Geoffrey F. Strouse’s research while affiliated with Florida State University and other places

What is this page?


This page lists works of an author who doesn't have a ResearchGate profile or hasn't added the works to their profile yet. It is automatically generated from public (personal) data to further our legitimate goal of comprehensive and accurate scientific recordkeeping. If you are this author and want this page removed, please let us know.

Publications (207)


Cooling Mixed A-Site Halide Perovskites: Impact of Temperature on Optical and Structural Properties
  • Article

September 2024

·

8 Reads

Chemistry of Materials

Colette M. Sullivan

·

Jason E. Kuszynski

·

Alexey Kovalev

·

[...]

·




Optical and structural characterization of CTO nanocrystals. a) pXRD of CTO PSNCs with corresponding inverse spinel CTO reflections. b) HAADF‐STEM of CTO PSNCs showing octahedron‐like shape. c) UV–vis–NIR absorption spectrum with a Tauc plot inset showing a calculated optical Eg of 3.89 eV. d) Extinction spectrum of the LSPR fitted to a three‐mode simplified Drude approximation illustrating the corner, edge, and face contributions.
HAADF‐STEM experiments of CTO PSNCs. a) Tilting images at 30°, 0°, and –30° probing different PSNC orientations showing octahedron‐like shape. b) Two neighboring PSNCs express different morphologies depending on the PSNC orientation relative to the electron beam. c,d) Simulated and HAADF‐STEM of CTO PSNCs showing d‐spacing of 2.65 Å (222). An obtuse angle of 109.47° is drawn to illustrate the dihedral angle for an octahedron shape. e,f) Simulated and HAADF‐STEM of CTO PSNCs showing d‐spacing of 3.24 Å (220).
Overall density of state (DOS) and detailed orbital makeup of a) Cd2SnO4, b) Cd1.5Sn1.5O4, c) CdSn2O4. d) Quadratic fit of the optical bandgaps calculated from the DOS as a function of Sn stoichiometry with an inset showing the representative unit cell for Cd2‐xSnx+1O4 used for calculations. The fit yields an optical bandgap of 3.84 eV for an NC with a Cd1.86Sn1.14O4 composition.
Dropcasted CTO on a quartz substrate was measured through magnetic field‐dependent extinction (top) and VH‐MCD spectroscopy (bottom) of the Eg band edge respectively.
¹¹³Cd and ¹¹⁹Sn SSNMR spectra of pristine a,d) and titrated b,e) CTO nanocrystals collected using a WURST‐CPMG pulse sequence. ¹¹³Cd and ¹¹⁹Sn SSNMR spectra of pristine CTO samples c,f) were acquired using a CP‐CPMG pulse sequence. All data were acquired at 18.8 T under static conditions.
Observing Metallic Carriers in Highly Faceted Plasmonic Cd2SnO4 Inverse Spinel Nanocrystals
  • Article
  • Publisher preview available

June 2024

·

48 Reads

Correlating data from optical, structural, and theoretical methods allows the properties of highly faceted Cd2SnO4 (CTO) inverted spinel plasmonic semiconductor nanocrystals (PSNCs) to be fully evaluated. The use of Sn(II) in the colloidal reaction for CTO results in reproducible octahedral PSNCs with an aspect ratio of 1.30. Correlating extinction spectra with magnetic circular dichroism yields a carrier density (n = 5.19 × 1019 cm⁻³) and carrier effective mass (m* = 0.022me) respectively. ¹¹³Cd and ¹¹⁹Sn solid‐state NMR experiments show clear evidence of metallic‐like carriers in CTO NCs based upon the observation of Knight shifts. These data suggest that carrier formation in CTO arises from Sn antisite occupation of octahedral Cd sites (SnCd). From a broader perspective, the results point to wide‐bandgap spinels as being an important but understudied class of plasmonic PSNCs.

View access options

Tailoring the aluminum nanocrystal surface oxide for all-aluminum-based antenna-reactor plasmonic photocatalysts

March 2024

·

129 Reads

·

2 Citations

Proceedings of the National Academy of Sciences

Aluminum nanocrystals (AlNCs) are of increasing interest as sustainable, earth-abundant nanoparticles for visible wavelength plasmonics and as versatile nanoantennas for energy-efficient plasmonic photocatalysis. Here, we show that annealing AlNCs under various gases and thermal conditions induces substantial, systematic changes in their surface oxide, modifying crystalline phase, surface morphology, density, and defect type and concentration. Tailoring the surface oxide properties enables AlNCs to function as all-aluminum-based antenna-reactor plasmonic photocatalysts, with the modified surface oxides providing varying reactivities and selectivities for several chemical reactions.


