The Finite Primitive Basis Theorem for Computational Imaging: Formal Foundations of the OperatorGraph Representation
Organizations: NextGen PlatformAI C Corp, USA
Abstract
Computational imaging forward models, from coded aperture spectral cameras to MRI scanners, are traditionally implemented as monolithic, modality-specific codes. We prove that every forward model in a broad, precisely defined operator class Cimg (encompassing clinical, scientific, and industrial imaging modalities, both linear and nonlinear) admits an epsilon-approximate representation as a typed directed acyclic graph (DAG) whose nodes are drawn from a library of exactly 11 canonical primitives: Propagate, Modulate, Project, Encode, Convolve, Accumulate, Detect, Sample, Disperse, Scatter, and Transform. We call this the Finite Primitive Basis Theorem. The proof is constructive: we provide an algorithm that, given any H in Cimg, produces a DAG G with relative operator error at most epsilon and graph complexity within prescribed bounds. We further prove that the library is minimal: removing any single primitive causes at least one modality to lose its epsilon-approximate representation. A systematic analysis of nonlinearities in imaging physics shows they fall into two structural categories: pointwise scalar functions (handled by Transform) and self-consistent iterations (unrolled into existing linear primitives). Empirical validation on 31 linear modalities confirms eimg below 0.01 with at most 5 nodes and depth 5, and we provide constructive DAG decompositions for 9 additional nonlinear modalities. These results establish mathematical foundations for the Physics World Model (PWM) framework.
Figures & tables
| Modality | Carrier | DAG Primitives | #N | Depth | |
|---|---|---|---|---|---|
| Full-validation modalities (forward model verified against reference implementation) | |||||
| CASSI [ 22 ] | Photon | 4 | 4 | ||
| CACTI [ 27 ] | Photon | 3 | 3 | ||
| SPC [ 28 ] | Photon | 3 | 3 | ||
| Lensless [ 29 ] | Photon | 2 | 2 | ||
| Ptychography [ 30 ] | Photon | 3 | 3 | ||
| Modality | #Nodes / Depth | New Prim.? | |
|---|---|---|---|
| Held-out (existing primitives expected) | |||
| OCT | 4 / 3 | N | |
| Photoacoustic | 3 / 3 | N | |
| SIM | 3 / 3 | N | |
| Phase-contrast X-ray | 4 / 4 | N | |
| Electron ptycho | 3 / 3 | N | |
| Modality | DAG Primitives | ? |
|---|---|---|
| Polychromatic CT (beam hard.) | Y | |
| Phase-wrapped MRI | Y | |
| Nonlinear ultrasound | Y | |
| MPI (Langevin response) | Y | |
| DOT (strong mult. scatt.) | N | |
| EIT (impedance tomo.) | N |
Appendix figures & tables4 assets
Supplementary material from the paper’s appendix.
Appendix
| Primitive | Relative error | Pass ( )? |
|---|---|---|
| Propagate | Y | |
| Modulate | Y | |
| Project | Y | |
| Encode | Y | |
| Convolve | Y | |
| Accumulate | Y |
| Modality | Primitive | ? | |
| CASSI | (binary mask) | Y | |
| (unitary shift) | Y | ||
| ( ) | Y | ||
| (normalized gain) | Y | ||
| MRI | (normalized) | Y | |
| (unitary DFT) | Y |
| Modality | Carrier | DAG Primitives | #N | Depth |
|---|---|---|---|---|
| Neutron imaging | Neutron | 2 | 2 | |
| Holography | Photon | 3 | 3 | |
| STED | Photon | 2 | 2 | |
| Light-field | Photon | 3 | 3 | |
| FPM | Photon | 3 | 3 | |
| Spectral CT | X-ray | 3 | 3 |
| Q# | Question | Yes | No |
|---|---|---|---|
| 1 | Does involve free-space carrier evolution (propagation through vacuum, air, tissue, etc.)? | Propagation family or | Go to Q2 |
| 2 | Does involve carrier–matter interaction? | Go to Q2a | Go to Q3 |
| 2a | Does the interaction change carrier direction or energy? | Scattering family (or for multiple scattering) | Elastic interaction |
| 3 | Does map spatial information to a measurement coordinate? | Go to Q3a | Detection–readout |
| 3a | Is the mapping a line integral (projection geometry)? | (Fourier encoding) |