Synthèses et propriétés thermiques et photophysiques de nouveaux polymères de coordination à base de CuX (X = Cl, Br, I) et de ligands mono- ou dithioéthers

La recherche sur la conception de nouveaux matériaux, dits intelligents, est en constant progrès depuis plus de 30 ans. Historiquement, les premiers matériaux utilisés et transformés par l’homme étaient le bois, les minéraux et ses dérivés (pierre, métaux, etc.). C’est à la fin du 19e siècle que la synthèse des polymères organiques et inorganiques ainsi que leurs utilisations se développèrent. Ce progrès continue de nos jours. Ainsi, c’est dans cette direction que cette thèse fut rédigée, l’étude de polymères de coordination basés sur le cuivre(I). Elle s’orchestra en six principales sections de recherche. La première section, i.e. le chapitre 2 traite de la coordination de différents ligands monothioéthers sur du CuX (X = I, Br) pour former plusieurs types de polymères de coordination (CPs). Ainsi, le CP 1D [(Me[indice inférieur 2]S)[indice inférieur 3]{Cu[indice inférieur 2]([mu]-I)[indice inférieur 2}][indice inférieur n] est obtenu quand CuI et Sme[indice inférieur 2] réagissent ensemble dans le n-heptane, alors qu’ils entrainent la formation du CP 2D [(Me[indice inférieur 2]S) [indice inférieur 3] {Cu[indice inférieur 4]([mu]-I) [indice inférieur 4]}] [indice inférieur n] dans le MeCN. Ce dernier contient des unités de construction secondaire (SBU ; Secondary Building Units en anglais) en forme de cluster Cu[indice inférieur 4]I[indice inférieur 4] « cubane partiellement ouvert ». En faisant réagir le MeSEt avec du CuI, le CP 2D [(MeSEt) [indice inférieur 2]{Cu[indice inférieur 4] ([mu][indice inférieur 3]-I) [indice inférieur 2] ([mu][indice inférieur 2]-I) [indice inférieur 2]}(MeCN) [indice inférieur 2]] [indice inférieur n] contenant des SBUs de type Cu[indice inférieur 4]I[indice inférieur 4] « cubanes en escalier » a été isolé dans MeCN, alors qu’ils entrainent l’obtention du polymère 1D [(MeSEt) [indice inférieur 3]{Cu[indice inférieur 4] ([mu][indice inférieur 3]-I) [indice inférieur 4]}] [indice inférieur n] dans le n-heptane contenant quant à lui des clusters de types Cu[indice inférieur 4]I[indice inférieur 4] « cubanes fermés ». Alors que le traitement de MeSPr avec du CuI forme le CP 1D [(MeSPr) [indice inférieur 3]{Cu[indice inférieur 4] ([mu][indice inférieur 3]-I) [indice inférieur 4]}] [indice inférieur n], les composés [(L) [indice inférieur 4]{Cu[indice inférieur 4] ([mu][indice inférieur 3]-I) [indice inférieur 4]}] (L = EtSPr, Pr[indice inférieur 2]S) sont respectivement obtenus avec le EtSPr et le Pr[indice inférieur 2]S. À partir du [indice supérieur i]Pr[indice inférieur 2]S et de CuI, le cluster [([indice supérieur i]Pr[indice inférieur 2]S) [indice inférieur 6]{Cu[indice inférieur 8] ([mu][indice inférieur 3]-I) [indice inférieur 3]}([mu][indice inférieur 4]-I) [indice inférieur 2]}] est obtenu alors que l’on forme un CP 2D [(Cu[indice inférieur 3]Br[indice inférieur 3])(MeSEt) [indice inférieur 3]] [indice inférieur n] à partir de CuBr et MeSEt dans l’heptane. Ce dernier incorpore à la fois des Cu([mu][indice inférieur 2]-Br) [indice inférieur 2]Cu rhomboédriques et des SBUs de type Cu[indice inférieur 4]Br[indice inférieur 4] « cubanes ouverts ». Le MeSPr forme, quant à lui avec