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We have carried out high-field resistivity measurements up to 27\,T inEuFe$_2$As$_2$ at $P$\,=\,2.5\,GPa, a virtually optimal pressure for the$P$-induced superconductivity, where $T_\mathrm{c}$\,=\,30\,K. The$B_\mathrm{c2}-T_\mathrm{c}$ phase diagram has been constructed in a widetemperature range with a minimum temperature of 1.6 K ($\approx 0.05 \timesT_\mathrm{c}$), for both $B \parallel ab$ ($B_\mathrm{c2}^\mathrm{ab}$) and $B\parallel c$ ($B_\mathrm{c2}^\mathrm{c}$). The upper critical fields$B_\mathrm{c2}^\mathrm{ab}$(0) and $B_\mathrm{c2}^\mathrm{c}$(0), determined bythe onset of resistive transitions, are 25 T and 22 T, respectively, which aresignificantly smaller than those of other Fe-based superconductors with similarvalues of $T_\mathrm{c}$. The small $B_\mathrm{c2}(0)$ values and the$B_\mathrm{c2}(T)$ curves with positive curvature around 20 K can be explainedby a multiple pair-breaking model that includes the exchange field due to themagnetic Eu$^{2+}$ moments. The anisotropy parameter,$\Gamma=B_\mathrm{c2}^{ab}/B_\mathrm{c2}^{c}$, in EuFe$_2$As$_2$ at lowtemperatures is comparable to that of other "122" Fe-based systems.

Upper Critical Field of Pressure-Induced Superconductor EuFe$_2$As$_2$