Low-temperature measurements of asymmetric carbon nanotube (CNT) quantum dots are reported. The CNTs are end-contacted with one ferromagnetic and one normal-metal electrode. The measurements show a spin-dependent rectification of the current caused by the asymmetry of the device. This rectification occurs for gate voltages for which the normal-metal lead is resonant with a level of the quantum dot. At the gate voltages at which the current is at the maximum current, a significant decrease in the current shot noise is observed.Carbon nanotubes 1 are ballistic conductors that have long mean-free paths and spin diffusion lengths 2,3 . CNTs can therefore be used as spacers for spin valves [4][5][6] or in other systems that require spin coherence over their lengths 7 . Additionally, short CNT sections behave like quantum dots at low temperatures 8 . Short CNT sections are therefore promising materials for charge detection 9 , the separation of spin-entangled pairs of electrons 10,11 , or the rectification of current based on the electron spin 12,13 . Recently spin-based current rectification, or a spin diode effect [13][14][15][16][17][18] , has been observed in a lateral ferromagnet-CNT-normal metal device 19 . Shot noise measurements can provide an additional window into the dynamics of a system 20 . Noise measurements are useful for examining the correlation of tunneling events in a system, and have been studied for double-barrier tunnel junctions [21][22][23] . Here we extend upon previous results by considering the current noise of a CNT-based spin diode.A schematic of our device is given in Figure 1 (a). It consists of a single-walled carbon nanotube (SWNT) grown by chemical vapor deposition 24 and end-contacted to alternating niobium and cobalt electrodes. Devices are measured by applying a bias voltage and a capacatively-coupled gate voltage and measuring the two-terminal current. A representative AFM image of a device is shown in Figure 1 (b). We have also measured the resistance of sections of the niobium electrode as a function of temperature, which is shown in Figure 1 (c). We observe that there the resistance drops to zero around 6.5 K as the niobium electrode becomes superconducting. Electronic transport measurements were performed at temperatures ranging from 4.2 K to 10K.