How Do Killing Vector Fields Form a Basis on S2?

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The discussion revolves around the formation of Killing vector fields on the sphere S2, specifically through the Killing equation, which leads to three differential equations for the components of the vector field. The user successfully derives the Killing vector fields and identifies them as a basis for the Killing Lie algebra. However, confusion arises regarding the teacher's instructions, which suggest a different method of solving the Killing equations that seems to imply the equations yield individual Killing vector fields rather than components of a single vector field. The user questions the validity of the teacher's approach, believing it to be both confusing and incorrect. Clarification on the relationship between the equations and the resulting vector fields is sought.
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Homework Statement
I am asked to find the Killing vector fields on ##S^2## where the line element is given by ##ds^2=d\theta\otimes d\theta +\sin^2\theta d\phi\otimes d\phi##.

- Solve the Killing equation for the ##(\theta,\theta)## components, that is ##(\mathcal L_\xi g)_{\theta\theta}=0## and show that it gives a Killing vector field ##\xi^{(1)}## that is only a function of ##\phi##, ##\xi^{(1)}=F(\phi)##. Show that this function has to be periodic and assume that it has the simple form ##\xi^{(1)}=A\sin(\phi-\phi_0)##

- Integrate the other Killing component equations and obtain two more Killing vector fields ##\xi^{(2)}## and ##\xi^{(3)}## that will depend on integration constant ##\phi_0, c_1,c_2##. By giving these constants simples values, recover the **Killing operators** ##\xi_1,\xi_2,\xi_3## given in the directions associated to the **Killing vector fields** ##\xi^{(1)},\xi^{(2)},\xi^{(3)}##.
Relevant Equations
$$\mathcal L_\xi g=0$$

$$\xi_1=(-\sin\phi,-\cot\theta\cos\phi)$$
$$\xi_2=(\cos\phi,-\cot\theta\sin\phi)$$
$$\xi_3=(0,1)$$
I know how to solve this problem by considering the Killing equation, namely ##\mathcal L_\xi g=0## that gives three differential equations involving the components of ##\xi=(\xi^\theta,\xi^\phi)## that can be integrated. The result I get, which I know to be true because this is a common result that can be found anywhere on the web, is:

$$\xi^\theta=\nu\cos\phi-\mu\sin\phi$$
$$\xi^\phi=\delta-\cot \theta(\mu\cos\phi+\nu\sin\phi)$$

Where ##\mu,\nu,\delta## are integration constants. By setting these constants to ##(\mu,\nu,\delta)=\{(1,0,0),(0,1,0),(0,0,1)\}##, I obtain three independent vector fields that constitute a basis for the Killing Lie algebra on ##S^2##. These are, in the chart:

$$\xi_1=(-\sin\phi,-\cot\theta\cos\phi)$$
$$\xi_2=(\cos\phi,-\cot\theta\sin\phi)$$
$$\xi_3=(0,1)$$

So, this is no big deal. However, the directions of my assignment insist that we strictly stick to the following procedure to find ##\xi_1,\xi_2,\xi_3## (these are given in the directions and match the vectors I wrote above) which is the source of my confusion:

- Solve the Killing equation for the ##(\theta,\theta)## components, that is ##(\mathcal L_\xi g)_{\theta\theta}=0## and show that it gives a Killing vector field ##\xi^{(1)}## that is only a function of ##\phi##, ##\xi^{(1)}=F(\phi)##. Show that this function has to be periodic and assume that it has the simple form ##\xi^{(1)}=A\sin(\phi-\phi_0)##

- Integrate the other Killing component equations and obtain two more Killing vector fields ##\xi^{(2)}## and ##\xi^{(3)}## that will depend on integration constant ##\phi_0, c_1,c_2##. By giving these constants simples values, recover the **Killing operators** ##\xi_1,\xi_2,\xi_3## given in the directions associated to the **Killing vector fields** ##\xi^{(1)},\xi^{(2)},\xi^{(3)}##.

I must admit that I am very confused with what my teacher is saying. He is basically saying that solving the three Killing component equations ##(\mathcal L_\xi g)_{\theta\theta}=(\mathcal L_\xi g)_{\theta\phi}=(\mathcal L_\xi g)_{\phi\phi}=0## give three Killing vector fields that depend on integration constants whereas, to my understanding, those three equation are solved for the two components of one generic vector field ##\xi=(\xi^\theta,\xi^\phi)## that give rise to three independent Killing vector fields when the integration constants are given some values.

For example, the first Killing component equation reads : ##\partial_\theta\xi^\theta=0##, which tells us that the ##\theta##-component of the Killing vector field is a function that only depends on ##\phi##. This is very different compared to saying that this equation gives a Killing vector field, isn't it?

Can someone make sense of what my teacher is trying to say or is that just wrong overall? I really do think that the directions are not only confusing but wrong. Any insight would be very much appreciated.
 
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At first, I derived that: $$\nabla \frac 1{\mu}=-\frac 1{{\mu}^3}\left((1-\beta^2)+\frac{\dot{\vec\beta}\cdot\vec R}c\right)\vec R$$ (dot means differentiation with respect to ##t'##). I assume this result is true because it gives valid result for magnetic field. To find electric field one should also derive partial derivative of ##\vec A## with respect to ##t##. I've used chain rule, substituted ##\vec A## and used derivative of product formula. $$\frac {\partial \vec A}{\partial t}=\frac...