We describe the formation of deposition patterns that are observed in many different experiments where a three-phase contact line of a volatile nanoparticle suspension or polymer solution recedes. A dynamical model based on a long-wave approximation predicts the deposition of irregular and regular line patterns due to self-organised pinning-depinning cycles corresponding to a stick-slip motion of the contact line. We analyze how the line pattern properties depend on the evaporation rate and solute concentration. PACS numbers: 68.15.+e, 81.15.Lm, 81.16.Rf The last decade has seen huge growth in interest in phenomena that accompany evaporative and convective dewetting of suspensions and solutions. Well known are the detailed studies of the coffee stain effect [1,2] that analyse the deposition and resulting structures left behind by a receding three-phase contact line of an evaporating drop of suspension upon a solid substrate. In particular, Ref.[2] describes a large range of different deposition patterns including cellular and lamellar structures, single and multiple rings, and Sierpinski gaskets. Other observed structures include crack [3] and chevron [4] patterns. Recently it has been shown that evaporating polymer solutions [5][6][7] and (nano)particle suspensions [8-10] may be used to fabricate strikingly regular stripe patterns, where the deposited stripes are parallel to the receding contact line and have typical distances ranging from 10-100µm. The goal is to use this effect as a non-lithographic technique for covering large areas with regular arrays of small-scale structures, such as, e.g., concentric gold rings with potential uses as resonators in advanced optical communications systems [11]. The deposited patterns from more complex fluids, such as polymer mixtures [12] and DNA solutions [13], are also investigated. The occurrence of regular stripe patterns is a somewhat generic phenomenon, that is not only observed for different combinations of substances but also in a variety of experimental setups that allow for slow evaporation. Examples include the meniscus technique in a sphere-on-flat geometry [7,9], a controlled continuous supply of liquid between two sliding plates to maintain a meniscus-like surface [5] and dewetting forced by a pressure gradient [10]. Interestingly, besides the stripes parallel to the receding contact line, a variety of other patterns are observed, including regular orthogonal stripes [9], superpositions of orthogonal and parallel stripes [5], regular arrays of drops [5,14] and irregularly branched structures [14,15]. This behaviour is highly sensitive to the particular experimental setup and parameters.Despite the extensive number and variety of experiments, an explanation of the formation of the regular patterns has been rather elusive. Although most studies agree that the patterns result from a stick-slip motion of the contact line caused by pinning/depinning events [2,6,11,16] no dynamical model of the periodic deposition process ex-