Analyticity and the Cauchy Riemann Equations
Proposition Suppose fx and fy exist in a neighborhood of z. If fx and fy are continuous at z and fy = ifx there, then f is differentiable at z.
Proof Let f = u + iv, h = ξ + iη. By the Mean-Value Theorem (for real functions of a real variable)
u(z + h) − u(z)
h = u(x + ξ, y + η) − u(x, y) ξ + iη
= u(x + ξ, y + η) − u(x + ξ, y)
ξ + iη +u(x + ξ, y) − u(x, y) ξ + iη
= η
ξ + iηuy(x + ξ, y + θ1η) + ξ
ξ + iηux(x + θ2ξ, y)
= η
ξ + iηuy(z1) + ξ
ξ + iηux(z2) and
v(z + h) − v(z)
h = η
ξ + iηvy(x + ξ, y + θ3η) + ξ
ξ + iηvx(x + θ4ξ, y)
= η
ξ + iηvy(z3) + ξ
ξ + iηvx(z4) for some 0 < θk < 1, k = 1, 2, 3, 4. Thus
f (z + h) − f (z)
h = η
ξ + iηuy(z1) + ivy(z3) + ξ
ξ + iηux(z2) + ivx(z4) Since fy = ifx at z,
fx(z) = ξ + iη
ξ + iηfx(z) = ξ
ξ + iηfx(z) + η
ξ + iηfy(z), and thus
f (z + h) − f (z)
h − fx(z) = f (z + h) − f (z)
h − ξ
ξ + iηfx(z) − η
ξ + iηfy(z)
= η
ξ + iηuy(z1) − uy(z) + i vy(z3) − vy(z)
+ ξ
ξ + iηux(z2) − ux(z) + i vx(z4) − vx(z).
Since lim
h→0|zk − z| = 0 for each 1 ≤ k ≤ 4,
η ξ + iη
,
η ξ + iη
≤ 1 and fx = ux + ivx and fy = uy+ ivy are continuous at z, we have
h→0lim
f (z + h) − f (z)
h − fx(z) = 0.
Examples
(a) Let f (z) = |z|2 = x2+ y2, z ∈ C.
Since fx = 2x, fy = 2y are continuous for all z ∈ C, f is differentiable if and only if fy = ifx
by the above proposition. Hence f is differentiable only at z = 0.
(b) The converse of the above proposition is not true. For example, consider
f (x, y) =
xy(x + iy)
x2+ y2 if z 6= 0
0 if z = 0.
Note that f = 0 on both axes so thatfx = fy = 0 at the origin but since limz→0
f (z) − f (0)
z = lim
(x,y)→(0,0)
xy x2+ y2
y=αx= α
1 + α2 depends on α, the limit does not exist and f is not differentiable at z = 0. In fact,fx and fy
fx(x, y) =
2xy3+ iy2(y2− x2)
(x2+ y2)2 if z 6= 0
0 if z = 0,
fy(x, y) =
x2(x2− y2) + 2ix3y
(x2 + y2)2 if z 6= 0
0 if z = 0
are not continuous at z = 0.
(c) Consider the real-valued function f : R2 → R defined by
f (x, y) =
x2+ y2 sin
1
x2+ y2
if (x, y) 6= (0, 0)
0 if (x, y) = (0, 0).
Note that f is real-differentiable at every point (x, y) ∈ R2,
fx(x, y) =
2x sin
1
x2 + y2
− 2x
x2+ y2 cos
1
x2 + y2
if (x, y) 6= (0, 0)
0 if (x, y) = (0, 0),
and
fy(x, y) =
2y sin
1
x2+ y2
− 2y
x2+ y2 cos
1
x2+ y2
if (x, y) 6= (0, 0)
0 if (x, y) = (0, 0)
with fx(0, 0) = 0 = fy(0, 0), but fx, fy are not bounded (hence not continuous) in a neighborhood of (0, 0).
Remark (An algebraic interpretation of the Cauchy-Riemann equations) Consider the complex polynomial
p(z) =
n
X
k=0
ckzk.