le CuBr dans l’heptane, le CP 1D [(Cu[indice inférieur 3]Br[indice inférieur 3])(MeSPr) [indice inférieur 3]] [indice inférieur n] qui, après recristallisation dans le MeCN, est converti en un CP 2D [(Cu[indice inférieur 5]Br[indice inférieur 5])([mu][indice inférieur 2]-MeSPr) [indice inférieur 3]] [indice inférieur n] incorporant des SBUs [(Cu[indice inférieur 5] ([mu][indice inférieur 4]-Br)([mu][indice inférieur 2]-Br)]. Les propriétés de stabilités thermiques et photophysiques de ces matériaux ont aussi été reportées.   Dans la section 2, i.e. au chapitre 3, les réactions entre des ligands dithioétherbutanes (1,4-bis(phénylthio)butane et 1,4-bis(cyclohexylthio)butane) avec CuX (X = Br, I) ont été étudiées. En faisant réagir les CuX avec le 1,4-bis(cyclohexylthio)butane, dans le ratio (1:1), les CPs 1D, peu luminescents, isostructuraux [(Cu[indice inférieur 2]X[indice inférieur 2])([mu]-CyS(CH[indice inférieur 2]) [indice inférieur 4])SCy) [indice inférieur 2]] [indice inférieur n] (X = Br, I) sont obtenus. Inversement, quand CuI réagit avec 1,4-bis(phénylthio)butane, dans le ratio (2:1), il se forme le préalablement reporté CP 2D [(Cu[indice inférieur 4]I[indice inférieur 4])([mu]- PhS(CH[indice inférieur 2]) [indice inférieur 4])SPh) [indice inférieur 2]] [indice inférieur n], alors qu’avec le CyS(CH[indice inférieur 2]) [indice inférieur 4])SCy, un nouveau composé luminescent est obtenu, mais sa structure n’a pas pu être résolue.(1) Les caractérisations habituelles en photophysique et en stabilité thermique ont été menées sur ces matériaux. Dans la troisième section, i.e. dans le chapitre 4, les réactions de coordination de CuX (Br, I) sur les ligands dithioétherbutènes E- et Z-PhS(CH[indice inférieur 2]CH=CHCH[indice inférieur 2])SPh, E- et Z-pTolS(CH[indice inférieur 2]CH=CHCH[indice inférieur 2])S-pTol ont été comparées. Quand les sels CuX réagissent avec E-PhS(CH[indice inférieur 2]CH=CHCH[indice inférieur 2])SPh les CP 2D [Cu[indice inférieur 2]X[indice inférieur 2]{[mu]-E-PhS(CH[indice inférieur 2]CH=CHCH[indice inférieur 2])SPh}[indice inférieur 2]] [indice inférieur n] (X = I, Br), composés isostructuraux, sont obtenus. Incorporant une structure sans-précédente, ces réseaux sont formés à partir de couches 2D en alternance ABAB, contenants des SBUs Cu[indice inférieur 2] ([mu][indice inférieur 2]-X) [indice inférieur 2] rhomboédriques. Inversement, quand l’isomère Z-PhS(CH[indice inférieur 2]CH=CHCH[indice inférieur 2])SPh réagit avec des sels de CuX, deux structures différentes sont obtenues : le CP 2D [Cu[indice inférieur 4] ([mu][indice inférieur 3]-I) [indice inférieur 4] ([mu]-Z-PhS(CH[indice inférieur 2]CH=CHCH[indice inférieur 2])SPh}[indice inférieur 2]] [indice inférieur n] contenant des SBUs de type « cubane fermé » et le complexe 0D [Cu[indice inférieur 2]Br[indice inférieur 2]{[mu]-Z-PhS(CH[indice inférieur 2]CH=CHCH[indice inférieur 2])SPh}[indice inférieur 2]]. De par la réaction de E-pTolS(CH[indice inférieur 2]CH=CHCH[indice inférieur 2])S-pTol avec CuI, le CP 2D [{Cu([mu][indice inférieur 3]-I)} [indice inférieur 2] ([mu]-E-pTolS(CH[indice inférieur 2]CH=CHCH[indice inférieur 2])S-pTol)]n contenant des rubans parallèles en escalier est obtenu, alors que la structure issue de CuBr n’a pas pu être résolue. Finalement, quand CuX réagit avec