Spectrally correlated photon pairs can be used to improve performance of long range fiber based quantum communication protocols. We present a source based on spontaneous parametric down-conversion producing polarization entangled photons without spectral filtering. In addition, the spectral correlation within the photon pair can be controlled by changing the pump pulse duration or coupled spatial modes characteristics. The spectral and polarization correlations were characterized. The generated photon pairs feature both positive spectral correlations, no correlations, or negative correlations and polarization entanglement with the fidelity as high as 0.97 (no background subtraction) with the expected Bell state. © 2018 Optical Society of America OCIS codes: 190.4410,300.6190,270.4180,270.5565 Controlling the spectral correlations of a polarization entangled photon pair produced via spontaneous parametric down-conversion (SPDC) could have important benefits to applications in optical quantum information. Photonic quantum gates require pure states, which can be created by heralded sources producing pairs of spectrally decorrelated photons [1][2][3][4][5][6][7][8][9][10][11]. On the other hand, long distance fiber based quantum communication and quantum metrology [12,13] suffers from chromatic dispersion, which could potentially be improved [14] with positive spectral correlations [15][16][17]. Here we experimentally demonstrate the effective control of spectral correlations in a photon pair source, based on a ÎČâbarium borate (BBO) crystal which we characterized previously in Ref. [18]. It produces polarization entangled pairs in the telecom band and can be tuned to create negative, none or positive spectral correlations. In addition to that we show high quality polarization entanglement without using spectral filtering or compensation crystals by adopting the compensation scheme shown in Ref. [19].In the SPDC process, one photon of the pump converts into a photon pair. Energy and momentum conservation relations, jointly described as phase matching, and the properties of the pump photons, govern the characteristics of the generated photons. The probability amplitude for a photon pair emission in a given direction and at a given frequency can be described by the product of the pump spatio-temporal amplitude and the phase matching function [5,19]. The phase matching depending on the properties of the nonlinear media specifies the allowed emissions. Typically, the output photons are coupled into optical fibers. This corresponds to collecting photons from a specific range of directions, defined by the fiber and the optics. From this point of view, coupling can be understood as an additional condition to phase matching. Therefore, one can introduce an effective phase matching function (EPMF) [5,18], which fully describes the joint effect of the crystal and coupling into fibers. We approximate the EPMF using a Gaussian function with the characteristic width Ï. The spectral part of the pump can also be approximated by...