Look at complex-valued polynomials of real variables x, y:
p(x, y) =
n
X
m=0
X
k+`=m,k, `≥0
ck, `xky` with ck, `= ∂k+`p
∂xk∂y`(0, 0) (∗)
and take a ”new basis” as z = x + iy and ¯z = x − iy. Write the polynomial in z, ¯z:
p(z, ¯z) =
n
X
m=0
X
k+`=m,k, `≥0
dk, `zkz¯` (†)
We claim that there’s a 1 − 1 correspondence between polynomials given by (∗) and (†). In fact, since z = x + iy and ¯z = x − iy implies that x = z + ¯z
2 , y = z − ¯z
2i and by the Chain Rule
∂
∂z = ∂x
∂z
∂
∂x +∂y
∂z
∂
∂z = 1 2
∂
∂x − i ∂
∂y, ∂
∂ ¯z = ∂x
∂ ¯z
∂
∂x +∂y
∂ ¯z
∂
∂y = 1 2
∂
∂x + i ∂
∂y.
Claim We have the equalities
∂
∂ ¯z(zkz¯`) = `zkz¯`−1
∂
∂z(zkz¯`) = kzk−1z¯` Proof of Claim We simply check
∂
∂ ¯z(zkz¯`) = 1 2
∂
∂x + i ∂
∂y (x + iy)k(x − iy)`
= 1
2k(x + iy)k−1(x − iy)`+ `(x + iy)k(x − iy)`−1 + i
2ki(x + iy)k−1(x − iy)`− i`(x + iy)k(x − iy)`−1
= 1
2kzk−1z¯`+ `zkz¯`−1 + i
2kizk−1z¯`− i`zkz¯`−1
= `zkz¯`−1
Claim (equivalent form of CR equations) f (z) satisfies CR equations ⇐⇒ ∂
∂ ¯zf = 0.
Proof of Claim Since
∂f
∂ ¯z = 1 2
∂f
∂x + i∂f
∂y
=⇒ fy = ifx ⇐⇒ ∂f
∂ ¯z = 0.
Remark The conclusion is that
p(z, ¯z) =
n
X
m=0
X
k+`=m, k, `≥0
dk, `zkz¯`
is holomorphic if and only if dk, `= 0 for ` > 0 (e.g. no ¯z’s). Alternatively, p(x, y) =
n
X
m=0
X
k+`=m, k, `≥0
ck, `xky`
is holomorphic if it can be written as p(z) =
n
X
k=0
ckzk.
Let’s give some basic hints that holomorphic functions behave a bit like power series:
Proposition
(a) If f = u + iv is analytic in a region D and u is constant, then f is constant.
Proof Since u is constant,
ux = uy = 0 in D, and, by the Cauchy-Riemann equations,
vx = vy = 0 in D.
By the Mean Value Theorem, u and v are constants along any line segment in D. So f = u + iv is constant on D.
(b) If f is analytic in a region D and if |f | is constant there,then f is constant.
Proof If |f | = 0, the proof is immediate. Otherwise u2+ v2 ≡ C 6= 0 on D.
Taking the partial derivatives with respect to x and y, we see that u ux+ v vx ≡ 0
u uy+ v vy ≡ 0 Making use of the Cauchy-Riemann equations, we obtain
u ux− v uy ≡ 0 v ux+ u uy ≡ 0 so that
(u2+ v2)ux ≡ 0 on D
and ux = vy ≡ 0. Similarly, uy and vx are identically zero, hence f is constant.
The Functions ez, sin z, cos z, log z, zα
In general, either one of the following methods will be used to define a complex analogue of a real analytic function.
(i) we determine the same fundamental defining properties;
(ii) we use its power series to obtain a holomorphic extension.
Definitions
(1) To define an extension f (z) = ez of the real exponential function f (x) = ex, we observe that
(i) e0 = 1, d
dxex = ex, . . . , which implies for each fixed x1 ∈ R, d
dx ex+x1
ex = exex+x1 − ex+x1ex
(ex)2 = 0 =⇒ ex+x1
ex = constant = ex1 =⇒ ex+x1 = exex1 implies that f (x) = ex is infinitely differentiableand satisfies that
f (0) = 1, df
dx = f and f (x + x1) = f (x)f (x1) for all x, x1 ∈ R.
(ii) ex=
∞
X
k=0
xk
k! is convergent for all x ∈ R,implies that f (x) = ex is a real analytic function defined by a convergent power series for all x ∈ R.
So we should define f (z) such that
(i) f (x) = ex for all z = x + i 0 ∈ R and f (z1+ z2) = f (z1)f (z2) for all z1, z2 ∈ C.
