In the realm of quantum mechanics, particles like electrons have wave-like properties. This is elegantly captured by the De Broglie wavelength. According to the De Broglie hypothesis, any moving particle or object has an associated wavelength. This wavelength is given by the equation:\[\lambda = \frac{h}{p}\]Where:
- \(\lambda\) is the wavelength.
- \(h\) is Planck's constant, \(6.626 \times 10^{-34}\) Js.
- \(p\) is the momentum of the particle.
The momentum \(p\) is the product of mass and velocity for objects with mass. But for photons, which have no rest mass, the momentum is instead derived from their energy. This concept bridges the gap between traditional physics, where particles are seen as point-mass objects, and modern physics, where wave and particle properties converge. When calculating the De Broglie wavelength for a photon, it's crucial to initially equate the photon's momentum with that of another particle, like an electron, as in our example exercise. This leads to meaningful comparisons and deeper insights into particle-wave symmetry.