TY - JOUR
T1 - Copper Thiocyanate and Copper Selenocyanate Hole Transport Layers
T2 - Determination of Band Offsets with Silicon and Hybrid Perovskites from First Principles
AU - Sajjad, Muhammad
AU - Singh, Nirpendra
AU - De Bastiani, Michele
AU - De Wolf, Stefaan
AU - Schwingenschlögl, Udo
N1 - Publisher Copyright:
© 2019 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim
PY - 2019/11/1
Y1 - 2019/11/1
N2 - Copper thiocyanate (CuSCN) and copper selenocyanate (CuSeCN) combine a high work function with a high optical transparency. To elucidate their potential as transparent hole selective materials, herein, first-principles calculations of the structural and electronic properties are reported, with special attention to the band offsets with crystalline Si and hybrid perovskites (CH3NH3PbI3, CH3NH3PbBr3, and CHN2H4PbBr3). The structural parameters and electronic band structure are obtained using the Perdew–Burke–Ernzerhof functional, resulting in indirect and direct bandgaps of 2.13 and 1.81 eV for CuSCN and CuSeCN, respectively. The (100) surfaces of the two materials do not feature in-gap states, maintaining the semiconducting nature. Band offsets are determined by the electrostatic potential lineup method using slab calculations. Small valence band offsets of 0.10 eV for CuSCN/Si and 0.08 eV for CuSCN/CH3NH3PbI3 are desirably found, i.e., a promising hole transport layer character of CuSCN for Si and CH3NH3PbI3-based solar cells. Type-II band alignment is obtained for all studied heterojunctions.
AB - Copper thiocyanate (CuSCN) and copper selenocyanate (CuSeCN) combine a high work function with a high optical transparency. To elucidate their potential as transparent hole selective materials, herein, first-principles calculations of the structural and electronic properties are reported, with special attention to the band offsets with crystalline Si and hybrid perovskites (CH3NH3PbI3, CH3NH3PbBr3, and CHN2H4PbBr3). The structural parameters and electronic band structure are obtained using the Perdew–Burke–Ernzerhof functional, resulting in indirect and direct bandgaps of 2.13 and 1.81 eV for CuSCN and CuSeCN, respectively. The (100) surfaces of the two materials do not feature in-gap states, maintaining the semiconducting nature. Band offsets are determined by the electrostatic potential lineup method using slab calculations. Small valence band offsets of 0.10 eV for CuSCN/Si and 0.08 eV for CuSCN/CH3NH3PbI3 are desirably found, i.e., a promising hole transport layer character of CuSCN for Si and CH3NH3PbI3-based solar cells. Type-II band alignment is obtained for all studied heterojunctions.
KW - band offsets
KW - first-principles calculations
KW - heterojunctions
KW - hole transport layers
UR - http://www.scopus.com/inward/record.url?scp=85071148467&partnerID=8YFLogxK
U2 - 10.1002/pssr.201900328
DO - 10.1002/pssr.201900328
M3 - Article
AN - SCOPUS:85071148467
SN - 1862-6254
VL - 13
JO - Physica Status Solidi - Rapid Research Letters
JF - Physica Status Solidi - Rapid Research Letters
IS - 11
M1 - 1900328
ER -