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Structural, opto-electronic characteristics and second harmonic generation of solution processed CH3NH3PbI3-xClx thin film prepared by spray pyrolysis

[Display omitted] •Nanorods like crystalline CH3NH3PbI3-xClx thin film at an ambient atmosphere by spray deposition.•High absorption coefficient with a band gap of 1.64 eV.•Structural phase transition from tetragonal (at RT) to orthorhombic (at 80 K).•Generation of second harmonic emission. Nanorod...

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Published in:Materials science & engineering. B, Solid-state materials for advanced technology Solid-state materials for advanced technology, 2020-09, Vol.259, p.114599, Article 114599
Main Authors: Tanveer Karim, A.M.M., Khan, M.K.R., Hossain, M.S., Kamruzzaman, M., Azizar Rahman, M., Mozibur Rahman, M.
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cited_by cdi_FETCH-LOGICAL-c328t-8e91c5ab6920f378f91b7ebf0657b12916766e11e7dfa7585022c1df4687271a3
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container_title Materials science & engineering. B, Solid-state materials for advanced technology
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creator Tanveer Karim, A.M.M.
Khan, M.K.R.
Hossain, M.S.
Kamruzzaman, M.
Azizar Rahman, M.
Mozibur Rahman, M.
description [Display omitted] •Nanorods like crystalline CH3NH3PbI3-xClx thin film at an ambient atmosphere by spray deposition.•High absorption coefficient with a band gap of 1.64 eV.•Structural phase transition from tetragonal (at RT) to orthorhombic (at 80 K).•Generation of second harmonic emission. Nanorod like crystalline CH3NH3PbI3-xClx thin film was prepared by spray pyrolysis at an ambient atmosphere. X-ray diffraction (XRD) and Raman studies reveal the tetragonal perovskite phase of spray deposited film. The optical band gap of CH3NH3PbI3-xClx is estimated to ~1.64 eV which is consistent with vacuum based deposited perovskites. The CH3NH3PbI3-xClx film exhibits a high absorption coefficient of the order of 106 m−1. Photoluminescence (PL) study suggests that band-to-band radiative recombination occurs in CH3NH3PbI3-xClx film. Cathodoluminescence study confirms the emission of 1.67 eV at 80 K and 1.80 eV at 300 K. In this study, the second harmonic generation at photon energy 3.6 eV is reported for the first time at room temperature (RT). It is noted that the band edge peak position at 1.67 eV is being diffused and shifted to 1.80 eV at RT while the second harmonic peak position at 3.6 eV remains unchanged.
doi_str_mv 10.1016/j.mseb.2020.114599
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Nanorod like crystalline CH3NH3PbI3-xClx thin film was prepared by spray pyrolysis at an ambient atmosphere. X-ray diffraction (XRD) and Raman studies reveal the tetragonal perovskite phase of spray deposited film. The optical band gap of CH3NH3PbI3-xClx is estimated to ~1.64 eV which is consistent with vacuum based deposited perovskites. The CH3NH3PbI3-xClx film exhibits a high absorption coefficient of the order of 106 m−1. Photoluminescence (PL) study suggests that band-to-band radiative recombination occurs in CH3NH3PbI3-xClx film. Cathodoluminescence study confirms the emission of 1.67 eV at 80 K and 1.80 eV at 300 K. In this study, the second harmonic generation at photon energy 3.6 eV is reported for the first time at room temperature (RT). 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B, Solid-state materials for advanced technology</title><description>[Display omitted] •Nanorods like crystalline CH3NH3PbI3-xClx thin film at an ambient atmosphere by spray deposition.•High absorption coefficient with a band gap of 1.64 eV.•Structural phase transition from tetragonal (at RT) to orthorhombic (at 80 K).•Generation of second harmonic emission. Nanorod like crystalline CH3NH3PbI3-xClx thin film was prepared by spray pyrolysis at an ambient atmosphere. X-ray diffraction (XRD) and Raman studies reveal the tetragonal perovskite phase of spray deposited film. The optical band gap of CH3NH3PbI3-xClx is estimated to ~1.64 eV which is consistent with vacuum based deposited perovskites. The CH3NH3PbI3-xClx film exhibits a high absorption coefficient of the order of 106 m−1. Photoluminescence (PL) study suggests that band-to-band radiative recombination occurs in CH3NH3PbI3-xClx film. Cathodoluminescence study confirms the emission of 1.67 eV at 80 K and 1.80 eV at 300 K. In this study, the second harmonic generation at photon energy 3.6 eV is reported for the first time at room temperature (RT). It is noted that the band edge peak position at 1.67 eV is being diffused and shifted to 1.80 eV at RT while the second harmonic peak position at 3.6 eV remains unchanged.