Let
Dd := {z=(z1,…,zd)∈Cd: ∣z1∣,…,∣zd∣<1}
be the unit polydisc, and let the Schur class Sd be the set of analytic functions f:Dd→D.
[Kne2025-def-polydisc] [Kne2025-def-Schur]
Writing the power series expansion f(z)=∑α∈N0dfαzα, define the coefficient-wise ℓ1 norm
∥f∥1:=∑α∣fα∣ and the dilation fr(z):=f(rz).
[Kne2025-def-l1] [Kne2025-def-fr]
The Bohr radius Kd is defined by
Kd := sup{r>0: ∥fr∥1≤1 for all f∈Sd}.
[Kne2025-def-Kd]
Equivalently, Kd is the largest number such that for every power series ∑αcαzα with ∑αcαzα<1 on Dd, one has ∑α∣cαzα∣<1 whenever max1≤j≤d∣zj∣<Kd.
[BK1997-def-Kn]
We define
C59 := K2,
the Bohr radius for the bidisc D2.
Bohr’s one-variable theorem gives K1=1/3, and in particular implies K2≤1/3.
[BK1997-Bohr-1d] [BK1997-ub-1-3]
The exact value of Kd is unknown for every d>1; in particular, the exact value of K2 is open.
[BK1997-open]
The best established range currently is
0.3006 ≤ K2 < 0.302825279492.
[Kne2025-lb-K2-0-3006] [P2026-ub-K2-0-302825279492]