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Sandbox Physics
Interference as a record and a ruler

Apparatus · Observation · Inference

Gabor: a photograph that preserves a wave reference

Sandbox Physics ·

How can an intensity record later reconstruct the direction and curvature of a wave?

  1. Object and coherent reference
  2. Interference recording
  3. Developed optical record
  4. Illuminate to reconstruct
Wavefront reconstruction requires an optical record and a specified reconstruction beam; this is not a floating image emitted into empty space.

The cross term carries the missing relation

An ordinary photograph records intensity and generally loses the phase needed to propagate a complex object wave backward. Gabor’s method adds a known coherent reference during exposure. Their interference makes relative phase affect the recorded fringes.

Normalize the object and reference field amplitudes so that squared modulus gives intensity. The equation expands the recorded intensity into object and reference backgrounds plus two cross terms. An asterisk denotes complex conjugation. The terms encode a relative phase; they do not measure an absolute phase independent of the reference.

I=∣O+R∣2=∣O∣2+∣R∣2+OR∗+O∗RI=|O+R|^2=|O|^2+|R|^2+OR^*+O^*R

Sources: [2]

The first ambition was electron microscopy

Gabor developed wavefront reconstruction while seeking a route around electron-lens limitations. Early optical demonstrations used filtered conventional light. The 1971 lecture traces the later transformation brought by lasers and off-axis recording.

It is therefore inaccurate to require a laser for every historical realization of holography. Adequate spatial and temporal coherence, geometry and recording resolution are the physical requirements. A laser made many useful arrangements much more practical.

Sources: [2][1]

Reconstruction is a second physical step

After development, the recorded pattern modulates a reconstruction beam. In a simple linear thin-record approximation, multiplication by a matching reference can generate an object-wave term, along with a conjugate image and background. The viewer receives a wave with directional information, which can support parallax and refocusing.

The approximation assumes an appropriate recording response. Saturation, finite pixel or grain size, wavelength mismatch and mechanical motion can spoil the result. A decorative three-dimensional render does not demonstrate this recording-to-reconstruction chain.

Sources: [2]

The twin image explains a historical obstacle

In-line recording lets conjugate contributions overlap. Their simultaneous presence limits a straightforward interpretation of the reconstructed image. Off-axis reference geometry shifts terms into different angular or spatial-frequency regions so that suitable filtering can separate them.

Separation consumes recording bandwidth. A steeper reference angle needs finer fringes; finite sampling and numerical aperture constrain the field of view and resolution. Holography keeps phase information through interference, but does not remove those instrumental limits.

Sources: [2]

Keep the fringe record beside the reconstruction

Follow Gabor’s recording and reconstruction figures in pairs. In the linked studio, change the reference geometry and inspect both the stored interference and the reconstructed result. The explanatory test is whether the latter changes through the former, with sampling limits kept visible.

Sources: [2]

Sources and reading notes

The original lecture is read in the linked hosted PDF. The thin-record explanation states a linear approximation; no historical hologram has been numerically reconstructed here.

  1. Nobel Foundation, Laser: historical award context

    Institutional chronology read for the 1964 laureates and Maiman’s 1960 working laser. Its simplified holography description is not used.

  2. D. Gabor, Holography, 1948–1971, Nobel lecture (1971)

    Recording, reconstruction and twin-image passages read in the hosted original lecture; official PDF returned 403. Read the hosted original

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