In analogy to conventional semiconductor diodes, the Josephson diode exhibits superconducting properties that are asymmetric in applied bias. The effect has been investigated in number of systems recently, and requires a combination of broken time-reversal and inversion symmetries. We demonstrate a dual of the usual Josephson diode effect, a nonreciprocal response of Andreev bound states to a superconducting phase difference across the normal region of a superconductor-normalsuperconductor Josephson junction, fabricated using an epitaxial InAs/Al heterostructure. Phase asymmetry of the subgap Andreev spectrum is absent in the absence of in-plane magnetic field and reaches a maximum at 0.15 T applied in the plane of the junction transverse to the current direction. We interpret the phase diode effect in this system as resulting from finite-momentum Cooper pairing due to orbital coupling to the in-plane magnetic field, without invoking Zeeman or spin-orbit coupling.Nonreciprocal effects in superconducting systems have attracted significant recent interest. A primary motivation is to engineer a superconducting diode, a circuit element that supports dissipationless flow of current in one direction but is resistive in the opposite [1]. Nonreciprocity of supercurrent flow has been observed in thin film superconductors [2][3][4][5][6][7][8][9][10][11] and Josephson junction devices [12][13][14][15][16]. In general, nonreciprocal superconductivity requires the breaking of time-reversal and inversion symmetries [17][18][19][20][21][22][23][24][25][26][27][28], also prerequisites for various topological superconducting states. Nonreciprocal effects may therefore also serve as a marker for unconventional superconducting order [9,10,18,20,29].