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Title: Majority Carrier Properties of Single Crystal Cu 2− x ZnSnSe 4 with Varying Copper Composition

Journal Article · · Physica Status Solidi B. Basic Solid State Physics
ORCiD logo [1];  [2];  [1]
  1. Institute of Energy Conversion University of Delaware 451 Wyoming Road Newark DE 19716 USA
  2. IBM TJ Watson Research Center 1101 Kitchawan Rd Yorktown Heights NY 10598 USA

The dependence of carrier concentration on copper content in Cu 2− x ZnSnSe 4 single crystals, grown without fluxing agents, is presented over the composition range Cu/(Zn + Sn) of 0.77–0.93 and Zn/Sn from 1.3 (low Cu content) to 1.3 (high Cu content). Single phase mono‐crystals with facets up to 5 mm are synthesized from high‐purity elements and validated using Laue diffraction. A direct optical band gap of 0.98 eV is observed for a crystal with Cu/(Zn + Sn) = 0.85. Van der Pauw–Hall resistance analysis shows decreasing hole concentration, from 10 19  cm −3 to 2 × 10 15  cm −3 , with decreasing copper content over the composition range. Hole mobility varies from 50 cm 2  V −1  s −1 to 160 cm 2  V −1  s −1 , with no dependence on copper concentration. A linear temperature dependence of the Seebeck coefficient is found for all crystals. The Seebeck coefficient–carrier concentration dependence is used to determine the valence band density of states, N V , and corresponding effective mass, μ h *. Crystals with Cu/(Zn + Sn) < 0.9 have N V  = 4 × 10 18  cm −3 and μ h * = 0.4 m 0 while crystals with elevated copper concentration, Cu/(Zn + Sn) > 0.9, exhibit higher density of states, N V  = 3 × 10 19  cm −3 and hole effective mass μ h * = 0.9 m 0 . The increased valence band density of states at elevated copper composition is consistent with more Cu–Zn exchange sites contributing to bulk defects and band edge fluctuations. Temperature‐dependent conductivity measurements indicate a transition from metallic‐type to semiconductor‐type conduction at Cu/(Zn + Sn) < 0.9. At lower copper content, for a crystal with Cu/(Zn + Sn) = 0.83 and p  = 10 17  cm −3 the activation energy for intrinsic conduction is 60 meV. This behavior is attributed to the copper vacancy defect, V Cu , and is comparable to reported values obtained in thin films and by first‐principles predictions.

Sponsoring Organization:
USDOE
Grant/Contract Number:
DE‐EE0006334
OSTI ID:
1542679
Journal Information:
Physica Status Solidi B. Basic Solid State Physics, Journal Name: Physica Status Solidi B. Basic Solid State Physics Vol. 256 Journal Issue: 11; ISSN 0370-1972
Publisher:
Wiley Blackwell (John Wiley & Sons)Copyright Statement
Country of Publication:
Germany
Language:
English
Citation Metrics:
Cited by: 2 works
Citation information provided by
Web of Science

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Cu 2 ZnSnSe 4 Thin-Film Solar Cells by Thermal Co-evaporation with 11.6% Efficiency and Improved Minority Carrier Diffusion Length journal December 2014
Temperature dependent electrical characterization of thin film Cu 2 ZnSnSe 4 solar cells journal January 2016
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Luminescence of Cu 2 ZnSnS 4 polycrystals described by the fluctuating potential model journal June 2013
Modification of defects and potential fluctuations in slow-cooled and quenched Cu 2 ZnSnSe 4 single crystals journal February 2017
Classification of Lattice Defects in the Kesterite Cu 2 ZnSnS 4 and Cu 2 ZnSnSe 4 Earth-Abundant Solar Cell Absorbers journal February 2013
Correlation between intrinsic defects and electrical properties in the high-quality Cu 2 ZnSnS 4 single crystal journal September 2013
Growth of Cu2ZnSnSe4 single crystals from Sn solutions journal September 2012