap effect, provided the spatial alignment of the halos is properly taken into account. Our findings suggest distinct origins: lopsidedness arises from simple halo overlap, while bulging reflects alignment with large-scale filaments. We examine the impact of projection and selection effects by conducting the same analysis in two dimensions and in a mock catalog that replicates the selection effects of the Sloan Digital Sky Survey galaxy sample. We find that the 3D-to-2D projection significantly suppresses the bulging distribution, with particularly strong effects at large d sep , small M p , and large M s / M p .

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Publication Details

Journal
The Astrophysical Journal
Published
2025-10-03
DOI
https://doi.org/10.3847/1538-4357/adfede
Primary Topic
Stellar, planetary, and galactic studies
Type
article
Field-Weighted Citation Impact
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article

Lopsided and Bulging Distribution of Satellites around Paired Halos. II. 3D Analysis and Dependence on Projection and Selection Effects

Qianyu Ma, Yi-Qing Guo, Cheng Li
The Astrophysical Journal
Stellar, planetary, and galactic studies
article

Lopsided and Bulging Distribution of Satellites around Paired Halos. II. 3D Analysis and Dependence on Projection and Selection Effects

Qianyu Ma, Yi-Qing Guo, Cheng Li
article en

Abstract

Abstract We use the Illustris-TNG300 simulation to investigate the anisotropic distribution of subhalos in/around dark matter halo pairs. We measure the position angle ( θ ) of each subhalo by the angle between the line connecting it to the nearest host halo and the line connecting the paired halos, and examine <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>P</mml:mi> <mml:mo stretchy="false">(</mml:mo> <mml:mi>cos</mml:mi> <mml:mi>θ</mml:mi> <mml:mo stretchy="false">)</mml:mo> </mml:math> (the distribution of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>cos</mml:mi> <mml:mi>θ</mml:mi> </mml:math> of all subhalos) for halo pairs with various separations ( d sep ), primary halo masses ( M p ), and secondary-to-primary halo mass ratios ( M s / M p ). We find that <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>P</mml:mi> <mml:mo stretchy="false">(</mml:mo> <mml:mi>cos</mml:mi> <mml:mi>θ</mml:mi> <mml:mo stretchy="false">)</mml:mo> </mml:math> generally exhibits a combined result of two distinct features: the “bulging” distribution characterized by an overabundance along the pairwise direction, and the “lopsided” distribution showing an overabundance in the region between the paired halos. The bulging signal is stronger for halo pairs with larger d sep and smaller M p , while the lopsidedness strengthens as M p increases. Both signals depend weakly on M s / M p , and are primarily contributed by subhalos that are relatively distant from the host halos. Remarkably, these measurements can be broadly reproduced by the overlap effect, provided the spatial alignment of the halos is properly taken into account. Our findings suggest distinct origins: lopsidedness arises from simple halo overlap, while bulging reflects alignment with large-scale filaments. We examine the impact of projection and selection effects by conducting the same analysis in two dimensions and in a mock catalog that replicates the selection effects of the Sloan Digital Sky Survey galaxy sample. We find that the 3D-to-2D projection significantly suppresses the bulging distribution, with particularly strong effects at large d sep , small M p , and large M s / M p .

The Astrophysical JournalVol. 992(1)
Openalex Percentile: Top 81%
Stellar, planetary, and galactic studies
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