End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric Field-induced Second Harmonic Generation in Ferroelectric Thin Film BaSrTiO3 K. A. Grishunin1, N. A. Ilyin1, N. E. Sherstyuk1, E. D. Mishina1, A. Kimel2, V. M. Mukhortov3, A. V. Ovchinnikov4, O. V. Chefonov4, and M. B. Agranat4 1MIREA, Moscow Technological University, Xxxxxxxxx Xxx. 00, Xxxxxx 000000, Xxxxxx 2Institute for Molecules and Materials, Radboud University Nijmegen, 6525 AJ, Nijmegen, The Netherlands 3Southern Scientific Center of Russian Academy of Sciences, Chehova 41, Rostov-on-Don 344006, Russia 4Joint Institute for High Temperatures of Russian Academy of Sciences (JIHT) Izhorskayast. 13, Bd. 2, Moscow 125412, Russia Abstract— Strong modulation of the Second Harmonic Generation (SHG) signal by THz nearly single cycle pulse in ferroelectric thin film BaSrTiO3 was observed. As the employed THz pulses pumps the medium in the range of phononic excitations, the THz electric field induced ferro- electric polarization is due to the ionic contribution. The proposed model describes this effect in terms of electric polarization induced in the plane of the film. The net SHG signal responds to the THz excitation as if the THz pulse induces a 90-degrees switching of the polarization in parts of the sample on the time scale of the period of the soft mode. According to the proposed model, under action of the THz pulse the latter acquires an in-plane component up to 6% of the net polarization.
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric Field-induced Second Harmonic Generation The parietal epithelial cell is crucially involved in Ferroelectric Thin Film BaSrTiO3 K. A. Grishunin1human idiopathic focal segmental glomerulosclerosis1 XXXXX XXXXXXX,2 XXXX XXXXXX,2 XXXXXX XXX XXX XXXX, N. A. Ilyin1, N. E. Sherstyuk1, E. D. Mishina1, A. Kimel2, V. M. Mukhortov3, A. V. Ovchinnikov4, O. V. Chefonov4XXXX XXXXXXXXXXX, and M. B. Agranat4 1MIREA, Moscow Technological University, Xxxxxxxxx Xxx. 00, Xxxxxx 000000, Xxxxxx 2Institute for Molecules and Materials, Radboud University Nijmegen, 6525 AJ, Nijmegen, The Netherlands 3Southern Scientific Center of Russian Academy of Sciences, Chehova 41, Rostov-on-Don 344006, Russia 4Joint Institute for High Temperatures of Russian Academy of Sciences (JIHT) Izhorskayast. 13, Bd. 2, Moscow 125412, Russia Abstract— Strong modulation of the Second Harmonic Generation (SHG) signal by THz nearly single cycle pulse in ferroelectric thin film BaSrTiO3 was observed. As the employed THz pulses pumps the medium in the range of phononic excitations, the THz electric field induced ferro- electric polarization is due to the ionic contribution. The proposed model describes this effect in terms of electric polarization induced in the plane of the film. The net SHG signal responds to the THz excitation as if the THz pulse induces a 90-degrees switching of the polarization in parts of the sample on the time scale of the period of the soft mode. According to the proposed model, under action of the THz pulse the latter acquires an in-plane component up to 6% of the net polarization.XXXX XXXXXXX
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric FieldMethods OFFICIAL JOURNAL Xxxxxx X. Xxxxx-induced Second Harmonic Generation in Ferroelectric Thin Film BaSrTiO3 K. A. Grishunin1, N. A. Ilyin1, N. E. Sherstyuk1, E. D. Mishina1, A. Kimel2, V. M. Mukhortov3, A. V. Ovchinnikov4, O. V. Chefonov4, xxx Xxxxxxxx,1∗ † Xxxxxxxxx Xxxxxxxx,1 † Xxxxx X. Xxxxxx,2,3 Xxxxxx Xxxxxx,1 Xxxxxxx X.X. xxx Xxxx-Xxxxxxxxxxxx,1 Xxxxxx X.X. xxx Bon,1 Xxxxx X. Xxxxxx,1 Xxxx X. Sistermans,4 Xxx X. Xxxxxxx,1 Xxxxx X.X. xx Xxxxxxx,1 and M. B. Agranat4 1MIREA, Moscow Technological University, Xxxxxxxxx Xxx. 00, Xxxxxx 000000, Xxxxxx 2Institute for Molecules and Materials, Radboud University Nijmegen, 6525 AJ, Nijmegen, The Netherlands 3Southern Scientific Center of Russian Academy of Sciences, Chehova 41, Rostov-on-Don 344006, Russia 4Joint Institute for High Temperatures of Russian Academy of Sciences (JIHT) Izhorskayast. 13, Bd. 2, Moscow 125412, Russia Abstract— Strong modulation of the Second Harmonic Generation (SHG) signal by THz nearly single cycle pulse in ferroelectric thin film BaSrTiO3 was observed. As the employed THz pulses pumps the medium in the range of phononic excitations, the THz electric field induced ferro- electric polarization is due to the ionic contribution. The proposed model describes this effect in terms of electric polarization induced in the plane of the film. The net SHG signal responds to the THz excitation as if the THz pulse induces a 90-degrees switching of the polarization in parts of the sample on the time scale of the period of the soft mode. According to the proposed model, under action of the THz pulse the latter acquires an in-plane component up to 6% of the net polarization.Xxxx X.X. de Vries1
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric FieldAGORA, a Data- and Biobank for Birth Defects and Childhood Cancer Xxxx X.X.X. xxx Xxxxx*1, Xxxx X.X. van der Zanden1, Xxxxx X.X.X. Bongers2, Xxxxxxx X. Renkema3, Xxxxxxxxx X.X. Wijers1, Xxxxxxxx Thonissen4, Elisabeth X.X. Dokter1,5, Xxxxx X.X. Marcelis2, Ivo de Blaauw6,7, Xxxx X.X.X. Wijnen6, Xxxxx X. Hoogerbrugge8, Xxx X.X. Bokkerink8, Xxxxxxx X. Schreuder8, Xxxxx Xxxxxx-induced Second Harmonic Generation in Ferroelectric Thin Film BaSrTiO3 K. A. Grishunin1Kamphuis8, N. A. Ilyin1Xxxxxxxxx X.X. Cornelissen8, N. E. Sherstyuk1Livia Kapusta8, E. D. Mishina1Xxxx X.X. van Heijst8, A. Kimel2Xxxx X. Liem8, V. M. Mukhortov3Xxxxxx P.E. de Gier9, A. V. Ovchinnikov4Xxxx Xxxxx Xxxxxxxx-Jagtman4, O. V. Chefonov4Xxxxxx X.X. Admiraal10, Xxxxxxx X. Berg´e11, Xxx Xxxx van der Biezen5, An Verdonck12, Xxxxxxx Xxxxxx Poorten13, Greet Hens13, Jasmien Roosenboom14, Xxxx X. Lilien15, Xxx X. de Jong16,17, Xxxx Broens18, Xxxx Wijnen7, Xxxxx Brooks19, Xxxxxxx Franke2,20, Xxx X. Brunner2, Xxxxxx E.L. Carels4,12, Nine V.A.M. Knoers3, Wout F.J. Feitz9, and M. B. Agranat4 1MIREANel Roeleveld1,8 BACKGROUND: Research regarding the etiology of birth defects and childhood cancer is essential to develop preventive measures, Moscow Technological Universitybut often requires large study populations. Therefore, Xxxxxxxxx Xxxwe established the AGORA data- and biobank in the Netherlands. 00In this study, Xxxxxx 000000we describe its rationale, Xxxxxx 2Institute design, and ongoing data collection. METHODS: Children diagnosed with and/or treated for Molecules a structural birth defect or childhood cancer and Materialstheir parents are invited to participate in the AGORA data- and biobank. Controls are recruited through random sampling from municipal registries. The parents receive questionnaires about demographics, Radboud University Nijmegenfamily and pregnancy history, 6525 AJhealth status, Nijmegenprescribed medication, lifestyle, and occupational exposures before and during the index pregnancy. In addition, blood or saliva is collected from children and parents, while medical records are reviewed for diagnostic information. RESULTS: So far, we have collected data from over 6,860 families (3,747 birth defects, 905 childhood cancers, and 2,208 controls). The Netherlands 3Southern Scientific Center types of Russian Academy of Sciences, Chehova 41, Rostov-on-Don 344006, Russia 4Joint Institute for High Temperatures of Russian Academy of Sciences (JIHT) Izhorskayast. 13, Bd. 2, Moscow 125412, Russia Abstract— Strong modulation birth defects vary widely and comprise malformations of the Second Harmonic Generation (SHG) signal by THz nearly single cycle pulse in ferroelectric thin film BaSrTiO3 was observed. As the employed THz pulses pumps the medium in the range of phononic excitationsdigestive, the THz electric field induced ferro- electric polarization is due to the ionic contributionrespiratory, and urogenital tracts as well as facial, cardiovascular, kidney, skeletal, and central nervous system anomalies. The proposed model describes this effect in terms of electric polarization induced in the plane most frequently occurring childhood cancer types are acute lymphatic leukemia, Hodgkin and non-Hodgkin lymphoma, Wilms’ tumor, and brain and spinal cord tumors. Our genetic and/or epidemiologic studies have been focused on hypospadias, anorectal malformations, congenital anomalies of the filmkidney and urinary tract (CAKUT), and orofacial clefts. CONCLUSION: The net SHG signal responds large AGORA data- and biobank offers great opportunities for investigating genetic and nongenetic risk factors for disorders in children and is open to the THz excitation as if the THz pulse induces a 90-degrees switching of the polarization in parts of the sample on the time scale of the period of the soft modecollaborative initiatives. According to the proposed modelBirth Defects Research (Part A) 106:675–684, under action of the THz pulse the latter acquires an in-plane component up to 6% of the net polarization2016.
