Self-assembly of molecular nanostructures from single macromolecules offers nanoscience a powerful alternative to both top-down miniaturization and bottom-up nanofabrication approaches.[1] Research on the control over the conformation of single polymeric molecules is inspired by biomacromolecules, which exhibit highly ordered hierarchical structures driven by non-covalent interactions, such as hydrophobic interactions, p-stacking, or hydrogen-bonding.[2] Folding of proteins, for example, leads to complex tertiary and quaternary structures, which determine their properties and functions. [3][4][5][6] Recently, ordering phenomena on different length scales controlled by hydrogen bonds [7][8][9][10][11][12][13] have been studied for single synthetic polymers exhibiting helical secondary structures. A plectonemic supercoil conformation has been observed for polystyrenes jacketed by alkylated monodendrons. [14] Dendronized polymers (denpols), [15] when turned into amphiphilic polyelectrolytes by charging their peripheral functional groups, exhibit patterns of hydrophobic and hydrophilic regions on the nanometer scale. [16] With cryo-transmission electron microscopy (TEM) double-helices of cationically charged polymers of this sort were discovered, the driving force for which was suggested to be hydrophobic interactions.[17] Additionally, scanning force microscopy (SFM) revealed several structural and mechanical properties of single denpols adsorbed onto solid substrates in air. [16,[18][19][20][21] These observations triggered more systematic studies on supramolecular structure formation with denpols aiming at, first, an understanding of the underlying principles and, second, the rational use of these polymers for the construction of predetermined complex architectures as was impressively shown, for example, by Seeman with DNA. [22] We report here the first observation of self-folding of a single synthetic polymer by a SFM investigation of individualized second-and third-generation denpols ( Fig. 1) both with neutral (PG2a, PG3a) and negatively charged peripheral groups (PG2b, PG3b), respectively, deposited from highly diluted solutions onto native and precoated mica and graphite surfaces. Accompanying simulation of the Janus chain model [23] for dendronized polymers supports the findings and furthermore provides details about the dynamics and microscopic nature of the backfolding process. While all polymers used had virtually identical absolute chain lengths and length distributions, a statistical analysis of the lengths and widths of the observed wormlike objects reveals that those formed from the charged denpols are much shorter and also wider than from their non-charged analogues. This is attributed to the formation of self-folded duplex superstructures of the former. Furthermore, the effort to decomplex the self-folded duplex through annealing, vacuum drying, and SFM tip manipulation will be described as an additional proof for the proposed duplex structures. The samples of PG2a [16] and PG3a [24] were synthesize...