Coupling between InGaAs/ GaAs quantum dots is investigated using differential transmission spectroscopy. Two-color pump-probe techniques are used to spectrally resolve the carrier dynamics, revealing carrier transfer between quantum dots at room temperature. The time constant for this process is shown to increase from 35 ps at room temperature to 130 ps at 230 K.Self-assembled semiconductor quantum dots (QDs) are remarkably flexible structures that are impacting many areas of optoelectronics. At low temperatures, they exhibit atomiclike properties due to their three-dimensional electronic confinement and are promising for such applications as quantum computing and cryptography. Self-assembled QDs have also proven useful when incorporated into conventional devices such as semiconductor lasers and amplifiers. Unfortunately, many of the major device improvements anticipated due to the unique QD density of states have not been realized. This is due in part to the as yet unavoidable size distribution in QD ensembles, but also due to the significant temperature-dependent coupling of individual QD transitions. Temperature-dependent coupling affects the threshold current density in QD lasers 1 and limits the isolation between channels in a QD semiconductor optical amplifier and other multichannel devices. 2,3 Coupling between QDs in optoelectronic devices occurs via both electromagnetic and electronic mechanisms. The former couples all QDs within a homogeneous linewidth of the individual transition. The latter can couple all QDs within the inhomogeneous linewidth as electrons and holes move between QDs with different ground state energies. Each of these effects can result in Fermi level pinning and, therefore, explain the observed single-mode operation of QD lasers at room temperature. 4 In actuality, both of these processes contribute to the collective action of QD ensembles and can be difficult to distinguish. Recently, coupling in self-assembled QD ensembles has been studied extensively. The room temperature homogeneous broadening of the transition has been measured by four wave mixing 5 and single QD emission 6,7 with values ranging from a few nanometers up to more than 10 nanometers. Electronic coupling of QDs via thermal emission and subsequent recapture has been inferred from temperature dependent continuous-wave 8,9 and time-resolved 10,11 photoluminesence (PL) measurements. Unfortunately, this method relies on numerous assumptions and a multivariable fit to a series of data. Results from resonant differential transmission (DT) measurements 12,13 show an initial fast recovery of the QD absorption indicating that carriers are quickly leaving the states that they were initially created in. These experiments cannot determine whether the resonantly excited carriers are moving to other QDs or different states of the same QD.This paper is orginized as follows. Section I contains information on the growth and preparation of the sample as well as the experimental methods employed for this study. Section II contains room ...