Cool Carriers: Triplet Diffusion Dominates Upconversion Yield

November 2023

·

11 Reads

·

3 Citations

Nanoscale

Perovskites have gained popularity both as the active material in photovoltaics and as bulk triplet sensitizers for solid-state triplet-triplet annihilation upconversion (TTA-UC). Prior to widespread implementation into commercial photovoltaics, an in-depth understanding of the environmental influences on device performance is required. To this point, the temperature-dependent structure-function properties of TTA-UC within methylammonium formamidinium lead triiodide (MAFA)/rubrene UC devices are explored. A strong temperature dependence of the underlying UC dynamics is observed, where the maximum UC efficiency is achieved at 170 K, reflecting the competition between triplet diffusion length, diffusion rate, and triplet-triplet encounter events. A combination of spectroscopic and structural methods and theoretical modelling illustrates that despite the significantly increased carrier lifetime of the perovskite at low temperatures, the TTA-UC dynamics are not governed by the underlying sensitizer properties but rather limited by the underlying triplet diffusion.


(a) Representative linear sweep voltammograms of FeCo nanocarbides in 1.0 M KOH, with a dashed line denoting the benchmarking standard current density of 10 mA cm⁻². Note that RuO2 achieved an overpotential of 0.36 V at 10 mA cm⁻² (per geometric surface area). (b) The linear regions of the Tafel plots were fitted, using the kinetically-controlled region of the voltammetry from part (a) to determine Tafel slopes, indicated by the dashed lines. Note that the Tafel slope obtained for RuO2 was 85 mV dec⁻¹
(a) Overpotentials (n = 3) required to achieve 10 mA cm⁻² (per ECSA) for FexCo1−xCy of varying % Fe, in 1.0 M KOH. (b) Tafel slopes for FexCo1−xCy of varying % Fe
(a) 3D contour plot tracking the evolution of the major carbide phase as a function of % Fe, using pXRD patterns. The black intensity represents the XRD signal, I, normalized to the maximum signal, Imax, where the most intense peaks appear darkest. Phase references are broadened to reflect 10 nm materials and overlaid (in color) to highlight differences. The references shown are for M7C3 (dark blue, ICSD: 76830), M5C2 (light blue, ICSD: 423885), M3C (blue-green, ICSD: 43521) and M2C (green, COD: 1528415). (b) Proposed phase diagram of metastable bimetallic carbides, where relative phase contributions are plotted against % Fe. The error plot (top) represents the % error (±) in each fit. Fits for select samples are shown in ESI Fig. S4.† TEM images of select FexCo1−xCy for (c) 0% Fe, (d) 15% Fe, (e) 25% Fe, (f) 75% Fe, and (g) 100% Fe. Sizes of the nanocrystals increase, as the Fe content decreases, based on histogram size analysis (n = 50–100)
Stacked X-ray photoelectron spectra for FexCo1−xCy samples of varying Fe concentrations are shown for (a) Co 2p, (b) Fe 2p, (c) O 1s, and (d) C 1s with respective contributions of chemical species below. Black lines represent raw data, red lines represent overall fits, the gray lines show the background (bkrd) and specified chemical species are shown in dark blue, green and light blue lines
(a) CVs of the 1st, 25th, and 200th cycles at a scan rate of 5 mV s⁻¹ for the FeCo nanocarbide, containing 15% Fe. (b) Overpotentials were extracted from CVs at a current density of 10 mA cm⁻² over 200 cycles. (c) Plot showing phase contributions from (Fe0.5Co0.5)2O4 (i.e. oxide) derived from XRD analysis of 15% FeCo post-electrocatalytic OER, with increasing CV cycles, using a Mo Kα source. Insets shown in (c) depict a carbide surface with an M2C crystalline phase (orthorhombic lattice) and a partially oxidized carbide surface containing (Fe0.5Co0.5)2O4 (cubic lattice), embedded in the surface layer. These lattice structures were generated using CrystalMaker software
Electrocatalytic activity and surface oxide reconstruction of bimetallic iron–cobalt nanocarbide electrocatalysts for the oxygen evolution reaction

