Line defects on the surface of rutile TiO 2 ð110Þ form in pairs separated by 1.2 nm creating a quantum well. The well is effectively closed by the presence of two charged structures at both ends separated by a distance in the 10-20 nm range. As expected for quantum confinement a long period oscillatory feature of the local density of states is observed and attributed to the formation of discrete quantum states inside the system. It is at first glance surprising that the lowest energy quantum state of the well can be observed at room temperature. The properties of the quantum state cannot be explained in an independent-electron, band-like theory. Instead, electron-electron correlation must be included to give a satisfactory picture of the spatial distribution of the charge density. Theory predicts charging energies of 1.30 eV and 1.14 eV for quantum well lengths of 14 nm and 16 nm, respectively, in good agreement with a classical calculation and the size dependence of the capacitance. This observation opens up the possibility of experimentally imaging the transition from a Coulomb blockade localized in a zero-dimensional system to an independent-particle or band-like behavior in an extended one-dimensional system.capacitor | Coulomb blockage | quantum confinement | titanium dioxide | scanning tunneling microscopy O ne of the most striking features of quantum mechanics is the distinctive electronic behavior associated with each level of dimensionality. Advances in scanning probe techniques coupled with the ability to prepare low-dimensional systems of unprecedented quality permits the direct observation of a number of manifestations of quantum mechanics in dimensionally confined systems (1). For example, a recent study revealed the presence of one-dimensional electronic states in the region between selforganized metallic nanowires on a semiconducting surface (2), a textbook illustration of an electron in a one-dimensional box. The famous picture of electron waves in a quantum corral is another beautiful example of imaging the density distribution of electrons in quantum confining structures (3-5). The electronic behavior of such systems may often be successfully understood within the independent-electron picture. When dimensionality is further reduced from quasi one-dimension (Q1D) to quasi zero-dimension (Q0D), electron-electron correlations are increasingly important and, in some instances, even dominate. In that case, the singleelectron picture breaks down. The failure of the single-electron description is exemplified by Coulomb blockade behavior (6, 7). Here, the presence of a net charge in the structure and the associated Coulomb repulsive potential hinder the addition of an extra electron. A convenient way to understand this behavior is through the concept of charging energy, similar to the energy stored on the plates of a conventional capacitor. For a typical spherical quantum well with tens of nanometer radius, the equivalent capacitance is on the order of the 10 −17 F, which corresponds to a charging ener...