Two-particle correlations of identical charged pion pairs from Au+Au collisions at√ s N N = 62.4and 200 GeV were measured by the PHOBOS experiment at RHIC. Data for the 15% most central events were analyzed with Bertsch-Pratt and Yano-Koonin-Podgoretskii parameterizations using pairs with rapidities of 0.4 < yππ < 1.3 and transverse momenta 0.1 < kT < 1.4 GeV/c. The Bertsch-Pratt radii Ro and R ℓ decrease as a function of pair transverse momentum, while Rs is consistent with a weaker dependence. Ro and Rs are independent of collision energy, while R ℓ shows a slight increase. The source rapidity y YKP scales roughly with the pair rapidity yππ, indicating strong dynamical correlations. Recent experimental results from all four experiments at the Relativistic Heavy Ion Collider (RHIC) have concluded that Au+Au collisions at the top RHIC energy ( √ s N N = 200 GeV) have produced an extremely hot and dense state of matter [1, 2,3,4]. This matter may have degrees of freedom that are purely hadronic ("hadronic gas"), purely partonic ("Quark-Gluon Plasma", QGP), or an admixture of both. Identical-particle correlation measurements (Hanbury-Brown and Twiss, HBT) yield valuable information on the size, shape, duration, and spatiotemporal evolution of the emission source. Because the dynamics of a hadron gas and a QGP are naïvely expected to be quite different, HBT may allow us to discriminate between these three scenarios [5,6].Experimentally, the correlation function C(q) is defined aswhere p 1 and p 2 are the particle four-momenta, P (p 1 , p 2 ) is the probability of a pair being measured with relative four-momentum q = p 1 − p 2 , and P (p 1 ) and P (p 2 ) are the single-particle probabilities. The numerator is determined directly from data, while the denominator is constructed using a standard event-mixing technique. C(q) can be fit to the Bertsch-Pratt parameterization of a Gaussian source in three dimensions [6,7,8],where q ℓ is the component of q along the beam direction; q o is the component along the pair transverse momentum k T = 1 2 ( p T 1 + p T 2 ); and q s is the component orthogonal to the other two. The q o q ℓ cross-term vanishes only for symmetric collisions with acceptances centered around midrapidity. The λ parameter represents the correlation strength and is expected to be unity for a completely incoherent source. According to the definitions of q o and q s , R o probes a mixture of the spatial and temporal extent of the source, while R s measures only the spatial component. In the special case of a boost-invariant, transparent, azimuthally symmetric source, the ratio R o /R s may be a good indicator of the duration of the emission of particles from the source. Predictions for this quantity from hydrodynamic and transport models varied by over an order of magnitude [9,10], but mostly focused on values between 1.5-2.0, while the first results from RHIC at