First Chern Form on $\mathbb{CP}^1$¶
A complex line bundle is characterized by the curvature of a unitary connection. On an affine chart of $\mathbb{CP}^1$, use the complex coordinate
$$u=r e^{2\pi i\theta},\qquad \bar u=r e^{-2\pi i\theta}.$$
We compute a Fubini--Study connection, its curvature, and the normalized first Chern form.
Polar chart and connection one-form¶
The chart variables are $(r,\theta)$ with $r\ge0$ and $0\le\theta<1$. The local connection is
$$\omega=\frac{\bar u\,du}{1+u\bar u}.$$
declare symbol r, θ : MathValue
def params : Vector MathValue := [| r, θ |]
def u : MathValue := r * e ^ (2 * π * i * θ)
def ū : MathValue := r * e ^ ((-2) * π * i * θ)
def d (X : MathValue) : DiffForm MathValue :=
!(flip ∂/∂) params X
def ω : DiffForm MathValue := ū * d u / '(1 + u * ū)
ω
Curvature two-form¶
For a line bundle the connection is Abelian, so $\omega\wedge\omega=0$ and $\Omega=d\omega$. We display its antisymmetric component matrix explicitly.
def ωr : MathValue := ω_1
def ωθ : MathValue := ω_2
def Ωrθ : MathValue :=
(∂/∂ ωθ r - ∂/∂ ωr θ) / 2
def Ω : DiffForm MathValue :=
[| [| 0, Ωrθ |], [| -Ωrθ, 0 |] |]
Ω
First Chern form¶
With the orientation and connection convention used here,
$$c_1=\frac{\Omega}{-2\pi i}.$$
def c1Form : DiffForm MathValue := Ω / ((-2) * π * i)
c1Form
The full antisymmetric form contributes twice its upper component, so its oriented density is
$$-\frac{2r}{(1+r^2)^2}\,dr\wedge d\theta.$$
Integrating over $r\in[0,\infty)$ and $\theta\in[0,1)$ gives
$$\int_0^\infty\frac{-2r}{(1+r^2)^2}\,dr=-1.$$
Thus this convention describes the degree $-1$ line bundle. Reversing the orientation or using the dual connection reverses the Chern number.