In this paper, we investigate, using molecular dynamics simulations, the conformation and diffusion of longer and shorter single-strand DNA ͑ssDNA͒ as a function of water film thickness. While the conformation of the shorter ssDNA is significantly affected and the diffusion is suppressed with reduction in water film thickness, the conformation and diffusion of the longer DNA is not influenced. We explain our observations by considering the competition between stacking interaction of bases and solvation tendency of ssDNA. This paper suggests an approach to control the surface motion of ssDNA in nanoscale water films using film thickness. © 2010 American Institute of Physics. ͓doi:10.1063/1.3366725͔ DNA separation is an essential technique for gene sequencing and DNA fingerprinting. The development of accurate and versatile DNA separation technique is currently a significant issue in nanobiotechnology. 1 Recently, Pernodet et al. 2 reported separation of DNA chains on a surface without any topological restrictions or any solution sieving media. This can be a significant benefit over conventional separation methods. However, a detailed physical understanding of surface transport of DNA is currently not available. 3 For example, it is commonly known that the diffusion coefficient of DNA decreases with increase in DNA size in free solution 4 and under two-dimensional confinement. 5 However, a recent experimental study on electrophoresis of DNA on an atomic force microscopy surface showed the faster movement of longer DNA in a thin pure water film. 6 According to the Nernst-Einstein relation between mobility and diffusion, this implies that the longer DNA has higher diffusion than the shorter DNA.To understand the reasons behind the ambiguities in the physics of surface transport of DNA, in this paper, we investigate, using extensive molecular dynamics ͑MD͒ simulations, the diffusion of DNA in nanometer-thick water films by considering DNA of various sizes. As shown in the schematic in Fig. 1͑a͒, a single-strand DNA ͑ssDNA͒ was solvated in a pure water film on a solid surface. Following the experiment, 6 the surface was made by grafting the poly͑eth-ylene glycol͒-silanes ͑PEG-silanes͒ on a solid substrate. The size of the surface is 20ϫ 20 nm 2 and it consists of 1600 PEG-silane molecules. The PEG-silane has 32 atoms and it is attached to the substrate atom ͓see Fig. 1͑b͔͒. The initial configuration and the atomic partial charges of PEG-silane molecule were obtained from PRODRG ͑Ref. 7͒ using GRO-MOS forcefield and charge. The substrate atoms were assumed frozen and their atomic charges were adjusted to make the entire system neutral. We considered two small ssDNAs fragments with 6 and 12 bases. Although recent DNA sequencing technologies utilize tens of millions of small DNA fragments, 8 efficient separation of such small fragments is still challenging. 9 The longer 12-base ssDNA of 5Ј − CGCGAATTCGCG− 3Ј was prepared by unzipping the well-known Dickerson's B-DNA dodecamer ͑double stranded͒, 10 while the shorter 6-bas...