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric Field8892 Macromolecules 2010, 43, 8892–8903 DOI: 10.1021/ma101792v Rhodium-induced Second Harmonic Generation in Ferroelectric Thin Film BaSrTiO3 K. A. Grishunin1Mediated Stereospecific Carbene Polymerization: From Homopolymers to Random and Block Copolymers ) ) Xxxxx Xxxxxxx,† Xxxx X. Xxxxxxxxx,† Xxxx Xxxxxxx xxx Xxxxxxxxx,‡ Xxxxxx X. Xxxxxxxx,§ Xxxx X. Xxxxxxxxx,§ Xxx X. Xxxxxxxxxx, N. A. Ilyin1,# Xxxxxxxxxx Xxxxxxxxx, N. E. Sherstyuk1Xxxxx X. Xxxxxxxxxxxx, E. D. Mishina1, A. Kimel2, V. M. Mukhortov3, A. V. Ovchinnikov4, O. V. Chefonov4Xxx Xxxxxxxxx,^ Xxxxx X. X. xxx Xxx,^ Xxxxx X. X. Xxxx,† and Xxx xx Xxxxx*,† ) †Homogeneous and Supramolecular Catalysis Group, and M. B. Agranat4 1MIREA‡Zernike Institute for Advanced Materials, Moscow Technological UniversityUniversity of Groningen, Xxxxxxxxx Xxx. 00Xxxxxxxxxx 0, Xxxxxx 0000000000 XX Xxxxxxxxx, Xxxxxx 2Institute Xxx Xxxxxxxxxxx, §Faculty of Aerospace Engineering, Delft University of Technology, Xxxxxxxxxx 0, 2629 HS Delft, The Netherlands, and ^Institute for Molecules and Materials, Radboud University Nijmegen, 6525 AJXxxxxxxxxxxxxx 000, Nijmegen0000 XX Xxxxxxxx, Xxx Xxxxxxxxxxx. #Current address: Institute of Analytical Chemistry, Xxxxxxxx Xxxxxx University, 0000 Xxxx, Xxxxxxx. ABSTRACT: New stereoregular homo- and copolymers with an ester group at every backbone carbon atom were prepared from ethyl, benzyl and tert-butyl diazoacetate (Mw of homopolymers up to 690 kDa and copolymers up to 430 kDa). With polarizing optical microscopy we found that the homopolymers poly- (ethyl 2-ylideneacetate) and poly(benzyl 2-ylideneacetate) are able to form stable and accessible thermotropic and lyotropic nematic phases. Both two polymers show relatively high storage moduli up to the glass transition temperature (Tg), as evidenced by dynamic mechanical thermal analysis. The Netherlands 3Southern Scientific Center materials retain quite decent storage moduli in a broad elevated temperature range between Tg and Tm. The formation of Russian Academy (block) copolymers was confirmed by a combination of SciencesNMR spectroscopy, Chehova 41differential scanning calorimetry and size-exclusion chromatography. 2D-solubility-gradient chromatography-SEC as well as pyrolysis-gas chromatography-mass spectrometry (Py-GC-MS) showed a clear difference in the composition of the random and block copolymers with benzyl and ethyl ester groups. Thermal analysis showed that the homopolymers and block copolymers are semicrystalline, Rostovwhile the random copolymers are completely amorphous. The polymers are thermally stable toward decomposition up to 300 °C (and polymers containing tert-onbutyl ester groups up to 200 °C). The formation of cross-Don 344006linked polymer was achieved by heating copolymers containing tert-butyl ester groups. Introduction A long-standing challenge in polymer synthesis is the con- trolled synthesis of highly stereoregular, Russia 4Joint Institute high molecular weight carbon-chain polymers with a controllable amount of polar functionalities. Over the past years, several new approaches have been developed to reach this goal. Considerable progress in this field has been achieved with lanthanide metallocene complexes, group 4 early transition metal metallocenes, and alike, which polymerize polar vinyl monomers via coordination-addition polymerization mechanisms (metal-controlled anionic poly- merization), allowing the controlled synthesis of both syndiotac- tic and isotactic (rich) polymers from methylacrylates, acrylates, (meth)acrylamides, acrylonitriles, and vinylketones.1,2 High triad selectivities can be reached with these methods, but generally low temperatures are required to achieve high stereospecificities. These reactions bear some similarities with anionic polymeriza- tion of (meth)acrylates at low temperatures, which also allow a decent stereocontrol.3 The living character of both anionic and coordination-addition polymerization reactions provides inter- esting opportunities to prepare block copolymers. Progress in the development of new late transition metal catalysts for High Temperatures coordination-insertion-type polymerization reac- + + *Corresponding author. Telephone: 00 00 000 0000. Fax: 31 20 000 0000. E-mail: x.xxxxxxx@xxx.xx. tions has made it possible to prepare (random) copolymers of Russian Academy polar vinyl monomers and (aliphatic) alkenes, hence producing interesting new materials with varying microstructures (e.g., side- chain functionalized, main-chain functionalized, random, and block copolymers).1,4 These catalytic systems produce more than one chain per metal ion (chain transfer), and the most recently developed catalysts even allow a decent control over the amount of Sciences the incorporated functionalities. So far there are no reported examples of late transition metal catalysts capable of stereospe- cific polymerization of polar vinyl monomers or stereospecific copolymerization of polar vinyl monomers with olefins.1 Fascinating new developments in the field of radical-type polymerization reactions show the possibility to gain excellent control over polymer lengths and polydispersities, and modern radical polymerization techniques even make it possible to gain some (JIHTalbeit still limited) Izhorskayastcontrol over the polymer tacticities.5 Despite all these intriguing new developments, the problem is by no means solved and many important challenges are still remaining.1 For example, the synthesis of stereoregular carbon- chain polymers which are functionalized at every carbon-atom of the polymer backbone has proven to be difficult using olefinic monomers, and even the formation of atactic polymers by radical polymerization of 1,2-difunctionalized olefins is nontrivial in some cases.6 In this respect, C1 polymerization (or “carbene” polymerization) techniques may offer valuable alternative syn- thetic methods for the synthesis of new materials that are not so xxxx.xxx.xxx/Xxxxxxxxxxxxxx Published on Web 10/07/2010 Ⓒ 2010 American Chemical Society Article Macromolecules, Vol. 1343, BdNo. 21, 2010 8893 Scheme 2. Synthesis of Catalyst Precursors 1 and 2 easily accessible by the more common polymerization of CdC double bonds.7-9 We recently contributed to this field by show- ing that Rh-mediated carbene polymerization, using diazoesters (ROC(dO)CHdN2) as carbene precursors, allows the prepara- tion of fully functionalized, high molecular weight, and highly syndiotactic carbon-chain polymers,10-13 in good yields.13 Pre- sently, this is the only available method to prepare such densely functionalized, sp3-hybridized14 polymers in a stereoregular manner. The reaction follows a migratory carbene insertion chain propagation mechanism (Scheme 1), and the high syndio-specificity is most likely determined by chain-end control.11 With a method in hand to prepare high molecular weight and highly stereoregular fully functionalized polycarbenes, we decided to expand the scope of this new reaction toward the pre- paration of random and block-type copolymers using three different carbene precursors. The results are described in this paper. Another important goal of this paper is to address the unusual thermal and thermo-mechanical properties of the new highly functionalized, stereoregular polycarbenes. Polar side- chain functionalities of carbon-chain polymers in general have a large and important influence on the polymer material properties (e.g., toughness, paintability/printability, solvent resistance, mis- cibility).4a However, their influence has so far only been investi- gated for materials in which the mutual influence of the dipole moments of the applied functionalities have a poorly defined (atactic materials)6,8 and/or diluted effect (C2-polymerization of monofunctionalized olefins in general). In this paper we present for the first time efforts to unravel the influence of multiple dipolar interactions in close proximity along a fully functiona- lized and stereoregular carbon-chain polymer chain on the material properties of these poly carbenes. As a result we here dis- close the unusual material properties of new poly carbene materials, which includes a broad end-use temperature range as well as thermotropic (and lyotropic) liquid crystalline behavior in a broad temperature range (rigid rod behavior). Results and Discussion Catalyst Precursors. Previously, we reported different [(diene)RhI(N,O-ligand)] complexes (diene =1,5-cycloocta- diene (cod) (1 in Scheme 2), endo-dicyclopentadiene (dcp), or 2,5-norbornadiene (nbd)) for polymerization of carbenes from ethyl diazoacetate (EDA).10,11 We showed that the diene ligand plays an important role during the propagation steps, while the N,O-ligand is likely involved in the initiation
Figure 1. Carbene precursors: ethyl, benzyl, and tert-butyl diazo- acetate. of the polymerization. The highest yields were obtained with [(L-prolinate)RhI(1,5-cyclooctadiene)] (1) (50%)10,11 and [(L-prolinate)RhI(1,5-dimethyl-1,5-cyclooctadiene)] (2) (up to 80%) and therefore these catalyst precursors were selected for copolymerization reactions. Complex 2 was stored for several days in air prior to its use in the polymer- ization reactions in order to obtain higher polymer yields, following the procedures described in one of our previous papers.13 Complexes 1 and 2 are easily prepared by reacting the corresponding [{RhI(diene)(μ-Cl)}]2 (diene=1,5-cyclooc- tadiene (cod) or 1,5-dimethyl-1,5-cyclooctadiene (dmcod)) with deprotonated L-proline in methanol at room tempera- ture (Scheme 2). Homopolymerization of Different Diazoesters. We first investigated the behavior of catalyst precursors 1 and 2 in the homopolymerization of different diazoesters. The sub- strates are ethyl diazoacetate (EDA), a diazoester with an aromatic substituent: benzyl diazoacetate (BnDA) and one with a sterically demanding side group: tert-butyl diazoace- xxxx (tBuDA) (Figure 1). EDA and tBuDA are commercially available and BnDA was prepared by published proce- dures.15,16 The homopolymerization reactions were performed by addition of 50 equiv of diazoester to a solution of catalyst precursor 1 or 2 in chloroform.10,11 The solution was stirred for 14 h at room temperature. The polymer was obtained by evaporation of the solvent and subsequent precipitation with methanol. After washing with methanol and drying, a white solid was obtained. Carbenes from EDA and BnDA are polymerized to poly- (ethyl 2-ylidene-acetate) (poly(EA)) and poly(benzyl 2-yli- dene-acetate) (poly(BnA)), respectively, of high molecular weight (up to 690 kDa) and in moderate to good yields (entries 1, 2, Moscow 1254124, Russia Abstract— Strong modulation and 5 in Table 1). EDA and BnDA are completely converted into polymers (major fraction), and some dimeric (dialkyl fumarate and maleate) and oligomeric byproducts. The byproducts are soluble in methanol and are separated from the polymer during the precipitation step, as described before.10-12 Precatalyst 2 gives higher yields than precatalyst 1 for both substrates. The bulky diazoester tBuDA is polymerized to poly(tert- butyl 2-ylidene-acetate) (poly(tBuA)) in