This is a common conservation of angular momentum problem. The key is that \( I \propto R^2 \), so if \( R \) halves, \( I \) becomes \( 1/4 \) of its original value. To conserve \( I\omega \), \( \omega \) must become 4 times larger, meaning the period \( T \) becomes \( 1/4 \) of its original value.