Read · Light quanta: from entropy to an energy scale

Introduction · a heuristic viewpoint

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Introduction · a heuristic viewpoint

A qualification

Keep what waves explain

Why question the description of light without discarding interference?

The 4 printed paragraphs this passage explains
  • Introduction, paragraph 1: Physicists describe a gas or any other body by a finite, if very large, number of atoms and electrons, while Maxwell's theory describes light by quantities spread continuously through space. So a body's energy cannot be divided without limit, but the energy of a light ray spreading from a point is thought to spread over an ever larger volume.
  • Introduction, paragraph 2: The wave theory of light works superbly for optics and will probably never be replaced there, but optical observations measure averages over time. It is conceivable that the theory conflicts with experience when it is applied to how light is produced and transformed.
  • Introduction, paragraph 3: Einstein's proposal: black radiation, photoluminescence, the production of cathode rays by ultraviolet light and related effects seem easier to understand if the energy of light is distributed discontinuously in space. On this assumption a ray from a point carries a finite number of energy quanta, localized at points, which move without dividing and are absorbed or produced only as wholes.
  • Introduction, paragraph 4: He will set out the reasoning and the facts that led him to this view, in the hope that it may be of use to other researchers.

A wave can spread through space and interfere with another wave. Those successes are not withdrawn by the light-quantum proposal. The question changes: what happens when radiation is generated, absorbed, or converted into another form?

The introduction contrasts a continuously distributed field with matter described through a finite number of moving constituents. Einstein proposes considering independently moving energy elements whose energy remains localized during propagation and is exchanged as a whole. In this paper that is a heuristic viewpoint: something to investigate through consequences, not a conclusion supplied by an animation.

In the wave-optics laboratory, double the field amplitude while holding the wave shape and medium fixed. The model intensity becomes four times as large. That establishes a consequence of the wave model; it does not settle how an individual energy-transfer event occurs.

Show every step here: Keep what waves explain

The introduction sets two descriptions side by side. In the physics of 1905, matter is described by a finite number of atoms and electrons, so the energy of a body sits in a finite number of places. Light, in Maxwell's theory, is a field: its energy is spread continuously through any region the light fills, however small the region is taken. The paper keeps the field for what it describes well and asks about something else.

  1. Name the observable before choosing a description. An interference pattern is a question about how light travels. The energy that an electron carries away from an illuminated metal is a question about how light exchanges energy with matter.
  2. For travel, keep the wave description. Two waves arriving at one place add, and where a crest meets a trough they cancel. That is interference, and the paper does not withdraw it or any other success of wave optics.
  3. Work the wave model's own arithmetic. In that model the intensity, the energy delivered per unit area and per unit time, is proportional to the square of the field amplitude. Double the amplitude and the intensity becomes 2 × 2 = 4 times as large; triple it and it becomes 3 × 3 = 9 times as large.
  4. Notice what optical observations measure: averages over many oscillations. The paper points out that this is why a continuous field can fit them so well while leaving open what happens in a single, brief exchange of energy.
  5. State the new question precisely. When light is emitted, absorbed, or converted into light of another colour, does its energy behave as if it were spread continuously, or as if it were concentrated in a finite number of separate portions that travel without dividing and are absorbed or produced only whole?
  6. Mark the status of the proposal. The paper calls its viewpoint heuristic: a way of looking that is to be judged by its consequences for particular phenomena. The introduction states it; it does not prove it.
  7. See where the consequences are drawn. Sections 1 to 6 build an argument from the entropy of radiation, and sections 7 to 9 apply the resulting picture to fluorescence, to electrons released from solids by light, and to the ionization of gases by ultraviolet light.
  8. Keep the drawing honest. A picture of separate dots moving through space illustrates the hypothesis; it is not evidence for it. Evidence can come only from comparing the consequences with observations made independently of the picture.

Modern qualifications

Modern photon language and later quantum theory are not premises of this reconstruction. The proposal does not say that purely optical wave phenomena have disappeared.

Assumptions and limits: Keep what waves explain

Assumed here

  • A continuous electromagnetic field describes optical propagation.
  • A model of propagation need not yet explain how matter exchanges energy with radiation.

What this does not establish

  • Drawing isolated light packets does not prove that radiation consists of them.
  • The wave description keeps its successes, interference and diffraction among them; the proposal concerns how light exchanges energy with matter.

Source context: German source · English · Interlinear gloss · Facsimile

References

A. Einstein, Über einen die Erzeugung und Verwandlung des Lichtes betreffenden heuristischen Gesichtspunkt. Annalen der Physik (4), 17, 132–148 (1905).

A. Einstein, On the motion of particles suspended in liquids at rest required by the molecular-kinetic theory of heat. Annalen der Physik (4), 17, 549–560 (1905), §§1–5. Bibliographic pointer; this preview is not a source transcription or translation.

A. Einstein, Zur Elektrodynamik bewegter Körper. Annalen der Physik (4), 17, 891–921 (1905).

A. Einstein, Does the inertia of a body depend upon its energy content? Annalen der Physik (4), 18, 639–641 (1905). External 1923 Perrett–Jeffery translation, electronically transcribed by John Walker; its notation was modernized. A reference for this explanatory preview, not this edition’s translation or its pinned facsimile.

R. A. Millikan, A Direct Photoelectric Determination of Planck's "h". Physical Review (2), 7 (3), 355–388 (1916).

26 foundation readings sit behind this argument.

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