November 2023

·

26 Reads

·

2 Citations

For renewable energy technology to become ubiquitous, it is imperative to develop efficient oxygen evolution reaction (OER) electrocatalysts, which is challenging due to the kinetically and thermodynamically unfavorable OER mechanism. Transition metal carbides (TMCs) have recently been investigated as desirable OER pre-catalysts, but the ability to tune electrocatalytic performance of bimetallic catalysts and understand their transformation under electrochemical oxidation requires further study. In an effort to understand the tunable TMC material properties for enhancing electrocatalytic activity, we synthesized bimetallic FeCo nanocarbides with a complex mixture of FeCo carbide crystal phases. The synthesized FeCo nanocarbides were tuned by percent proportion Fe (i.e. % Fe), and analysis revealed a non-linear dependence of OER electrocatalytic activity on % Fe, with a minimum overpotential of 0.42 V (15–20% Fe) in alkaline conditions. In an effort to understand the effects of Fe composition on electrocatalytic performance of FeCo nanocarbides, we assessed the structural phase and electronic state of the carbides. Although we did not identify a single activity descriptor for tuning activity for FeCo nanocarbides, we found that surface reconstruction of the carbide surface to oxide during water oxidation plays a pivotal role in defining electrocatalytic activity over time. We observed that a rapid increase of the (FexCo1−x)2O4 phase on the carbide surface correlated with lower electrocatalytic activity (i.e. higher overpotential). We have demonstrated that the electrochemical performance of carbides under harsh alkaline conditions has the potential to be fine-tuned via Fe incorporation and with control, or suppression, of the growth of the oxide phase.



Figure 1: a) Temperature dependent absorption spectra (left) for the 100 nm MAFArub bilayer highlighting the changes to the perovskite onset as the film is cooled from 300 K to 20 K (red to blue). Talc plots (right) for the two phases, denoted by grey octagons and stars, with the phase transition at 110 K included. b) Direct PL spectra for MAFArub bilayer cooling from 300 K to 20 K collected under 405 nm excitation. Three spectra were collected at each temperature then averaged. Spectral inset highlights the growth of the high energy feature at 750 nm. Grey arrows are included as guides to the eye. c) MAFArub XRD patterns (left) collected from 290 K to 30 K. Astrik denotes the instrumental artifacts. Grey dashed lines are included to highlight peak change. Calculated full-width at half max (FWHM) for the (220) plane across the temperature range.
Figure 2: a) UCPL for the 100 nm MAFArub bilayer collected under 780 nm excitation while cooling from 300 K to 20 K where three spectra were collected at each temperature then averaged. b) Direct emission of the MAFArub bilayer under 405 nm excitation collected while cooling from 300 K to 20 K. A 700 nm short-pass filter was used to isolate dye emission. Three spectra were collected at each temperature then averaged. Grey arrows are included as guides to the eye. c) (top) Integrated direct (lavender) and upconverted (red) emission for the bilayer film. (middle) Integrated UCPL (ηUC,ex) normalized to the absorption overlap of the bilayer film with the excitation laser (α(E)). Dashed grey line represents Tmax = 170 K. (bottom) The absorption, normalized integrated UCPL spectra normalized by the quantum yield of rub under direct excitation, with the equation included. Here, Tmax ' is 230 K, indicated via the dashed grey line. d) Photographs of the MAFArub bilayer under 780 nm excitation at select temperatures.
Figure 3: a) Temperature-dependent perovskite PL decays for the neat MAFA film (left) and MAFArub bilayer (right) collected under 635 nm pulsed excitation (125 kHz). Triexponential fits are included as grey lines for the MAFA decays. The grey arrow is included as a guide to the eye for the MAFArub decays. b) Amplitude weighted lifetimes (tave) for the MAFA (top) and MAFArub (bottom) films. Grey arrows are included as guides to the eye.
Figure 4: a) Temperature dependent transient absorption spectra extracted at specific delay times for the 30 nm MAFArub bilayer film. The characteristic perovskite high energy photobleach (PB1), ground state bleach (GSB), and photoinduced absorption (PIA) features are labeled. The rub T1 à T3 transition at 510 nm is included in the spectral inserts. Excess pump scattering is denoted
Fitting parameters for MAFA (black) and MAFArub (red) perovskite PL decays based on a triexponential fit.
Cool Carriers: Triplet Diffusion Dominates Upconversion Yield

September 2023

·

46 Reads

Perovskites have gained popularity both as the active material in photovoltaics and as bulk triplet sensitizers for solid-state triplet-triplet annihilation upconversion (TTA-UC). Prior to widespread implementation into commercial photovoltaics an in-depth understanding of the environmental influences on device performance is required. To this point, the temperature dependent structure-function properties of TTA-UC within methylammonium formamidinium lead triiodide (MAFA)/rubrene UC devices are explored. A strong temperature dependence of the underlying UC dynamics is observed, where the maximum UC efficiency is achieved at 170 K reflecting the competition between triplet diffusion length, diffusion rate, and triplet-triplet encounter events. A combination of spectroscopic and structural methods and theoretical modelling illustrates that despite the significantly increased carrier lifetime of the perovskite at low temperatures, the TTA-UC dynamics are not governed by the underlying sensitizer properties but rather limited by the underlying triplet diffusion.


