high-energy beams as microscopes
An ordinary microscope uses light to magnify small things, but it hits a hard wall: it can never resolve anything much smaller than the wavelength of the light it uses, which is far larger than an atom. To see smaller, you need a probe with a shorter wavelength. Since every particle has a wavelength that shrinks as its energy grows, a beam of high-energy particles becomes the most powerful microscope ever built. A particle accelerator is, at heart, a giant microscope for looking inside matter.
The chain of reasoning is short and rigid. A particle's wavelength is Planck's constant divided by its momentum, so more energetic particles have shorter wavelengths, and shorter wavelengths resolve finer detail. Electrons in an electron microscope already beat light microscopes by huge factors for exactly this reason. Push the energy far higher, into millions and billions of electronvolts, and the wavelength shrinks below the size of a proton, letting the beam feel structure deep inside. The picture is not literal seeing: physicists fire the beam at a target or another beam and read off how the particles scatter, then reconstruct the inner structure from the pattern of deflections.
This principle is why the history of particle physics is a history of ever-bigger machines. Firing high-energy electrons into protons revealed the quarks inside (deep inelastic scattering); colliding protons at the highest energies let the Large Hadron Collider reach distances small enough to study the Higgs and search for new physics. The catch is steep and unavoidable: each step to a smaller distance demands a roughly proportional step up in energy, and the machines grow correspondingly in size, cost, and difficulty. There is no cheap microscope for the subatomic world; resolution is bought with energy.
The Stanford accelerator's high-energy electrons in the late 1960s acted as a microscope sharp enough to feel the three quarks inside a proton — something no light microscope could ever do.
An accelerator is a microscope whose magnifying power is its beam energy.
The beam does not produce an image to look at; structure is inferred from how particles scatter, so reaching smaller distances always costs proportionally more energy.