The transversity distribution function, , a leading twist parton distribution function, is a fundamental component of the spin structure of the nucleon. describes the distributions of transversely polarized quarks inside a transversely polarized nucleon, where x is the longitudinal8momentum fraction of the proton carried by quark q. It is loosely constrained by global fits. Being chiral odd, can be accessed only when it is coupled with another chiral-odd partner, such as the spin-dependent Collins fragmentation function (FF) or the interference fragmentation function (IFF), which serves as a quark polarimeter. In transversely polarized proton-proton () collisions, the resulting azimuthal correlation between the spin of the fragmenting quark and the final state single charged hadron in jets (involving Collins FF) or di-hadron (involving IFF) can be measured, which are sensitive to quark transversity. The STAR experiment at RHIC has previously measured IFF asymmetries for pairs using collision data from 2006 at = 200 GeV ( = 1.8 ) and from 2011 at = 500 GeV ( = 25 ) and Collins asymmetries for charged pions within jets from 2011 at = 500 GeV. Non-zero IFF and Collins asymmetries were reported which are consistent with predictions based on global analyses of and SIDIS data. In 2012 and 2015, STAR collected 14 48 of data at = 200 GeV, respectively. These datasets provide the most precise measurements of the Collins and IFF asymmetries in collisions at = 200 GeV to date, especially at the quark momentum fractions 0.1< x <0.4. We will present preliminary results for Collins asymmetries of identified pions, kaons, and protons in jets based on 2012 and 2015 datasets and the status update for IFF asymmetries based on 2015 dataset at = 200 GeV.