Figure 1. Depiction of ZrO 2 -A interface with the approximate thickness of 10 and 25 cycles of ALD (i.e., TMA/H 2 O) assuming complete Al 2 O 3 layer growth at a rate of 1.1 Å per cycle.
Figure 2. ATR-IR spectra of ZrO 2 , ZrO 2 -A, ZrO 2 -A-Zn, and ZrO 2 -A-Zn after 10 cycles of ALD (ZrO 2 -A-Zn + Al 2 O 3 ) as well as neat powders of Al 2 O 3 , A, and Zn(OAc) 2 .
Influence of Al2O3 Overlayers on Intermolecular Interactions between Metal Oxide Bound Molecules

June 2023

·

43 Reads

Molecules

Intermolecular interactions on inorganic substrates can have a critical impact on the electrochemical and photophysical properties of the materials and subsequent performance in hybrid electronics. Critical to the intentional formation or inhibition of these processes is controlling interactions between molecules on a surface. In this report, we investigated the impact of surface loading and atomic-layer-deposited Al2O3 overlayers on the intermolecular interactions of a ZrO2-bound anthracene derivative as probed by the photophysical properties of the interface. While surface loading density had no impact on the absorption spectra of the films, there was an increase in excimer features with surface loading as observed by both emission and transient absorption. The addition of ALD overlayers of Al2O3 resulted in a decrease in excimer formation, but the emission and transient absorption spectra were still dominated by excimer features. These results suggest that ALD may provide a post-surface loading means of influencing such intermolecular interactions.


Citations (72)


... Analogous to binary copper sulfide nanocrystals, the decreased Fe content leaves metal vacancies in the nanocrystal lattice; charge-compensating holes resonate, generating the high optical absorbance seen in the NIR-II [35]. A recent transient absorption study by Kuszynski et al. demonstrates that in bornite, both the hole effective mass and hole density increase as Fe content decreases, thereby increasing carrier-mediated thermal conductivity [39]. This material characteristic likely contributes to contrast in photoacoustic imaging and heating efficiency in photothermal therapy. ...

Reference:

Bornite (Cu5FeS4) nanocrystals as an ultrasmall biocompatible NIR-II contrast agent for photoacoustic imaging
Iron Intermediate Band Governs Relaxation Kinetics of Bornite Plasmonic Semiconductor Nanocrystals
  • Citing Article
  • July 2024

ACS Materials Letters

... Until now, various methods have been developed for improving HER performance, including alloy [37][38][39], doping [40,41], selenization [42,43], carbonization [44][45][46][47][48], nitridation [49][50][51][52], etc. The design of cathode electrocatalysts has been introduced in many other reviews [53][54][55]; herein, we only provide some representative work. ...

Electrocatalytic activity and surface oxide reconstruction of bimetallic iron–cobalt nanocarbide electrocatalysts for the oxygen evolution reaction

... 7-10 Various methodologies have been investigated for the effective harvesting of triplet excitons within purely organic luminophores. [11][12][13] One prevalent method involves the conversion of triplet excitons into uorescent singlets via thermally activated delayed uorescence (TADF), [14][15][16][17] necessitating a molecular architecture that minimizes orbital overlap between the highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO). Alternatively, phosphorescence can be facilitated through radiative decay of triplet excitons. ...

Cool Carriers: Triplet Diffusion Dominates Upconversion Yield
  • Citing Article
  • November 2023

Nanoscale

... Combining those two advantages, microwave irradiation shows a promising prospect for the reactor design of energy-intensive processes. Recent research works have focused on processes such as methane conversion, ammonia synthesis, pyrolysis, hydrogenation, and gasification, and the synergistic effect of microwave irradiation in enhancing feedstock conversion and product yield has been brought up [19,[28][29][30][31][32][33][34][35][36][37][38][39][40][41][42][43][44][45][46][47]. The research regarding microwave-incorporated catalytic gasifier design, even under the laboratory scale, is still comparatively scarce [48]. ...

