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Physics · Ch 11 — Dual Nature of Radiation and Matter

de Broglie Wavelength: Formula, Verification and Simple Applications

11.10

de Broglie Wavelength: Formula, Verification and Simple Applications

The formula for an accelerated electron. An electron of charge magnitude ee and mass mm, starting from rest and accelerated through a potential difference VV, gains kinetic energy eVeV, which is related to its momentum pp by eV=p22meV=\dfrac{p^2}{2m}, so that p=2meVp=\sqrt{2meV}. Substituting into de Broglie's relation λ=h/p\lambda=h/p gives the electron's de Broglie wavelength directly in terms of the accelerating voltage:

λ=h2meV\lambda = \frac{h}{\sqrt{2meV}}

Substituting the standard values h=6.63×10−34 J sh=6.63\times10^{-34}\ \text{J s}, m=9.11×10−31 kgm=9.11\times10^{-31}\ \text{kg} and e=1.6×10−19 Ce=1.6\times10^{-19}\ \text{C} gives the convenient numerical form

λ≈1.23V nm(V in volts)\lambda \approx \frac{1.23}{\sqrt{V}}\ \text{nm} \qquad (V\text{ in volts})

so that, for instance, an electron accelerated through just 150 V150\ \text{V} already has a de Broglie wavelength of about 0.1 nm0.1\ \text{nm} -- comparable to the spacing between neighbouring atoms in a typical crystal (about 0.10.1-0.3 nm0.3\ \text{nm}), 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. …

Figure 1Electron-diffraction observation (Davisson-Germer type) confirming matter waves

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 …