Abstract. In this presentation, I discussed a) the charm total cross-section and its comparisons to measurements at other beam energies and pQCD calculations; b) the semileptonic decay of charmed hadrons and the sensitivity of non-photonic leptons to charm quark collective flow and freeze-out; c) semileptonic decayed electron spectrum at high transverse momentum, its comparison to FONLL in p+p and d+Au collisions, and heavy-quark energy loss in Au+Au collisions.In relativistic heavy-ion collisions, charm quarks are believed to be produced in the early stage via initial gluon fusion and their production cross-section can be evaluated using perturbative QCD [1]. Study of the N bin scaling properties of the charm total cross-section in p+p, d+Au and Au+Au collisions can test if heavy-flavor quarks, which are used as a probe, are produced exclusively at the initial impact. The interactions of heavy quarks with the medium provide a unique tool for probing the hot and dense matter created in ultra-relativistic heavy-ion collisions at the early times. At RHIC energies, heavy quark energy loss [2], charm quark coalescence [3,4,5,6], the effect of J/ψ production from charm quark coalescence on the interpretation of possible J/ψ suppression due to color screening [7], and charm flow [8,9,10] have been proposed as important tools in studying the properties of matter created in heavy ion collisions. The last three effects depend strongly on the charm total cross-section and spectrum at low p T .Since the beginning of RHIC operation, PHENIX and STAR collaborations have made pioneer measurements in charm related physics [11,12,13,14,15,16] ‡. New measurements presented at this conference are: (i) muon spectra at forward rapidity (1.4 < |y| < 2.2) from charm semileptonic decay by PHENIX Collaboration [16]. This enables us to study the rapidity dependence of nuclear effects of charm production.(ii) muon spectra at low p T (0.17 < p T < 0.25 GeV/c) from charm semileptonic decay by STAR Collaboration [15]. This improves the charm total cross-section measurements and better constrains the charm spectrum for studying the charm radial flow. ‡ The overviews of charm elliptic flow and quarkonium can be found elsewhere [17,18]