Physics · Ch 11 — Dual Nature of Radiation and Matter
de Broglie Wavelength: Formula, Verification and Simple Applications
de Broglie Wavelength: Formula, Verification and Simple Applications
The formula for an accelerated electron. An electron of charge magnitude and mass , starting from rest and accelerated through a potential difference , gains kinetic energy , which is related to its momentum by , so that . Substituting into de Broglie's relation gives the electron's de Broglie wavelength directly in terms of the accelerating voltage:
Substituting the standard values , and gives the convenient numerical form
so that, for instance, an electron accelerated through just already has a de Broglie wavelength of about -- comparable to the spacing between neighbouring atoms in a typical crystal (about -), which is exactly the condition needed for the electron beam to show diffraction when it strikes a crystal, in precisely the same way a beam of X-rays of a similar wavelength does.
The Davisson-Germer confirmation. In 1927, Clinton Davisson and Lester Germer, while studying the scattering of electrons off a nickel target (originally for an unrelated purpose), observed exactly this kind of diffraction: this section's figure shows the arrangement, in which an electron beam accelerated through a known voltage is directed onto a nickel crystal, and a detector records a pronounced INTENSITY MAXIMUM at one particular scattering angle -- a diffraction peak, not the smooth scattering a stream of classical particles alone would give. Careful measurement showed that the wavelength implied by the position of this peak (using the same crystal-diffraction relation already familiar from X-ray diffraction) matched, to good accuracy, the wavelength de Broglie's formula predicted for electrons accelerated through that same voltage -- direct, quantitative experimental proof that electrons genuinely possess wave character, exactly as de Broglie had proposed three years earlier. …
What this figure shows. An electron gun, inside an evacuated chamber, accelerates a narrow beam of electrons through a known, adjustable potential difference and directs them onto the surface of a nickel crystal target. A detector, mounted on an arm that can be swung around the target through a range of scattering angles, measures the intensity (number) of electrons scattered in each direction. A polar plot of the detected intensity against scattering angle, drawn for a fixed accelerating voltage, shows a pronounced, sharp intensity MAXIMUM at one particular scattering angle -- a diffraction peak, of exactly the same character as the maxima seen when X-rays of a known wavelength are diffracted by the same regularly-spaced planes of atoms in the crystal -- rather than the smooth, featureless spread of intensity with angle that a stream of cl …