{"id":167,"date":"2023-08-01T14:59:21","date_gmt":"2023-08-01T21:59:21","guid":{"rendered":"https:\/\/dornsife.usc.edu\/compbionano\/?page_id=167"},"modified":"2023-08-01T14:59:22","modified_gmt":"2023-08-01T21:59:22","slug":"research","status":"publish","type":"page","link":"https:\/\/dornsife.usc.edu\/compbionano\/research\/","title":{"rendered":"Ongoing research projects"},"content":{"rendered":"\n\n  \n    \n\n\n\n\n\n\n<div\n  class=\"cc--component-container cc--rich-text \"\n\n  \n  \n  \n  \n  \n  \n  >\n  <div class=\"c--component c--rich-text\"\n    \n      >\n\n    \n      \n<div class=\"f--field f--wysiwyg\">\n\n    \n  <div class=\"html-content\">\n<h3>Q4Q: Quantum computation for Quantum prediction of materials and molecular properties<\/h3>\n<p>We aim at showing that quantum computers are already useful to solve cutting-edge problems in materials science and chemistry, accessing information otherwise elusive. We pursue two objectives, making use of the two quantum computing paradigms that are currently implemented in commercial and cloud quantum hardware.\u00a0Objective 1: adiabatic quantum optimization on materials databases (D-Wave). Objective 2: electronic structure of highly correlated systems on gate-model qubit arrays (IBM, Rigetti).\u00a0<a href=\"https:\/\/q4q.usc.edu\">This project\u00a0<\/a>is funded by the Department of Energy Office of Science, Basic Energy Sciences, under award number\u00a0DE-SC0019432.<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"size-full wp-image-153 aligncenter\" src=\"https:\/\/dornsife.usc.edu\/compbionano\/wp-content\/uploads\/sites\/258\/2023\/08\/OOS-brandtrans-sm.png\" alt=\"Office of Science\" width=\"300\" height=\"50\" \/><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter wp-image-155 size-large\" src=\"https:\/\/dornsife.usc.edu\/compbionano\/wp-content\/uploads\/sites\/258\/2023\/08\/q4q-baner-1024x352.jpg\" alt=\"Quantum computation\" width=\"1024\" height=\"352\" srcset=\"https:\/\/dornsife.usc.edu\/compbionano\/wp-content\/uploads\/sites\/258\/2023\/08\/q4q-baner-1024x352.jpg 1024w, https:\/\/dornsife.usc.edu\/compbionano\/wp-content\/uploads\/sites\/258\/2023\/08\/q4q-baner-300x103.jpg 300w, https:\/\/dornsife.usc.edu\/compbionano\/wp-content\/uploads\/sites\/258\/2023\/08\/q4q-baner-768x264.jpg 768w, https:\/\/dornsife.usc.edu\/compbionano\/wp-content\/uploads\/sites\/258\/2023\/08\/q4q-baner-1536x527.jpg 1536w, https:\/\/dornsife.usc.edu\/compbionano\/wp-content\/uploads\/sites\/258\/2023\/08\/q4q-baner-2048x703.jpg 2048w\" sizes=\"(max-width: 1024px) 100vw, 1024px\" \/><\/p>\n<p>&nbsp;<\/p>\n<\/div>\n<div class=\"html-content\">\n<h3>Binding mechanisms of class 2 CRISPR systems by a molecular dynamics simulations including enhanced sampling techniques<\/h3>\n<p>The contemporary version of genetic engineering is redefined genome editing, after the advent of molecular systems endowed with recognition properties against the DNA to be corrected. Specifically, class 2 CRISPR (clustered regularly interspaced short palindromic repeats) systems offer a unique protocol for genome editing. In order to be employed as a therapeutic tool to correct genetic imperfections or as a tool to artificially engineer crops for large-scale use, the protocol needs to be precisely sequence specific, which is still a limitation. CRISPR\/Cas9 and CRISPR\/Cpf1 systems share the same RNA-guided approach to cleave double-stranded DNA (dsDNA) close to the protospacer adjacent motif (PAM) that is recognized by the protein. The availability of several crystal structures of Cas9 fueled a fast development of the CRISPR\/Cas9 technique. Cpf1 was harnessed for genome editing more recently, with the first demonstration in 2015. A common feature of all crystal structures is the total or partial lack of the unwound non-target DNA strand. We interrogate binding mechanisms in two class 2 CRISPR systems, with the Cas9 and Cpf1 effector proteins, by means of enhanced sampling molecular dynamics (MD) simulations, with the aim of proposing a structural\/energetic framework to improve specificity. We will start from crystal structures that contain part on the unwound non-target DNA strand and use structural modeling to complete the structures. Our computational work is complemented by site-directed spin labeling (SDSL) experiments that report shape information, done in the lab of Peter Z. Qin (USC Department of Chemistry).