We show that individual colloidal CdSe-core quantum dots can be optically trapped and manipulated in three dimensions by an infrared continuous wave laser operated at low laser powers. This makes possible utilizing quantum dots not only for visualization but also for manipulation, an important advantage for single molecule experiments. Moreover, we provide quantitative information about the magnitude of forces applicable to a single quantum dot and of the polarizability of an individual quantum dot.Colloidal quantum dots (QDs) are fluorescent semiconductor nanocrystals.1 They are bright and photostable with a broad excitation spectrum and a narrow emission spectrum, normally distributed around a specific wavelength, dependent on the size of the QD. Absorption of any photons with wavelengths above this specific wavelength causes the formation of an electron-hole pair, the recombination of which results in photon emission. The fluorescent blinking of nanocrystal quantum dots is the result of a bistability between an emitting state where the quantum dot is described as on and the nonemitting off state.2 The extreme brightness and photostability of QDs make them excellent choices as markers to visualize biological systems. For instance they have been used to mark individual receptors in cell membranes 3 or to label living embryos at different stages. 4 It has long been a goal to optically trap or otherwise control quantum dots 5 to establish a combined visualization and optical manipulation technique. Optical trapping of aggregates of colloidal quantum dots in two dimensions was recently proved possible 6 using a pulsed YLF laser, and it was claimed that to trap quantum dots with a continuous wave (CW) laser one would need extremely high powers on the order of 20 W. In this Letter, we prove that optical trapping of individual quantum dots using a CW infrared laser operated at only 0.5 W is, in fact, possible. By observing the Brownian motion of the trapped quantum dots, we deduced the strength of the optical trap and thus found the magnitude of the optical forces acting on a single quantum dot. We used two independent approaches to render probable that it was indeed a single quantum dot in the trap and not an aggregate.An inducible dipole in an inhomogeneous field experiences a force in the direction of the field gradient, the gradient force, F b grad . A particle with an induced dipole moment will be forced toward the laser focus by this three-dimensional restoring force. Hence, the existence of an induced QD dipole moment is essential for optical trapping. Opposing the gradient force are the scattering force, F b scat , and the absorption force, F b abs , which are proportional to the scattering and absorption cross sections, respectively. If infrared laser light, with a wavelength that exceeds the maximum emitted wavelength of the QDs by far, is used for trapping and if the QDs are physically very small in comparison to the focus area of the trapping laser light, then the scattering and absorption forces ...