We present a particularly simple model of axion monodromy: Our axion is the lowest-lying KK-mode of the RR-2-form-potential C 2 in the standard Klebanov-Strassler throat. One can think of this inflaton candidate as being defined by the integral of C 2 over the S 2 cycle of the throat. It obtains an exponentially small mass from the IR-region in which the S 2 shrinks to zero size both with respect to the Planck scale and the mass scale of local modes of the throat.Crucially, the S 2 cycle has to be shared between two throats, such that the second locus where the S 2 shrinks is also in a warped region. Well-known problems like the potentially dangerous back-reaction of brane/antibrane pairs and explicit supersymmetry breaking are not present in our scenario. However, the inflaton back-reaction starts to deform the geometry strongly once the field excursion approaches the Planck scale. We derive the system of differential equations required to treat this effect quantitatively. Numerical work is required to decide whether back-reaction makes the model suitable for realistic inflation. While we have to leave this crucial issue to future studies, we find it interesting that such a simple and explicit stringy monodromy model allows an originally sub-Planckian axion to go through many periods with full quantitative control before back-reaction becomes strong. Also, the mere existence of our ultra-light throat mode (with double exponentially suppressed mass) is noteworthy.An important question in string cosmology is whether string theory compactifications allow for large-field inflation. On the one hand, many proposals for realizing inflation in string theory exist. At the same time, no-go theorems for large-field inflation have been put forward in various corners of the string theory landscape [1][2][3][4][5][6][7][8][9][10][11][12][13][14]. By studying large-field inflation in string theory one may thus hope to learn about fundamental properties of string theory compactifications.Furthermore, observation may force us to address these questions. For models of singlefield slow-roll inflation, there is a direct link between the tensor-to-scalar ratio r and the nature of inflation. To achieve r 0.01 the inflaton has to traverse a trans-Planckian field range during inflation, thus requiring inflation to be of large-field type [15]. The most recent observational constraint by BICEP2 and the Keck Array on the tensor-to-scalar ratio is r ≤ 0.07 at 95 % confidence [16], which is compatible with large-field inflation. Currently, considerable effort is being expended towards more precise measurements of r.One challenge faced by models of large-field inflation is their sensitivity to an infinite tower of corrections to the inflaton potential. One way of controlling these corrections is to identify the inflaton with an axion-like field (henceforth axion), so that the shift symmetry of the axion protects the potential from dangerous corrections. A promising approach for realizing axion inflation in string theory is axion monodromy in...