Microwave Inhibition of the Hydrogenation of CO 2 for Methane Formation
  • Citing Article
  • May 2023

The Journal of Physical Chemistry C

... [4] Conjugated diradicals are of the Kekulé-(one or more closed shell resonance forms, e. g. ortho-and paraquinodimethane (QDM), Figure 1a) or non-Kekulé-type, void of any closed shell resonance structure. [1] Examples of Kekulé diradicals include Tchichibabin's hydrocarbon, [5] Wu's zethrenes, [6] Kubo's bisphenalenyls, [7] and Haley's indenofluorenes, [8] whereas some triangulenes [9] (including Clar's hydrocarbon), [10] 1,14 : 11,12-dibenzopentacene [11] and extended tribenzo [f,k,m]tetraphenes [12] represent non-Kekulé diradicals. [13] Substitution and/or regioisomerism can tailor diradical character and singlet-triplet gaps (ΔE ST ). ...

Design and Synthesis of Kekulè and Non-Kekulè Diradicaloids via the Radical Periannulation Strategy: The Power of Seven Clar’s Sextets
  • Citing Article
  • December 2022

Journal of the American Chemical Society

... Work by the Nienhaus and Bawendi groups into the influence of a surface solvent treatment has shown that not only does a change to the underlying dopant level occur of the LHP but also to the overall upconversion process. [38,53] Interfacial traps are generated when polar solvents such as isopropanol are utilized as they can readily dissolve the FAI and MAI within the perovskite structure. [38] These films also exhibit an increase to the UC yields likely due to trap-assisted TTA-UC. ...

Surface Doping Boosts Triplet Generation Yield in Perovskite‐Sensitized Upconversion

... Compared to the above-mentioned gas-solid strategy, a wet-chemistry synthesis has been employed to prepare high-quality cobalt carbides with a shorter synthesis time and simple procedure. Recently, oleylamine or octadecylamine could act as a solvent and capping agent to prepare cobalt carbides with various morphologies and structures [10][11][12]16]. In an oleylamine-based system, the preformed cobalt nanostructures are sensitive to carburization to form Co 2 C at a high temperature [17]. ...

A Single Source, Scalable Route for Direct Isolation of Earth-Abundant Nanometal Carbide Water-Splitting Electrocatalysts
  • Citing Article
  • August 2022

Inorganic Chemistry

... Copper iron sulfides have large infrared LSPRs at ultrasmall sizes due to p-type doping [6,35,37,38]. Lee et al. described the emergence of pronounced NIR-II LSPR in colloidal chalcopyrite (CuFeS 2 ) and bornite (Cu 5 FeS 4 ) compositions of copper iron sulfide when the NPs undergo oxidation-induced Fe leaching upon exposure to air. Analogous to binary copper sulfide nanocrystals, the decreased Fe content leaves metal vacancies in the nanocrystal lattice; charge-compensating holes resonate, generating the high optical absorbance seen in the NIR-II [35]. ...

Effective Mass for Holes in Paramagnetic, Plasmonic Cu 5 FeS 4 Semiconductor Nanocrystals
  • Citing Article
  • July 2022

The Journal of Physical Chemistry C

... In an effort to determine the exact mechanism governing the LHP free-carrier sensitization, ultrafast transient absorption (TA) investigations by Conti III et al. interrogated the interfacial charge transfer between the LHP and rubreneDBP annihilator. [52] Here, FA-rich LHPs (FA 0.85 MA 0.15 PbI 3 , FAMA) serve as the sensitizer and by selectively pumping the FAMA via 700 nm pump, the evolution of rubrene signatures in the 6 ns time window signify successful triplet population within the bilayer. In addition to the rapid sub-nanosecond triplet generation, the authors found evidence for hot-carrier extraction from the FAMA to rubrene. ...

Ultrafast Triplet Generation at the Lead Halide Perovskite/Rubrene Interface
  • Citing Article
  • January 2022

ACS Energy Letters

... With x = 0.03 replacement, the T C stayed almost same, but the magnetization rose noticeably, and thus, the (BH) max increased by 130%. Moreover, a recent study reported a significantly enhanced H C from 17.7 kOe to 26.2 kOe at x = 0.10 for (Fe 1−x Cu x ) 3 Se 4 samples prepared by the solvothermal method [28]. Previous calculations, on the other hand, were mostly limited to experimental investigations. ...

Increasing Magnetic Hardness of Fe 3 Se 4 via Cu Doping
  • Citing Article
  • November 2021

The Journal of Physical Chemistry C