Z-pTolS(CH[indice inférieur 2]CH=CHCH[indice inférieur 2])S-pTol, les CPs 2D iso-structuraux [Cu[indice inférieur 2]X[indice inférieur 2]{[mu]-Z-pTolS(CH[indice inférieur 2]CH=CHCH[indice inférieur 2])S-pTol}[indice inférieur 2]] (X = I, Br) sont formés. Dans ce cas, contrairement, aux premières structures obtenues, les couches de ces CPs sont composées de grilles incorporant des SBUs rhomboédriques Cu[indice inférieur 2] ([mu][indice inférieur 2]-X) [indice inférieur 2] dont les distances Cu···Cu sont identiques d’une couche à l’autre. Les caractérisations habituelles en photophysique et en stabilités thermiques ont été menées sur ces matériaux. De plus, des calculs théoriques ont été réalisés afin de mieux comprendre les propriétés photophysiques de ces composés. La quatrième section, i.e. le chapitre 5, traite des réactions de CuX (Br, I, Cl) sur des ligands dithioétherbutynes (1,4-bis(pTolthio)but-2-yne et 1,4-bis(benzylthio)but-2-yne. Quand CuBr réagit avec 1,4-bis(pTolthio)but-2-yne, le CP 1D [{Cu([mu][indice inférieur 2]-Br) [indice inférieur 2]Cu}([mu]-pTolSCH[indice inférieur 2]C≡CCH[indice inférieur 2]S-pTol) [indice inférieur 2]] [indice inférieur n] est obtenu, alors que le CP 2D [{Cu[indice inférieur 4] ([mu][indice inférieur 3]-I) [indice inférieur 4]}([mu]-pTolSCH[indice inférieur 2]C≡CCH[indice inférieur 2]S-pTol) [indice inférieur 2]] [indice inférieur n], préalablement reporté, est formé.(2) La réaction des sels CuI et CuCl avec 1,4-bis(benzylthio)but-2-yne engendre la formation de complexes isomorphes 0D [{Cu([mu][indice inférieur 2]-X) [indice inférieur 2]Cu}([mu]-PhCH[indice inférieur 2]SCH[indice inférieur 2]C≡CCH[indice inférieur 2]SCH[indice inférieur 2]Ph) [indice inférieur 2]] (X = I, Br). Contrairement à l’utilisation de CuCl, qui avec PhCH[indice inférieur 2]SCH[indice inférieur 2]C≡CCH[indice inférieur 2]SCH[indice inférieur 2]Ph forme le CP 2D [{Cu[indice inférieur 2] ([mu][indice inférieur 2]-Cl)([mu] [indice inférieur 3]-Cl)}([mu]-PhCH[indice inférieur 2]SCH[indice inférieur 2]C≡CCH[indice inférieur 2]SCH[indice inférieur 2]Ph)] [indice inférieur n]. Notons que ce CP présente des propriétés de photophysique peu communes pour un dérivé chloré, car il émet de la lumière autour de 600 nm. La cinquième section, i.e. le chapitre 6, traite des réactions de CuI avec PhS(CH[indice inférieur 2]) [indice inférieur 8]SPh et pTolS(CH[indice inférieur 2]) [indice inférieur 8]S-pTol qui génèrent respectivement les CPs luminescents 1D [Cu[indice inférieur 4]I[indice inférieur 4]{[mu][indice inférieur 2]-PhS(CH[indice inférieur 2]) [indice inférieur 8]SPh}[indice inférieur 2]] [indice inférieur n] et 2D [Cu8I8{[mu]2-pTolS(CH2)8S-pTol}3(MeCN)2]n. Le CP 2D [Cu8I8{[mu]2-pTolS(CH2)8S-pTol}3 (MeCN)2]n présente un réseau qui n’avait jamais été rencontré dans la littérature auparavant, c.