only low yields by both catalyst precursors 1 and 2 (Table 1, entries 3 and 6). ∼ ∼ ∼ ∼ The conversion is not complete (65% for 1 and 50% for 2) and unreacted tBuDA was recovered after the reaction. Most of the Second Harmonic Generation reacted tBuDA was converted into oligomers ( 80%, Mw 1500 Da, PDI 1.4) and a small amount of dimeric products, di-tert-butyl fumarate and maleate ( 15%). Dur- ing the polymerization reaction the polymeric poly(tBuA) product precipitates from the reaction mixture in chloro- form, which in part explains the low yields (SHGand probably low molecular weights) signal by THz nearly single cycle pulse obtained in ferroelectric thin film BaSrTiO3 was observed. As the employed THz pulses pumps the medium in the range of phononic excitations, the THz electric field induced ferro- electric polarization is due to the ionic contributionthese reactions. The proposed model describes this effect isolated white solid is insoluble in terms most organic solvents, such as chloroform (with and without trifluoroacetic acid), dichlor- omethane, methanol, toluene, and benzene. Because of electric polarization induced in the plane of the filmits poor solubility, poly(tBuA) was analyzed by solid state IR spectroscopy (see Supporting Information). The net SHG signal responds to solubility behavior of poly(tBuA) contrasts markedly with the THz excitation as if the THz pulse induces a 90-degrees switching polymer obtained by radical polymerization of the polarization in parts 8894 Macromolecules, Vol. 43, No. 21, 2010 Xxxxxxx et al. Table 1. Homopolymerization of the sample on the time scale of the period of the soft modeEDA, BnDA, and tBuDA with 1 and 2a entry catalyst precursor diene substrate polymer polymer yield (%)b Mw (kDa)c PDIc 111 1 cod EDA poly(EA) 50 150 3.6 213 1 cod BnDA poly(BnA) 20 80 6.3 3 1 cod tBuA poly(tBuA) <5 n.d. According to the proposed model, under action of the THz pulse the latter acquires an in-plane component up to 6% of the net polarization.n.d. 413 2 dmcod EDA poly(EA) 80 670 3.3 513 2 dmcod BnDA poly(BnA) 50 690 2.7
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric Field-induced Second Harmonic Generation in Ferroelectric Thin Film BaSrTiO3 K. A. Grishunin1, N. A. Ilyin1, N. E. Sherstyuk1, E. D. Mishina1, A. Kimel2, V. M. Mukhortov3, A. V. Ovchinnikov4, O. V. Chefonov4, and M. B. Agranat4 1MIREA, Moscow Technological University, Xxxxxxxxx XxxPublished on 04 May 2020. 00, Xxxxxx 000000, Xxxxxx 2Institute for Molecules and Materials, Downloaded by Radboud University NijmegenNijmegen on 11/11/2020 1:37:58 PM. PCCP PAPER Cite this: Phys. Chem. Chem. Phys., 6525 AJ2020, Nijmegen22, 11572 Received 25th March 2020, Accepted 4th May 2020 DOI: 10.1039/d0cp01613f xxx.xx/xxxx The Netherlands 3Southern Scientific Center structures of Russian Academy of Sciencescationic gold clusters probed by far-infrared spectroscopy† Xxxxx Xxxxxxx, Chehova 41*a Xxx-Xxx Xxx, Rostov-on-Don 344006a Xxxx X. Xxxxxxxxxxx,b Xxxxxxx Xxxxx, Russia 4Joint Institute for High Temperatures of Russian Academy of Sciences (JIHT) Izhorskayast. 13, Bd. 2, Moscow 125412, Russia Abstract— Strong modulation of the Second Harmonic Generation (SHG) signal by THz nearly single cycle pulse in ferroelectric thin film BaSrTiO3 was observed. As the employed THz pulses pumps the medium in the range of phononic excitations, the THz electric field induced ferro- electric polarization is due to the ionic contribution. The proposed model describes this effect in terms of electric polarization induced in the plane of the film. The net SHG signal responds to the THz excitation as if the THz pulse induces a 90-degrees switching of the polarization in parts of the sample on the time scale of the period of the soft mode. According to the proposed model, under action of the THz pulse the latter acquires an in-plane component up to 6% of the net polarization.c Xxxxx X. Xxxxxx b and Xxxxx Xxxxxxxx *a
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric FieldBLACK HOLE PHYSICS A dust-induced Second Harmonic Generation enshrouded tidal disruption event with a resolved radio jet in Ferroelectric Thin Film BaSrTiO3 a galaxy merger S. Mattila1,2*†, X. Xxxxx-Torres3,4*†, A. Efstathiou5, P. Mimica6, M. Fraser7,8, E. Kankare9, A. Alberdi3, M. Á. Aloy6, T. Heikkilä1, P. G. Jonker10,11, P. Lundqvist12, X. Xxxxx-Vidal13, W. P. S. Meikle14, X. Xxxxxx-Cañizales15,16, S. J. Smartt9, S. Tsygankov1, X. Varenius13,17, X. Xxxxxx-Herrero18, M. Bondi19, C. Fransson12, X. Xxxxxxx-Illana20, T. Kangas1,21, R. Kotak1,9, X. Xxxxxxx-Olivencia3, P. Väisänen22,23, X. X. Beswick17, D. L. Clements14, R. Greimel24, X. Harmanen1, X. Kotilainen2,1, Downloaded from xxxxx://xxx.xxxxxxx.xxx at Radboud University Nijmegen on May 03, 2024 K. A. Grishunin1Nandra25, T. Reynolds1, S. Ryder26, N. A. Ilyin1Walton8, N. E. Sherstyuk1X. Wiik1, E. D. Mishina1, A. Kimel2, V. M. Mukhortov3, A. V. Ovchinnikov4, O. V. Chefonov4, and M. B. Agranat4 1MIREA, Moscow Technological University, Xxxxxxxxx XxxG. Östlin12 Tidal disruption events (TDEs) are transient flares produced when a star is ripped apart by the gravitational field of a supermassive black hole (SMBH). 00, Xxxxxx 000000, Xxxxxx 2Institute for Molecules and Materials, Radboud University Nijmegen, 6525 AJ, Nijmegen, The Netherlands 3Southern Scientific Center of Russian Academy of Sciences, Chehova 41, Rostov-on-Don 344006, Russia 4Joint Institute for High Temperatures of Russian Academy of Sciences (JIHT) Izhorskayast. 13, Bd. 2, Moscow 125412, Russia Abstract— Strong modulation We have observed a transient source in the western nucleus of the Second Harmonic Generation merging galaxy pair Arp 299 that radiated >1.5 × 1052 erg at infrared and radio wavelengths but was not luminous at optical or x-ray wavelengths. We interpret this as a TDE with much of its emission reradiated at infrared wavelengths by dust. Efficient reprocessing by dense gas and dust may explain the difference between theoretical predictions and observed luminosities of TDEs. The radio observations resolve an expanding and decelerating jet, probing the jet formation and evolution around a SMBH. T that the nuclear outburst had a peak brightness comparable to that of the entire galaxy nucleus at both near-IR and radio wavelengths (SHGFig. 1) signal by THz nearly single cycle pulse in ferroelectric thin film BaSrTiO3 was observed(7). As Based on the employed THz pulses pumps the medium in the range energetics and multiwavelength behavior of phononic excitationsArp 299-B AT1 over a decade of obser- vations (Figs. 1 to 3), the THz electric field induced ferro- electric polarization is due two broad scenarios to ex- plain its origin are plausible: (i) an event unrelated to the ionic contributionSMBH, such as an extremely energetic SN, or a gamma-ray burst; or (ii) accretion-induced SMBH variability, such as an AGN flare, or a TDE. The proposed model describes this effect in terms of electric polarization induced in High–angular resolution [100 milli-arcsec (mas)], adaptive optics–assisted, near-IR imaging observations from the plane of the film. The net SHG signal responds to the THz excitation as if the THz pulse induces a 90Gemini-degrees switching of the polarization in parts of the sample on the time scale of the period of the soft mode. According to the proposed model, under action of the THz pulse the latter acquires an in-plane component up to 6% of the net polarization.North telescope
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric Field-induced Second Harmonic Generation in Ferroelectric Thin Film BaSrTiO3 15 juli 2021, nr. C791/19 (X. Xxxxxxxx, X. Xxxxx xx Xxxxxxxx, A. Arabadjiev, X. Xxxxxxx, X. Xxxxxxx, X. Xxxxxx, X. Kumin, X. Xxxx, X. von Xxxxxxx, X. Toader, K. A. Grishunin1Xxxxxxx, X. Xxxxxxxxx, N. A. Ilyin1Xxxxxxxxx, N. E. Sherstyuk1X. Xxxxxxx, E. D. Mishina1, A. Kimel2, V. M. Mukhortov3, A. V. Ovchinnikov4, O. V. Chefonov4, and M. B. Agranat4 1MIREA, Moscow Technological University, Xxxxxxxxx XxxX. Passer) m.nt. 00, Xxxxxx 000000, Xxxxxx 2Institute for Molecules and Materials, Radboud University Nijmegen, 6525 AJ, Nijmegen, The Netherlands 3Southern Scientific Center of Russian Academy of Sciences, Chehova 41, Rostov-on-Don 344006, Russia 4Joint Institute for High Temperatures of Russian Academy of Sciences (JIHT) Izhorskayast. 13, BdP.P.T. Bovend’Eert* Art. 2, Moscow 125412, Russia Abstract— Strong modulation of the Second Harmonic Generation (SHG) signal by THz nearly single cycle pulse in ferroelectric thin film BaSrTiO3 was observed19 VEU; art. As the employed THz pulses pumps the medium in the range of phononic excitations, the THz electric field induced ferro- electric polarization is due to the ionic contribution47 Handvest Grondrechten EU; art. The proposed model describes this effect in terms of electric polarization induced in the plane of the film. The net SHG signal responds to the THz excitation as if the THz pulse induces a 90-degrees switching of the polarization in parts of the sample on the time scale of the period of the soft mode. According to the proposed model, under action of the THz pulse the latter acquires an in-plane component up to 6% of the net polarization.267 VWEU
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric Field-induced Second Harmonic Generation in Ferroelectric Thin Film BaSrTiO3 K. A. Grishunin1Xxx Beyne1, N. A. Ilyin1Yu Long Chen1, N. E. Sherstyuk1, E. D. Mishina1, A. Kimel2, V. M. Mukhortov3, A. V. Ovchinnikov4, O. V. Chefonov4Christoph Dobraunig2, and M. B. Agranat4 1MIREABart Mennink3(✉) 1 KU Leuven and imec-COSIC, Moscow Technological Leuven, Belgium 2 Lamarr Security Research, Graz, Austria 3 Radboud University, Xxxxxxxxx Xxx. 00, Xxxxxx 000000, Xxxxxx 2Institute for Molecules and Materials, Radboud University Nijmegen, 6525 AJ, Nijmegen, The Netherlands 3Southern Scientific Center of Russian Academy of Sciences, Chehova 41, Rostov-on-Don 344006, Russia 4Joint Institute for High Temperatures of Russian Academy of Sciences (JIHT) IzhorskayastAbstract. 13, Bd. 2, Moscow 125412, Russia Abstract— Strong modulation One of the Second Harmonic Generation (SHG) signal by THz nearly single cycle pulse in ferroelectric thin film BaSrTiO3 was observed. As the employed THz pulses pumps the medium finalists in the range of phononic excitationsNIST Lightweight Cryptography competition is Elephant v2, a parallelizable, permutation-based authen- ticated encryption scheme. The original first/second-round submission Elephant v1/v1.1 was proven secure against nonce-respecting adversaries in the single-user setting. For the final round, the THz electric field induced ferro- electric polarization is due to mode has undergone certain subtle modifications, the ionic contribution. The proposed model describes this effect in terms of electric polarization induced most important one being a change in the plane authentication portion of the film. The net SHG signal responds to the THz excitation as if the THz pulse induces a 90-degrees switching of the polarization in parts of the sample on the time scale of the period of the soft mode. According to These changes require a new dedicated security proof.
