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DefinitionDefinition: Literature-sourcedProof: Not applicablePipeline-generatedjudge pass (gpt-6-luna)verified 2026-10-22 (gpt-6.1-sol)
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Simple surface and geodesic X-ray transform

Definition

Let (M,g) be a compact, connected, nonempty smooth two-dimensional Riemannian manifold with smooth boundary. For x∈∂M, let νout(x) be the outward unit normal. The boundary is strictly convex if

g(∇wνout,w)>0

for every x∈∂M and every nonzero w∈Tx∂M. A Jacobi field along a unit-speed geodesic γ is a smooth vector field J along γ satisfying

Dt2J+R(J,γ˙)γ˙=0,

where R(X,Y)Z=∇X∇YZ−∇Y∇XZ−∇[X,Y]Z. The manifold has no conjugate points if, on every unit-speed geodesic segment γ:[a,b]→M, a Jacobi field with J(a)=J(b)=0 must be identically zero. It is nontrapping if every maximal unit-speed geodesic starting in M∘ reaches ∂M in finite forward and backward time. The pair (M,g) is a simple surface if its boundary is strictly convex, it has no conjugate points, and it is nontrapping.

The unit tangent bundle is SM={(x,v):x∈M, v∈TxM, gx(v,v)=1}. Write νin=−νout and

∂+SM={(x,v)∈SM:x∈∂M, gx(v,νin)>0}

for inward-pointing unit boundary vectors. For (x,v)∈∂+SM, let γx,v be the unit-speed geodesic with γx,v(0)=x and γ˙x,v(0)=v, and let τ+(x,v) be its first positive exit time from M. For f∈C∞(M), its scalar geodesic X-ray transform is the function on ∂+SM defined by

I0f(x,v)=∫0τ+(x,v)f(γx,v(t)) dt.

The geodesic equation is interpreted up to first boundary exit; local smooth extensions of the metric are used only to solve the coordinate ODE at boundary initial data.

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