</description><subject>Absorptivity</subject><subject>Cathodoluminescence</subject><subject>Emission analysis</subject><subject>Nanorods</subject><subject>Optoelectronics</subject><subject>Perovskite thin film</subject><subject>Perovskites</subject><subject>Photoluminescence</subject><subject>Radiative recombination</subject><subject>Raman spectroscopy</subject><subject>Room temperature</subject><subject>Second harmonic emission</subject><subject>Second harmonic generation</subject><subject>Spray pyrolysis</subject><subject>Thin films</subject><subject>XRD</subject><issn>0921-5107</issn><issn>1873-4944</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><recordid>eNp9kMFO3DAQhq2qlbqlvEBPlnptFtuJ40TqBa1KFwkBEnC2HGdcvMrGweMg8iJ9XrwsZ04z8ny_Z_QR8oOzNWe8Ptut9wjdWjCRH3gl2_YTWfFGlUXVVtVnsmKt4IXkTH0l3xB3jDEuhFiR_3cpzjbN0Qy_aJhSKGAAm2IYvaX20URjE0SPyVukZuwpgg255Mn-jfkHI0STfBhpcBTDML_1UwwWEKGnm215vS1vu8uyeNkMLzQ9-pE6P-wzA5OJGekWilM0C52WGIYFPX4nX5wZEE7f6wl5uPhzv9kWVzd_LzfnV4UtRZOKBlpupenqVjBXqsa1vFPQOVZL1XHR8lrVNXAOqndGyUYyISzvXVU3SihuyhPy8_hvvvdpBkx6F-Y45pVaVDJTTSllpsSRsjEgRnB6in5v4qI50wf_eqcP_vXBvz76z6HfxxDk-589RI3Ww2ih9zEb1n3wH8VfAcJ3kLc</recordid><startdate>202009</startdate><enddate>202009</enddate><creator>Tanveer Karim, A.M.M.</creator><creator>Khan, M.K.R.</creator><creator>Hossain, M.S.</creator><creator>Kamruzzaman, M.</creator><creator>Azizar Rahman, M.</creator><creator>Mozibur Rahman, M.</creator><general>Elsevier B.V</general><general>Elsevier BV</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>202009</creationdate><title>Structural, opto-electronic characteristics and second harmonic generation of solution processed CH3NH3PbI3-xClx thin film prepared by spray pyrolysis</title><author>Tanveer Karim, A.M.M. ; Khan, M.K.R. ; Hossain, M.S. ; Kamruzzaman, M. ; Azizar Rahman, M. ; Mozibur Rahman, M.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c328t-8e91c5ab6920f378f91b7ebf0657b12916766e11e7dfa7585022c1df4687271a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>Absorptivity</topic><topic>Cathodoluminescence</topic><topic>Emission analysis</topic><topic>Nanorods</topic><topic>Optoelectronics</topic><topic>Perovskite thin film</topic><topic>Perovskites</topic><topic>Photoluminescence</topic><topic>Radiative recombination</topic><topic>Raman spectroscopy</topic><topic>Room temperature</topic><topic>Second harmonic emission</topic><topic>Second harmonic generation</topic><topic>Spray pyrolysis</topic><topic>Thin films</topic><topic>XRD</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Tanveer Karim, A.M.M.</creatorcontrib><creatorcontrib>Khan, M.K.R.</creatorcontrib><creatorcontrib>Hossain, M.S.</creatorcontrib><creatorcontrib>Kamruzzaman, M.</creatorcontrib><creatorcontrib>Azizar Rahman, M.</creatorcontrib><creatorcontrib>Mozibur Rahman, M.</creatorcontrib><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Materials science &amp; engineering. 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Photoluminescence (PL) study suggests that band-to-band radiative recombination occurs in CH3NH3PbI3-xClx film. Cathodoluminescence study confirms the emission of 1.67 eV at 80 K and 1.80 eV at 300 K. In this study, the second harmonic generation at photon energy 3.6 eV is reported for the first time at room temperature (RT). It is noted that the band edge peak position at 1.67 eV is being diffused and shifted to 1.80 eV at RT while the second harmonic peak position at 3.6 eV remains unchanged.</abstract><cop>Lausanne</cop><pub>Elsevier B.V</pub><doi>10.1016/j.mseb.2020.114599</doi></addata></record>
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subjects Absorptivity
Cathodoluminescence
Emission analysis
Nanorods
Optoelectronics
Perovskite thin film
Perovskites
Photoluminescence
Radiative recombination
Raman spectroscopy
Room temperature
Second harmonic emission
Second harmonic generation
Spray pyrolysis
Thin films
XRD
title Structural, opto-electronic characteristics and second harmonic generation of solution processed CH3NH3PbI3-xClx thin film prepared by spray pyrolysis
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