Leonas Valkunas’s research while affiliated with Center for Physical Sciences and Technology and other places

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Publications (194)


Single Pixel Reconstruction Imaging: taking confocal imaging to the extreme
  • Article

December 2024

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55 Reads

Lithuanian Journal of Physics

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Dmitrij Frolov

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Jevgenij Chmeliov

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[...]

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Light nanoscopy is attracting widespread interest for the visualization of fluorescent structures at the nanometre scale. Recently, a variety of methods have overcome the diffraction limit, yet in practice they are often constrained by the requirement of special fluorophores, nontrivial data processing, or a high price and complex implementation. Therefore, confocal microscopy, yielding a relatively low resolution, is still the dominant method in biosciences. It was shown that image scanning microscopy (ISM) with an array detector could improve the resolution of confocal microscopy. Here, we review the principles of the confocal microscopy and present a simple method based on ISM with a different image reconstruction approach, which can be easily implemented in any camera-based laser-scanning set-up to experimentally obtain the theoretical resolution limit of confocal microscopy. Our method, single pixel reconstruction imaging (SPiRI), enables high-resolution 3D imaging utilizing image formation only from a single pixel of each of the recorded frames. We achieve the experimental axial resolution of 330 nm, which was not shown before by basic confocal or ISM-based systems. The SPiRI method exhibits a low lateral-to-axial FWHM aspect ratio, which means a considerable improvement in 3D fluorescence imaging. As a demonstration of SPiRI, we present the 3D-structure of a bacterial chromosome with an excellent precision.


Application of the frozen-modes approximation to classical harmonic oscillator systems

October 2024

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16 Reads

Lithuanian Journal of Physics

The problems of open classical systems usually correspond to a motion of a test particle that interacts with a large number of bath oscillators. Often, the test particle itself can be considered a harmonic oscillator. For such composite systems, exact numerical solutions are available, but they can become increasingly costly for a large number of bath oscillators. Here we take inspiration from the recent work on open quantum systems and investigate the applicability of the frozen-modes approximation to such classical systems. This approach assumes that some part of the low-frequency bath modes are frozen, thus only their initial values need to be considered. We show that by applying the frozen-modes approximation one can significantly increase the accuracy of the perturbative multiple-scales solution, especially for slow baths. This approach provides a good accuracy even for strong system–bath couplings, a regime that is not accessible to straightforward applications of the perturbation theory. We also suggest a rule for the splitting of spectral density to the fast and slow bath modes. We find that our approach gives excellent results for the ohmic spectral density, but it could be applied for other similar spectral densities as well.


Fig. 1. Chemical structures of Cstilbene (a) and Tstilbene (c). CARS images, captured at resonance frequencies at 1635 cm -1 of pure Cstilbene (b) and diluted solution of Tstilbene in DMSO (d) with resonance frequency 1600 cm -1 . Measured CARS spectra of pure Cstilbene and mono-molecular Tstilbene (e). CARS spectrum of DMSO is shown for reference. Calculated Raman spectra of Cstilbene and Tstilbene molecules (f).
Fig. 2. CARS images of various films of Tstilbene and PS mixtures at 1600 cm -1 (left). CARS spectra at the selected points indicated with arrows (middle). Polarized CARS signal measured at 1600 cm -1 at the same selected spatial point (right). Each data point is the result of averaging over an area of about 1 µm 2 at the chosen position of the sample. (a)-(d) Types of the films are indicated in the middle panels.
Fig. 3. (a) AFM representative 30μm × 30μm topography images of Tstilbene-containing PS films. (b) Intensity profiles (the distance in the Z direction from the film surface) along the red lines indicated in (a). (c) CARS images of the same films at 1600 cm -1 in the similarly sized 30μm × 30μm range.
Fig. 4. Steady-state absorption (blue lines), FL excitation (orange lines) and FL (dark cyan lines) spectra of Tstilbene films, dependent on concentration of Tstilbene in PS matrix of the 175-nm film thickness (a), and on the film thickness for 80 % Tstilbene (b). All the spectra are normalized and shifted along the linear vertical axis for clarity.
Fig. 5. Results of the two-component analysis of the measured fluorescence spectra and kinetics. (a) The measured FL spectra and their fits are shown with black circles and red lines, respectively. For clarity, all the spectra are shifted along the linear vertical axis. Decomposed normalized FL spectra of the molecular and crystallite forms of Tstilbene is also shown (dark yellow and green lines, respectively). (b) Relative weighting factors of the crystallite Tstilbene in different samples, corresponding to the 2-components fits of the FL spectra shown in panel (a). (c) The determined FL decay kinetics of the monomeric stilbene (dark yellow line, obtained from the measurements of the 175-nm films prepared at 0.5% stilbene concentration), small molecular aggregates (blue line), and crystallites (green lines). For clarity, all the measured FL decay kinetics at the main peak of FL spectrum (circles) and their fits (red lines) shifted along the logarithmic vertical axis, gray line represents IRF. (d) Relative contributions of the crystallite and aggregate FL decay kinetics in various samples shown in panel (c). Upper bars correspond to the kinetics measured at the main spectral peak (around 360 nm) and lower bars represent the results for the kinetics measured at the secondary right peak (around 375 nm).
Trans-stilbene aggregates and crystallites in polystyrene films: microscopy and spectroscopy
  • Article
  • Full-text available