1. In addition, our security analysis is in the proposed modelmulti-user setting and demonstrates that Elephant v2 fares well if multiple devices use Elephant v2 with independent keys. Moreover, our proof shows that Elephant v2 even ensures authenticity under action of the THz pulse the latter acquires an innonce misuse. Keywords: Authenticated encryption · Lightweight · Elephant · Multi-plane component up to 6% of the net polarization.user security · Nonce-misuse
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric Field6 Gerechtshof Amsterdam (Ondernemingskamer) 10 juli 2018, nr. 200.213.190/01 OK, ECLI:NL:GHAMS:2018:2380 (xx. Xxxxxxx, mr. Xxx Boer, xx. Xxxxxxxxxxxx-induced Second Harmonic Generation Xxxxxxxx, prof. xx. Xxxxxxxxxxx RA, drs. Streppel) Noot prof. mr. C.D.J. Bulten [BW art. 2:342] RBS, voor de toepassing van art. 2:342 XX xxxxxx beschouwing moeten blijven. Met betrekking tot xx xxxxxxxx van Xxxx dat een vordering op grond van art. 2:342 BW xxx eenvoudig kan xxxxxx xx- frustreerd door er “een facility agent tussen te schuiven”, overweegt de OK dat ook in Ferroelectric Thin Film BaSrTiO3 K. A. Grishunin1het geval dat een facility agent/pandhouder contractueel gehouden is in het kader van de uitoefening van het stemrecht op instructie van een ander xx xxx- xxxxx, N. A. Ilyin1heeft xx xxxxxx dat voor de beoordeling van een beroep op art. 2:342 BW bepalend zal zijn of de pandhouder door de gedragingen zoals hij die, N. E. Sherstyuk1al xxx niet op instructie, E. D. Mishina1daadwerkelijk heeft ver- richt het belang van de vennootschap zodanig xxxxxxx dat in redelijkheid niet xxx xxxxxx geduld dat hij het stemrecht blijft uitoefenen. In het geval van handelingen die niet vallen binnen dit beoor- delingskader van art. 2:342 BW zal een vordering op andere grondslag zijn aangewezen indien der- gelijke handelingen xxxxxx toebrengen xxx wel in concreto dreigen toe te brengen aan de vennoot- xxxxx. In ieder geval kan uit de door Xxxx genoem- de situatie niet de conclusie xxxxxx getrokken dat art. 2:342 BW zo moet xxxxxx uitgelegd dat han- delingen xxx xxxxxx met een contractuele instruc- tie- bevoegdheid – zoals in dit geval de Junior Lenders – zonder meer aan de pandhouder zouden moeten xxxxxx toegerekend. Ook voor xx xxxxxxxx dat de Junior Lenders voor de toepassing van art. 2:342 BW als pandhouders moeten xxxxxx be- schouwd, A. Kimel2, V. M. Mukhortov3, A. V. Ovchinnikov4, O. V. Chefonov4, and M. B. Agranat4 1MIREA, Moscow Technological University, Xxxxxxxxx Xxx. 00, Xxxxxx 000000, Xxxxxx 2Institute for Molecules and Materials, Radboud University Nijmegen, 6525 AJ, Nijmegen, The Netherlands 3Southern Scientific Center of Russian Academy of Sciences, Chehova 41, Rostov-on-Don 344006, Russia 4Joint Institute for High Temperatures of Russian Academy of Sciences (JIHT) Izhorskayast. 13, Bd. 2, Moscow 125412, Russia Abstract— Strong modulation of the Second Harmonic Generation (SHG) signal by THz nearly single cycle pulse in ferroelectric thin film BaSrTiO3 was observed. As the employed THz pulses pumps the medium in the range of phononic excitations, the THz electric field induced ferro- electric polarization is due to the ionic contribution. The proposed model describes this effect in terms of electric polarization induced in the plane of the film. The net SHG signal responds to the THz excitation as if the THz pulse induces a 90-degrees switching of the polarization in parts of the sample on the time scale of the period of the soft mode. According to the proposed model, under action of the THz pulse the latter acquires an in-plane component up to 6% of the net polarizationbestaat geen grond.
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric Field-induced Second Harmonic Generation in Ferroelectric Thin Film BaSrTiO3 K. A. Grishunin1Xxxxxxx Xx¨lsing1(✉), N. A. Ilyin1Joost Rijneveld2(✉), N. E. Sherstyuk1, E. D. Mishina1, A. Kimel2, V. M. Mukhortov3, A. V. Ovchinnikov4, O. V. Chefonov4Xxxx Schanck3,4(✉), and M. B. Agranat4 1MIREAXxxxx Schwabe2(✉) 1 Department of Mathematics and Computer Science, Moscow Technological UniversityTechnische Universiteit Eindhoven, Xxxxxxxxx Xxx. 00, Xxxxxx 000000, Xxxxxx 2Institute for Molecules and Materials, Radboud University Nijmegen, 6525 AJ, NijmegenEindhoven, The Netherlands 3Southern Scientific Center of Russian Academy of Sciences, Chehova 41, Rostov-on-Don 344006, Russia 4Joint 3 Institute for High Temperatures Quantum Computing, University of Russian Academy of Sciences (JIHT) Izhorskayast. 13Waterloo, Bd. 2Waterloo, Moscow 125412, Russia Abstract— Strong modulation of the Second Harmonic Generation (SHG) signal by THz nearly single cycle pulse in ferroelectric thin film BaSrTiO3 was observed. As the employed THz pulses pumps the medium in the range of phononic excitations, the THz electric field induced ferro- electric polarization is due to the ionic contribution. The proposed model describes this effect in terms of electric polarization induced in the plane of the film. The net SHG signal responds to the THz excitation as if the THz pulse induces a 90Canada Keywords: Post-degrees switching of the polarization in parts of the sample on the time scale of the period of the soft mode. According to the proposed model, under action of the THz pulse the latter acquires an inquantum crypto · Lattice-plane component up to 6% of the net polarization.based crypto · NTRU · CCA2-secure KEM · QROM · AVX2
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric Field-induced Second Harmonic Generation in Ferroelectric Thin Film BaSrTiO3 K. A. Grishunin1Financiering, N. A. Ilyin1zekerheden en insolventie 214 Gemeenschappelijk Hof van Justitie van Aruba, N. E. Sherstyuk1Curaçao, E. D. Mishina1Sint Maarten en van Bonaire, A. Kimel2Sint Eustatius en Saba 13 oktober 2020, V. M. Mukhortov3registratienrs. CUR202000211–CUR2020H00072, A. V. Ovchinnikov4ECLI:NL:OGHACMB:2020:243 (mr. Xxx xxx Xxxx, O. V. Chefonov4mr. Meijer, and M. B. Agranat4 1MIREAmr. Nijhuis) Noot xx. X.X. Xxxxxx Noot[xx.X.X.Xxxxxx BW art. 3:94, Moscow Technological University6:159, Xxxxxxxxx Xxx6:162] gemachtigde: mr. 00J.A.M. Burgers, Xxxxxx 000000tegen de stichting Stichting SONA te Curaçao, Xxxxxx 2Institute for Molecules and Materialsgeïntimeerde, Radboud University Nijmegen, 6525 AJ, Nijmegen, The Netherlands 3Southern Scientific Center of Russian Academy of Sciences, Chehova 41, Rostov-on-Don 344006, Russia 4Joint Institute for High Temperatures of Russian Academy of Sciences gemachtigden: xx. X. Frielink en xx. X.X. Xxxxx. (JIHT) Izhorskayast. 13, Bd. 2, Moscow 125412, Russia Abstract— Strong modulation of the Second Harmonic Generation (SHG) signal by THz nearly single cycle pulse in ferroelectric thin film BaSrTiO3 was observed. As the employed THz pulses pumps the medium in the range of phononic excitations, the THz electric field induced ferro- electric polarization is due to the ionic contribution. The proposed model describes this effect in terms of electric polarization induced in the plane of the film. The net SHG signal responds to the THz excitation as if the THz pulse induces a 90-degrees switching of the polarization in parts of the sample on the time scale of the period of the soft mode. According to the proposed model, under action of the THz pulse the latter acquires an in-plane component up to 6% of the net polarization...; red.)
