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BEACON: JWST NIRCam Pure-parallel Imaging Survey. III. Constraints on the Ultraviolet Luminosity Function and the Clustering of z ∼ 7–14 Galaxies

  • Authors: Kimi C. Kreilgaard, Charlotte A. Mason, Takahiro Morishita, Yechi Zhang, Viola Gelli, Nicha Leethochawalit, Tommaso Treu, Michele Trenti, Abdurro'uf, Hakim Atek, Maruša Bradac, Larry D. Bradley, Andrew J. Bunker, Novan Saputra Haryana, Matthew J. Hayes, Zhaoran Liu, Vihang Mehta, Marc Rafelski, Guido Roberts-Borsani, Claudia Scarlata, Massimo Stiavelli, Ryo A. Sutanto, Kosuke Takahashi, Benedetta Vulcani

Kimi C. Kreilgaard et al 2026 The Astrophysical Journal 1009 .

  • Provider: AAS Journals

Caption: Figure 10.

Distributions of the probability of observing Nobs sources or more in a field where ﹩{N}_{{\rm{\exp }}}﹩ sources are expected, measured for, respectively, all fields (orange) and fields hosting at least one bright MUV < − 20.5 source (black, hatched), in three redshift bins: 7 < z < 8.5, 8.5 < z < 10, and 10 < z < 11.5 (left to right panel). The lower the value of ﹩P(N\,\geqslant \,{N}_{{\rm{obs}}}| {N}_{{\rm{\exp }}})﹩, the more unlikely it is that we observed Nobs galaxies, and thus the more statistically significant it is that a field is overdense. The dashed lines mark regions corresponding to Poisson probabilities of ﹩P(N\,\geqslant \,{N}_{{\rm{obs}}}| {N}_{{\rm{\exp }}})\lt 0.003﹩ and <0.05, equivalent to the one-sided 3σ and 2σ tail probabilities of a Gaussian distribution, respectively. Throughout the paper we refer to these thresholds as the 3σ and 2σ overdensity levels.

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