September 2024

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66 Reads

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1 Citation

Physical Chemistry Chemical Physics

Solid and liquid stilbene forms have been characterized by a range of tools: from AFM microscopy to CARS microspectroscopy and optical spectroscopy. Obtained experimental observations are analyzed by means of...

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Left: PSI–LHCI supercomplex (PDB ID: 4XK8) (Qin et al., 2015). Right: Lhca4 light-harvesting complex. Chlorophylls a are depicted in green and Chlorophylls b are depicted in magenta. Carotenoids (BCR, XAT and LUT) are depicted in orange.
Energy level diagram of isolated (left column) monomer energies and monomer energies predetermined by the environment (right column). The energy levels of chlorophylls a and b are depicted in blue and pink respectively.
Energy level diagram of the isolated (left column) dimer CT state energies and CT energies predetermined by the environment (right column). In the right column, energies of the CT states, whose first pigment is negatively charged and the second one is positively charged, are given in dash. Cases, where the first pigment is positively charged and the second one is negatively charged, are given in solid lines. Black dashed lines mark the lowest and the highest monomer Qy energies predetermined by the environment.
The difference between the energy shifts of the CT states, calculated in estimated protonation environment and the non-standard protonation state of the specific amino acid indicated at the bottom of each column.
Spatial arrangement of the dimers a602–a603 (A), a603–a608 (B), b607–a609 (C) and b607–b615 (D) together with amino acids that have the largest influence on the Qy energies of the monomers and the CT energies of the dimers.
Environment-dependent chlorophyll–chlorophyll charge transfer states in Lhca4 pigment–protein complex

August 2024

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76 Reads

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1 Citation

Photosystem I (PSI) light-harvesting antenna complexes LHCI contain spectral forms that absorb and emit photons of lower energy than that of its primary electron donor, P700. The most red-shifted fluorescence is associated with the Lhca4 complex. It has been suggested that this red emission is related to the inter-chlorophyll charge transfer (CT) states. In this work we present a systematic quantum-chemical study of the CT states in Lhca4, accounting for the influence of the protein environment by estimating the electrostatic interactions. We show that significant energy shifts result from these interactions and propose that the emission of the Lhca4 complex is related not only to the previously proposed a603⁺–a608⁻ state, but also to the a602⁺–a603⁻ state. We also investigate how different protonation patterns of protein amino acids affect the energetics of the CT states.



Concentration Quenching of Fluorescence Decay Kinetics of Molecular Systems

May 2024

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7 Reads

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6 Citations

The Journal of Physical Chemistry B

Fluorescence concentration quenching occurs when increasing molecular concentration of fluorophores results in a decreasing fluorescence quantum yield. Even though this phenomenon has been studied for decades, its mechanisms and signatures are not yet fully understood. The complexity of the problem arises due to energy migration and trapping in huge networks of molecules. Most of the available theoretical work focuses on integral quantities like fluorescence quantum yield and mean excitation lifetime. In this work, we present a numerical study of the fluorescence decay kinetics of three-dimensional and two-dimensional molecular systems. We investigate the differences arising from the variations in models of trap formations. We also analyze the influence of the molecular orientations to the fluorescence decay kinetics. We compare our results to the well-known analytical models and discuss their ranges of validity. Our findings suggest that the analytical models can provide inspiration for different ways of approximating the fluorescence kinetics, yet more detailed analysis of the experimental data should be done by comparison with numerical simulations.



