high quality thin film growth of bazrs3 by pulsed laser

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Professor Ravichandran's Laboratory for Complex Materials and Devices aims to characterize potential materials for semiconductor applications. Currently, my Ph.D. mentor synthesizes thin film crystals to measure the material's microscale properties. The benefits of Dr. Ravichandran's research include greater accessibility of photovoltaics, since the chalcogenide perovskites have the potential to form a cost- effective, energy efficient source. Take initiative to study topics on your own to get the best value out of SHINE. Ask your mentors any questions you may have and remember that they want you to succeed! Don't be shy. Enjoy your cohort's company in these 7 weeks :) Many thanks to Professor Ravichandran, my mentor Mythili Surendran, Huandong Chen, my partner Athalia Meron, Boyang Zhao, Dr. Katherine Mills, Cathalina Juarez, Erica de Guzman, the Center Mentors, and the whole cohort for their encouragement and guidance. I am very grateful SHINE 2020 continued virtually. Thank you to my parents and teachers for their "cheerleading." :D The lab previously synthesized bulk crystals of chalcogenide perovskites. The lab produces bulk crystals through vapor transport and flux growth methods: BaS + Zr + 2S →BaZrS 3 The bandgap of BaZrS 3 was confirmed to be 1.8 eV using Photoluminescense Spectroscopy. To study the properties of the BaZrS 3 further, thin films of BaZrS 3 were deposited onto an SrTiO 3 / Si substrate from a target using Pulsed Laser Deposition (PLD). The BaZrS 3 powder was pressed into a pellet (seen in Figures 4 and 5 above) and characterized by X-Ray Diffraction. Perovskites are a class of materials of the form ABX 3 . This unique structure gives them a variety of functional properties that make them strong candidates for photovoltaic applications, since chalcogenides (materials containing S, Se, or Te) have a promising bandgap and tunability that provide beneficial optoelectrical properties. I. Structural and Surface After producing the thin films, the lab conducts X-Ray Reflectivity, a surface scattering technique, to measure thin film qualities such as density and thickness. Using Bragg's Law, we can see that the intensity corresponds to a thickness of 68 nm. With Atomic Force Microscopy, we can measure the material's roughness to be 1.5 nm. II. Chemical X-Ray Fluorescence (XRF) also demonstrates that the films, grown in optimal conditions, are stoichiometric. Introduction Synthesis of Bulk BZS Crystals Synthesis of Thin Film BZS by PLD The Next Steps for the Lab Acknowledgements Fig. 2: Perovskite Solar Cell Models PC: Energy.gov Objective & Impact of Professor’s Research High Quality Thin Film Growth of BaZrS 3 by Pulsed Laser Deposition Maanasi Dhiraj ([email protected]) Immaculate Heart High School, Class of 2021 Mork Family Department of Chemical Engineering and Materials Science, SHINE 2020 Advice for Future SHINE Students Ravichandran lab will try to optimize growth conditions for high quality, crystalline epitaxial thin films of BaZrS 3 . With more detailed microscopic analysis, the lab can demonstrate applications in photovoltaic devices. In the Ravichandran Materials Science lab, I learned semiconductor basics and MATLAB software to plot spectrocopy data. My previous math and chemistry classes allowed me to appreciate the emphasis on structure and characterization. I plan to apply these research principles in my AP Capstone class and my Math and Science Club. I look forward to visiting the lab in person. How This Relates to My STEM Coursework / Future Fig. 1: Structure of BaZrS3 PC: Shanyuan Niu Fig. 3: PL of BaZrS 3 PC: Maanasi Dhiraj Fig. 4: BaZrS 3 Pellet PC: Mythili Surendran Fig. 5: Pellet Mounted onto PLD Stage PC: Mythili Surendran Fig. 6: PLD Schematic PC: ResearchGate Fig. 7: PLD Chamber at Ravichandran Lab PC: Mythili Surendran Fig. 9: XRR Plot of BaZrS 3 film on SrTiO 3 / Si substrate PC: Maanasi Dhiraj Characterization Fig. 9: XRF Plot of BaZrS 3 film on SrTiO3 / Si substrate PC: Mythili Surendran Fig. 3: XRD of BaZrS 3 Pellet PC: Maanasi Dhiraj

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Page 1: High Quality Thin Film Growth of BaZrS3 by Pulsed Laser

Professor Ravichandran's Laboratory for Complex Materials and Devices aims to characterize potential materials for semiconductor applications. Currently, my Ph.D. mentor synthesizes thin film crystals to measure the material's microscale properties.

