Gregory J. Galloway’s research while affiliated with University of Miami and other places

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Publications (150)


Rigidity Aspects of Penrose’s Singularity Theorem
  • Article
  • Full-text available

January 2025

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3 Reads

Communications in Mathematical Physics

Gregory Galloway

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Eric Ling

In this paper, we study rigidity aspects of Penrose’s singularity theorem. Specifically, we aim to answer the following question: if a spacetime satisfies the hypotheses of Penrose’s singularity theorem except with weakly trapped surfaces instead of trapped surfaces, then what can be said about the global spacetime structure if the spacetime is null geodesically complete? In this setting, we show that we obtain a foliation of MOTS which generate totally geodesic null hypersurfaces. Depending on our starting assumptions, we obtain either local or global rigidity results. We apply our arguments to cosmological spacetimes (i.e., spacetimes with compact Cauchy surfaces) and scenarios involving topological censorship.

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Aspects of the geometry and topology of expanding horizons

November 2024

Proceedings of the American Mathematical Society

The aim of this paper is to extend some basic results about marginally outer trapped surfaces to the context of surfaces having general null expansion. Motivated in part by recent work of Chai-Wan, we introduce the notion of g \mathfrak {g} -stability for a general closed hypersurface Σ \Sigma in an ambient initial data set and prove that, under natural energy conditions, Σ \Sigma has positive Yamabe type, that is, Σ \Sigma admits a metric of positive scalar curvature, provided Σ \Sigma is g \mathfrak {g} -stable. A similar result is obtained when Σ \Sigma is embedded in a null hypersurface of a spacetime satisfying the dominant energy condition. Area bounds under similar conditions are obtained in the case where Σ \Sigma is 2 2 -dimensional. Conditions implying g \mathfrak {g} -stability are also discussed. Finally, we obtain a spacetime positive mass theorem for initial data sets with compact boundary Σ \Sigma of positive null expansion, assuming that the dominant energy condition is sufficiently strict near Σ \Sigma . This extends recent results of Galloway-Lee and Lee-Lesourd-Unger.


A CMC existence result for expanding cosmological spacetimes

October 2024

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6 Reads

We establish a new CMC (constant mean curvature) existence result for cosmological spacetimes, i.e., globally hyperbolic spacetimes with compact Cauchy surfaces satisfying the strong energy condition. If the spacetime contains an expanding Cauchy surface and is future timelike geodesically complete, then the spacetime contains a CMC Cauchy surface. This result settles, under certain circumstances, a conjecture of the authors and a conjecture of Dilts and Holst. Our proof relies on the construction of barriers in the support sense, and the CMC Cauchy surface is found as the asymptotic limit of mean curvature flow. Analogous results are also obtained in the case of a positive cosmological constant Λ>0\Lambda > 0. Lastly, we include some comments concerning the future causal boundary for cosmological spacetimes which pertain to the CMC conjecture of the authors.


Some rigidity results for charged initial data sets

July 2024

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8 Reads

In this note, we consider some initial data rigidity results concerning marginally outer trapped surfaces (MOTS). As is well known, MOTS play an important role in the theory of black holes and, at the same time, are interesting spacetime analogues of minimal surfaces in Riemannian geometry. The main results presented here expand upon earlier works by the authors, specifically addressing initial data sets incorporating charge.


Mean Curvature, Singularities and Time Functions in Cosmology

July 2024

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16 Reads

In this contribution, we study spacetimes of cosmological interest, without making any symmetry assumptions. We prove a rigid Hawking singularity theorem for positive cosmological constant, which sharpens known results. In particular, it implies that any spacetime with Ricng\operatorname{Ric} \geq -ng in timelike directions and containing a compact Cauchy hypersurface with mean curvature HnH \geq n is timelike incomplete. We also study the properties of cosmological time and volume functions, addressing questions such as: When do they satisfy the regularity condition? When are the level sets Cauchy hypersurfaces? What can one say about the mean curvature of the level sets? This naturally leads to consideration of Hawking type singularity theorems for Cauchy surfaces satisfying mean curvature inequalities in a certain weak sense.


A note on null distance and causality encoding

December 2023

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2 Reads

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3 Citations

Under natural conditions, the null distance introduced by Sormani and Vega [10] is a metric space distance function on spacetime, which, in a certain precise sense, can encode the causality of spacetime. The null distance function requires the choice of a time function. The purpose of this note is to observe that the causality assumptions related to such a choice in results used to establish global encoding of causality, due to Sakovich and Sormani [9] and to Burtscher and García-Heveling [2], can be weakened.


Remarks on the size of apparent horizons

Letters in Mathematical Physics

Marginally outer trapped surfaces (also referred to as apparent horizons) that are stable in 3-dimensional initial data sets obeying the dominant energy condition strictly are known to satisfy an area bound. The main purpose of this note is to show (in several ways) that such surfaces also satisfy a diameter bound. Some comments about higher dimensions are also presented.


