Redshift tomography of the kinematic matter dipole

The dipole anisotropy induced by our peculiar motion in the sky distribution of cosmologically distant sources is an important consistency test of the standard Friedmann-Lemaître-Robertson-Walker cosmology. In this work, we formalize how to compute the kinematic matter dipole in redshift bins. Apart from the usual terms arising from angular aberration and flux boosting, there is a contribution from the boosting of the redshifts that becomes important when considering a sample selected on observed redshift, leading to nonvanishing correction terms. We discuss examples and provide expressions to incorporate arbitrary redshift selection functions. We also discuss the effect of redshift measurement uncertainties in this context, in particular in upcoming surveys for which we provide estimates of the correction terms. Depending on the shape of a sample’s redshift distribution and on the applied redshift cuts, the correction terms can become substantial, even to the degree that the direction of the dipole is reversed. Lastly, we discuss how cuts on variables correlated with observed redshift, such as color, can induce additional correction terms.

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Publication Details

Journal
Physical review. D/Physical review. D.
Published
2025-06-24
DOI
https://doi.org/10.1103/physrevd.111.123547
Citations
2
Primary Topic
Gamma-ray bursts and supernovae
Type
article
Field-Weighted Citation Impact
2.31

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article

Redshift tomography of the kinematic matter dipole

Sebastian von Hausegger, Charles Dalang
2 citations
Physical review. D/Physical review. D.
Gamma-ray bursts and supernovae
2.31
article

Redshift tomography of the kinematic matter dipole

Sebastian von Hausegger, Charles Dalang
article en
2 citations

Abstract

The dipole anisotropy induced by our peculiar motion in the sky distribution of cosmologically distant sources is an important consistency test of the standard Friedmann-Lemaître-Robertson-Walker cosmology. In this work, we formalize how to compute the kinematic matter dipole in redshift bins. Apart from the usual terms arising from angular aberration and flux boosting, there is a contribution from the boosting of the redshifts that becomes important when considering a sample selected on observed redshift, leading to nonvanishing correction terms. We discuss examples and provide expressions to incorporate arbitrary redshift selection functions. We also discuss the effect of redshift measurement uncertainties in this context, in particular in upcoming surveys for which we provide estimates of the correction terms. Depending on the shape of a sample’s redshift distribution and on the applied redshift cuts, the correction terms can become substantial, even to the degree that the direction of the dipole is reversed. Lastly, we discuss how cuts on variables correlated with observed redshift, such as color, can induce additional correction terms.

Physical review. D/Physical review. D.Vol. 111(12)
Queen Mary University of London (GB), University of Oxford (GB), University of Portsmouth (GB)
European Research Council
Openalex Percentile: Top 11%
Gamma-ray bursts and supernovae
2.31
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Redshift tomography of the kinematic matter dipole — Sebastian von Hausegger, Charles Dalang · Physical review. D/Physical review. D. (2025) | TGRS Research Map | TGRS