<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter wp-image-152 size-full\" src=\"https:\/\/dornsife.usc.edu\/compbionano\/wp-content\/uploads\/sites\/258\/2023\/08\/crispr_test.jpg\" alt=\"Crispr test\n\" width=\"536\" height=\"670\" srcset=\"https:\/\/dornsife.usc.edu\/compbionano\/wp-content\/uploads\/sites\/258\/2023\/08\/crispr_test.jpg 536w, https:\/\/dornsife.usc.edu\/compbionano\/wp-content\/uploads\/sites\/258\/2023\/08\/crispr_test-240x300.jpg 240w\" sizes=\"(max-width: 536px) 100vw, 536px\" \/><\/p>\n<p>MD analysis of a Cas9 ternary complex containing the unwound DNA. (A) Overlay of the two centroid structures of the\u00a0most and second-most populated clusters. For clarity, only the\u00a0nuclease domains (transparent surfaces) and the DNA strands (blue =\u00a0target; black = nontarget; yellow = PAM) are shown. The red spheres\u00a0indicate the P atoms to which the R5a labels are attached.\u00a0Representative residues in the positively charged patch (K855 and\u00a0K862 in HNH, H982 and K1047 in RuvC) are highlighted. (B)\u00a0Histogram of distances between R5a labels modeled at the nucleotides\u00a0equivalent to c33 and n26. (C) Partial RMSD traces for segments of\u00a0the DNA nontarget strand with respect to the final snapshot of the\u00a0minimization\u2212equilibration phase. Nucleotides included\u00a0to represent each segment are PAM duplex, \u22121 to \u22128\u00a0downstream of PAM; PAM-proximal, +1 to +8 upstream of PAM;\u00a0PAM-distal, +12 to +16 upstream of PAM.\u00a0From our work: N. S. Tanprasertchai, R. Di Felice, X. Zhang, I. M. Slaymaker, C. Vazquez Reyes, W. Jian, R. Rohs, P. Z. Qin, <em>ACS Chem. Biol.<\/em> 2017, 12, 1489-1493; Angana Ray and Rosa Di Felice,\u00a0\u201cProtein-Mutation-Induced Conformational Changes of the DNA and Nuclease Domain in CRISPR\/Cas9 Systems by Molecular Dynamics Simulations\u201d,\u00a0<i>J. Phys. Chem. B<\/i>\u00a0<strong>124<\/strong>, 2168 (2020).<\/p>\n<p>We have just published our outreach article in the leading science communication publication, Scientia.\u00a0<a href=\"https:\/\/urldefense.com\/v3\/__https:\/\/www.scientia.global\/wp-content\/uploads\/Rosa-Di-Felice.pdf__;!!LIr3w8kk_Xxm!8fSf_pmlPNC7aj98cCHZNrBEGlfiKm3G84qzk19achgIRKCHT9Th6ewZKHuO40M$\">https:\/\/www.scientia.global\/wp-content\/uploads\/Rosa-Di-Felice.pdf<\/a><\/p>\n<\/div>\n<div class=\"html-content\">\n<h3><\/h3>\n<h3>Fate of amyloid-\u03b2 peptides on nanoparticles<\/h3>\n<p>The increasing technological importance of nanomaterials naturally raises the concern for possible toxic effects when they accidentally contact living organisms. Such effects will likely involve the interactions of nanomaterials with the protein arsenal of the body. On the other hand nanoparticles (NPs) have been proposed for innovative diagnostic and therapeutic approaches, applications which define the emerging field of\u00a0<em>theranostics<\/em>\u00a0(therapy + diagnostic) nanomedicine. In particular recent experimental works tackled the effect, in vitro, of NPs on protein fibrillation. Protein fibrillation is involved in many human diseases, including Alzheimer\u2019s, Parkinson\u2019s, Creutzfeld-Jacob&#8217;s and dialysis-related amyloidosis. The NPs have been found either to enhance or to inhibit the rate of formation of fibrils, therefore they can potentially lead to novel mechanisms for amyloid diseases as well as to therapeutic opportunities for their treatment. Although these results are of broad relevance, the underlying molecular mechanism (how is the NP interfering with the fibrillation process?) is poorly understood. Large scale computations have the potential to clarify such mechanism, but\u00a0 atomistic simulation of the problem are still in their infancy. This problem is also paradigmatic of the general field of protein-inorganic material interactions, of paramount importance in natural systems and currently a hot topic for experiments and theory.