Put . Since has no zeros and the unit disc is simply connected, it has a holomorphic logarithm. Thus is holomorphic with and . The Cayley transform between the half-plane and disk gives
The Schwarz lemma yields , so the Carathéodory derivative bound for the right half-plane gives . Since , the sharp answer is
Equality in the Schwarz lemma holds exactly when , . Solving for and exponentiating gives exactly the extremizers
Their logarithmic real part is , so each is indeed a zero-free map into the unit disc with the prescribed value at zero.
For a fixed , put . Apply the Harnack inequality on the unit disk to the positive harmonic function and then exponentiate its negative. The zero-free Schwarz lemma gives
For both endpoints are attained: take for the lower endpoint and for the upper endpoint in the displayed extremizers. At zero both are . If the question is interpreted as allowing to vary as well, the sharp infimum and supremum over all admissible pairs are respectively and , approached as ; neither value is attained inside the unit disc. An individual function need not have these global extremal values: the constant function is a simple example.
The Harnack inequality on the unit disk states that a nonnegative harmonic function satisfies
One proof applies the Poisson integral on the unit disk on a circle of radius : the Poisson kernel on the circle lies between and its reciprocal. The mean value property for harmonic functions identifies the mean boundary value with ; let .
A harmonic conjugate on the simply connected unit disc makes holomorphic. The Carathéodory derivative bound for the right half-plane gives . The Cauchy-Riemann equations give , so . For a fixed , use the disk automorphism
The chain rule and conformality multiply the gradient length by . Applying the estimate at zero to proves the sharp gradient bound for positive harmonic functions:
Sharpness follows from , which has equality at zero, and then composing with . These extremizers are positive multiples of the Poisson kernel on the circle with its boundary pole fixed at one point.

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