Davorin Peceli
University of Central Florida
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by Davorin Peceli.
Journal of the American Chemical Society | 2009
Susan A. Odom; Scott Webster; Lazaro A. Padilha; Davorin Peceli; Honghua Hu; Gero Nootz; Sung-Jae Chung; Shino Ohira; Jonathan D. Matichak; Olga V. Przhonska; Alexei D. Kachkovski; Stephen Barlow; Jean-Luc Brédas; Harry L. Anderson; David J. Hagan; Eric W. Van Stryland; Seth R. Marder
A chromophore in which zinc porphyrin donors are linked through their meso positions by ethynyl bridges to a bis(indolinylidenemethyl) squaraine core has been synthesized using Sonogashira coupling. The chromophore exhibits a two-photon absorption spectrum characterized by a peak cross section of 11,000 GM and, more unusually, also exhibits a large cross section of >780 GM over a photon-wavelength window 750 nm in width.
Journal of Physical Chemistry A | 2010
Lazaro A. Padilha; Scott Webster; Olga V. Przhonska; Honghua Hu; Davorin Peceli; Trenton R. Ensley; Mykhailo V. Bondar; Andriy O. Gerasov; Yuriy P. Kovtun; Mykola P. Shandura; Alexey D. Kachkovski; David J. Hagan; Eric W. Van Stryland
We present an experimental and theoretical investigation of the linear and nonlinear optical properties of a series of acceptor-pi-acceptor symmetrical anionic polymethine dyes with diethylamino-coumarin-dioxaborine terminal groups and different conjugation lengths. Two-photon absorption (2PA) cross sections (delta(2PA)) are enhanced with an increase of pi-conjugation length in the investigated series of dyes. 2PA spectra for all dyes consist of two well-separated bands. The first band, located within the telecommunications window, occurs upon two-photon excitation into the vibrational levels of the main S(0) --> S(1) transition, reaching a large delta(2PA) = 2200 GM (1 GM = 1 x 10(-50) cm(4) s/photon) at 1600 nm for the longest conjugated dye. The position of the second, and strongest, 2PA band for all anionic molecules corresponds to the second-excited final state, which is confirmed by quantum-chemical calculations and excitation anisotropy measurements. Large delta(2PA) values up to 17,000 GM at 1100 nm are explained by the combination of the large ground- and excited-state transition dipole moments. The three shortest dyes show good photochemical stability and surprisingly large fluorescence quantum yields of approximately 0.90, approximately 0.66, and approximately 0.18 at the red to near-IR region of approximately 640, approximately 730, and approximately 840 nm, respectively. The excited-state absorption spectra for all samples are also studied and exhibit intense bands throughout the visible wavelength region with peak cross section close to 5 x 10(-16) cm(2) with a corresponding red shift with increasing conjugation lengths.
Journal of Materials Chemistry | 2009
Lazaro A. Padilha; Scott Webster; Olga V. Przhonska; Honghua Hu; Davorin Peceli; Jonathan L. Rosch; Mikhail V. Bondar; Andriy O. Gerasov; Yuriy P. Kovtun; Mykola P. Shandura; Alexey D. Kachkovski; David J. Hagan; Eric W. Van Stryland
A detailed experimental and theoretical study of the linear and nonlinear absorption of a series of asymmetrical D–π–A cyanine dyes with the same trimethylindolin donor (D) and diethylamino-coumarin-dioxaborine acceptor (A) terminal groups and different conjugation lengths, is presented. Strong solvatochromic behavior affecting the fluorescence quantum yields, lifetimes, and the linear and nonlinear absorption properties is observed due to the presence of permanent ground state dipole moments. Detailed experimental studies of lifetime dynamics are performed by direct time-correlated single photon counting and pump–probe techniques. We find that an increase in π-conjugation in the investigated series of dyes leads to an enhancement of the excited-state absorption and two-photon absorption (2PA) cross-sections (δ2PA). The 2PA spectra for all of the investigated dyes consist of two well-separated bands. The first band occurs at two-photon excitation into the vibrational levels and not into the absorption peak of the main transition, S0 → S1, which is more typical of that observed for symmetrical cyanines. The position of the second 2PA band for all the molecules remains unchanged in solvents of different polarity contrary to the large solvatochromic shift of the S0 → S1 band, resulting in a large intermediate state resonance enhancement and, therefore, a larger 2PA in acetronitrile (δ2PA ≈ 10000 GM) compared to toluene (δ2PA ≈ 4700 GM).
