Planck relation

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The Planck relation[1][2][3] (referred to as Planck's energy–frequency relation,[4] the Planck–Einstein relation,[5] Planck equation,[6] and Planck formula,[7] though the latter might also refer to Planck's law[8][9]) is a fundamental equation in quantum mechanics which states that the photon energy Template:Mvar is proportional to the photon frequency Template:Mvar (or Template:Mvar): E=hν=hf. The constant of proportionality, Template:Math, is known as the Planck constant. Several equivalent forms of the relation exist, including in terms of angular frequency Template:Mvar: E=ℏω, where the reduced Planck constant is ℏ=h/2π.

The relation accounts for the quantized nature of light and plays a key role in understanding phenomena such as the photoelectric effect and black-body radiation (where the related Planck postulate can be used to derive Planck's law).

Spectral forms

Light can be characterized using several spectral quantities, such as frequency Template:Mvar, wavelength Template:Mvar, wavenumber ν~, and their angular equivalents (angular frequency Template:Mvar, angular wavelength Template:Mvar, and angular wavenumber Template:Mvar). These quantities are related through ν=cλ=cν~=ω2π=c2πy=ck2π, so the Planck relation can take the following "standard" forms: E=hν=hcλ=hcν~, as well as the following "angular" forms: E=ℏω=ℏcy=ℏck.

The standard forms make use of the Planck constant Template:Mvar. The angular forms make use of the reduced Planck constant Template:Math. Here Template:Mvar is the speed of light.

de Broglie relation

Template:See also The de Broglie relation,[10][11][12] also known as de Broglie's momentum–wavelength relation,[4] generalizes the Planck relation to matter waves. Louis de Broglie argued that if particles had a wave nature, the relation Template:Math would also apply to them, and postulated that particles would have a wavelength equal to Template:Math. Combining de Broglie's postulate with the Planck–Einstein relation leads to p=hν~ or p=ℏk.

The de Broglie relation is also often encountered in vector form 𝐩=ℏ𝐤, where Template:Math is the momentum vector, and Template:Math is the angular wave vector.

Bohr's frequency condition

Bohr's frequency condition[13] states that the frequency of a photon absorbed or emitted during an electronic transition is related to the energy difference (Template:Math) between the two energy levels involved in the transition:[14] ΔE=hν.

This is a direct consequence of the Planck–Einstein relation.

See also

References

Template:Reflist

Cited bibliography

  • Cohen-Tannoudji, C., Diu, B., Laloë, F. (1973/1977). Quantum Mechanics, translated from the French by S.R. Hemley, N. Ostrowsky, D. Ostrowsky, second edition, volume 1, Wiley, New York, Template:ISBN.
  • French, A.P., Taylor, E.F. (1978). An Introduction to Quantum Physics, Van Nostrand Reinhold, London, Template:ISBN.
  • Griffiths, D.J. (1995). Introduction to Quantum Mechanics, Prentice Hall, Upper Saddle River NJ, Template:ISBN.
  • Landé, A. (1951). Quantum Mechanics, Sir Isaac Pitman & Sons, London.
  • Landsberg, P.T. (1978). Thermodynamics and Statistical Mechanics, Oxford University Press, Oxford UK, Template:ISBN.
  • Messiah, A. (1958/1961). Quantum Mechanics, volume 1, translated from the French by G.M. Temmer, North-Holland, Amsterdam.
  • Schwinger, J. (2001). Quantum Mechanics: Symbolism of Atomic Measurements, edited by B.-G. Englert, Springer, Berlin, Template:ISBN.
  • van der Waerden, B.L. (1967). Sources of Quantum Mechanics, edited with a historical introduction by B.L. van der Waerden, North-Holland Publishing, Amsterdam.
  • Weinberg, S. (1995). The Quantum Theory of Fields, volume 1, Foundations, Cambridge University Press, Cambridge UK, Template:ISBN.
  • Weinberg, S. (2013). Lectures on Quantum Mechanics, Cambridge University Press, Cambridge UK, Template:ISBN.

Template:Albert Einstein

  1. ↑ French & Taylor (1978), pp. 24, 55.
  2. ↑ Cohen-Tannoudji, Diu & Laloë (1973/1977), pp. 10–11.
  3. ↑ Template:CitationTemplate:Rp
  4. ↑ 4.0 4.1 Schwinger (2001), p. 203.
  5. ↑ Landsberg (1978), p. 199.
  6. ↑ Landé (1951), p. 12.
  7. ↑ Griffiths, D. J. (1995), pp. 143, 216.
  8. ↑ Griffiths, D. J. (1995), pp. 217, 312.
  9. ↑ Weinberg (2013), pp. 24, 28, 31.
  10. ↑ Weinberg (1995), p. 3.
  11. ↑ Messiah (1958/1961), p. 14.
  12. ↑ Cohen-Tannoudji, Diu & Laloë (1973/1977), p. 27.
  13. ↑ Flowers et al. (n.d), 6.2 The Bohr Model
  14. ↑ van der Waerden (1967), p. 5.