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Stationary Lorentzian data and tensor conventions
Definition
Work in ZFC, including the axiom of choice. Stationary Lorentzian data here consist of a connected smooth four-manifold without boundary, an orientation, a smooth Lorentzian metric of signature , a time orientation , and a smooth vector field satisfying . The orientation is a smooth choice of a positive ray in at each point. The time orientation is a smooth field with ; a timelike vector is future-directed when .
The metric is a smooth symmetric nondegenerate covariant two-tensor with one negative and three positive directions at each point. The Lie derivative is , where is the local flow of ; a field satisfying its vanishing is called a Killing field. Thus stationary refers here to the specified pair ; it does not assert that is timelike everywhere or that its flow is complete. For a designated open region called an end, the additional convention that it is a stationary end requires to be future timelike throughout that region. Further topology or asymptotic conditions on an end must be stated separately.
Let be the Levi–Civita connection: the unique torsion-free affine connection compatible with . Its curvature convention is . In a coordinate frame write and . The Ricci tensor is denoted .
Put and . In coordinates, and denotes the inverse matrix of . Repeated upper and lower indices are summed from to . Raising indices uses and lowering them uses ; a contraction or raised tensor associated with another metric uses that metric and its own inverse.
Definition references
Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model
Killing fields of a Lorentzian metric
Metric compatibility, torsion freedom and the metric-selected connection class
The inverse metric, musical isomorphisms and index raising
The Riemann curvature operator and the derived Ricci, scalar and Einstein tensors
Facts & Assumptions
The set-theoretic convention is ZFC, including the axiom of choice. The Axiom of Choice
The Lorentzian interface gives the metric, time-orientation and future-directed conventions stated above. Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model
The Killing-field interface defines the Lie derivative using the local flow and defines a Killing field by its vanishing. Killing fields of a Lorentzian metric
A metric-selected connection is torsion-free and metric-compatible; for the stated smooth nondegenerate metric there is exactly one such connection. Metric compatibility, torsion freedom and the metric-selected connection class Existence and uniqueness of the metric-selected connection of a nondegenerate metric, and its extension to tensor fields
The inverse-metric interface supplies the inverse and the lowering and raising maps for the stated nondegenerate metric. The inverse metric, musical isomorphisms and index raising
The curvature interface fixes the displayed curvature and Ricci conventions for the metric-selected connection. The Riemann curvature operator and the derived Ricci, scalar and Einstein tensors
An orientation is a smooth choice of a ray in the determinant line of each tangent space. Oriented smooth manifolds and oriented charts
Justification
Given: The data and hypotheses in the Definition.
Goal: Show that the named fields and conventions are well-defined under those hypotheses.
1.1 The metric and time-orientation hypotheses place in the Lorentzian interface; the chosen orientation is the determinant-line datum in that interface's smooth-manifold setting. The local-flow Lie derivative and the Killing condition therefore have the stated meanings. The end condition is a further pointwise requirement on the designated region, not an assertion that such a region exists. [given, F1, F2, F6]
2.1 Nondegeneracy and smoothness supply the unique metric-compatible torsion-free connection and the inverse metric. The curvature interface then supplies the displayed Ricci contraction, while and are pointwise contractions of the supplied smooth fields. Raising and lowering with the inverse and metric of the metric currently specified is consequently unambiguous. This establishes the stated conventions without asserting completeness or an existence theorem for an end. [given, F3, F4, F5, step 1.1] ∎
External input
Carroll supplies the symmetric nondegenerate metric and Lorentzian signature conventions in Chapter 2. The flow definition of the Lie derivative and the Killing condition are recorded in Chapter 5; only their restriction to local flow domains is used here. Time orientation and future direction use the declared Lorentzian interface.
Depends on
- Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model
- Killing fields of a Lorentzian metric
- Metric compatibility, torsion freedom and the metric-selected connection class
- Existence and uniqueness of the metric-selected connection of a nondegenerate metric, and its extension to tensor fields
- The inverse metric, musical isomorphisms and index raising
- The Riemann curvature operator and the derived Ricci, scalar and Einstein tensors
- Oriented smooth manifolds and oriented charts
- The Axiom of Choice
- Sean M. Carroll, Lecture Notes on General Relativity (1997) · Chapter 2, printed pp. 47 and 49 (PDF pp. 54 and 56), equations (2.28), (2.34) and adjacent metric/signature definitions.