Journal of Physical Chemistry B | 2009
Scott Webster; Susan A. Odom; Lazaro A. Padilha; Olga V. Przhonska; Davorin Peceli; Honghua Hu; Gero Nootz; Alexei D. Kachkovski; Jonathan D. Matichak; Stephen Barlow; Harry L. Anderson; Seth R. Marder; David J. Hagan; Eric W. Van Stryland
The linear and nonlinear absorption properties of a squaraine-bridged porphyrin dimer (POR-SQU-POR) are investigated using femto-, pico-, and nanosecond pulses to understand intramolecular processes, obtain molecular optical parameters, and perform modeling of the excited-state dynamics. The optical behavior of POR-SQU-POR is compared with its separate porphyrin and squaraine constituent moieties. Linear spectroscopic studies include absorption, fluorescence, excitation and emission anisotropy, and quantum yield measurements. Nonlinear spectroscopic studies are performed across a wide range (approximately 150 fs, approximately 25 ps, and approximately 5 ns) of pulsewidths and include two-photon absorption (2PA), single and double pump-probe, and Z-scan measurements with detailed analysis of excited-state absorption induced by both one- and two-photon absorption processes. The 2PA from the constituent moieties shows relatively small 2PA cross sections; below 10 GM (1 GM = 1 x 10(-50) cm4 s/photon) for the porphyrin constituent and below 100 GM for the squaraine constituent except near their one-photon resonances. In stark contrast, the composite POR-SQU-POR molecule shows 2PA cross sections greater than 10(3) GM over most of the spectral range from 850 to 1600 nm (the minimum value being 780 GM at 1600 nm). The maximum value is approximately 11,000 GM near the Nd:YAG laser wavelength of 1064 nm. This broad spectral range of large 2PA cross sections is unprecedented in any other molecular system and can be explained by intramolecular charge transfer. A theoretical quantum-chemical analysis in combination with different experimental techniques allows insight into the energy-level structure and origin of the nonlinear absorption behavior of POR-SQU-POR.
Optica | 2014
Matthew Reichert; Honghua Hu; Manuel R. Ferdinandus; Marcus Seidel; Peng Zhao; Trenton R. Ensley; Davorin Peceli; Jennifer M. Reed; Dmitry A. Fishman; Scott Webster; David J. Hagan; Eric W. Van Stryland
Carbon disulfide is the most popular material for applications of nonlinear optical (NLO) liquids, and is frequently used as a reference standard for NLO measurements. Although it has been the subject of many investigations, determination of the third-order optical nonlinearity of CS2 has been incomplete. This is in part because of several strong mechanisms for nonlinear refraction (NLR), leading to a complex pulse width dependence. We expand upon the recently developed beam deflection technique, which we apply, along with degenerate four-wave mixing and Z-scan, to quantitatively characterize (in detail) the NLO response of CS2, over a broad temporal range, spanning 6 orders of magnitude (∼32u2009u2009fs to 17xa0ns). The third-order response function, consisting of both nearly instantaneous bound-electronic and noninstantaneous nuclear contributions, along with the polarization and wavelength dependence from 390 to 1550xa0nm, is extracted from these measurements. This paper provides a self-consistent, quantitative picture of the third-order NLO response of liquid CS2, establishing it as an accurate reference material over this broad temporal and spectral range. These results allow prediction of the outcome of any NLR experiment on CS2.
Journal of Physical Chemistry A | 2013
Davorin Peceli; Honghua Hu; Dmitry A. Fishman; Scott Webster; Olga V. Przhonska; Vladimir V. Kurdyukov; Yurii L. Slominsky; Alexey I. Tolmachev; Alexey D. Kachkovski; Andrey O. Gerasov; Artem̈ E. Masunov; David J. Hagan; Eric W. Van Stryland
Two different approaches to increase intersystem crossing rates in polymethine-like molecules are presented: traditional heavy-atom substitution and molecular levels engineering. Linear and nonlinear optical properties of a series of polymethine dyes with Br- and Se-atom substitution, and a series of new squaraine molecules, where one or two oxygen atoms in a squaraine bridge are replaced with sulfur atoms, are investigated. A consequence of the oxygen-to-sulfur substitution in squaraines is the inversion of their lowest-lying ππ* and nπ* states leading to a significant reduction of singlet-triplet energy difference and opening of an additional intersystem channel of relaxation. Experimental studies show that triplet quantum yields for polymethine dyes with heavy-atom substitutions are small (not more than 10%), while for sulfur-containing squaraines these values reach almost unity. Linear spectroscopic characterization includes absorption, fluorescence, quantum yield, anisotropy, and singlet oxygen generation measurements. Nonlinear characterization, performed by picosecond and femtosecond laser systems (pump-probe and Z-scan measurements), includes measurements of the triplet quantum yields, excited state absorption, two-photon absorption, and singlet and triplet state lifetimes. Experimental results are in agreement with density functional theory calculations allowing determination of the energy positions, spin-orbital coupling, and electronic configurations of the lowest electronic transitions.
