Katy Hartman
Massachusetts Institute of Technology
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Featured researches published by Katy Hartman.
Applied Physics Letters | 2013
Prasert Sinsermsuksakul; Katy Hartman; Sang Bok Kim; Jaeyeong Heo; Leizhi Sun; Helen Hejin Park; Rupak Chakraborty; Tonio Buonassisi; Roy G. Gordon
SnS is a promising earth-abundant material for photovoltaic applications. Heterojuction solar cells were made by vapor deposition of p-type tin(II) sulfide, SnS, and n-type zinc oxysulfide, Zn(O,S), using a device structure of soda-lime glass/Mo/SnS/Zn(O,S)/ZnO/ITO. A record efficiency was achieved for SnS-based thin-film solar cells by varying the oxygen-to-sulfur ratio in Zn(O,S). Increasing the sulfur content in Zn(O,S) raises the conduction band offset between Zn(O,S) and SnS to an optimum slightly positive value. A record SnS/Zn(O,S) solar cell with a S/Zn ratio of 0.37 exhibits short circuit current density (Jsc), open circuit voltage (Voc), and fill factor (FF) of 19.4 mA/cm2, 0.244 V, and 42.97%, respectively, as well as an NREL-certified total-area power-conversion efficiency of 2.04% and an uncertified active-area efficiency of 2.46%.
Advanced Materials | 2014
Vera Steinmann; R. Jaramillo; Katy Hartman; Rupak Chakraborty; Riley E. Brandt; Jeremy R. Poindexter; Yun Seog Lee; Leizhi Sun; Alexander Polizzotti; Helen Hejin Park; Roy G. Gordon; Tonio Buonassisi
Tin sulfide (SnS), as a promising absorber material in thin-film photovoltaic devices, is described. Here, it is confirmed that SnS evaporates congruently, which provides facile composition control akin to cadmium telluride. A SnS heterojunction solar cell is demons trated, which has a power conversion efficiency of 3.88% (certified), and an empirical loss analysis is presented to guide further performance improvements.
Applied Physics Letters | 2008
Katy Hartman; Mariana I. Bertoni; James G. Serdy; Tonio Buonassisi
We propose and demonstrate a method to remove performance-limiting dislocations from multicrystalline silicon (mc-Si) solar cell material, appropriate for wafers or bricks. Dislocation density reductions of >95% are achieved in commercial mc-Si via high temperature annealing with an impurity diffusion barrier, with controlled ambient and time-temperature profiles. The dislocation density reduction follows temperature-dependent models developed by Kuhlmann [Proc. Phys. Soc., London, Sect. A 64, 140 (1951)] and Nes [Acta Metall. Mater. 43, 2189 (1995)]. It is believed that higher annealing temperatures (>1170 °C) allow dislocation movement unconstrained by crystallographic glide planes, leading to dislocation annihilation within minutes.
Applied Physics Letters | 2014
Vladan Stevanović; Katy Hartman; R. Jaramillo; Shriram Ramanathan; Tonio Buonassisi; Peter Graf
We investigated the dependence of absolute SnS band-edge energies on surface orientation using density functional theory and GW method for all surfaces with Miller indices −3≤h,k,l≤3 and found variations as large as 0.9 eV as a function of (hkl). Variations of this magnitude may affect significantly the performance of photovoltaic devices based on polycrystalline SnS thin-films and, in particular, may contribute to the relatively low measured open circuit voltage of SnS solar cells. X-ray diffraction measurements confirm that our thermally evaporated SnS films exhibit a wide distribution of different grain orientations, and the results of Kelvin force microscopy support the theoretically predicted variations of the absolute band-edge energies.
Journal of Applied Physics | 2016
R. Jaramillo; Meng-Ju Sher; Benjamin K. Ofori-Okai; Vera Steinmann; Chuanxi Yang; Katy Hartman; Keith A. Nelson; Aaron M. Lindenberg; Roy G. Gordon; Tonio Buonassisi
Materials research with a focus on enhancing the minority-carrier lifetime of the light-absorbing semiconductor is key to advancing solar energy technology for both early-stage and mature material platforms alike. Tin sulfide (SnS) is an absorber material with several clear advantages for manufacturing and deployment, but the record power conversion efficiency remains below 5%. We report measurements of bulk and interface minority-carrier recombination rates in SnS thin films using optical-pump, terahertz (THz)-probe transient photoconductivity (TPC) measurements. Post-growth thermal annealing in H_2S gas increases the minority-carrier lifetime, and oxidation of the surface reduces the surface recombination velocity. However, the minority-carrier lifetime remains below 100 ps for all tested combinations of growth technique and post-growth processing. Significant improvement in SnS solar cell performance will hinge on finding and mitigating as-yet-unknown recombination-active defects. We describe in detail our methodology for TPC experiments, and we share our data analysis routines as freely-available software.
