The micromagnetic structure of a La 0.7 Sr 0.3 MnO 3 film was studied using magnetic force microscopy and micromagnetic simulations. For a 150 nm thick epitaxial, strain relaxed film grown on SrTiO 3 evidence is presented from experiment and simulation that magnetic domains have a typical size of 1 µm at room temperature.There is hardly another class of materials with such extensively studied magnetotransport properties as the colossal magnetoresistance manganites [1,2]. Apart from the colossal magnetoresistance itself, the manganites show a wealth of other magnetotransport effects, namely anisotropic magnetoresistance as an intrinsic phenomenon and spin-polarized tunnelling as well as grain-boundary magnetoresistance as extrinsic phenomena [2]. The latter magnetotransport effects depend in a crucial way on the magnetic domain structure. Therefore it is surprising that the number of studies of the micromagnetic structure is rather limited. These comprise magneto-optical techniques [3][4][5][6][7], magnetic force microscopy (MFM) [8][9][10][11][12][13][14][15][16][17][18], scanning SQUID and scanning Hall probe microscopy [19,20], spin-polarized scanning tunnelling microscopy [21], Bitter decoration [22] and Lorentz electron microscopy [23]. Most of the studies are focused on the interplay between structural and magnetic domains [5,7] as well as electronic phase separation [19,22] in case of single crystals and on strain effects in case of thin films [9, 13-15, 17, 24]. It has been well established that compressive strain leads to an uniaxial anisotropy with the substrate normal as easy axis and a clear maze-or stripe-like perpendicular magnetic domain pattern. For easyplane anisotropy often a "feather-like" magnetic pattern has been observed [3,9,11,14,15,17,18] which, however, has not been analyzed in detail. By various authors it has been tacitly assumed that this "feather-like" pattern corresponds to magnetic domain contrast [3,9,11,14,15,17]. However, this assumption has been criticized lately [18] and an alternative interpretation has been put forward according to which the magnetic contrast indicates a sub-domain structure, so-called "ripples", with the real magnetic domains being much larger with typical lateral sizes of 20 µm or more [18].The aim of this work is the study of the micromagnetic structure in La 0.7 Sr 0.3 MnO 3 (LSMO) films with an easy-plane anisotropy. For this a 150 nm thick LSMO film on SrTiO 3 was chosen, since it showed an easy-plane anisotropy with [110] easy axes. This is demonstrated in Fig. 1 showing the magnetization hysteresis loops for applied fields along [100], [110] and [001], respectively. It is evident that the substrate normal is the hard axis. Furthermore the in-plane magnetization curves indicate that at 300 K the [110] axis is energetically more favourable; at about 330 K a reorientation transition of the anisotropy axes occurs with the [100] direction being the easy axis for 330 K < T < T C [25]. The magnetocrystalline anisotropy constant K 1 in cubic symmetry was de...