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Oppenheimer–Snyder

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Oppenheimer–Snyder
NameOppenheimer–Snyder
FieldPhysics, General relativity
AuthorsJ. Robert Oppenheimer, Hartland S. Snyder
Year1939
Known forGravitational collapse model, analytic black hole formation

Oppenheimer–Snyder The Oppenheimer–Snyder solution is a seminal 1939 analytic model describing gravitational collapse of a homogeneous dust sphere within General relativity, demonstrating formation of an event horizon and a singularity. Developed by J. Robert Oppenheimer and Hartland S. Snyder, it connects solutions of the Schwarzschild metric with interior Friedmann–Lemaître–Robertson–Walker dynamics and influenced later work by physicists and institutions studying gravitational collapse, including researchers at Princeton University, California Institute of Technology, and Institute for Advanced Study.

Introduction

The Oppenheimer–Snyder model provided the first clear analytic demonstration that nonrotating matter can collapse to form a black hole within Einstein field equations, linking the homogeneous dust solution of Friedmann equations to the exterior Schwarzschild solution. Its publication catalyzed research by contemporaries such as Subrahmanyan Chandrasekhar, Lev Landau, John Wheeler, Roger Penrose, and Stephen Hawking, and shaped programs at institutions like Cambridge University and Harvard University. The model remains a pedagogical cornerstone in treatments in texts by Misner, Thorne & Wheeler, Carroll, and Weinberg.

Historical background and development

Work leading to the model drew on earlier results by Karl Schwarzschild (Schwarzschild interior and exterior solutions), Alexander Friedmann (expanding universe models), and contributions by Georges Lemaître and Howard Robertson. Oppenheimer and Snyder, then associated with University of California, Berkeley and Cornell University respectively, synthesized collapse and stellar evolution insights from figures like Arthur Eddington, S. Chandrasekhar, and Walter Baade. The model appeared in the context of contemporaneous studies by Fritz Zwicky and Walter Baade on supernovae and compact remnants, and preceded rigorous singularity theorems later proven by Roger Penrose and Stephen Hawking with links to work at University of Cambridge and Institute for Advanced Study.

Oppenheimer–Snyder model

The model idealizes a spherical, pressureless dust cloud with uniform density collapsing from rest, matching an interior closed Friedmann–Lemaître–Robertson–Walker spacetime to an exterior Schwarzschild metric across a comoving boundary. It assumes no rotation or charge, distinguishing it from solutions like Kerr metric and Reissner–Nordström metric. The model’s matter content is a pressureless fluid aligned with Tolman–Oppenheimer–Volkoff considerations but simplified to zero pressure, contrasting with realistic neutron-star models by Oppenheimer and Volkoff and later numerical simulations by groups at Max Planck Institute for Gravitational Physics and Caltech. The scenario illustrates key notions tied to Event Horizon formation described in later work by John Archibald Wheeler and David Finkelstein.

Mathematical formulation

Mathematically, the interior uses a closed FLRW metric with scale factor obeying Friedmann equations for dust, while the exterior is the static Schwarzschild solution with mass parameter set by the total dust mass. Matching conditions employ the Darmois–Israel junction formalism later formalized by Werner Israel, ensuring continuity of the induced metric and extrinsic curvature across the boundary. Coordinates used include comoving synchronous coordinates for the interior and Schwarzschild coordinates for the exterior; alternative coordinate systems such as Eddington–Finkelstein coordinates and Kruskal–Szekeres coordinates clarify causal structure, a technique refined by Martin Kruskal and George Szekeres. The collapse yields a central curvature singularity where scalars like the Kretschmann scalar diverge, a phenomenon connected to singularity theorems by Roger Penrose.

Physical interpretation and implications

Physically, the model demonstrates that a sufficiently massive, pressureless, nonrotating sphere collapses to form an event horizon before a singularity forms, implying observational consequences explored by Subrahmanyan Chandrasekhar and James B. Hartle. It highlights coordinate-dependent descriptions: observers at infinity (Schwarzschild observer) see the surface asymptotically approach the Schwarzschild radius, while comoving observers reach the singularity in finite proper time, an insight emphasized in lectures by Wheeler and Misner. The model influenced the conceptual framework for astrophysical objects such as black hole candidates in x-ray binaries like Cygnus X-1 and informed theoretical work on cosmic censorship by Roger Penrose and on Hawking radiation by Stephen Hawking. It also underpins thought experiments by Leonard Susskind and Gerard 't Hooft concerning complementarity and entropy bounds by Jacob Bekenstein.

Extensions and generalizations

Extensions incorporate nonzero pressure, radiation, anisotropy, rotation, charge, inhomogeneity, and alternative equations of state, connecting to solutions such as the Tolman–Bondi metric (inhomogeneous dust), Vaidya metric (radiating bodies), Kerr metric (rotating collapse approximations), and charged collapse studies using the Reissner–Nordström metric. Numerical relativity groups at Max Planck Institute for Gravitational Physics, Syracuse University, University of Illinois Urbana–Champaign, and Caltech have simulated collapse including microphysics from nuclear equations of state studied by J. M. Lattimer and F. D. Swesty. Quantum gravity motivated modifications involve approaches by Loop Quantum Gravity researchers like Abhay Ashtekar and string theory groups at Princeton University and Institute for Advanced Study, exploring singularity resolution and horizon structure modifications.

Criticisms and limitations

Criticisms focus on idealizations: strict spherical symmetry, zero pressure, absence of rotation and magnetic fields, and perfect homogeneity, which limit direct astrophysical applicability compared to realistic collapse in supernovae studied by H. A. Bethe and collective simulations by teams at Oak Ridge National Laboratory and Los Alamos National Laboratory. The model does not capture neutrino transport central to core-collapse supernova theory advanced by Stan Woosley and Chris Fryer, nor does it include angular momentum effects central to accretion-disk and jet formation studied by Blandford–Znajek mechanisms attributed to Roger Blandford and Roman Znajek. Despite limitations, the model remains a clear, exact solution within Einstein field equations and a benchmark for comparing more complex scenarios investigated by contemporary researchers at MIT, Stanford University, and Rutgers University.

Category:General relativity