The laws and particle properties of our universe allow hydrogen and other stable atoms to exist, providing the foundation for stars, chemistry, water, and life.
Why do the properties of particles and forces allow stable atoms and a rich chemistry to exist?
Hydrogen is the simplest atom: one proton with one electron. It is also the most abundant ordinary element in the universe.
Hydrogen fuels long-lived stars and is part of water and nearly every important class of biological molecule.
Stable atoms depend upon several pieces of physics working together. Protons must be sufficiently stable. Electrons must have suitable properties. Electromagnetism must allow electrons to remain bound to nuclei, while nuclear interactions must permit useful nuclei to exist.
Atomic stability is therefore not controlled by a single constant.
Without stable atoms there is no ordinary chemistry. Without hydrogen, the history of stars and the chemical environment of life would be radically different.
Hydrogen is stable under ordinary conditions and makes up most of the ordinary atomic matter in the universe by number. Stable atoms provide the basis for chemistry.
Physics explains atomic stability through quantum mechanics, electromagnetism, particle masses, and nuclear physics. Fine-tuning arguments ask a different question: why do those laws and properties collectively permit stable and chemically useful matter?
It is difficult to determine every possible form that complex matter could take under different laws. We therefore should be cautious about claiming that only chemistry exactly like ours could ever support complexity or life.
Hydrogen is the most abundant chemical element in ordinary cosmic matter and is the principal fuel for main-sequence stars.
The existence of stable atomic matter illustrates the cumulative character of fine-tuning arguments. Several features of physics must cooperate before chemistry becomes possible.
This record should be used as an integration point linking several more specific evidence records rather than as a separate probability argument.