Gravity can arise in a conventional non-Abelian gauge theory in which
a specific phenomenon takes place. Suppose there is a condensation of
polarized instantons and anti-instantons in the vacuum state. Then the
excitations of the gauge field in the classical approximation are des
cribed through the variables of Riemann geometry satisfying the Einste
in equations of general relativity. There are no dimensional coupling
constants in the theory.