We present the magnetic and superconducting phase diagram of EuFe 2 As 2 for B c and B ab. The antiferromagnetic phase of the Eu 2+ moments is completely enclosed in the superconducting phase. The upper critical field vs. temperature curves exhibit strong concave curvatures, which can be explained by the Jaccarino-Peter compensation effect due to the antiferromagnetic exchange interaction between the Eu 2+ moments and conduction electrons.Key words: EuFe 2 As 2 , iron pnictides, pressure-induced superconductivity PACS: 74.62.Fj, 74.25.Dw Since the discovery of superconductivity (SC) at a transition temperature T c = 26 K in LaFeAsO 1−x F x by Kamihara et al. [1] extensive studies of SC in layered iron pnictides and related compounds have been performed. There were some reports that the 122 parent compounds AFe 2 As 2 (A = Ca, Sr, Ba, and Eu) could be tuned to SC by the application of high pressure P [2,3,4,5,6,7,8,9]. However, most of these reports were based only on resistivity measurements and hence could not establish the bulk nature of P-induced SC. Recently, we have proved from ac magnetic susceptibility measurements that P-induced bulk SC does occur in EuFe 2 As 2 and further that it coexists with the antiferromagnetic order of the Eu 2+ moments below T N (< T c ) [10]. P-induced bulk SC has also been confirmed for SrFe 2 As 2 [11]. The occurrence of the bulk SC in the parent compounds has an important implication: the key to SC in the iron pnictides is not carrier doping but suppression of the magnetic/structural transition. Here we present B appl (applied magnetic field)-T (temperature) phase diagrams of EuFe 2 As 2 for P ∼ 26 kbar. Figure 1 shows ac magnetic susceptibility along the c axis of EuFe 2 As 2 at P = 25.7 kbar. (We recalibrated Manganin wire used for pressure gauges after the publication of Ref. [10] and found that the pressure was estimated about 9% larger in Ref. [10]. For the pressures of 28 and 29 kbar of the c-axis and ab-plane susceptibility measurements in Ref.[10], read 25.7 and 26.3 kbar, respectively.) The susceptibility at zero field exhibits a large drop below T c = 31 K, then increases with decreasing T to show a peak around T N = 21 K, where the Eu 2+ moments order antiferromagnetically, and finally decreases again. The size of diamagnetism is consistent with 100% shielding. With increasing B appl , the superconducting transition shifts to lower T . The feature associated with T N is barely visible at B appl = 0.25 T, but is already absent at B appl = 0.5 T. The susceptibility vs. B appl curves for T < T N show drops at low fields. It indicates a field-induced transition from the antiferromagnetic to paramagnetic state of the Eu 2+ moments. The characteristic field B m for this transition is defined in the figure. (The definitions of T N and B m given in Fig. 1 are different from conventional ones. They have been adopted for practical purposes.) In the case of the a-axis susceptibility, the zero-field curve shows a plateau below T N , and hence we define T N2 as the l...