Applied Physics Letters | 2015
Ritayan Chakraborty; Vera Steinmann; Niall M. Mangan; Riley E. Brandt; Jeremy R. Poindexter; R. Jaramillo; Jonathan P. Mailoa; Katy Hartman; Alexander Polizzotti; Chuanxi Yang; Roy G. Gordon; Tonio Buonassisi
We quantify the effects of growth temperature on material and device properties of thermally evaporated SnS thin-films and test structures. Grain size, Hall mobility, and majority-carrier concentration monotonically increase with growth temperature. However, the charge collection as measured by the long-wavelength contribution to short-circuit current exhibits a non-monotonic behavior: the collection decreases with increased growth temperature from 150 °C to 240 °C and then recovers at 285 °C. Fits to the experimental internal quantum efficiency using an opto-electronic model indicate that the non-monotonic behavior of charge-carrier collection can be explained by a transition from drift- to diffusion-assisted components of carrier collection. The results show a promising increase in the extracted minority-carrier diffusion length at the highest growth temperature of 285 °C. These findings illustrate how coupled mechanisms can affect early stage device development, highlighting the critical role of direct...
Journal of Visualized Experiments | 2015
R. Jaramillo; Vera Steinmann; Chuanxi Yang; Katy Hartman; Rupak Chakraborty; Jeremy R. Poindexter; Mariela Lizet Castillo; Roy G. Gordon; Tonio Buonassisi
Tin sulfide (SnS) is a candidate absorber material for Earth-abundant, non-toxic solar cells. SnS offers easy phase control and rapid growth by congruent thermal evaporation, and it absorbs visible light strongly. However, for a long time the record power conversion efficiency of SnS solar cells remained below 2%. Recently we demonstrated new certified record efficiencies of 4.36% using SnS deposited by atomic layer deposition, and 3.88% using thermal evaporation. Here the fabrication procedure for these record solar cells is described, and the statistical distribution of the fabrication process is reported. The standard deviation of efficiency measured on a single substrate is typically over 0.5%. All steps including substrate selection and cleaning, Mo sputtering for the rear contact (cathode), SnS deposition, annealing, surface passivation, Zn(O,S) buffer layer selection and deposition, transparent conductor (anode) deposition, and metallization are described. On each substrate we fabricate 11 individual devices, each with active area 0.25 cm(2). Further, a system for high throughput measurements of current-voltage curves under simulated solar light, and external quantum efficiency measurement with variable light bias is described. With this system we are able to measure full data sets on all 11 devices in an automated manner and in minimal time. These results illustrate the value of studying large sample sets, rather than focusing narrowly on the highest performing devices. Large data sets help us to distinguish and remedy individual loss mechanisms affecting our devices.
photovoltaic specialists conference | 2014
Niall M. Mangan; Riley E. Brandt; Vera Steinmann; R. Jaramillo; Jian V. Li; Jeremy R. Poindexter; Katy Hartman; Leizhi Sun; Roy G. Gordon; Tonio Buonassisi
We preform device simulations of a tin sulfide (SnS) device stack using SCAPS to define a path to 10% efficient devices. We determine and constrain a baseline device model using recent experimental results on one of our 3.9% efficient cells. Through a multistep fitting process, we find a conduction band cliff of -0.2 eV between SnS and Zn(O,S) to be limiting the open circuit voltage (VOC). To move towards a higher efficiency, we can optimize the buffer layer band alignment. Improvement of the SnS lifetime to >1 ns is necessary to reach 10% efficiency. Additionally, absorber-buffer interface recombination must be suppressed, either by reducing recombination activity of defects or creating a strong inversion layer at the interface.
photovoltaic specialists conference | 2014
Katy Hartman; Vera Steinmann; R. Jaramillo; Rupak Chakraborty; Helen Hejin Park; Leizhi Sun; Riley E. Brandt; Yun Seog Lee; Roy G. Gordon; Tonio Buonassisi
Tin sulfide is regarded as a possible earth-abundant alternative for chalcogenide thin film photovoltaics. The material has strong absorption in the visible wavelength region and the possibility for high carrier mobility. We review recent progress for SnS solar cell efficiencies. Annealing in H2S gas and surface passivation of SnS are thought to be two key components that increase efficiency of SnS devices. An efficiency of η = 3.88% [1] was achieved via thermal evaporation, a manufacturing-friendly deposition method.
photovoltaic specialists conference | 2014
Rupak Chakraborty; Vera Steinmann; R. Jaramillo; Katy Hartman; Riley E. Brandt; Helen Hejin Park; Jeremy R. Poindexter; Yun Seog Lee; Roy G. Gordon; Tonio Buonassisi
Tin (II) sulfide is a promising earth-abundant thin-film solar absorber material due to its strong absorption and near-optimal bandgap. We demonstrate phase-pure evaporation of SnS in a CdTe-like manufacturing process, achieving phase-pure SnS thin-films through thermal evaporation of SnS powder. We investigate the effects of SnS film thickness and growth rate on film morphology and correlate results with device performance. Working devices are achieved with SnS film thicknesses as low as 370 nm and growth rates of up to 50 Å/s, with efficiencies ranging from 1.1% to 2.6% in as-grown films.