This implies that
f (x + iy) = f (x)f (iy) = exf (iy) ∀x, y ∈ R and, by setting x = 0 and using f (0) = 1, we have
f (iy) = A(y) + iB(y),
where A, B are real-valued functions satisfying A(0) = 1, B(0) = 0, and f (x + iy) = exA(y) + iexB(y).
Using the Cauchy-Riemann equations fy = ifx, A(0) = 1 and B(0) = 0, we get (A0(y) = −B(y)
B0(y) = A(y) =⇒
(A00(y) + A(y) = 0
B00(y) + B(y) = 0 =⇒ A(y) = cos y and B(y) = sin y.
This implies that f (z) = ez should be defined by
ez = ex(cos y + i sin y) ⇐⇒ eiy = cos y + i sin y for all z = x + iy ∈ C.
(ii) f (z) =
∞
X
k=0
zk
k! for all z ∈ C.
Since
lim
k→∞
1 k!
1/k
= 0,
the radius of convergence is ∞, f (z) =
∞
X
k=0
zk
k! is convergent and differentiable for all z ∈ C. Since
f (0) = 1, f0(z) = f (z), · · · ∀ z ∈ C, by the term-by-term differentiation theorem, and
d dz
f (z + w)
f (z) = f (z)f (z + w) − f (z + w)f (z)
[f (z)]2 = 0 for a fixed w ∈ C,
we obtain that
f (z)f (w) = f (z + w) for all z, w ∈ C which implies that f (z) =
∞
X
k=0
zk
k! = ez for all z ∈ C.
(2) Let f (z) = sin z, cos z for z ∈ C.
Since
eiz = 1 + (iz) + (iz)2
2! + · · · = 1 − z2 2! +z4
4! + · · · + i z − z3 3! +z5
5! + · · ·, we have
eix =
∞
X
k=0
(−1)k
(2k)! x2k + i
∞
X
k=0
(−1)k
(2k + 1)!x2k+1=: cos x + i sin x for x ∈ R and
cos x = eix+ e−ix
2 and sin x = eix − e−ix
2i for x ∈ R.
So sin z, cos z should be defined by cos z = eiz+ e−iz
2 and sin z = eiz− e−iz
2i for z ∈ C.
We can verify the usual properties that
∂
∂z cos z = − sin z, ∂
∂z sin z = cos z,
cos 0 = 1, sin 0 = 0, cos(−z) = cos z, sin(−z) = − sin z, etc.
Check the addition formulas for cos(z1 + z2) and sin(z1+ z2).
(3) Let w = log z ⇐⇒ z = ew for z ∈ C.
For w = a + bi ∈ C, since
z = ew = ea(cos b + i sin b) = reiθ,
log z should be defined by
log z = log r + iθ + i(2πn), z ∈ C so the complex log is multi-valued.
By writing z = reiθ = r(cos θ + i sin θ), we define the principal branch of log z as follows.
For each z ∈ C \ {z = x + 0 · i ∈ C | x ≤ 0}, the principal branch of log z is defined by log z = log |z| + iArg(z), where Arg(z) ∈ (−π, π).
So the principal branch of log z has imaginary part in (−π, π).
Claim log z is holomorphic given a branch cut, and
∂
∂z log z = 1
z for all z ∈ C \ {z = x + 0 · i ∈ C | x ≤ 0}.
Proof of Claim Cosider
h→0lim
log(z + h) − log z
h .
Setting w1 = log(z + h), w = log z, since log is continuous given a branch cut, we have lim
h→0w1 = w and thus
lim
h→0
log(z + h) − log z
h = lim
h→0
w1− w
ew1 − ew = 1
wlim1→w
ew1 − ew w1− w
= 1 ew = 1
z.
Intuitively, log z looks like a helix above C \ {0}; we call this the Riemann surface for log z.
(4) For α ∈ R, let f (z) = zα for z ∈ C.
Define
zα = eα log z = eα(log z+2πni), for z ∈ C
which is potentially multi-valued. eα log z is the principal branch; now examine e2πnαi. If α /∈ Q, e2πnαi takes infinitely many values.
If α = k
l ∈ Q, e2πnαi takes l values (e.g. eπni= ±1 for α = 1 2).
For example, when considering√
z, we still need a branch cut
√
reiθ =√
reiθ/2, θ ∈ (−π, π).