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric Field6 mei 2003, 39343/98; 39651/98; 43147/98; 46664/99. ( Xx. Xxxxxxxxx (president) Xx. Xxxxxxx Xx. Xxxxx Xx. Xxxx Mr. Bratza Xx. Xxxxxxxx Xx. Xxxxxxxxxx Xx. Xxxxxxxxx Mr. Butkevych Xx. Xxxxx Xx. Xxxxxxx Xx. Xxxxxxxxx Xx. Xxxxxx-induced Second Harmonic Generation Xxxxxxxxxx Xx. Xxxx Mr. Traja Xx. Xxxxxxxxxxxx Xx. Xxxxxxxxxxx ) Xxxxx x.x., xxxxx Nederland. Objectieve onpartijdigheid [EVRM - 6] De aan het hof voorgelegde vraag was of xx Xxxx van State, xxxxx op de aan xx Xxxx toekomende taken van advisering en rechtspraak, onpartijdig geacht xxx xxxxxx in Ferroelectric Thin Film BaSrTiO3 K. A. Grishunin1de zin van art. 6 lid 1. In de aan het hof voorgelegde casus had xx Xxxx geadviseerd over de Tracéwet en werd vervolgens gevraagd recht te spreken betreffende een Tracébesluit. Ten aanzien van de ontvankelijkheid had de Nederlandse regering verweer gevoerd, N. A. Ilyin1inhoudende dat alle klagers, N. E. Sherstyuk1met uitzondering van xx xxxx en mevrouw Xxxxxxxxx, E. D. Mishina1niet de nationale rechtsmiddelen uit putten door niet ook de grieven voor te leggen aan de civiele rechter. Het hof stelt dienaangaande vast dat die rechtsgang, A. Kimel2mede gelet op de afwijzing door de civiele rechter van het beroep xxx Xxxxxxxxx, V. M. Mukhortov3geen redelijke kans op succes bood en dus niet in de weg kan staan aan de ontvankelijkheid. Ten aanzien van de klacht gebaseerd op art. 6 lid 1 concludeert het hof dat er in de voorgelegde zaak niet sprake was van strijd met xx xxxxx van onafhankelijkheid of van (subjectieve xxx wel objectieve) onpartijdigheid. De combinatie van advies en rechtspraak werd in de voorgelegde zaak niet in strijd met art. 6 bevonden omdat er niet sprake was van advisering en rechtspraak in dezelfde zaak: het advies van xx Xxxx van State had betrekking gehad op de Tracéwet, A. V. Ovchinnikov4, O. V. Chefonov4, and M. B. Agranat4 1MIREA, Moscow Technological University, Xxxxxxxxx Xxxterwijl het geding het Tracébesluit betrof. 00, Xxxxxx 000000, Xxxxxx 2Institute for Molecules and Materials, Radboud University Nijmegen, 6525 AJ, Nijmegen, The Netherlands 3Southern Scientific Center of Russian Academy of Sciences, Chehova 41, Rostov-on-Don 344006, Russia 4Joint Institute for High Temperatures of Russian Academy of Sciences (JIHT) IzhorskayastWel wijst het hof er op dat niet uitgesloten is dat de werkwijze en regeling van werkzaamheden van xx Xxxx van State strijd opleveren met art. 13, Bd6. 2, Moscow 125412, Russia Abstract— Strong modulation of the Second Harmonic Generation (SHG) signal by THz nearly single cycle pulse Omdat het hof slechts kan oordelen over de voorgelegde zaak en niet in ferroelectric thin film BaSrTiO3 was observed. As the employed THz pulses pumps the medium in the range of phononic excitations, the THz electric field induced ferro- electric polarization is due to the ionic contribution. The proposed model describes this effect in terms of electric polarization induced in the plane of the film. The net SHG signal responds to the THz excitation as if the THz pulse induces a 90-degrees switching of the polarization in parts of the sample on the time scale of the period of the soft mode. According to the proposed model, under action of the THz pulse the latter acquires an in-plane component up to 6% of the net polarizationabstracto wordt over dit punt niet verder uitgewijd.
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric Field-induced Second Harmonic Generation in Ferroelectric Thin Film BaSrTiO3 K. A. Grishunin1Xxxxxxx K¨onighofer1,2(✉), N. A. Ilyin1Florian Lorber3, N. E. Sherstyuk1, E. D. Mishina1, A. Kimel2, V. M. Mukhortov3, A. V. Ovchinnikov4, O. V. Chefonov4Nils Jansen4, and M. B. Agranat4 1MIREAXxxxxxxx Bloem1 1 Institute IAIK, Moscow Technological Graz University of Technology, Graz, Austria 2 Silicon Austria Labs, TU-Graz XXX DES Lab, Graz, Austria 3 Department of Computer Science, Aalborg University, Xxxxxxxxx Xxx. 00Aalborg, Xxxxxx 000000, Xxxxxx 2Institute for Molecules and Materials, Denmark 4 Radboud University Nijmegen, 6525 AJ, Nijmegen, The Netherlands 3Southern Scientific Center of Russian Academy of Sciences, Chehova 41, Rostov-on-Don 344006, Russia 4Joint Institute for High Temperatures of Russian Academy of Sciences (JIHT) Izhorskayast. 13, Bd. 2, Moscow 125412, Russia Abstract— Strong modulation of the Second Harmonic Generation (SHG) signal by THz nearly single cycle pulse in ferroelectric thin film BaSrTiO3 was observed. As the employed THz pulses pumps the medium in the range of phononic excitations, the THz electric field induced ferro- electric polarization is due to the ionic contribution. The proposed model describes this effect in terms of electric polarization induced in the plane of the film. The net SHG signal responds to the THz excitation as if the THz pulse induces a 90-degrees switching of the polarization in parts of the sample on the time scale of the period of the soft mode. According to the proposed model, under action of the THz pulse the latter acquires an in-plane component up to 6% of the net polarization.Netherlands
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric FieldARTIKEL
1. Inleiding
1. HR 3 maart 1905, ECLI:NL:HR:1905:1, X. 1905, 8191 (Blaauboer/Berlips). Zie over de historie van het onderscheid: E.B. Rank-induced Second Harmonic Generation Berenschot,
2. Het begrip ‘scheidend denken’ ontleen ik aan H.C.F. Schoordijk, ‘Recensie. Over de scheidslijn tussen goederen- en verbintenissenrecht’, NJB 1992, afl. 37, p. 1206, par. 15.
3. Rank-Berenschot 1992, p. 35 e.v. en J. Broese van Groenou, De rechtsverhouding tussen erfpachter en erfverpachter (Recht en Praktijk nr. VG10) (diss. Heerlen), Deventer: Wolters Kluwer 2019, p. 47-91.
4. Vgl. X.X. Xxxxxxx & A.I.M. xxx Xxxxxx (x.x.x. X.X. Xxxxxxx), Mr. C. Assers Handleiding tot de beoefening van het Nederlands Burgerlijk Recht. 3. Vermogensrecht algemeen. Xxxx IV. Algemeen goederenrecht, Deventer: Wolters Kluwer 2021/23 slot.
5. X.X. Xxxxxxx & X. Xxxxxxxxxx, ‘Betalingsverplichtingen uit het zakenrecht in Ferroelectric Thin Film BaSrTiO3 K. A. Grishunin1faillissement’, N. A. Ilyin1in: X.X.X. Xxxxx e.a. (red.), N. E. Sherstyuk1Overeenkomsten en insolventie, E. D. Mishina1Deventer: Kluwer 2012, A. Kimel2i.h.b. p. 79, V. M. Mukhortov382 en Rank-Berenschot 1992, A. V. Ovchinnikov4i.h.b. p. 143, O. V. Chefonov4333-334.
6. W.J.M. xxx Xxxxx & X.X. xxx Xxxxxx, and M. B. Agranat4 1MIREA‘Over wederkerige overeenkomsten en boedelschulden. Beschouwingen naar aanleiding van HR 19 april 2013 inzake Xxxx Xxxxxx/Xxxxxxx q.q.’, Moscow Technological UniversityTvI 2013/26 onder het kopje ‘goederenrechtelijke verplichtingen’ en X.X. Xxxxx, Xxxxxxxxx XxxDe flexibiliteit van het recht van erfpacht (diss. 00Groningen), Den Xxxx: BJu 2013, i.h.b. p. 145-152. Zie ook: X.X. Xxxxx, ‘Goederenrechtelijke verplichtingen tot een doen in faillissement’, TvI 2010/8. Xxx Xxxxxx 000000heeft zijn positie recent bevestigd in X.X. xxx Xxxxxx, Xxxxxx 2Institute for Molecules and MaterialsClassificatie van verplichtingen in faillissement (oratie Groningen), Radboud University NijmegenDeventer: Wolters Kluwer 2022, 6525 AJp. 23-26, Nijmegen28-29.
7. Zie Rb. Noord-Nederland 26 juni 2021, The Netherlands 3Southern Scientific Center ECLI:NL:RBNNE:2021:2575, JOR 2022/129, m.nt. X.X. Xxxxxxx en in xxxxx beroep Hof Arnhem- Leeuwarden 4 oktober 2022, ECLI:NL:GHARL:2022:8502, JOR 2023/23, m.nt. J. Oppatja. Het hof sluit zich in r.o. 3.1 aan bij het oordeel van de rechtbank. De rechtbank verwijst in r.o. 4.38 expliciet naar Van Andel en Van Zanten.
