The variations of kinetic energy $K(x)$,potential energy $U(x)$,and total energy $E$ as a function of displacement $x$ of a particle in $SHM$ are as shown in the figure. The value of $|x_0|$ is
- A$2A$
- B$\frac{A}{\sqrt{2}}$
- C$\sqrt{2}A$
- D$\frac{A}{2}$
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