-à-d., des couches de polymère construites à partir de deux cubanes fermés pontés ensemble par un rhomboèdre comme SBUs. Leurs propriétés physiques et de stabilités thermiques ont été étudiées et présentent quelques différences notables. La sixième section, i.e. le chapitre 7, traite des réactions entre CuI avec le ligand flexible pTolS(CH[indice inférieur 2]) [indice inférieur 8]S-pTol dans le MeCN ou EtCN et p-[indice supérieur t]BuC[indice inférieur 6]H[indice inférieur 4]S(CH[indice inférieur 2]) [indice inférieur 8]SC[indice inférieur 6]H[indice inférieur 4]-p-[indice supérieur t]Bu L2 dans EtCN. Les synthèses issues de pTolS(CH[indice inférieur 2]) [indice inférieur 8]S-pTol permettent l’obtention de CPs 2D [Cu[indice inférieur 8]I[indice inférieur 8]{pTolS(CH[indice inférieur 2]) [indice inférieur 8]S-pTol}[indice inférieur 3] (solvant) [indice inférieur 2]] [indice inférieur n] (1•MeCN et 1•EtCN) contenant des nœuds de connexion de type Cu[indice inférieur 8]I[indice inférieur 8]. Par opposition, l’utilisation du ligand p-[indice supérieur t]BuC[indice inférieur 6]H[indice inférieur 4]S(CH[indice inférieur 2]) [indice inférieur 8]SC[indice inférieur 6]H[indice inférieur 4]-p-[indice supérieur t]Bu dans EtCN entraine la formation d’un CP 1D [Cu[indice inférieur 4]I[indice inférieur 4]{p-[indice supérieur t]BuC[indice inférieur 6]H[indice inférieur 4]S(CH[indice inférieur 2]) [indice inférieur 8]SC[indice inférieur 6]H[indice inférieur 4]-p-[indice supérieur t]Bu}[indice inférieur 2] (EtCN) [indice inférieur 2]] [indice inférieur n] incorporant les SBUs de type cubane fermé. Les CPs 2D 1•MeCN et 1•EtCN, contrairement à 2•EtCN, présentent l’habilité de pouvoir perdre le solvant initialement incorporé dans leur structure sous vide et de le readsorber ou d’adsorber un autre solvant, chose qui peut être suivie à l’aide de la variation de la luminescence, la stabilité thermique, ou encore par diffraction des rayons X sur poudre. La septième section, i.e. le chapitre 8 traite des réactions, une fois encore, entre un ligand dithioéther, contenant un pont flexible butane (EtS(CH[indice inférieur 2]) [indice inférieur 4]SEt) et les sels CuX (X = I, Br). Dans ce cas, il se forme avec le CuI un CP luminescent 2D [Cu[indice inférieur 4]I[indice inférieur 4]{[mu]-EtS(CH[indice inférieur 2]) [indice inférieur 4]SEt}[indice inférieur 2]] [indice inférieur n], alors qu’il génère avec CuBr, le CP 3D [(Cu[indice inférieur 2]Br[indice inférieur 2]){[mu]-EtS(CH[indice inférieur 2]) [indice inférieur 4]SEt}][indice inférieur n] faiblement luminescent, construit sur des couches en parallèle pontées par les soufres doublement n-donneurs. Il est intéressant de remarquer qu’une migration de l’énergie d’excitation se produit dans le CP 3D (dérivé bromé) contrairement au CP 2D (dérivé iodé) sous excitation de haute intensité. Très peu d’exemples présentent ce type de processus parmi tous les CPs ( < 10). Pour conclure, les réactions entre les sels CuX (X = Cl, Br, I) avec des ligands thioéthers de types différents (mono-, di-thio, rigide ou flexible) peuvent offrir des matériaux de structures variables (CP 0D, 1D, 2D, 3D avec et sans cavités) présentant leurs propres spécificités (luminescence, stabilité thermique, adsorption de gaz, solvatochromisme, etc.). Le résultat le plus important à noter, en comparaison avec la littérature est, qu’il est très difficile, voire impossible, de pouvoir prédire la dimensionnalité, la structure et les propriétés dont résultera la coordination des ligands thioéthers sur des sels de CuX (X = Cl, Br, I). Par conséquent, de nombreuses combinaisons et études restent encore à être menées pour mieux comprendre ces matériaux et trouver la, ou les meilleures combinaisons possibles pour concevoir des MOFs luminescents à partir de CuX.

