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    Matching collapse and expansion across matter trapping surfaces in inhomogeneous ΛCDM models

    Alan Maciel1,*, M. Le Delliou2,3,4,†, and José P. Mimoso5,‡

    • 1Centro de Matemática, Computação e Cognição, Universidade Federal do ABC, Avenida dos Estados 5001, CEP 09210-580, Santo André, São Paulo, Brazil
    • 2Institute of Theoretical Physics and Research Center of Gravitation, Lanzhou University, Lanzhou 730000, China, Key Laboratory of Quantum Theory and Applications of MoE, Lanzhou University, Lanzhou 730000, China, and Lanzhou Center for Theoretical Physics and Key Laboratory of Theoretical Physics of Gansu Province, Lanzhou University, Lanzhou 730000, China
    • 3Instituto de Astrofísica e Ciências do Espaço, Universidade de Lisboa, Faculdade de Ciências, Edifício C8, Campo Grande, 1769-016 Lisboa, Portugal
    • 4Université de Paris-Cité, APC-Astroparticule et Cosmologie (UMR-CNRS 7164), F-75006 Paris, France
    • 5Departamento de Física and Instituto de Astrofísica e Ciências do Espaço, Faculdade de Ciências da Universidade de Lisboa, Campo Grande, Edifício C8 1749-016 Lisboa, Portugal

    • *Contact author: alan.silva@ufabc.edu.br
    • †Contact author: delliou@lzu.edu.cn, Morgan.LeDelliou.IFT@gmail.com
    • ‡Contact author: jpmimoso@fc.ul.pt, jpmimoso@ciencias.ulisboa.pt

    Phys. Rev. D 114, 064004 – Published 2 September, 2026

    DOI: https://doi.org/10.1103/hh9p-jwh2

    Abstract

    In previous works, matter trapping surfaces (MTS) were defined as hypersurfaces separating cosmologically expanding regions of spacetime from regions where collapse can take place independently. In the present work we examine the MTS, for the restriction to spherical dust plus Λ, proving that it actually is a characteristic surface of the Cauchy problem (generated by its characteristic curves), which opens the possibility for infinite solutions. This translate as the MTS being a boundary between arbitrarily independent solutions, reminiscent of the Birkhoff theorem effects. This property is illustrated with combinations of three examples containing MTSs and Λ (ΛCDM, Schwarzschild–de Sitter, Λ+Lemaître–Tolman–Bondi: ΛLTB—i.e., the inhomogeneous, spherically symmetric ΛCDM). The ΛLTB model presents a static, stable MTS for the first time.

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