Fig. 1. A) Normalized absorption spectra of trans-stilbene in PS matrix, in the inset dependence of the absorption at 312 nm on the trans-stilbene concentration in PS matrix is shown. B) Normalized fluorescence spectra of trans-stilbene in PS matrix under 300 nm excitation.
Fig. 2. Integrated fluorescence intensity of trans-stilbene dependence on concentration in PS matrix under 300 nm excitation. Molecular structure of transstilbene is also shown.
Fig. 5. Molecular dynamics simulations and global minima according DFT studies: A -Stilbene parametrized as monomer can create temporary dimers even in 100 ps simulations time line; B -Stilbene parametrized as dimer create many complexes even in its first 2 ps of the simulations; C -dihedral angles after optimisations with B3LYP computational level for chosen complex of the 6 stilbenes from MD simulations (figure B); D -Potential energy surface of a single stilbene molecule with respect to twisting along the single-bond (β angle). In figures A and B distance R is chosen between dimers two atoms labelled as A in figure D.
Two phases of trans-stilbene in polystyrene matrix

August 2023

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132 Reads

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3 Citations

Physical Chemistry Chemical Physics

Variability in the spectral properties of solid conformations of stilbene under various external conditions still remains obscure. The photophysical properties of trans-stilbene solution in solid polystyrene glass have been studied by absorption and time-resolved fluorescence. Concentration-induced quenching has been observed for small concentrations of stilbene. At large concentrations, the spectroscopic characteristics become split between the two phases of the sample: single-molecule properties are responsible for absorption, while the micro-crystalline phase dominates in fluorescence. Ab initio and molecular dynamics analyses suggest permanent twisting of the stilbene molecular structure upon crystallization, which supports spectroscopic phase separation.



Application of artificial neural networks for modeling of electronic excitation dynamics in 2D lattice: Direct and inverse problems

March 2023

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74 Reads

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1 Citation

Machine learning (ML) approaches are attracting wide interest in the chemical physics community since a trained ML system can predict numerical properties of various molecular systems with a small computational cost. In this work, we analyze the applicability of deep, sequential, and fully connected neural networks (NNs) to predict the excitation decay kinetics of a simple two-dimensional lattice model, which can be adapted to describe numerous real-life systems, such as aggregates of photosynthetic molecular complexes. After choosing a suitable loss function for NN training, we have achieved excellent accuracy for a direct problem—predictions of lattice excitation decay kinetics from the model parameter values. For an inverse problem—prediction of the model parameter values from the kinetics—we found that even though the kinetics obtained from estimated values differ from the actual ones, the values themselves are predicted with a reasonable accuracy. Finally, we discuss possibilities for applications of NNs for solving global optimization problems that are related to the need to fit experimental data using similar models.


Citations (68)


... Its molecular structure consists of a large ring composed of four benzene rings and four nitrogen atoms, with the chromium ions coordinated at the center of the ring. CrPc exhibits strong fluorescent properties, typically appearing as green to blue fluorescence [25,26]. The fluorescent characteristics of CrPc, along with its unique properties of light absorption and emission, make it an indispensable material in many optical and optoelectronic applications [27,28]. ...

Reference:

Chitosan-Derived Nanocarrier Polymers for Drug Delivery and pH-Controlled Release in Type 2 Diabetes Treatment
Concentration quenching of fluorescence in thin films of zinc-phthalocyanine
  • Citing Article
  • May 2023

Chemical Physics

... The optimization of the structures was carried out based on the density functional theory (DFT) [30] calculation method, utilizing the B3LYP [31] functional and 6-31g(d) [32] basis set, along with DFT-D3 [33] correction. Subsequently, the B3LYP [34,35] function set and 6-31g(d) base set were used for the electronic excitation calculation using the TD-DFT calculation method, followed by the visualization and analysis of the excitation results using Multiwfn [36]. The UV-Vis spectra, ECD spectra, TMD and Raman spectra of the system were generated using Origin 2022 software [37]. ...

Mechanism of proton transfer in bacteriorhodopsin
  • Citing Article
  • October 2022

Lithuanian Journal of Physics

... 67 Due to the late determination of the atomic structure, there are still only a few modeling studies present to this day compared to other LHCs. [68][69][70] However, for the present study, this is just another small-sized complex involving Chl pigments. Hence, the same type of parameterization and DFT/TD-DFT calculation was performed for chlorophyll a and c molecules, which are the main pigments in FCP. ...

Structure-Based Model of Fucoxanthin-Chlorophyll Protein Complex: Calculations of Chlorophyll Electronic Couplings
  • Citing Article
  • May 2022

... As the major task was to describe ν₁ shifts and get data on what it can cause, the computational data wasn't scaled. According to previous studies, various scaling factors can be used to fit experimental values (see 21,29,65 ). All structures were neglected which had imaginary frequencies. ...