8. S. Baeyens, Vermogensrechten en faillissement. Een rechtsvergelijkend onderzoek naar de tegenwerpelijkheid en afdwingbaarheid van verwervingsrechten, gebruiksrechten en verbodsrechten in faillissement (diss. Leuven), Leuven: KU Leuven 2022 (niet-uitgegeven tekst).
2. Inhoud van het beperkte recht: bundle of Russian Academy of Sciences, Chehova 41, Rostov-on-Don 344006, Russia 4Joint Institute for High Temperatures of Russian Academy of Sciences (JIHT) Izhorskayast. 13, Bd. 2, Moscow 125412, Russia Abstract— Strong modulation of the Second Harmonic Generation (SHG) signal by THz nearly single cycle pulse in ferroelectric thin film BaSrTiO3 was observed. As the employed THz pulses pumps the medium in the range of phononic excitations, the THz electric field induced ferro- electric polarization is due to the ionic contribution. The proposed model describes this effect in terms of electric polarization induced in the plane of the film. The net SHG signal responds to the THz excitation as if the THz pulse induces a 90-degrees switching of the polarization in parts of the sample on the time scale of the period of the soft mode. According to the proposed model, under action of the THz pulse the latter acquires an in-plane component up to 6% of the net polarization.rights
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric Field11 juni 2015, nr. C-649/13 (X. Xxxxxxx, X. Xxxx Barthet, X. Xxxxxx, X. Xxxxxx, X. Xxxxxxx; X-induced Second Harmonic Generation in Ferroelectric Thin Film BaSrTiO3 K. A. Grishunin1X X. Xxxxxxxx) m.nt. P.M. Veder Art. 2 onder g, N. A. Ilyin1, N. E. Sherstyuk1, E. D. Mishina1, A. Kimel2, V. M. Mukhortov3, A. V. Ovchinnikov4, O. V. Chefonov4, and M. B. Agranat4 1MIREA, Moscow Technological University, Xxxxxxxxx Xxxart. 00, Xxxxxx 000000, Xxxxxx 2Institute for Molecules and Materials, Radboud University Nijmegen, 6525 AJ, Nijmegen, The Netherlands 3Southern Scientific Center of Russian Academy of Sciences, Chehova 41, Rostov-on-Don 344006, Russia 4Joint Institute for High Temperatures of Russian Academy of Sciences (JIHT) Izhorskayast. 13, Bd. 3 lid 2, Moscow 125412, Russia Abstract— Strong modulation of the Second Harmonic Generation art. 27 Verordening (SHGEG) signal by THz nearly single cycle pulse in ferroelectric thin film BaSrTiO3 was observednr. As the employed THz pulses pumps the medium in the range of phononic excitations, the THz electric field induced ferro- electric polarization is due to the ionic contribution. The proposed model describes this effect in terms of electric polarization induced in the plane of the film. The net SHG signal responds to the THz excitation as if the THz pulse induces a 90-degrees switching of the polarization in parts of the sample on the time scale of the period of the soft mode. According to the proposed model, under action of the THz pulse the latter acquires an in-plane component up to 6% of the net polarization.44/2001 (Insolventieverordening) RvdW 2015/1166 ECLI:EU:C:2015:44 ECLI:EU:C:2015:384
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric Field-induced Second Harmonic Generation X. X. XXX XXXX et al.: Coherent Plasmon–Phonon Oscillations in Ferroelectric Thin Film BaSrTiO3 K. A. Grishunin1a GaAs Sample 9l phys. stat. sol. (b) 204, N. A. Ilyin19l (l997) Subject classification: 00.00.Xx; 72.30.+q; 73.30.+y; S7.l2 Coherent Plasmon–Phonon Oscillations in a GaAs Schottky Barrier Sample X. X. XXX XXXX (a), N. E. Sherstyuk1X. xx XXXX (b), E. D. Mishina1, A. Kimel2, V. M. Mukhortov3, A. V. Ovchinnikov4, O. V. Chefonov4X. XXX XxxxXxx (b), and M. B. Agranat4 1MIREATh. RASiNG (b)
(a) Physics Department, Moscow Technological UniversityEindhoven University of Technology, Xxxxxxxxx Xxx. 00PO Box 513, Xxxxxx 000000NL−5600 MB Eindhoven, Xxxxxx 2Institute The Netherlands l)
(b) Research Institute for Molecules and Materials, Radboud University NijmegenToernooiveld, 6525 AJ, NL−6525 ED Nijmegen, The Netherlands 3Southern Scientific Center of Russian Academy of Sciences, Chehova 41, Rostov-on-Don 344006, Russia 4Joint Institute for High Temperatures of Russian Academy of Sciences (JIHT) Izhorskayast. 13, Bd. 2, Moscow 125412, Russia Abstract— Strong modulation of the Second Harmonic Generation (SHG) signal by THz nearly single cycle pulse in ferroelectric thin film BaSrTiO3 was observed. As the employed THz pulses pumps the medium in the range of phononic excitations, the THz electric field induced ferro- electric polarization is due to the ionic contribution. The proposed model describes this effect in terms of electric polarization induced in the plane of the film. The net SHG signal responds to the THz excitation as if the THz pulse induces a 90-degrees switching of the polarization in parts of the sample on the time scale of the period of the soft mode. According to the proposed model, under action of the THz pulse the latter acquires an in-plane component up to 6% of the net polarization.Netherlands
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric Field-induced Second Harmonic Generation in Ferroelectric Thin Film BaSrTiO3 K. A. Grishunin1Transport Reviews, N. A. Ilyin12014 Vol. 34, N. E. Sherstyuk1No. 3, E. D. Mishina1335 – 355, A. Kimel2xxxx://xx.xxx.xxx/10.1080/01441647.2014.903531 Transport, V. M. Mukhortov3Development and Climate Change Mitigation: Towards an Integrated Approach XXXXXX XXXXXX∗,∗∗, A. V. Ovchinnikov4XXXX XXXXXXXXX†, O. V. Chefonov4HELEEN DE CONINCK‡ AND XXXXXX XXXXXXXX§ ∗ Deutsche Gesellschaft fu¨ er Internationale Zusammenarbeit (GIZ), 193/63 Lake Rajada Office Complex, New Xxxxxxxxxxxxx Xxxx, Xxxxxxxxxx, Xxxxxxx 00000, Xxxxxxxx; ∗∗Faculty of Geo- Information Science and M. B. Agranat4 1MIREAEarth Observation (ITC), Moscow Technological UniversityUniversity of Twente, Xxxxxxxxx Xxx. 00P.O. Box 217, Xxxxxx 0000007500 AE, Xxxxxx 2Institute Enschede, The Netherlands; †Centre for Molecules Transport Studies, University of Cape Town, Private Bag X3, Rondebosch 7701, South Africa; ‡Institute for Science, Innovation and MaterialsSociety (ISIS), Radboud University Nijmegen, 6525 AJP.O. Box 9010 (Mailbox 77), 6500 GL Nijmegen, The Netherlands 3Southern Scientific Center of Russian Academy of SciencesNetherlands; (Received 27 June 2013; revised 9 March 2014; accepted 9 March 2014) Abstract Transport and infrastructure development enables economic and social development, Chehova 41but is often detrimental to sustainable development due to congestion, Rostov-on-Don 344006accidents, Russia 4Joint Institute for High Temperatures of Russian Academy of Sciences (JIHT) Izhorskayastair pollution, as well as greenhouse gas emissions. 13Various policy frameworks have been created to connect transport with development, Bddevelopment with climate change and climate change mitigation with the trans- port sector. 2However, Moscow 125412, Russia Abstract— Strong modulation so far no consistent framework exists that addresses these three areas in an inte- grated manner.This article demonstrates that sustainable development of the Second Harmonic Generation (SHG) signal by THz nearly single cycle pulse in ferroelectric thin film BaSrTiO3 was observed. As transport sector is not viable on the employed THz pulses pumps the medium longer term in the range absence of phononic excitationssuch a three-way framework. First, current perspectives and practices on transport and (sustainable) development are reviewed, demonstrating that outcomes and policies are not consistently positive on all three dimensions. The article then re-evaluates the THz electric field induced ferro- electric polarization is due Avoid– Shift– Improve (ASI) approach, initially developed to address climate change mitigation and other environmental issues in the transport sector, adding two perspectives on sustainable devel- opment that are not generally taken into account when discussing ASI: transition theory and sus- tainable lifestyles. Together with attention to the ionic contribution. The proposed model describes development function of transport by incorporating Access into ASI, this effect in terms of electric polarization induced in the plane of the film. The net SHG signal responds to the THz excitation as if the THz pulse induces could enable a 90more long-degrees switching of the polarization in parts of the sample term sustainability-oriented view on the time scale of the period of the soft mode. According to the proposed modeltransport, under action of the THz pulse the latter acquires an in-plane component up to 6% of the net polarizationdevelopment and climate mitigation.
