The circular photogalvanic effect (CPGE) is a novel spin-related optoelectronic phenomenon based on the SOC of noncentrosymmetric systems. [15] Under the CPGE, a steady photocurrent is generated by the irradiation of circularly polarized light (CPL) without an external bias voltage, and the photocurrent direction is reversed by switching the photon helicity. [15,16] The CPGE originates from the asymmetric distribution of photocarriers in a momentum space (k-space) excited by CPL in interband transitions with a spin-flip between the spin-splitting states (Scheme 1). [16] The direction of the zero-bias photocurrent can be controlled based on the helicity of the CPL, as the asymmetric distribution of photocarriers arises from the selection rule of CPL excitation, Δm J = ±1, where m J is the magnetic quantum number of the total angular momentum (Scheme 1). [16] Hence, noncentrosymmetric systems, wherein SOC could induce spin-splitting in electronic states, are promising platforms to generate the CPGE. In fact, the CPGE has been observed in various polar systems, such as group III-V compound semiconductors, [16][17][18][19] the surface of topological insulators, [20][21][22] a bulk Rashba semiconductor, [23] and transition metal dichalcogenides. [24][25][26][27] In these studies, the correlation between polarity and the CPGE was investigated in detail, andThe control of the optoelectronic properties of 2D organic-inorganic hybrid perovskite (2D-OIHP) lead halides is an increasingly prevalent topic. Herein, the observation of the circular photogalvanic effect (CPGE) in new enantiomorphic 2D-OIHP lead iodides is reported, which are synthesized as a first OIHP-related system belonging to a chiral space group by incorporating organic chiral cations into the inorganic layers of lead iodides. The CPGE is an optoelectronic phenomenon associated with the spin-orbit coupling of heavy atoms in noncentrosymmetric systems. Owing to the CPGE, lighthelicity-dependent steady photocurrents are generated without an external bias voltage under the irradiation of circularly polarized light. Furthermore, the sign reversal of the CPGE photocurrent depending on the chirality of the designed 2D-OIHP lead iodides is observed. This result indicates formation of the theoretically predicted radial spin-polarized texture in k-space of chiral systems owing to spin-momentum locking. Hence, chiral 2D-OIHP lead halides can be a promising platform for engineering opto-spintronic functionalities.