Because of the zero dispersion wavelength (ZDWL) random fluctuations, the gain and noise figures deteriorate in optical parametric amplifiers based on highly nonlinear fibers (HNLFs). The detrimental role of ZDWL fluctuations on the gain and noise performance in dual-pump fiber optical parametric amplifiers (FOPAs) is presented. Numerical investigations of noise figure (NF) for different fibers with random fluctuation are analyzed. The noise figures for different fibers are varying even if the random fluctuation is small. Through choosing HNLFs with low ZDWL fluctuation and large nonlinear coefficient, high-gain and low-noise performance can be obtained.Fiber optical parametric amplifiers (FOPAs) [1][2][3][4][5][6][7][8] have attracted worldwide attention due to the potential properties for obtaining high gain [2] , large bandwidth [3] and low noise [4,6,9,10] . The dual-pump FOPA has more broad and flat gain spectrum with a higher gain compared with the one-pump FOPA. The highly nonlinear fibers (HNLFs) have higher nonlinear coefficient compared with the conventional dispersion shift fibers (DSFs). To obtain the same level gain, the required length of HNLF is shorter. Moreover, the introduction of HNLF can improve the performance of FOPAs. However, a serious problem is the fluctuation of the zero dispersion wavelengths (ZDWLs) along the propagation direction of the HNLF [5] . In most of previous reports, the fiber dispersion properties were considered to be constant along the whole HNLF [6] . But the longitudinal random variations of ZDWL are inevitable in practical HLNF. The ZDWL fluctuation is mainly caused by the random variations of the core diameter in fabrication process [11] .The ZDWL is crucial to achieve the phase matching. Moreover, the gain and noise figure (NF) also depend on ZDWL. In Ref. [7], the impacts of ZDWL random fluctuations on the gain performance of FOPA have been considered.In the multi-section FOPA, the gain ripple increases from 0.3 to 1 dB [8] . The noise characteristics of the one-pump FOPA in terms of ZDWL fluctuations have been investigated [12] . In this paper, the dual-pump FOPA is considered. The influence of ZDWL random variations on the noise figure is investigated. The numerical simulations show that the noise figure will vary greatly even if the ZDWL has small change. By reducing the spacing of the pumps, the bandwidth of FOPA decreases while the influence of ZDWL on noise becomes smaller. It is concluded that larger random fluctuation will bring larger impacts on the noise figure. To obtain the same level gain, only a shorter HNLF is needed due to its larger nonlinear coefficient, and at this time the effects of ZDWL variations are reduced.Two strong pumps and a weak signal are launched into the HNLF, and highly efficient four-wave mixing occurs. Considering the pump to be undepleted, the coupled non-linear Schrodinger (NLS) equations of the OPA can be written as follows [13] , including the ZDWL variations along the fiber,