The Gelfond–Schneider theorem says that if is algebraic and is algebraic irrational, then every value with is transcendental. Fix such a nonzero logarithm , and suppose is algebraic. The field then contains all values needed in Schneider lattice proof of the Gelfond–Schneider theorem.
Here is an outline including the parameter balance. For a large , choose polynomial degrees , , with constants large enough that . ImposeExpand these -linear equations in a rational basis and clear denominators. Siegel lemma gives a nonzero integer polynomial with . This follows because each coefficient in the grid equations has arithmetic height and the ratio of unknowns to constraints stays bounded away from one. The exponential polynomial is not identically zero: distinct exponentials are independent over the polynomial ring, as one sees by successively applying powers of to kill all but one term.
The irrationality of makes the grid points distinct. Their zeros make subsequent grid values extremely small. More precisely, if a whole grid has been obtained, take an outer radius . Growth gives . The product form of Schwarz's lemma contributes at the next grid points. Thereforefor large initial , unless the value is zero. But every such value is algebraic in the same , since . Its arithmetic height is , so the Liouville lower bound is incompatible with the displayed upper bound for a nonzero value. Induction extends the zero grid indefinitely.
A fixed nonzero exponential polynomial has only zeros in a disc of radius , by its exponential-type growth and Jensen's formula centered at a nonzero value. The grids give distinct zeros in a disc of radius , a contradiction. Thus is transcendental for every choice of logarithm, completing the Schneider lattice proof of the Gelfond–Schneider theorem.
A standard form of the Schneider-Lang theorem is this. Let be meromorphic functions with for a fixed number field . Suppose have algebraic independence over and have finite growth orders . There are at most points at which all the functions are finite and all their values lie in .
Take and , of orders zero and one. Their derivatives belong to . They have algebraic independence: a polynomial relation is impossible by exponential-polynomial independence, or by letting real tend to infinity and considering the largest .
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