Recently, I answered this question. A generalized version of what was proved is the following.
Lemma: For $n\in\mathbb{N}$ and $a_1,a_2,\ldots,a_{2n+1}\in \mathbb{Q}$, if for each $1\le i\le 2n+1$, the numbers $\{a_j:1\le j\le 2n+1\wedge j\neq i\}$ can be divided into two sets of size $n$ with equal sum, then all $a_i$ must be equal.
Proof: At first, we limit ourselves to $\mathbb{Z}$. If for some $a_1,a_2,\ldots,a_{2n+1}\in \mathbb{N}$, for all $1\le i\le 2n+1$, the numbers $\{a_j:1\le j\le 2n+1\wedge j\neq i\}$ can be divided into two sets of size $n$ with equal sum, we call $a_1,a_2,\ldots,a_{2n+1}$ a solution.
For any solution $a_1,a_2,\ldots,a_{2n+1}$ and a positive integer $m$, $a_1-m,a_2-m,\ldots,a_{2n+1}-m$ is also a solution. If all the $a_i$ are even, then $\frac12a_1,\frac12a_2,\ldots,\frac12a_{2n+1}$ is a solution as well.
Now, the sum of every $2n$ elements is even, therefore, each $a_i$ has the same parity as the sum of all $a_i$, therefore, all $a_i$ have the same parity.
WLOG, we can assume one of the $a_i$ to be $0$, so all $a_i$ are odd. This means we can divide them all by $2$ and still have a valid solution. However, since one of them is still $0$, they're all even again, so we can divide them all by $2$ again, but then one of them is still $0$ and so on. So all the $a_i$ are finite and divisible by arbitrarily large powers of $2$, so all $a_i$ are equal to $0$.
For $a_1,a_2,\ldots,a_{2n+1}\in\mathbb{Q}$, simply multiply all of the $a_i$ by the product of the denominators to translate the problem to the integers. Q.E.D.
Question: Is the lemma also true for $a_1,a_2,\ldots,a_{2n+1}\in \mathbb{R}$?
HINT:
For the proof you can use the following linear algebra result:
Let $V$ be a vector space over a field $k$ and $\phi_1$, $\ldots$, $\phi_m$, $\psi$ linear functionals on $V$ so that $\phi_1(v)= \cdots = \phi_m(v) = 0$ implies $\psi(v)=0$. Then $\psi$ is a linear combination of the $\phi_i$'s with coefficients in $k$.
Now consider $V=\mathbb{Q}^{2n+1}$, for the $\phi_i$'s all grouping differences, and for $\psi$ one of the $a_s-a_t$.