<\/p>\n<p>By means of enhanced-sampling molecular dynamics (MD) simulations with atomic precision, which ensure an accurate probe of the phase space of a peptide in different environments, we recently revealed that the interaction with a solid surface stimulates the formation of elongated structures of the amyloid-\u03b2-42 (A\u03b242) peptide.\u00a0Along with accumulated evidence that the propensity of the single monomer to adopt fiber-like conformations is directly related to the lag time for fiber formation, we have collected key evidence that contact to a flat substrate, which may be the external surface of the cell membrane or lipoproteins, as well as foreign agents, is pivotal to fibrillation-prone structural deformations. We are now interested in assessing the role of nanoparticles of different sizes and functionalization. The rationale is that if we find suitable nanoparticles that prevent fibrillation-prone conformations, those may be used to design therapeutic strategies against Alzheimer&#8217;s disease.<\/p>\n<\/div>\n<p>&nbsp;<\/p>\n<div class=\"html-content\">\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter wp-image-151 size-full\" src=\"https:\/\/dornsife.usc.edu\/compbionano\/wp-content\/uploads\/sites\/258\/2023\/08\/Bellucci_fig7.jpg\" alt=\"amyloid-\u03b2 peptides on nanoparticles\" width=\"835\" height=\"390\" srcset=\"https:\/\/dornsife.usc.edu\/compbionano\/wp-content\/uploads\/sites\/258\/2023\/08\/Bellucci_fig7.jpg 835w, https:\/\/dornsife.usc.edu\/compbionano\/wp-content\/uploads\/sites\/258\/2023\/08\/Bellucci_fig7-300x140.jpg 300w, https:\/\/dornsife.usc.edu\/compbionano\/wp-content\/uploads\/sites\/258\/2023\/08\/Bellucci_fig7-768x359.jpg 768w\" sizes=\"(max-width: 835px) 100vw, 835px\" \/><\/p>\n<p>Representative conformations obtained from the cluster analysis of ABWT-TREMD (A\u03b242 in solution, left) and ABAU-HTREMD (A\u03b242 adsorbed on hydrated Au(111), right). Representative structures of the first (A) and second (B) most populated ABWT-TREMD clusters: in both cases the conformers show a globular shape and a <strong>R<\/strong>g (radius of gyration)\u00a0value lower\u00a0than 1.15 nm. (C, D) Representative structures of ABWT-TREMD clusters with <strong>R<\/strong>g larger than 1.15 nm (the 17th and 28th in the decreasing order of\u00a0population, respectively): these are representative conformers for extended states. Representative structures of the first (E) and second (F) most\u00a0populated ABAU-HTREMD clusters: these are extended states, at odds with the behavior in solution. (G, H) Representative structures of\u00a0ABAU-HTREMD clusters with <strong>R<\/strong>g larger than 2 nm: these are representative conformers for totally extended states.\u00a0From our work: L. Bellucci, G. Bussi, R. Di Felice, S. Corni, <em>Nanoscale<\/em><strong>2017<\/strong>, 9, 2279-2290.<\/p>\n<\/div>\n\n\n\n<\/div>\n\n\n  <\/div><\/div>\n","protected":false},"excerpt":{"rendered":"","protected":false},"author":354,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"page-content-detail.php","meta":{"_acf_changed":false,"footnotes":""},"class_list":["post-167","page","type-page","status-publish","hentry"],"acf":[],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.1.1 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>Ongoing research projects - CompBioNano<\/title>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/dornsife.usc.edu\/compbionano\/research\/\" \/>\n<meta property=\"og:locale\" content=\"en_US\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Ongoing research projects - 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