K-transform

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In mathematics, the K transform (also called the Single-Pixel X-ray Transform) is an integral transform introduced by R. Scott Kemp and Ruaridh Macdonald in 2016.[1] The transform allows the structure of a N-dimensional inhomogeneous object to be reconstructed from scalar point measurements taken in the volume external to the object.

Gunther Uhlmann proved[2] that the K transform exhibits global uniqueness on n, meaning that different objects will always have a different K transform. This uniqueness arises by the use of a monotone, nonlinear transform of the X-ray transform. By selecting the exponential function for the monotone nonlinear function, the behavior of the K transform coincides with attenuation of particles in matter as described by the Beer–Lambert law, and the K transform can therefore be used to perform tomography of objects using a low-resolution single-pixel detector.

An inversion formula based on a linearization was offered by Lai et al., who also showed that the inversion is stable under certain assumptions.[3] A numerical inversion using the BFGS optimization algorithm was explored by Fichtlscherer.[4]

Definition

Let an object f be a function of compact support that maps into the positive real numbers f:Ω0+. The K-transform of the object f is defined as 𝒦:L1(Ω,0+)[0,1], 𝒦f(r)LD(r)e𝒫f(l)dl, where LD(r)L(r)L(D) is the set of all lines originating at a point r and terminating on the single-pixel detector D, and 𝒫 is the X-ray transform.

Proof of global uniqueness

Let 𝒫f be the X-ray transform transform on n and let 𝒦 be the non-linear operator defined above. Let L1 be the space of all Lebesgue integrable functions on n , and L be the essentially bounded measurable functions of the dual space. The following result says that 𝒦 is a monotone operator.

For f,gL1 such that 𝒦f,𝒦gL then 𝒦f𝒦g,fg0 and the inequality is strict when fg.

Proof. Note that 𝒫f(r,θ) is constant on lines in direction θ, so 𝒫f(r,θ)=𝒫f(Eθr,θ), where Eθ denotes orthogonal projection on θ. Therefore:

𝒦f𝒦g,fg=n𝕊n1(e𝒫f(r,θ)e𝒫g(r,θ))(fg)(r)dθdr

=𝕊n1n(e𝒫f(r,θ)e𝒫g(r,θ))(fg)(r)drdθ

=𝕊n1θ(e𝒫f(Eθr,θ)e𝒫g(Eθr,θ))(fg)(Eθr+sθ)dsdrHdθ

=𝕊n1θ(e𝒫f(Eθr,θ)e𝒫g(Eθr,θ))(𝒫f(Eθr,θ)𝒫g(Eθr,θ))drHdθ

where drH is the Lebesgue measure on the hyperplane θ. The integrand has the form (eset)(st), which is negative except when s=t and so 𝒦f𝒦g,fg<0 unless 𝒫f=𝒫g almost everywhere. Then uniqueness for the X-Ray transform implies that g=f almost everywhere.

Lai et al. generalized this proof to Riemannian manifolds.[3]

Applications

The K transform was originally developed as a means of performing a physical one-time pad encryption of a physical object.[1] The nonlinearity of the transform ensures the there is no one-to-one correspondence between the density f and the true mass 𝕊n1f(x+sθ)dsdθ, and therefore f cannot be estimated from a single projection.

References

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