Nano-objects composed of metals or semiconductors are known to display interesting electronic and optical properties. To a major extent, these properties are controlled by their size, due to specific confinement effects. Equally important, as far as confinement is concerned, is the dimensionality or shape of the nano-object. Quantum dots, wires, and films are characterized by extremely different densities of electronic states and, thus, by very different optoelectronic properties unique to each shape. [1,2] Further examples of these effects include the plasmonic properties, that is, absorption and scattering properties, of nano-objects composed of noble metals such as gold. Both the size and shape control the number of plasmonic resonance bands and their location on the frequency scale. [3,4] This paper is concerned with nano-objects composed of materials which display ferromagnetism in the bulk state, such as cobalt or iron. It is well known that such materials display superparamagnetism rather than ferromagnetism if prepared as nanoparticles, [5] the relaxation time and the blocking temperature being strongly dependent on the size. Such superparamagnetic systems are of interest for a broad range of applications, for example, in drug delivery or ferrofluids. [6,7] Thus, it is not surprising that the number of papers focusing on superparamagnetic particles is very high. There are also a smaller, but increasing, number of papers that consider the ferrimagnetic and ferromagnetic properties of nanorods. One of the motivations for these studies is that they are of interest for use in high-density storage systems, in particular for perpendicular magnetic recording and also for use as sensors and spintronic devices. [8][9][10][11] Experimental findings show characteristic magnetization features such as coercive force, remanence, and a hysteresis shape that becomes anisotropic. The hysteresis properties depend on the composition of the nanorods and the presence of imperfections. [12,13] Typical investigations considered rods characterized by axial ratios of up to 10 and diameters in the 10 to 100 nm range. These systems are predicted to exhibit spontaneous spin-polarized transport of charges.[14]To prepare these rod-shaped objects a variety of methods were employed including microlithography, vapor-liquid-solid growth, and template deposition based on electrodeposition or vapor deposition. [12,15] The axial ratio is in all cases limited, and the amount of materials that can be produced is often restricted, for instance in the case of the template approaches. Also, rod handling may pose a problem due to the strong aggregation effects that are known to take place with nanorods. This aggregation, in turn, will introduce magnetic interactions between the rods, affecting the magnetization behavior considerably. The preparation of nanofibers by electrospinning offers a promising alternative.[16]During electrospinning, a strong electrical field is applied to a droplet formed by a polymer solution or polymer melt at the tip of ...