Journal of Physical Chemistry Letters | 2012
Honghua Hu; Dmitry A. Fishman; Andrey O. Gerasov; Olga V. Przhonska; Scott Webster; Lazaro A. Padilha; Davorin Peceli; Mykola P. Shandura; Yuriy P. Kovtun; Alexey D. Kachkovski; Iffat H. Nayyar; Artem̈ E. Masunov; Paul Tongwa; Tatiana V. Timofeeva; David J. Hagan; Eric W. Van Stryland
The two-photon absorption (2PA) spectrum of an organic single crystal is reported. The crystal is grown by self-nucleation of a subsaturated hot solution of acetonitrile, and is composed of an asymmetrical donor-π-acceptor cyanine-like dye molecule. To our knowledge, this is the first report of the 2PA spectrum of single crystals made from a cyanine-like dye. The linear and nonlinear properties of the single crystalline material are investigated and compared with the molecular properties of a toluene solution of its monomeric form. The maximum polarization-dependent 2PA coefficient of the single crystal is 52 ± 9 cm/GW, which is more than twice as large as that for the inorganic semiconductor CdTe with a similar absorption edge. The optical properties, linear and nonlinear, are strongly dependent upon incident polarization due to anisotropic molecular packing. X-ray diffraction analysis shows π-stacking dimers formation in the crystal, similar to H-aggregates. Quantum chemical calculations demonstrate that this dimerization leads to the splitting of the energy bands and the appearance of new red-shifted 2PA bands when compared to the solution of monomers. This trend is opposite to the blue shift in the linear absorption spectra upon H-aggregation.
Journal of The Optical Society of America B-optical Physics | 2016
Trenton R. Ensley; Honghua Hu; Matthew Reichert; Manuel R. Ferdinandus; Davorin Peceli; Joel M. Hales; Joseph W. Perry; Zhong’an Li; Sei-Hum Jang; Alex K.-Y. Jen; Seth R. Marder; David J. Hagan; Eric W. Van Stryland
Materials with a large nonlinear refractive index (n2) and relatively small linear and nonlinear absorption losses, namely, two-photon absorption (2PA, of coefficient α2), have long been sought after for applications such as all-optical switching (AOS). Here we experimentally determine the linear and 2PA properties of several organic molecules, which we approximate as centrosymmetric, and use a simplified essential-state model (quasi-three-level model) to predict the dispersion of n2. We then compare these predictions with experimental measurements of n2 and find good agreement. Here “quasi”-three-level means using a single one-photon allowed intermediate state and multiple (here two) two-photon allowed states. This also allows predictions of the figure-of-merit (FOM), defined as the ratio of nonlinear refractive phase shift to the 2PA fractional loss, that determines the viability for such molecules to be used in device applications. The model predicts that the optimized wavelength range for a large FOM lies near the short wavelength linear absorption edge for cyanine-like dyes where the magnitude of n2 is quite large. However, 2PA bands lying close to the linear absorption edge in certain classes of molecules can greatly reduce this FOM. We identify two molecules having a large FOM for AOS. We note that the FOM is often defined as the ratio of real to imaginary parts of the third-order susceptibility (χ(3)) with multiple processes leading to both components. As explained later in this paper, such definitions require care to only include the 2PA contribution to the imaginary part of χ(3) in regions of transparency.
Journal of Physical Chemistry A | 2012
Davorin Peceli; Scott Webster; Dmitry A. Fishman; Claudiu M. Cirloganu; Honghua Hu; Olga V. Przhonska; Vladimir V. Kurdyukov; Yurii L. Slominsky; Alexey I. Tolmachev; Alexey D. Kachkovski; Raghunath R. Dasari; Stephen Barlow; Seth R. Marder; David J. Hagan; Eric W. Van Stryland
The double pump-probe technique (DPP), first introduced by Swatton et al. [Appl. Phys. Lett. 1997, 71, 10], is a variant of the standard pump-probe method but uses two pumps instead of one to create two sets of initial conditions for solving the rate equations, allowing a unique determination of singlet- and triplet-state absorption parameters and transition rates. We investigate the advantages and limitations of the DPP theoretically and experimentally and determine the influence of several experimental parameters on its accuracy. The accuracy with which the DPP determines the triplet-state parameters improves when the fraction of the population in the triplet state relative to the ground state is increased. To simplify the analysis of the DPP, an analytical model is presented, which is applicable to both the reverse saturable and the saturable absorption regimes. We show that the DPP is optimized by working in the saturable absorption regime. Although increased accuracy is in principle achievable by increasing the pump fluence in the reverse saturable absorption range, this can cause photoinduced decomposition in photochemically unstable molecules. Alternatively, we can tune the excitation wavelength to the spectral region of larger ground-state absorption, to achieve similar accuracy. This results in an accurate separation of triplet yield and excited-state absorption cross section. If the cross section at another wavelength is then desired, a second pump-probe experiment at that wavelength can be utilized given the previously measured triplet yield under the usually valid assumption that the triplet yield is independent of excitation wavelength.
Journal of The Optical Society of America B-optical Physics | 2016
Trenton R. Ensley; Honghua Hu; Matthew Reichert; Manuel R. Ferdinandus; Davorin Peceli; Joel M. Hales; Joseph W. Perry; Zhong’an Li; Sei-Hum Jang; Alex K.-Y. Jen; Seth R. Marder; David J. Hagan; Eric W. Van Stryland
This note corrects author affiliations, errors in one equation, and two equation callouts of J. Opt. Soc. Am. B33, 780 (2016)10.1364/JOSAB.33.000780JOBPDE0740-3224.