Fourier transform and symmetry were my working tools — not vocabulary borrowed from physics, the actual instruments.
In neutron scattering, the Fourier transform reveals what is invisible in real space: periodicities, lattice parameters,
spatial correlations already present in the material but not readable until the representation changes.
Symmetry governs what is conserved, what is invariant.
And nothing focuses a physicist's attention faster than symmetry breaking — the phase transition, the spontaneous reorganization,
the moment one stable order gives way to another.
Both series grow directly from this toolbox. In Q Space, the Fourier transform is applied to photographic data — same operation, different subject. The image encodes frequency content and spatial periodicity rather than object identity. But the mathematics alone does not determine the output: how the magnitude is handled, how the original color space maps to the resulting frequency field — these are decisions, not equations. That is where the work becomes authored rather than computed.
In Kaleidoscopes, it is symmetry that operates — but not to measure or analyze. Rotational symmetry is imposed on a photographic fragment: a wedge sampled, duplicated, closed. The source is forced into an order it never had. What makes the result interesting is that the imposed symmetry is immediately compromised by the source material — directional textures, residual asymmetries, edges that resist alignment. The image lives at that threshold.
Two fixed operations. In each, creative latitude appears at a different point: in Q Space at the rendering of the output, in Kaleidoscopes at the selection of the input and the handling of color.
Out of the lab, the same tools hold. What changed is what the physicist uses them to make.
Different domain. Identical logic.