Particles

Tiny particles are affected in different ways than we are by waves. There are several different effects that must be discussed.

The Photoelectric Effect

Many people believe that Albert Einstein won the Nobel Prize for his discovery of special relativity, as that is what he is most well-known for. However, his actual claim to fame in that respect had to with the photoelectric effect. He found that when light of a certain wavelength is incident on certain metals, electrons are ejected from the surface of the metal.

The number of photoelectrons emitted, the photocurrent, increases with intensity, though the kinetic energy does not. The kinetic energy only increases with an increase in energy of the light i.e. a decrease in the wavelength. Above a certain wavelength, no electrons are ejected.

ℎ𝑐𝜆0=𝑊0+𝐾𝐸𝑚𝑎𝑥

where 𝑊0 is the work function for the metal in question. You can think of it as an intrinsic quality of the metal. 𝜆0 is the cutoff wavelength after which no more electrons will be ejected.

Pair Production/Annihilation

When a high energy photon collides with a nucleus, it may “split” into an electron and a positron. When this split happens, the charge, momentum, and the mass-energy of all parties must be conserved:

𝐸𝑝ℎ𝑜𝑡𝑜𝑛=𝐾𝐸𝑝𝑜𝑠𝑖𝑡𝑟𝑜𝑛+𝐾𝐸𝑒𝑙𝑒𝑐𝑡𝑟𝑜𝑛+2𝐸0

where 𝐸0 is the rest mass-energy for each particle given by 𝐸=𝑚𝑐2, doubled since the electron and positron are identical.

The opposite operation can occur when an electron and a positron combining will annihilate the pair and create two identical photons with opposite momentum. The reason that there must be two photons and not just one is that the momentum must equal 0, so there has to be opposite momentum.

de Broglie Wavelength

All particles exhibit wave-like characteristics, which can be demonstrated by the double-slit experiment. The wavelength of a particle in this instance can be determined from the following equation:

𝜆=ℎ𝑝=ℎ𝑚𝑣=ℎ2𝑚𝐾𝐸

The wavelength of a photon is a little different, since photons are completely massless. The momentum and energy of a photon are related by a simpler equation 𝐸=𝑝𝑐, which applies to all massless particles, not just photons.

Uncertainty

One key problem for physicists studying particles is the Heisenberg Uncertainty Principle. In layman’s terms, the observation of a particle fundamentally changes its quality, so it can never be truly measured. In mathematical terms, the accuracy of a measurement of a position’s momentum and position at the same time is limited:

(Δ𝑝𝑦)(Δ𝑦)≥ℎ4𝜋

and the same function exists for simultaneous measurements of energy and time.