Electronic and Vibrational Properties of Allene Carotenoids

The Journal of Physical Chemistry A

... The conventional Liptay formalism is the most straightforward approach to modeling SF data of photosynthetic pigment-protein complexes, whose excitonic states often gain significantly large static dipole moments due to mixing with CT states. There is a debate concerning the applicability of the standard Liptay formalism as a mathematical tool for simulating the Stark spectra of systems with appreciably large static dipole moments in their excited states, such as different pigment-protein complexes of photosynthetic organisms (Novoderezhkin et al. 2007;Gottfried et al. 1991;Somsen et al. 1998;Moore et al. 1999;Braver et al. 2021). However, as far as the analysis of Stark data is concerned, no other effective substitutes for the Liptay formalism have been developed so far that can be used independently to analyze the data and yield detailed information about the associated electrostatic parameters (which is the ultimate goal in analyzing Stark data), although some recent theoretical investigations attempted to do so (Braver et al. 2021;Novoderezhkin 2023). ...

Stark absorption and Stark fluorescence spectroscopies: Theory and simulations
  • Citing Article
  • December 2021

... For this reason, approximate methods are employed when calculating the spectra of real complexes. Various theoretical approaches have been used to derive approximate expressions for the calculation of fluorescence spectra [13][14][15][16] , with the most common approaches relying on the second-order cumulant expansion 4,5,17,18 . Without additional approximations, the second-order cumulant expansion yields the full cumulant expansion (FCE) method 17 . ...

Quantum–Classical Approach for Calculations of Absorption and Fluorescence: Principles and Applications

Journal of Chemical Theory and Computation

... It is essential for deriving the absorption lineshape formula using the ctR theory [40] as well as for applying the HEOM method [50] and our FBTS/PBME-nH-Jeff approach [32] to optical spectra. The formula for the stationary fluorescence lineshape is similar to Eq. (13), with the exception of a different sign in the exponent [43,51]: ...

Derivation of the stationary fluorescence spectrum formula for molecular systems from the perspective of quantum electrodynamics
  • Citing Article
  • June 2021

Lithuanian Journal of Physics

... Although the unquenched (light-harvesting) conformation of LHCII is thermodynamically more favorable at room temperature than the quenched one, the free energy of transition between these conformations is negligible (~2.5 kT, where k is the Boltzmann constant and T is the absolute temperature) [70]. This is probably the reason why LHCII can switch to the quenched state under the action of relatively weak stimuli [71], such as changes in the thylakoid membrane rigidity [72,73] and thickness [74], induction of transmembrane asymmetry due to accumulation of digalactosyldiacylglycerol (DGDG) in the lumenal leaflet [74], aggregation of LHCII [75,76], and accumulation of Zea [77] or PsbS [78][79][80][81]. However, it remains unclear whether these factors are the causes of LHCII transition to the quenched state or just related phenomena. ...

Aggregation-related quenching of LHCII fluorescence in liposomes revealed by single-molecule spectroscopy
  • Citing Article
  • March 2021

Journal of Photochemistry and Photobiology B Biology

... A series of intermediated steps account for the isomerizations (from bR568 to K610 and from N530 to O646), proton transport (from L550 to M1-412 and from M2-412 to N530), and accessibility changes (from M1-412 to M2-412 and from O646 to bR568) of the photocycle [178]. It should be noted that proton transport starts from the J o u r n a l P r e -p r o o f middle of the protein structure with the proton transfer from Schiff base to Asp-85 residue, and its transport to the outer extracellular side of the proton pump [179,180]. Subsequently, the Schiff base is reprotonated [181]. The electron transport chain within the retina provides the energy for the proton motive force, which acts as a pump for both electrons and protons [172,177,182]. ...

Mechanism of Proton Transfer in Bacteriorhodopsin

... 22,23 In ref. 24 have been reported on the preparation and characterization of Cars complexed with CDs to achieve water solubility. Using a similar methodology together with the computational study, previously [25][26][27] , and we presented an analysis by analysing the β-ring dihedral angles and revealing three key all-trans-βcarotene conformers (trans-trans, trans-cis, cis-cis of β-ring), with ν₁ differing by 4 cm⁻¹ among them 26 . However, the unique properties of LYC arise from a different origin  its distinct ending group structures  resulting in unique complexation characteristics which are different for crystals and solvents by studding Raman spectra. ...

Unusual Temperature Dependence of the Fluorescence Decay in Heterostructured Stilbene
  • Citing Article
  • January 2021

Physical Chemistry Chemical Physics