A Holomorphic Function That Is Its Own Derivative
Let be an entire function satisfying
and .
Without assuming any knowledge of ODEs or the exponential function, prove using only complex-analytic tools (power series) that must satisfy
Then conclude: what is ?
Answer: A Holomorphic Function That Is Its Own Derivative
Key Idea / Intuition
The condition forces the Taylor coefficients of to be completely determined: they must be . Once you know the power series, the functional equation is not proved by plugging in the series naively — instead, the elegant trick is to fix and consider . Because has no zeros (shown from the functional equation, or by noting ), the ratio is well-defined and entire, satisfies , — so uniqueness from the power series argument forces .
Formal Proof / Solution
Step 1: The power series of is uniquely determined
Since is entire, write . The condition gives
Matching coefficients: for all , so
With , we get .
Uniqueness: Any entire solution with and must have this series — the recurrence determines all coefficients.
Step 2: has no zeros
From the series, (which we will prove momentarily from the functional equation, but can also be seen directly: is entire, its derivative is , so ). Hence for all .
Step 3: Proving the functional equation
Fix any . Define
Since , is entire. Compute:
- .
- .
So satisfies the same ODE and initial condition as . By Step 1, any entire function satisfying , must equal . Therefore , i.e.,
Step 4: Conclusion
The unique entire function with and is
The functional equation is the defining algebraic property of the exponential — derived here purely from complex analysis, without any reference to real exponentials or ODEs.
Why This Is Beautiful
The proof is a perfect loop: the power series forces uniqueness, uniqueness forces the functional equation, and the functional equation reveals the object is . The key trick — fixing and forming — is a clean, one-line idea that replaces any computation.
Source: Mathematical folklore / Complex Analysis (Stein–Shakarchi), Chapter 1