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric FieldXxxxxx Xxxxxxx-induced Second Harmonic Generation in Ferroelectric Thin Film BaSrTiO3 K. A. Grishunin1Xx¨bner1, N. A. Ilyin1Marit Hansen2, N. E. Sherstyuk1, E. D. Mishina1, A. Kimel2, V. M. Mukhortov3, A. V. Ovchinnikov4, O. V. Chefonov4Jaap-Henk Hoepman1,3,4, and M. B. Agranat4 1MIREAMeiko Jensen1(✉) 0 Xxxxxxxx Xxxxxxxxxx, Moscow Technological University, Xxxxxxxxx Xxx. 00Xxxxxxxx, Xxxxxx 000000, Xxxxxx 2Institute for Molecules and Materials, {xxxxxx.xxxxxxx-xxxxxxx,xxxxx.xxxxxx}@xxx.xx 3 Radboud University Nijmegen, 6525 AJUniversity, Nijmegen, The Netherlands 3Southern Scientific Center 4 University of Russian Academy of SciencesGroningen, Chehova 41Groningen, Rostov-on-Don 344006, Russia 4Joint Institute for High Temperatures of Russian Academy of Sciences (JIHT) Izhorskayast. 13, Bd. 2, Moscow 125412, Russia Abstract— Strong modulation of the Second Harmonic Generation (SHG) signal by THz nearly single cycle pulse in ferroelectric thin film BaSrTiO3 was observed. As the employed THz pulses pumps the medium in the range of phononic excitations, the THz electric field induced ferro- electric polarization is due to the ionic contribution. The proposed model describes this effect in terms of electric polarization induced in the plane of the film. The net SHG signal responds to the THz excitation as if the THz pulse induces a 90-degrees switching of the polarization in parts of the sample on the time scale of the period of the soft mode. According to the proposed model, under action of the THz pulse the latter acquires an in-plane component up to 6% of the net polarization.Netherlands
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric Field& Reaction Mechanisms An Unprecedented Retro-induced Second Harmonic Generation in Ferroelectric Thin Film BaSrTiO3 K. A. Grishunin1Xxxx Rearrangement Revealed by ESI- MS/MS, N. A. Ilyin1, N. E. Sherstyuk1, E. D. Mishina1, A. Kimel2, V. M. Mukhortov3, A. V. Ovchinnikov4, O. V. Chefonov4IRMPD Spectroscopy, and M. B. Agranat4 1MIREADFT Calculations** Xxxxxxx Xxxxxxxxx,*[a, Moscow Technological Universityb] Xxxxxxxx Xxxxx,[b] Xxxxxxxxxxxx Xxxxx,[b] Xxx Xxxxxx,[c] Xxxx Xxxxxx,[c] and Xxxxxxxxx Xx Xxxxxxx*[b] Abstract: Brønsted acids and protic solvents mediate acyl transfer, Xxxxxxxxx Xxxknown as the Xxxx rearrangement, from imidates to the corresponding acylamides. 00This represents a key step in several reactions, Xxxxxx 000000for example, Xxxxxx 2Institute for Molecules the Ugi four-component re- action (U-4CR) and MaterialsPasserini three-component reaction (P- 3CR). Herein, Radboud University Nijmegen, 6525 AJ, Nijmegen, The Netherlands 3Southern Scientific Center of Russian Academy of Sciences, Chehova 41, Rostov-on-Don 344006, Russia 4Joint Institute for High Temperatures of Russian Academy of Sciences (JIHT) Izhorskayast. 13, Bd. 2, Moscow 125412, Russia Abstract— Strong modulation an unprecedented break of the Second Harmonic Generation non-reversibili- ty of the Xxxx rearrangement is reported. A combination of electrospray tandem mass spectrometry (SHGESI-MS/MS), in- frared multiphoton dissociation (IRMPD) signal by THz nearly single cycle pulse in ferroelectric thin film BaSrTiO3 was observed. As ion spectroscopy and theoretical calculations demonstrates the employed THz pulses pumps occurrence of the medium retro-Xxxx rearrangement of protonated isopeptides in the gas phase. In the gas phase, the extra proton acquired during ESI promotes the backward isomerisation reaction in a catalytic fashion. Introduction First discovered in 1910,[1] the Xxxx rearrangement stands for intramolecular acyl transfer that describes the conversion of acylimidate into acylamide products. Although it was origi- xxxxx understood as a [1,3]O,N-acyl shift, its definition has been extended over the years to include a wider range of phononic excitationsacyl and thioacyl group transfers (Scheme 1).[2] Such generalisation arises essentially from the diffusion of isocyanide-based multi- component reactions, such as the Ugi and Passerini reactions, in which the Xxxx rearrangement represents the final reac- tion step.[3] Recent theoretical studies on these important chemical transformations show that the Xxxx rearrangement is not rate determining, but proceeds conversely with a rela- tively low activation barrier.[4] The Xxxx rearrangement was found to be strongly exothermic and thermodynamically drove the entire process.[4] The proton-transfer process that promotes isomerisation is also noteworthy. Brønsted acids, or even the
a) The Xxxx rearrangement as the originally intended [1,3]O,N- acyl shift.[1] b) The current extended Xxxx rearrangement concept.[2] solvent if protic media are used, have been shown to mediate acyl transfer.[4] Such protic partners also act as hydrogen-bond donors, and play a major role in imidate activation towards the Xxxx rearrangement.[4,5] Recently, the THz electric field induced ferro- electric polarization is due to the ionic contribution. The proposed model describes this effect in terms of electric polarization induced in the plane mechanism of the film. The net SHG signal responds Ugi four-component reac- tion (U-4CR) (Scheme 2) has been investigated by ESI-MS by us[6] and others.[7] This technique has evolved as a powerful tool[8] to the THz excitation as if the THz pulse induces a 90address fundamental questions in reaction-degrees switching of the polarization in parts of the sample on the time scale of the period of the soft mode. According to the proposed model, under action of the THz pulse the latter acquires an in-plane component up to 6% of the net polarization.mecha-
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric Field-induced Second Harmonic Generation in Ferroelectric Thin Film BaSrTiO3 K. A. Grishunin1Nicolas Bordes1(✉), N. A. Ilyin1Xxxx Daemen2, N. E. Sherstyuk1, E. D. Mishina1, A. Kimel2, V. M. Mukhortov3, A. V. Ovchinnikov4, O. V. Chefonov4Dani¨el Kuijsters2, and M. B. Agranat4 1MIREAGilles Van Assche3 1 Universit´e Grenoble Alpes, Moscow Technological Grenoble, France 2 Radboud University, Xxxxxxxxx Xxx. 00, Xxxxxx 000000, Xxxxxx 2Institute for Molecules and Materials, Radboud University Nijmegen, 6525 AJ, Nijmegen, The Netherlands 3Southern Scientific Center of Russian Academy of Sciences, Chehova 41, Rostov-on-Don 344006, Russia 4Joint Institute for High Temperatures of Russian Academy of Sciences (JIHT) Izhorskayast. 13, Bd. 2, Moscow 125412, Russia Abstract— Strong modulation {xxxx.xxxxxx,Xxxxxx.Xxxxxxxxx}@xx.xx 3 Modern block ciphers and cryptographic permutations consist of the Second Harmonic Generation iteration of a round function. In many cases this round function consists of a layer of nonlinear S-boxes, a mixing layer, a shuffle layer (SHGAKA a bit transposition or bit permutation), and the addition of a round key (in block ciphers) signal by THz nearly single cycle pulse or constant (in ferroelectric thin film BaSrTiO3 was observedcryptographic permutations). As Electronic supplementary material The online version of this chapter (https:// xxx.xxx/00.0000/000-0-000-00000-0 12) contains supplementary material, which is available to authorized users. Oc International Association for Cryptologic Research 2021 X. Xxxxxx and X. Xxxxxxx (Eds.): CRYPTO 2021, LNCS 12827, pp. 337–367, 2021. xxxxx://xxx.xxx/10.1007/978-3-030-84252-9_12 Many papers investigate S-boxes and try to find a good compromise between implementation cost and propagation properties or provide a classification of all invertible S-boxes of a given width, see, e.g., [27, 34]. Similarly, there is a rich literature on certain types of mixing layers. In particular, there have been many papers written about finding maximum-distance separable (MDS) mappings or near-MDS mappings with minimum implementation cost according to some met- ric, see, e.g., [28, 37]. Building a good cipher starts with taking a good S-box and mixing layer and the employed THz pulses pumps rich cryptographic literature on these components provides us with ample choice. However, how these building blocks are combined in a round function and the medium resulting propagation properties has received much less systematic attention. A standard way for designing a good round function from an S-box and an MDS mapping is the one followed in the range Advanced Encryption Standard (AES) [32] and is known as the wide trail strategy [14, 20]. This strategy gives criteria for the shuffle layer and comes with easy-to-verify bounds for the differen- tial probability (DP) of phononic excitationsdifferential trails (also known as characteristics) and the linear potential (LP) of linear trails. These bounds and its simplicity have made it one of the most applied design strategies, and AES has inspired a plethora of primitive designs, including lightweight ones. By adopting 4-bit S-boxes instead of 8-bit ones and modern lightweight MDS layers in a smart structure, multi- ple lightweight ciphers have been constructed. Many lessons were learned and this line of design has culminated in the block cipher of the NIST lightweight competition candidate Saturnin [12], a truly modern version of AES. Naturally, there are alternative design approaches. A popular design approach is the one underlying the 64-bit lightweight block cipher Present [10]. Its round function has no MDS layer and simply consists of an S-box layer, a bit shuffle, and a key addition. It gets its diffusion from the combination of a smart choice of the bit shuffle and specific propagation criteria from its well-chosen S-box and doing many rounds. The Present line of design has also been refined in the form of the Gift (64- and 128-bit) block ciphers [1] and the cryptographic permutations of the Spongent lightweight hash function [9] that is used in Elephant [7]. Another distinctive design approach is that of the cryptographic permutation of the SHA-3 standard [33], Keccak-f . Unlike Present, its round function does have a mixing layer, and it actually has all ingredients that AES has. Specifically, in their rationale, the THz electric field induced ferro- electric polarization is due designers also refer to the ionic contributionwide trail design strategy [6]. However, this wide-trail flavor does not appear to come with the simple bounds as in the case of AES, and designers have to resort to tedious and time-consuming programming efforts to obtain similar bounds. This is related to the fact that AES operates on bytes and Keccak-f on bits. The proposed model describes Keccak-f designers have discussed the difference between these two design approaches in [18]. In that paper, they have coined the term alignment to characterize this effect difference and supported it with some propagation experiments on Keccak-f . The Keccak-f line of design has also been refined and led to the 384-bit permutation that is used in terms Xoodyak [15], namely Xoodoo [16], a truly modern version of electric polarization induced Keccak-f . This treatment is not exhaustive and other distinctive design strategies exist. alternating Additions with Rotations and XOR (ARX) such as Salsa [3], or they iterate very simple round functions many times such as Simon [2]. In this paper we systematically analyze the impact of alignment on the differ- ential and linear propagation properties of ciphers. We show that certain design choices regarding how the S-box and mixing layers are combined have a pro- found impact on the propagation properties. We identify and name a number of effects that are relevant in the plane this context. Furthermore, we believe that this makes it possible to give a meaningful and non-ambiguous definition of the film. The net SHG signal responds to the THz excitation as if the THz pulse induces a 90-degrees switching of the polarization in parts of the sample on the time scale of the period of the soft mode. According to the proposed model, under action of the THz pulse the latter acquires an in-plane component up to 6% of the net polarizationterm alignment.
