We present the use of an ultra-narrow spectrum-sliced incoherent light source for transmission of 10-Gb/s non-returnto-zero signals for wavelength-division-multiplexed passive optical networks. In this light source, a broadband amplified spontaneous emission noise is spectrum-sliced by an ultra-narrow filter and then fed to a gain-saturated semiconductor optical amplifier to suppress the excess intensity noise of the incoherent light. 10-Gb/s modulation is followed using a polarizationinsensitive optical modulator. Thanks to the ultra-narrow linewidth of the source (~0.01 nm), not only is the 10-Gb/s incoherent signal successfully transmitted over 20-km standard single-mode fiber without any dispersion compensation, but also retains the noise suppression after passing through a 0.2-nmbandwidth narrow optical filter. Two different line rates of 10.7 and 12.5 Gb/s are experimentally demonstrated, assuming 7% and 25% forward error correction, respectively. Also presented is the 10-Gb/s upstream transmission over a loopback configured network.Keywords-spectrum-slicing, incoherent light, optical acess network, wavelength-division-multiplexing.Wavelength-division-multiplexing (WDM) passive optical networks (PONs) have been considered as a promising solution to the last-mile technology to meet the soaring demand for bandwidth. However, one of the biggest challenges of deploying large-scale WDM-PON systems is still low-cost implementation and management of wavelength-selective light sources. The light sources operating at specific wavelengths make the optical network units all different from others, and thus do not allow the transponder manufacturers to enjoy the benefits of mass production. The service providers should also stock up all the different kinds of optical transmitters at their storehouse to be braced for any service failure caused by optical transmitter breakdown.Spectrum-sliced incoherent light (SSIL) sources are very attractive in this regard. A wideband amplified spontaneous emission (ASE) from an optical amplifier is spectrum-sliced into multiple channels by an waveguide grating router (WGR) to be used as optical sources for WDM PON instead of costly wavelength-specific light sources for each channel [1]. Therefore, SSIL sources can easily generate multiple wavelength channels from a single wideband optical amplifier without requiring any wavelength-selective lasers.The biggest concern about these incoherent light sources is large excess intensity noise (EIN) originated from the spontaneous-spontaneous beating between different wavelength components of the SSIL. This noise limits the maximum achievable signal-to-noise ratio (SNR) of the signal at the receiver, which can be expressed as B o /B e for unpolarized light, where B o is the optical bandwidth and B e is the electrical bandwidth [1].A couple of techniques have been proposed to overcome this SNR limitation: gain-saturated semiconductor optical amplifier (SOA) and feed-forward noise reduction [4], [7]. Nonetheless, the conventional approach to acco...