The benefits of Dr. Ravichandran's research include greater accessibility of photovoltaics, since the chalcogenide perovskites have the potential to form a cost-effective, energy efficient source.

Take initiative to study topics on your own to get the best value out of SHINE. Ask your mentors any questions you may have and remember that they want you to succeed! Don't be shy. Enjoy yourcohort's company in these 7 weeks :)

Many thanks to Professor Ravichandran,my mentor Mythili Surendran, HuandongChen, my partner Athalia Meron, BoyangZhao, Dr. Katherine Mills, CathalinaJuarez, Erica de Guzman, the CenterMentors, and the whole cohort for their encouragement and guidance. I am very grateful SHINE 2020 continued virtually. Thank you to my parents and teachers for their "cheerleading." :D

The lab previously synthesized bulk crystals of chalcogenide perovskites. The lab produces bulk crystals through vapor transport and flux growth methods: BaS + Zr + 2S →BaZrS3

The bandgap ofBaZrS3 was confirmed

to be 1.8 eV usingPhotoluminescense

Spectroscopy.

To study the properties of the BaZrS3 further, thin films of BaZrS3 were deposited onto an SrTiO3 / Si substrate from a target using Pulsed Laser Deposition (PLD). The BaZrS3 powder was pressed into a pellet (seen in Figures 4 and 5 above) and characterized by X-Ray Diffraction.

Perovskites are a class of materials of the form ABX3. This unique structure gives them a variety of functional properties that make them strong candidates for photovoltaic applications, sincechalcogenides(materialscontaining S, Se, orTe) have a promising bandgapand tunability thatprovide beneficialoptoelectricalproperties.

I. Structural and SurfaceAfter producing the thin films, the lab conducts X-Ray Reflectivity, a surface scattering technique,to measure thin filmqualities such asdensity andthickness. UsingBragg's Law,we can see that theintensity correspondsto a thickness of 68 nm.

With Atomic Force Microscopy, we can measure the material's roughness to be 1.5 nm.

II. ChemicalX-Ray Fluorescence(XRF) alsodemonstratesthat the films,grown in optimalconditions,are stoichiometric.

Introduction Synthesis of Bulk BZS Crystals Synthesis of Thin Film BZS by PLD

The Next Steps for the Lab

Acknowledgements

Fig. 2: Perovskite Solar Cell ModelsPC: Energy.gov

Objective & Impact of Professor’s Research

High Quality Thin Film Growth of BaZrS3 by Pulsed Laser DepositionMaanasi Dhiraj ([email protected])

Immaculate Heart High School, Class of 2021Mork Family Department of Chemical Engineering and Materials Science, SHINE 2020

Advice for Future SHINE Students

Ravichandran lab will try to optimize growth conditions for high quality, crystalline epitaxial thin films of BaZrS3. With more detailed microscopic analysis, the lab can demonstrate applications in photovoltaic devices.

In the Ravichandran Materials Science lab, I learned semiconductor basics and MATLAB software to plot spectrocopy data. My previous math and chemistry classes allowed me to appreciate the emphasis on structure and characterization. I plan to apply these research principles in my AP Capstone class and my Math and Science Club. I look forward to visiting the lab in person.

How This Relates to My STEM Coursework / Future

Fig. 1: Structure of BaZrS3PC: Shanyuan Niu

Fig. 3: PL of BaZrS3PC: Maanasi Dhiraj

Fig. 4: BaZrS3 PelletPC: Mythili Surendran

Fig. 5: Pellet Mounted onto PLD Stage

PC: Mythili Surendran

Fig. 6: PLDSchematic

PC: ResearchGate

Fig. 7: PLDChamber at

Ravichandran LabPC: Mythili Surendran

Fig. 9: XRR Plot of BaZrS3film on SrTiO3 / Si

substratePC: Maanasi Dhiraj

Characterization

Fig. 9: XRF Plot of BaZrS3film on SrTiO3 / Si substratePC: Mythili Surendran

Fig. 3: XRD of BaZrS3 Pellet

PC: Maanasi Dhiraj