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End User Agreement. This publication is distributed under the terms of Article 25fa of the Dutch Copyright Act. This article entitles the maker of a short scientific work funded either wholly or partially by Dutch public funds to make that work publicly available for no consideration following a reasonable period of time after the work was first published, provided that clear reference is made to the source of the first publication of the work. Research outputs of researchers employed by Dutch Universities that comply with the legal requirements of Article 25fa of the Dutch Copyright Act, are distributed online and free of cost or other barriers in institutional repositories. Research outputs are distributed six months after their first online publication in the original published version and with proper attribution to the source of the original publication. You are permitted to download and use the publication for personal purposes. All rights remain with the author(s) and/or copyrights owner(s) of this work. Any use of the publication other than authorised under this licence or copyright law is prohibited. If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the University Library know, stating your reasons. In case of a legitimate complaint, the University Library will, as a precaution, make the material inaccessible and/or remove it from the website. Please contact the University Library through email: xxxxxxxxx@xxx.xx.xx. You will be contacted as soon as possible. University Library Radboud University THz Electric Field-induced Second Harmonic Generation APR-246/PRIMA-1MET rescues epidermal differentiation in Ferroelectric Thin Film BaSrTiO3 K. A. Grishunin1skin keratinocytes derived from EEC syndrome patients with p63 mutations Xxxxxxx Xxxxx,1,2, N. A. Ilyin1Xxxxx X. xxx xxx Xxxxxxxx,2, N. E. Sherstyuk1Xxxxxx X. Xxxxxxxxxxxx,2, E. D. Mishina1Xxxxxxxx X. X. Xxxxxx, A. Kimel2Xxxxx Xxxxxx, V. M. Mukhortov3Xxxxx Xxxxxx, A. V. Ovchinnikov4Xxxxxxxx X. Xxxxxxxxxx, O. V. Chefonov4Xxxxxxxxx Xxxxxxxxx, Xxxxx X. xxx Xxxxxxxxxx, Joost Schalkwijkb, Xxxx xxx Xxxxxxxxx, Xxxx X. Wimana,3, and M. B. Agranat4 1MIREAXxxxxxx Xxxxx,e,3 aDepartment of Oncology-Pathology, Moscow Technological UniversityCancer Center Karolinska, Xxxxxxxxx Xxx. 00Karolinska Institutet, Xxxxxx 000000SE-171 76 Stockholm, Xxxxxx 2Institute Sweden; bDepartment of Dermatology, Radboud University Nijmegen Medical Centre, Nijmegen Centre for Molecules Molecular Life Sciences, Nijmegen Institute for Infection, Inflammation and MaterialsImmunity, 6525 GA Nijmegen, The Netherlands; cDepartment of Human Genetics, Radboud University Nijmegen Medical Centre, Nijmegen Centre for Molecular Life Sciences, 6525 GA Nijmegen, The Netherlands; and dDepartment of Molecular Biology, and eDepartment of Molecular Developmental Biology, Faculty of Science, Centre for Molecular Life Sciences, Radboud University Nijmegen, 6525 AJ, GA Nijmegen, The Netherlands 3Southern Scientific Center of Russian Academy of SciencesCELL BIOLOGY Edited by Xxx X. Xxx, Chehova 41, Rostov-on-Don 344006, Russia 4Joint The Xxxxxxxx Family Institute for High Temperatures Breast Cancer Research, Ontario Cancer Institute at Princess Xxxxxxxx Hospital, University Health Network, Toronto, ON, Canada, and approved December 12, 2012 (received for review February 6, 2012) p53 and p63 share extensive sequence and structure homology. p53 is frequently mutated in cancer, whereas mutations in p63 cause developmental disorders manifested in ectodermal dysplasia, limb defects, and orofacial clefting. We have established primary adult skin keratinocytes from ectrodactyly, ectodermal dysplasia, and cleft lip/palate (EEC) syndrome patients with p63 mutations as an in vitro human model to study the disease mechanism in the skin of Russian Academy EEC patients. We show that these patient keratinocytes cultured either in submerged 2D cultures or in 3D skin equivalents have impaired epidermal differentiation and stratification. Treatment of Sciences these patient keratinocytes with the mutant p53-targeting com- pound APR-246/PRIMA-1MET (JIHTp53 reactivation and induction of massive apoptosis) Izhorskayastthat has been successfully tested in a phase I/ II clinical trial in cancer patients partially but consistently rescued morphological features and gene expression during epidermal stratification in both 2D and 3D models. 13This rescue coincides with restoration of p63 target-gene expression. Our data show that EEC patient keratinocytes with p63 mutations can be used for charac- terization of the abnormal molecular circuitry in patient skin and may open possibilities for the design of novel pharmacological treatment strategies for patients with mutant p63-associated developmental abnormalities. T he p53 family of transcription factors p53, Bdp63, and p73 share high sequence and structure homology, especially in their DNA-binding domains. p53 plays a key role in tumor suppression and is mutated in around 50% of human tumors (1), whereas p63 is a master regulator during ectodermal and epidermal development (2, Moscow 1254123). p63 is expressed as several isoforms with different N-ter- xxxxx ends, Russia Abstract— Strong modulation the TA and ΔN isoforms, and different C-terminal ends, designated α, β, γ, δ, and e (4). ΔNp63α is the major isoform expressed in the epidermis (5). The key role of p63 in ectodermal and epidermal development has been demonstrated in animal models as well as in human palate (AEC) syndrome, which differs from the EEC syndrome mainly by the severity of the Second Harmonic Generation (SHG) signal by THz nearly single cycle pulse in ferroelectric thin film BaSrTiO3 was observedskin phenotype, the occurrence of an eyelid fusion at birth, and the absence of limb malformations. As Mutations associated with the employed THz pulses pumps the medium AEC syndrome are localized in the range C-terminal XXX domain, which is absent in the p53 protein (7, 9). The cellular mechanisms of phononic excitationsepidermal differentiation and stratification controlled by p63 have mainly been studied in mouse models, including p63-deficient mice with or without rescue by p63 isoforms, and in mouse ES cells (10–12). However, these studies are not able to illustrate the disease mechanism underlying the phenotypes caused by heterozygous p63 point mutations in humans (4). Two knock-in models of p63 mutations have been reported so far, L514F for the AEC syndrome (13) and R279H for the EEC syndrome (14). The L514F mice fully recapitulate the human AEC syndrome with abnormalities in skin and craniofacial structures. In the R279H knock-in model, limb phenotypes re- sembling that of p63 knock-out mice have been observed, whereas clear skin phenotypes have not been reported. Furthermore, there is a clear clinical variability among EEC syndrome patients with p63 mutations (15), which suggests that individual genetic back- ground is one of the important determinants for the phenotypes. Therefore, mouse models established so far seem not be suitable to uncover the molecular circuitry in the skin that is affected in the EEC syndrome and to perform drug screening. The current therapy for disorders caused by p63 mutations is limited to cosmetic surgery. Opportunities for improved treatment may come from studies of the family member p53. Because of the important tumor-suppressor function of p53 (16, 17), novel strat- egies for targeting p53 for cancer therapy have been intensively pursued. Several compounds have been reported to restore wild- type function to mutant p53 and induce p53-dependent cell death (18). Previously, we found that the low molecular weight com- pounds PRIMA-1 and APR-246/PRIMA-1MET (henceforth re- ferred to as APR-246) restore conformation and tumor suppressor developmental disorders. Disruption of p63 in mice and zebrafish Downloaded at RADBOUD UNIVERSITEIT NIJMEGEN on February 6, 2020 causes severe epidermal and limb defects (2, 3, 6). In humans, heterozygous mutations in p63 give rise to several clinical con- ditions with autosomal dominant inheritance (7). The three major characteristics of these developmental disorders are limb defects, orofacial clefting, and ectodermal dysplasia, which are comprised of defects in skin, hair, teeth, nails, and several exocrine glands. Among these disorders, the THz electric field induced ferro- electric polarization is due to ectrodactyly, ectodermal dysplasia, and cleft lip/palate (EEC) syndrome displays all three major hallmarks. p63 mutations associated with the ionic contribution. The proposed model describes this effect in terms of electric polarization induced EEC syndrome are point mutations in the plane DNA-binding domain affecting all isoforms. Some of the filmamino acid residues mutated in the EEC syndrome correspond to hotspot tumor-associated mutant resi- dues in p53; p63 R204 corresponds to p53 R175H, p63 R304 to p53 R273, and p63 R279 to p53 R248 (8). The net SHG signal responds to Another p63-associated disorder is the THz excitation as if ankyloblepharon-ectodermal defects-cleft lip/ Author contributions: X. Xxxx, X.X.x.x.X., E.N.K., V.J.N.B., K.G.W., and H.Z. designed research; X. Xxxx, X.X.x.x.X., X.X.X., X.X., Q.Z., G.S.T., and H.Z. performed research; X. Xxxx, E.H.v.d.B., E.N.K., V.J.N.B., X.X., X.X.x.X., X. Schalkwijk, H.v.B., X.X.X., and H.Z. analyzed data; and X. Xxxx, X.X.x.x.X., E.N.K., V.J.N.B., K.G.W., and H.Z. wrote the THz pulse induces paper. Conflict of interest statement: K.G.W. and V.J.N.B. are cofounders and shareholders of Xxxxx XX, a 90company that develops p53-degrees switching based cancer therapy, including APR-246. K.G.W. is a member of the polarization in parts its board. This article is a PNAS Direct Submission. 1Present address: Department of the sample on the time scale Hematology, Institute of the period of the soft mode. According to the proposed modelStem Cell Biology and Regen- erative Medicine, under action of the THz pulse the latter acquires an in-plane component up to 6% of the net polarizationStanford University, Stanford, CA 94305.
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