- Sean M. Carroll, Lecture Notes on General Relativity (1997) · Chapter 5, printed pp. 135 and 140 (PDF pp. 142 and 147), equations (5.17)-(5.18) and (5.41).
Used by · 139
- Vacuum Killing and Ernst differential identities
- Smooth invariant Harrison primitive near the horizon and at infinity
- Regular Harrison Einstein–Maxwell family
- Hawking and rotational fields near a bifurcate sphere
- Connected smooth axisymmetric vacuum Kerr classification
- Ionescu–Klainerman local Kerr criterion with full interface
- Stationary maximal hypersurface existence with a horizon boundary
- Mean-curvature variation and the stationary lapse equation
- Stationary vacuum model and asymptotic normalization
- Physical expectation of late-time stationarity
- Killing two-form and normalized Ernst notation
- Lapse, shift, induced metric and second fundamental form
- Smooth stationary multiple-black-hole nonexistence
- Reported comparison and Bertotti–Robinson strategy
- Mass-one convention and Harrison denominator
- Positivity of the Harrison denominator and horizon bound
- Stationary Harrison one-form and metric
- Local Hawking and axial fields, boost and pole
- Cartan normalization at the bifurcation pole
- Invertibility, Lorentz signature and stationary norm
- Single-potential construction of the Harrison one-form family
- Mass-one Ernst and radial primitive asymptotics
- Proposition 2.1: Einstein–Maxwell equations and regularity
- Proposition 2.1: electric and magnetic fluxes
- Coordinate components of the transformed metric
- Uniform transformed component estimates
- Preservation of bifurcate horizons and surface gravity
- Stationary maximal graphs and normalized graph heights
- Stationary section time and translated maximal sections
- Comparison spheres and their stationary cylinders
- Stationary transfer of timelike curves
- Normalized outward null normal at large coordinate spheres
- Transformed lapse equation and bounds
- Proper stationary projection for continued slices
- Asymptotic maximal graph equation and coefficients
- Lemma 3.2: compact stationary-height bounds
- Compact-tube timelike length bound
- Local causality and temporal functions on compact tubes
- Lemma 3.3: common spacelike reference collar
- Boundary angle bound and normal-graph cone
- Horizon expansion variation and Einstein–Maxwell curvature
- The Killing derivative is an exact closed two-form
- Ricci contraction of the Killing derivative
- Vanishing divergence implies closed Hodge dual
- Killing flow preserves its complex two-form
- Closed Ernst contraction and the real potential
- Stationary exact corrections preserve two prescribed gauges
- Regular bifurcate null horizon data before rigidity
- Null second fundamental form descends to the screen quotient
- Metric transport along a null generator
- A branch-tangent Killing field restricts to the bifurcation sphere
- Positive Harrison denominator and its parameter identity
- Lifting a normalized stationary primitive to the Harrison parameter
- Regular Lorentzian metric from the normalized rank-one map
- Smooth Maxwell tensor formula without division by the stationary norm
- Scope of smooth field equations at an exterior horizon boundary
- Exact asymptotic and orbit package for the IK criterion
- Exact bifurcate-sphere package for the IK criterion
- Ernst sublevels and the Mars–Simon tensor interface
- Pathwise exhaustion by anchored Ernst sublevels
- Kerr exterior tensor including the extremal parameter range
- A specified future ingoing Kerr extension and its time orientation
- Asymptotic mass and axial angular-momentum conventions
- The Kerr end is an ADM rest frame
- Exact asymptotically stationary end contract
- Differentiated stationary end bounds imply the weighted Hölder interface
- A complete stationary flow preserves its compact tangent boundary
- Isometries preserve maximality and transported boundary
- Fixing the Ernst constant by integrable asymptotic twist
- Smooth global data for the axisymmetric comparison
- Gram determinant for the two symmetry directions
- Orthogonal projection away from the symmetry plane
- Algebraic reconstruction from orbit and horizontal metric data
- Exact AIK global, horizon and quantitative hypotheses
- Connected rotating degenerate vacuum comparison data
- Harmonic-map and Weyl reconstruction comparison data
- Identification of the spherical exterior and its positive stationary lapse
- A complete stationary flow transverse positively to a Cauchy section is a product
- Uniform spatial components and the cylinder scale
- Affine null-generator profiles vanish exactly on the bifurcation section
- Affine generator profiles give constant signed acceleration
- Complete regular static exterior data and its normalized end
- Vacuum curvature of a globally static product
- The bracket of two Killing fields is Killing
- Analytic Kerr coordinates across the chosen nondegenerate horizon
- A commuting axial action preserves the stationary field and its causal character
