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			<titleStmt><title level='a'>Ultrafast Heterodyne Infrared Nano-Imaging of Polaron Dynamics in Lead Halide Perovskites</title></titleStmt>
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				<date>2021 Fall</date>
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				<bibl> 
					<idno type="par_id">10317259</idno>
					<idno type="doi">10.1364/CLEO_QELS.2021.FTu4I.5</idno>
					<title level='j'>Quantum Electronics and Laser Science</title>
<idno>2160-8989</idno>
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					<author>J Nishida</author><author>J Ye</author><author>P Sharma</author><author>S. E. Shaheen</author><author>M. B. Raschke</author>
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			<abstract><ab><![CDATA[Ultrafast heterodyne infrared nano-imaging has been developed to reveal nanoscale heterogeneity of polaron formation, dynamics, and polaron-cation coupling in lead halide perovskites, with real space-time mapping of elementary electron-phonon coupling underlying their optoelectronic response.]]></ab></abstract>
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<div xmlns="http://www.tei-c.org/ns/1.0"><head n="1.">Introduction</head><p>Lead halide perovskites exhibit remarkable photovoltaic performance, characterized by long carrier lifetime and extraordinary defect tolerance. The highly dynamical lattice of the perovskites is believed to play a key role by forming a large polaron (Fig. <ref type="figure">1A</ref>), which arises from electron-phonon coupling across multiple unit cells and stabilizes the photoinduced carriers. On the other hand, the perovskite films are known to be spatially non-uniform in their optoelectronic response, yet the fundamental origin of such disorder, particularly in relation to the elementary electronphonon coupling, has remained elusive.</p><p>Here, we develop ultrafast heterodyne infrared nano-imaging <ref type="bibr">[1]</ref> to provide access to the full spatio-temporal-spectral response dynamics and apply to a triple cation perovskite film <ref type="bibr">[2]</ref> to reveal its polaron dynamics on the nanoscale. By directly probing the pump-induced mid-infrared "polaron absorption" (Fig. <ref type="figure">1B</ref>) with nanometer spatial resolution <ref type="bibr">[3]</ref>, we resolve the heterogeneity in the polaron formation and its dynamics on the picosecond scale. By taking advantage of the combined spatial, temporal, and spectral resolution, we also probe a nano-localized transient molecular vibrational response that signifies the coupling between polaron and molecular cations. We thus characterize the nanoscale disorder in perovskites from the perspective of the fundamental electron-phonon coupling, the control of which is critical for the engineering of perovskite-based optoelectronic devices.</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head n="2.">Ultrafast heterodyne infrared nano-imaging system</head><p>Fig. <ref type="figure">1C</ref> shows the schematic of our ultrafast heterodyne infrared nano-imaging and -spectroscopy system <ref type="bibr">[1]</ref>. The optical pump and mid-infrared probe pulses are collinearly focused to a metallic tip apex in an atomic force  microscope, inducing a nanoscale pump-probe signal <ref type="bibr">[4]</ref>. The near-field pump-probe signal is interfered with a reference pulse for heterodyne detection, implementing phase and spectral resolution (Fig. <ref type="figure">1D,</ref><ref type="figure">1E</ref>) and also eliminating contributions arising from the uncontrolled interference of the near-field signal with the far-field background scatter <ref type="bibr">[5]</ref>.</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head n="3.">Polaronic heterogeneity in a lead halide perovskite</head><p>We study a triple cation perovskite (Fig. <ref type="figure">2A</ref>), [(FA 0.83 MA 0.17 ) 0.95 Cs 0.05 ]Pb(I 0.83 Br 0.17 ) 3 , as a highly stable model system of the perovskites. Fig. <ref type="figure">2B</ref> shows conventional far-field visible-pump/mid-infrared-probe decay profiles with pronounced dependence on the pump fluence, suggesting that the observed carrier dynamics are dominated by the second and higher order carrier recombination. For a given fluence, we acquire pump-probe spectra (Fig. <ref type="figure">2C</ref>), demonstrating the peak-like structure around 1100-1200 cm -1 with tail on the high-frequency side, consistent with the spectral response expected for polaron absorption <ref type="bibr">[3]</ref>. The time evolution of the spectral line shape signifies increasing polaron size as the pump-probe waiting time is increased. Fig. <ref type="figure">2D</ref> shows a spatio-temporal mapping of such polaron absorption by ultrafast heterodyne infrared nano-imaging, demonstrating the heterogeneity both in polaron formation and polaron recombination dynamics <ref type="bibr">[2]</ref>. To further characterize the disordered nature of the coupling between the photoinduced carriers and perovskite lattice, we measure a transient vibrational response arising from the coupling between polaron and molecular cation at the nanoscale (Fig. <ref type="figure">2E</ref>). The spatial variation in the transient vibrational peak position (Fig. <ref type="figure">2F</ref>) demonstrates the non-uniform charge-cation coupling, suggesting that the observed heterogeneity in polaron absorption likely relates to the disorder in the dynamical lattice elasticity <ref type="bibr">[6]</ref>.</p></div>
<div xmlns="http://www.tei-c.org/ns/1.0"><head n="4.">Conclusions</head><p>In this work, we establish ultrafast heterodyne infrared nano-imaging as a tool to characterize the heterogeneity in polaron dynamics, as well as an enabling method for transient vibrational nano-spectroscopy which reveals disordered charge-lattice coupling. The technique is generally applicable to address disorder in electron-phonon coupling, which has been identified in a variety of systems including two-dimensional materials and superconductors. </p></div><note xmlns="http://www.tei-c.org/ns/1.0" place="foot" xml:id="foot_0"><p>Authorized licensed use limited to: UNIVERSITY OF COLORADO. Downloaded on February 28,2022 at 10:48:02 UTC from IEEE Xplore. Restrictions apply.</p></note>
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