Exploiting hyperentanglement of photon pairs, that is, simultaneous entanglement in multiple degrees of freedom(DOFs), increases the dimensionality of Hilbert spaces for quantum information processing. However, generation of hyperentangled photon pairs collinearlly, while produces high brightness, results in a smaller Hilbert space due to the two photons being in the same spatial mode. In this letter, we point out that one can recover the full dimensionality of such hyperentanglement through a simple interference set up, similar to the time-reversed Hong-Ou-Mandel (TR-HOM) process. Different from the standard TR-HOM, we point out a critical phase condition has to be satisfied in order to recover the hyperentanglement. We theoretically analyze the realization of this approach and discuss the feasibility of generating truly hyperentangled photon pairs. Our proposed approach does not require post-selection and hence enables efficient hyper-entangled photon pairs generation for high-dimensional quantum applications.Entangled photons play a critical role in many applications of quantum opticshorodecki2009quantum. Photons that are simultaneously entangled in more than one degree of freedom(DOF), the so-called 'hyperentangled' states, have attracted much recent interest [1][2][3]. Hyperentanglement expands the dimensionality of the Hilbert space of biphotons, enables complete Bell state analysis [4,5], increases the information capacity per pair photons [6,7] and therefore lays the fundation of superdense-coding quantum communication [8][9][10]. It has also become the key technology for certain tests of fundamental physics [11,12].The generation of entangled photons is most conveniently done in a nonlinear medium. When the phase matching can be satisfied over a bandwidth much greater than the pump bandwidth, the photons are frequency entangled as a result of energy conservation. Entanglement in another DOF can be arranged through various means, such as type II phase matching for polarizationentanglement[13], delayed interferometer for time-bin entanglement [14], or simultaneous phase matching for various orbital angular momentum modes [15]. Here, we consider hyper-entanglement in frequency and polarization DOFs, as frequency and polarization of photons are robust over large transmission distances in optical fibre. Entanglement in these two DOFs can also be generated relatively straightforwardly in fibre [16] and nonlinear waveguides [17]. While collinear photon pair generation in a fibre or a nonlinear waveguide is most efficient due to large nonlinear interaction length and no spatial filtering required (as opposed to non-collinear generation [18]), we will show that that collinear entangled photon pairs have a reduced dimensionality in Hilbert space.By "hyperentanglement", we mean not only the photons are entangled in both DOFs, but also that they are accessible individually, e.g. the hyperentangled photons are spatially separated. In collinear parametric processes such as type-II spontaneous parametric downconversion...