Some rigidity results for compact initial data sets

October 2023

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1 Citation

Transactions of the American Mathematical Society

In this paper, we prove several rigidity results for compact initial data sets, in both the boundary and no boundary cases. In particular, under natural energy, boundary, and topological conditions, we obtain a global version of the main result by Galloway and Mendes [Comm. Anal. Geom. 26 (2018), pp. 63–83]. We also obtain some extensions of results by Eichmair, Galloway, and Mendes [Comm. Math. Phys. 386 (2021), pp. 253–268]. A number of examples are given in order to illustrate some of the results presented in this paper.



A note on null distance and causality encoding

June 2023

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14 Reads

Under natural conditions, the null distance introduced by Sormani and Vega [10] is a metric space distance function on spacetime, which, in a certain precise sense, can encode the causality of spacetime. The null distance function requires the choice of a time function. The purpose of this note is to observe that the causality assumptions related to such a choice in results used to establish global encoding of causality, due to Sakovich and Sormani [9] and to Burtscher and Garc\'ia-Heveling [2], can be weakened.


Citations (61)


... We recall some basic constructions below. See [2,3,17,23,40,43,47] for more details and insights, and Section 4.3 for some proofs in the more general setting of cone structures. ...

Reference:

A conformal Hopf-Rinow theorem for semi-Riemannian spacetimes
A note on null distance and causality encoding

... An important precursor to the principle of topological censorship (in conjunction with the weak cosmic censorship conjecture) is the Gannon-Lee singularity theorem ([22, Prop. 1.2], [25]), which establishes conditions under which nontrivial topology leads to null geodesic incompleteness; see also [9,10,19,31]. In this section we obtain some rigidity results in this context. ...

The codimension 2 null cut locus with applications to spacetime topology
  • Citing Article
  • December 2022

... We refer to [8] for a discussion on the existence of CMC Cauchy surfaces in cosmological spacetimes. As explained in that reference, most existence results rely on barrier methods, see [11] for an application. Moreover, Bartnik constructed a timelike geodesically incomplete cosmological spacetime which satisfies the strong energy condition and which contains no CMC Cauchy surfaces via the following gluing argument: Take one half of maximally extended Schwarzschild and glue 1 it to an FLRW model which is spatially T 3 , then extend it to the Schwarzschild event horizon and attach there a time-inverted copy of the same spacetime. ...

Remarks on the Existence of CMC Cauchy Surfaces
  • Citing Chapter
  • October 2022

... In both cases, the proofs rely on the µ-bubble technique. (f ) It would be interesting to compare Theorem 1.5 with some recent progress in proving positive mass and rigidity results for ALH manifolds (see [1,16,17,26]); in this latter development, manifolds are often assumed to have nonempty inner boundary with the mean curvature bound H ≤ n − 1 (now H is computed with respect to the inner unit normal); such mean curvature bounds serve as barrier conditions in the method of 'marginally outer trapped surfaces' (MOTS), which can be viewed as a generalization of the µ-bubble technique. ...

Positive mass theorems for asymptotically hyperbolic Riemannian manifolds with boundary

... The initial data DEC is a main assumption in the (spacetime) positive mass theorem, whose first instances were proved back in the 1980s [16,19,20] but which lately lead to new results applying to nonspin manifolds [5], involving boundaries [6] and focusing on the equality case [13,14]. A more detailed (and more complete) account of these developments can be found in the recent textbook by Dan Lee [15]. ...

A note on the positive mass theorem with boundary

Letters in Mathematical Physics

... We refer to [CG21] for the precise definitions of the various objects involved in this statement. The proof relies on the fact that such a spacetime naturally leads to a triplet (M n , g, V ), corresponding to a spin asymptotically flat static vacuum with an outwarddirected equipotential photon surface Σ as boundary. ...

Photon surfaces with equipotential time slices
  • Citing Article
  • March 2021

... In order to state the result, some restrictions on the topology of the domain (Ω, g) and its relation to the surface of interest Σ, will be needed. In particular, we will utilize the so called homotopy condition from [9], which generalizes the situation in which there is a retraction of Ω onto its boundary component Σ. The manifold Ω will be said to satisfy the homotopy condition with respect Σ, if there exists a continuous map ρ : Ω → Σ such that its composition with inclusion ρ•i : Σ → Σ is homotopic to the identity. ...

Initial Data Rigidity Results

Communications in Mathematical Physics

... Much or our analysis will hold for arbitrary (positive) values of m, and sometimes for arbitrary κ. These cases have applications; e.g., see [5] for an application of the m = 1 case to cosmology. When κ = 0, then B is a symmetric (0, 2)-tensor, and even for the applications of interest in this paper the arbitrariness of m will be useful. ...

The Topology of General Cosmological Models

... While spt m j is connected along the sequence, spt m ∞ consists of two isolated points, lying on the future and past boundaries of the space. Although weights may seem exotic, they appear in physical contexts including Brans-Dicke theory [67] and the near horizon geometry of black holes [32]. Several possible interpretations of our example seem possible. ...

A Bakry–Émery Almost Splitting Result With Applications to the Topology of Black Holes

Communications in Mathematical Physics