DNA confined to rigid nanotubes shows density fluctuations around its stretched equilibrium conformation. We report an experimental investigation of the length-scale dependent dynamics of these density fluctuations. We find that for highly elongated molecules a Rouse description is consistent with observations at sufficiently large length scales. We further find that for strongly fluctuating molecules, or short length scales, such Rouse modes cannot be detected due to strong mixing of fluctuation modes. © 2011 American Institute of Physics. ͓doi:10.1063/1.3602922͔ DNA stretching in nanochannels is an emerging technique for genetic and epigenetic analysis of DNA.1 Apart from this practical motivation for investigating the dynamics of the stretching process, the DNA-nanochannel system is also a perfect test bed for the verification of models in polymer physics. That is in particular the case since the crossover between the major confinement regimes is possible within a single set of experiments.2 It has further importance in testing the basic dynamics that underly polymer-polymer diffusion processes, since the well-defined geometry is a controllable implementation of reptation tubes. 3,4 We are here addressing the question of fluctuations of a polymer within such tubes as a function of length scale. This letter was inspired by recent progress in the study of fluctuations in unconfined or weakly confined polymers. 5,6 In particular, for principal components ͑PC͒ of fluctuation of free DNA good agreement of experiment and theory was obtained while it was also established that the dynamics of these PC are not those of Zimm modes. [7][8][9] The work in nanochannels builds on a growing set of dynamic experimental studies of DNA in nanochannels, 10,11 and recent insights gained through simulation and theory. 12,13 We will report the observation of Rouse modes in the nanochannel system. DNA in one-dimensional nanochannels a few persistence lengths wide is described by noninterpenetrating blobs that line up to extend the molecule along the channel. 3 The lateral size of blobs is given by the channel dimensions while their longitudinal extent or nature is a subject of some discussion. When viewed at a sufficiently large length scales and at equilibrium, the details of the elongation mechanism are not observable due to the central limit theorem. While nanoconfined DNA has negligible long-range hydrodynamic selfinteraction, strong hydrodynamic interaction with the sidewalls is predicted to lead to an extension-dependent drag on the molecule.14 However, as long as the extension fluctuations are small, that is as long as the considered lengthscales are large, we again expect that a constant friction per contour length can be assumed, and thus Rouse dynamics are expected. 4 The eigenmodes of the autocorrelation of the monomer displacement from the equilibrium are the Rouse modes with circular wave number ͑or wave vector͒ k = / L for mode number . The corresponding relaxation times are ͑k͒ = / k 2 , and the mode amplitudes are a...