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Fig. 3. Models for MT interaction with the shmoo tip. (A) As hypothesized by Maddox et al. (Maddox et al., 2003 ), an unknown binding factor may interact with Kar3p to keep this motor near the cortex. Bim1p may link the plus end to the shmoo tip through Kar9p. During polymerization, Bim1p and Kar9p maintain the interactions between the plus end and the shmoo tip. A switch to depolymerization will cause Bim1p to leave the plus end while Kar3p maintains the attachment of the MT to the tip. (B) Plus end cycling hypothesis. In this model, the MT plus end can detach from the shmoo tip at some frequency governed by the affinity of +TIPs for either the cortex or the ends of actin cables. After detachment, the MT shrinks back to the SPB while a newly nucleated MT grows and interacts with the actin network. The newly nucleated MT is transported by Myo2p along the actin network towards the shmoo tip, generating movement of the nucleus towards the mating projection. Once at the shmoo tip, the MT attaches and begins to polymerize, moving the nucleus away from the shmoo tip. Therefore, the combination of MT transport and MT dynamics at the shmoo tip generates nuclear oscillations.
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