Development of Novel Time-Domain Electromagnetic Methods for Offshore Groundwater Studies: A Data Application from Bat Yam, Israel

Recent marine long-offset transient electromagnetic (LOTEM) measurements yielded the offshore delineation of a fresh groundwater body beneath the seafloor in the region of Bat Yam, Israel. The LOTEM application was effective in detecting this freshwater body underneath the Mediterranean Sea and allowed an estimation of its seaward extent. However, the measured data set was insufficient to understand the hydrogeological configuration and mechanism controlling the occurrence of this fresh groundwater discovery. Especially the lateral geometry of the freshwater boundary, important for the hydrogeological modelling, could not be resolved. Without such an understanding, a rational management of this unexploited groundwater reservoir is not possible. Two new high-resolution marine time-domain electromagnetic methods are theoretically developed to derive the hydrogeological structure of the western aquifer boundary. The first is called Circular Electric Dipole (CED). It is the land-based analogous of the Vertical Electric Dipole (VED), which is commonly applied to detect resistive structures in the subsurface. Although the CED shows exceptional detectability characteristics in the step-off signal towards the sub-seafloor freshwater body, an actual application was not carried out in the extent of this study. It was found that the method suffers from an insufficient signal strength to adequately delineate the resistive aquifer under realistic noise conditions. Moreover, modelling studies demonstrated that severe signal distortions are caused by the slightest geometrical inaccuracies. As a result, a successful application of CED in Israel proved to be rather doubtful. A second method called Differential Electric Dipole (DED) is developed as an alternative to the intended CED method. Compared to the conventional marine time-domain electromagnetic system that commonly applies a horizontal electric dipole transmitter, the DED is composed of two horizontal electric dipoles in an in-line configuration that share a common central electrode. Theoretically, DED has similar detectability/resolution characteristics compared to the conventional LOTEM system. However, the superior lateral resolution towards multi-dimensional resistivity structures make an application desirable. Furthermore, the method is less susceptible towards geometrical errors making an application in Israel feasible. In the extent of this thesis, the novel marine DED method is substantiated using several one-dimensional (1D) and multi-dimensional (2D/3D) modelling studies. The main emphasis lies on the application in Israel. Preliminary resistivity models are derived from the previous marine LOTEM measurement and tested for a DED application. The DED method is effective in locating the two-dimensional resistivity structure at the western aquifer boundary. Moreover, a prediction regarding the hydrogeological boundary conditions are feasible, provided a brackish water zone exists at the head of the interface. A seafloor-based DED transmitter/receiver system is designed and built at the Institute of Geophysics and Meteorology at the University of Cologne. The first DED measurements were carried out in Israel in April 2016. The acquired data set is the first of its kind. The measured data is processed and subsequently interpreted using 1D inversion. The intended aim of interpreting both step-on and step-off signals failed, due to the insufficient data quality of the latter. Yet, the 1D inversion models of the DED step-on signals clearly detect the freshwater body for receivers located close to the Israeli coast. Additionally, a lateral resistivity contrast is observable in the 1D inversion models that allow to constrain the seaward extent of this freshwater body. A large-scale 2D modelling study followed the 1D interpretation. In total, 425 600 forward calculations are conducted to find a sub-seafloor resistivity distribution that adequately explains the measured data. The results indicate that the western aquifer boundary is located at 3600 m - 3700 m before the coast. Moreover, a brackish water zone of 3 Omega*m to 5 Omega*m with a lateral extent of less than 300 m is likely located at the head of the freshwater aquifer. Based on these results, it is predicted that the sub-seafloor freshwater body is indeed open to the sea and may be vulnerable to seawater intrusion.

