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Flat Eleven-Dimensional CJS Bosonic Vacuum

Physical scope

Exact example of a source-free classical bosonic solution in the adopted two-derivative CJS truncation. It asserts neither supersymmetry nor quantum stability.

Statement

On M=R1,10 with coordinates x0,…,x10, orientation dx0∧⋯∧dx10, and metric

g=η=−(dx0)2+∑i=110(dxi)2,

take C3=0, so F4=dC3=0. This is an exact source-free bosonic solution of the field equations in Source-Free Eleven-Dimensional CJS Bosonic Field Equations for the action of Eleven-Dimensional CJS Supergravity Bosonic Action.

Facts & Assumptions

Given: The adopted source-free CJS bosonic action and its field equations, and the stated smooth flat Lorentzian fields on R1,10.

[F1]

Eleven-Dimensional Oriented Lorentzian Geometry fixes the signature and Hodge-star convention; Levi-Civita Connection on an Eleven-Dimensional Lorentzian Manifold gives the Levi-Civita coefficients from the metric.

[F2]

Eleven-Dimensional CJS Supergravity Bosonic Action and Source-Free Eleven-Dimensional CJS Bosonic Field Equations specify the model and the conditional classical equations being checked.

Proof

technique · direct substitution
1.1F1algebra

The metric components are constant, so every partial derivative ∂MgNQ vanishes. The Christoffel formula in Levi-Civita Connection on an Eleven-Dimensional Lorentzian Manifold therefore gives ΓPMN=0. Substitution in the stated curvature convention gives RPQMN=0, hence RMN=0 and R=0.

2.1F1F2step 1.1algebra

Since C3=0, F4=dC3=0; linearity of d and ∗g gives dF4=0, ∗gF4=0, d∗gF4=0, and F4∧F4=0. Thus the four-form equation is zero equals zero. Every component FMABCFNABC and FABCDFABCD is zero, while RMN=0 by step 1.1, so the Einstein equation also holds.

3.1F2step 1.1step 2.1∎

Each term of the action density vanishes for these fields. The configuration is therefore an exact solution of the stated source-free classical bosonic equations. No Killing-spinor condition or supersymmetry conclusion is asserted.

Depends on

Dependency tree · 2 levels