I. Introduction
Some fluorescent molecules, such as coumarin-red, can not only absorb sunlight over a relatively broad range of wavelengths up to the red region, but also re-emit light at longer wavelengths, where the spectral responsivity of a typical silicon solar cell is greater. Furthermore, such molecules can be easily embedded in the core of a stretch of plastic optical fiber (POF) so that it will not only absorb part of the sunlight over its whole length, but also guide part of the re-emitted light to a solar cell [1]. If the type of dopant, the fiber length, and the dopant concentration are appropriate, the solar cell will deliver greater electric power than it would under direct exposition to the sun. Besides, POFs are inexpensive, and they do not need to be aligned towards the sun [2].