The Question to solve:
For a set $A\subseteq \mathbb{R}^d$ and a point $x\in \mathbb{R}^d$, we say that $x$ is a Radon point of $A$ if $A$ can be partitioned into $A = A_1\cup A_2$ with $A_1\cap A_2 = \emptyset$ so that $x\in conv(A_1)\cap conv(A_2)$. Show that if $A$ is a set of $d+2$ points in general position, then $A$ has a unique Radon point.
I know Radon theorem says if $|A|\geq d+2$, we will have $conv(A_1)\cap conv(A_2)\neq \emptyset$. However, I don’t know how to show that if $|A|=d+2$, and the points are in general position, then $A$ has a unique $x\in conv(A_1)\in conv(A_2)$.
Your help would be really appreciated.
Let $A = \left\{\boldsymbol{a}_1,\ldots,\boldsymbol{a}_{d+2}\right\}$. If $\boldsymbol{x}$ and $\boldsymbol{y}$ are Radon points then you can find two sets of indices $I$, $J$ and $\alpha, \beta\in \mathbb R_{\ge 0}^{d+2}$ such that \begin{align} \boldsymbol{x} &= \sum_{i\in I} \alpha_i\boldsymbol{a}_i = \sum_{i\not\in I} \alpha_i \boldsymbol{a}_i\\ \boldsymbol{y} &= \sum_{i\in J} \beta_i\boldsymbol{a}_i = \sum_{i\not\in J} \beta_i \boldsymbol{a}_i\\ 1 &= \sum_{i\in I} \alpha_i = \sum_{i\not\in I} \alpha_i\\ 1 &= \sum_{i\in J} \beta_i = \sum_{i\not\in I} \beta_i. \end{align}
Let $u_i = \begin{cases} \alpha_i & \text{if $i\in I$}\\ -\alpha_i & \text{if $i\not\in I$} \end{cases}$ and $v_i = \begin{cases} \beta_i & \text{if $i\in J$}\\ -\beta_i & \text{if $i\not\in J$} \end{cases}$ such that:
\begin{align} \sum_{i=1}^{d+2} u_i &= \sum_{i=1}^{d+2} v_i = 0\\ \sum_{i=1}^{d+2} u_i\boldsymbol{a}_i &= \sum_{i=1}^{d+2} v_i\boldsymbol{a}_i = 0 \end{align}
Since the points are in general position $\boldsymbol{a}_1, \ldots, \boldsymbol{a}_{d+1}$ are affinely independent. So $u_{d+2}\neq 0$ and $v_{d+2}\neq 0$. Now let $\lambda = \frac{u_{d+2}}{v_{d+2}}$ then,
\begin{align} \sum_{i=1}^{d+1} \left(u_i - \lambda v_i\right) &= -u_{d+2} - \lambda \left(-v_{d+2}\right) = -u_{d+2} + \lambda v_{d+2} = 0\\ \sum_{i=1}^{d+1} \left(u_i - \lambda v_i\right)\boldsymbol{a}_i &= -u_{d+2}\boldsymbol{a}_{d+2} - \lambda \left(-v_{d+2}\right)\boldsymbol{a}_{d+2} = \left(-u_{d+2} + \lambda v_{d+2}\right)\boldsymbol{a}_{d+2} = 0 \end{align}
Again since $\boldsymbol{a}_1, \ldots, \boldsymbol{a}_{d+1}$ are affinely independent, $u_i - \lambda v_i = 0$ for $i\le d+1$. So $u = \lambda v$.
$$\boldsymbol{x} = \sum_{i\in I:\, \alpha_i>0} \alpha_i\boldsymbol{a}_i = \sum_{i\not\in J:\, \beta_i>0} \lambda \left(-\beta_i\right)\boldsymbol{a}_i = -\lambda \sum_{i\not\in J:\, \beta_i>0} \beta_i\boldsymbol{a}_i = \boldsymbol{y}$$
a similar proof can be done for the case where $\lambda > 0$.