- Weight-one regular axis gives elementary flatness of small axial orbits
- Vacuum metrics embed as stationary electrovacuum data with zero field
- A common positive Harrison domain across the compact sphere
- Stationary flow-box data for a nonzero Killing field
- Harrison equation residuals are continuous functions of stationary two-jets
- Passing a local Harrison identity through compatible stationary jets
- Extending smooth equation residuals from a dense nonzero-field locus
- AIK perturbative global regularity and bifurcation package
- Ernst and self-dual curvature data in the AIK convention
- Radu nontrapping global regularity package
- Stationary orbit space with its quotient topology
- Zero stationary energy along null geodesics
- Radu small-ADM global and bifurcation package
- Smooth event-boundary branches are achronal null geodesic sheets
- A compact spacelike surface has a normal exponential tube
- Smooth transverse horizon branches are the null axes of the normal tube
- The normal future and past quadrants are the local causal sets of the sphere
- Regular stationary event branches supply the local AIK horizon pair
- Circle-invariant normal coordinates linearize a bifurcate Killing boost
- The stationary product extends the local boost and circle to a complete collar
- Compact metric families have a common spacelike collar with fixed boost rate
- A timelike transverse field gives a fixed-boundary admissible graph neighborhood
- Stationary parameter families have a decaying reference-slice residual
- Stationarity supplies the weighted end differentiability estimates
- The global Dirichlet mean-curvature map is continuously differentiable
- An existing stationary graph supplies global projection before any estimate
- Stationary coefficients in a transverse collar retain the tangential motion
- Bounded boost times give a uniform Gaussian collar cone
- Compact estimates for arbitrary sequences of individually existing slices
- Timelike transfer supplies access to every sufficiently distant stationary cylinder
- The stationary Killing energy is constant along every affine null segment
- An asymptotically flat stationary end bounds null speed by Killing energy
- Compact normalized source data give a target-independent energy bound
- Distant targets force arbitrarily long source-normalized affine segments
- Sufficiently far stationary end points can be routed to a chosen cylinder
- Piecewise timelike transfer yields arrival on the cylinder under far-tail access
- Normalized Ernst data and zero Mars–Simon survive stationary gauges
- Zero stationary field gives the local bifurcate Killing-horizon and boundary data
- The stationary maximal vacuum divergence identity with the article sign
- A supplied complete maximal slice has zero extrinsic curvature in the zero-shift case
- A Riemannian Killing shift vanishing on the whole boundary vanishes globally
- Orthogonal flow coverage gives a global static product and the needed end bounds
- Normalized Komar data on a nonrotating horizon section
- A nonzero degenerate generator cannot vanish at a regular bifurcation section
- Geometric data for the analytic multiple-horizon comparison
- Canonical stationary end expansions give the precise source slice decay
- Cofinal stationary end representatives have the same causal exterior
- Stationary vacuum normal form and compatible regularity section
- Equivariant global Harrison primitive under weak original data
- External ADM–Komar equality on ordinary stationary vacuum ends
- Supplied CW logarithmic maximal ends have weak weighted initial data
- The same maximal slice has the differentiated article end gauge and a limiting old time
- Independent stationary maximal-gauge asymptotic expansion and KID input
Dependency tree · 2 levels
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External dependencies
A nondegenerate metric is a symmetric covariant two-tensor with an inverse; in four dimensions Lorentzian signature has one negative and three positive directions.
Hypotheses: A smooth four-manifold with the nondegenerate Lorentzian metric assumed here.
Reading limits: Read the cited PDF passages only; time orientation is supplied by the declared library interface.
The Lie derivative of the metric is its pullback derivative along the vector field flow at parameter zero; a Killing field has vanishing metric Lie derivative.
Hypotheses: A smooth metric and smooth vector field on a domain of its flow.
Reading limits: Read the cited definitions; use is restricted to local flow domains, without completeness.
Sources
- Sean M. Carroll, Lecture Notes on General Relativity (1997) · Chapter 2, printed pp. 47 and 49 (PDF pp. 54 and 56), equations (2.28), (2.34) and adjacent metric/signature definitions.
- Sean M. Carroll, Lecture Notes on General Relativity (1997) · Chapter 5, printed pp. 135 and 140 (PDF pp. 142 and 147), equations (5.17)-(5.18) and (5.41).