A novel photonic crystal fiber(PCF) polarization filter is designed and fabricated; it consists of two large apertures coated with gold. The asymmetric structure separates the resonance position in the vertical direction well. Due to the metal layer covering, loss is greatly improved. Finite element method is applied for numerical simulation. The influences of varying gold thickness and varying the diameters and the center positions of the larger apertures on filtering performance are evaluated. Theory of coupling between surface plasma and core mode is introduced. By modulating the parameters, we realize a single polarization filter at 1.31 μm and 1.55 μm. The basal mode loss in the y direction can reach 1408.80 dB/cm at 1.31 μm and 1911.22 dB/cm at 1.55 μm respectively, but basal mode loss in the x direction is relatively small, 0.82 dB/cm and 1.87 dB/cm. In addition, two kinds of broadband polarization filters are proposed. If the fiber length is set to 200 μm,the extinction ratio is greater than 20 dB with width of 570 nm and 490 nm. The filter has simple structure and excellent performance. A novel photonic crystal fiber (PCF) polarization filter is designed and manufactured; it consists of two large apertures coated with gold. The asymmetric structure separates the resonance position in the vertical direction well. Due to the metal layer covering, loss is greatly improved. The influences of varying gold thickness and varying the diameters and the center positions of the larger apertures on filtering performance are described. Theory of varying between gold and core modes is introduced. By modulating the parameters, we realize a single polarization filter at 1.31 μm and 1.55 μm. The basal mode loss in the y direction can reach 1408.80 dB / cm at 1.31 μm and 1911.22 dB / cm at 1.55 μm respectively, but basal mode loss in the x direction is relatively small, 0.82 dB / cm and 1.87 dB / cm. In addition, two kinds of broadband polarization filters are proposed. If the fiber length is set to 200 μm, the extinction ra tio is greater than 20 dB with width of 570 nm and 490 nm. The filter has simple structure and excellent performance.