Laying the path to consumer-level immersive simulation environment

Since the end of the long winter of virtual reality (VR) at the beginning of the 2010 decade, many improvements have been made in terms of hardware technologies and software platforms performances and costs. Many expect such trend will continue, pushing the penetration rate of virtual reality headsets to skyrocket at some point in the future, just as mobile platforms did before. In the meantime, virtual reality is slowly transitioning from a specialized laboratory-only technology, to a consumer electronics appliance, opening interesting opportunities and challenges. In this transition, two interesting research questions amount to how 2D-based content and applications may benefit (or be hurt) by the adoption of 3D-based immersive environments and to how to proficiently support such integration. Acknowledging the relevance of the former, we here consider the latter question, focusing our attention on the diversified family of PC-based simulation tools and platforms. VR-based visualization is, in fact, widely understood and appreciated in the simulation arena, but mainly confined to high performance computing laboratories. Our contribution here aims at characterizing the simulation tools which could benefit from immersive interfaces, along with a general framework and a preliminary implementation which may be put to good use to support their transition from uniquely 2D to blended 2D/3D environments.

Analisi cinematica dell'articolazione della caviglia tramite risonanza magnetica dinamica

Il piede è la struttura anatomica multi-articolare che media il contatto dell’apparato muscoloscheletrico con il suolo ed è, quindi, fondamentale per la locomozione e per la maggioranza dei task motori. Per questo, l’analisi cinematica intrarticolare in-vivo del complesso piede-caviglia risulta essere di grande interesse in ambito biomeccanico e in ambito clinico. La quantificazione del moto relativo è, però, complessa a causa del numero di ossa presenti nel piede, ben 26, e alla loro distribuzione. Tali limitazioni possono essere superate ricorrendo a misure in risonanza magnetica dinamica (DMRI). Questo elaborato presenta un primo approccio esplorativo per determinare la cinematica del piede. In particolare l’analisi si è concentrata, per semplicità, sullo studio del retropiede, quindi sul moto relativo tra tibia, talo e calcagno, nel caso di flessione plantare libera, ovvero senza alcun carico applicato. Il complesso piede-caviglia è stato scansionato suddividendo il range di movimento in 13 pose statiche. Da ognuna delle 13 acquisizioni di tipo volumetrico sono state simulate delle scansioni dinamiche, in modo da ottenere una cinematica certa di riferimento, per poter valutare la precisione dell’algoritmo utilizzato. La ricostruzione della cinematica tridimensionale del complesso esaminato si è basata su un algoritmo di registrazione, composto da un primo processo di inizializzazione semiautomatico ed una successiva registrazione 2D/3D automatica basata sull’intensità dei voxel. Di particolare interesse in questa indagine è la ricostruzione dei tre moti relativi: tibia-talo, tibia-calcagno e talo-calcagno. Per valutare la precisione dell’algoritmo nella ricostruzione della cinematica è stato calcolato l’errore medio in valore assoluto tra le coordinate dei modelli nelle pose di riferimento e le coordinate fornite dal codice. I risultati ottenuti sono di notevole interesse visto il carattere esplorativo dello studio.

Inhibition of immune complex-mediated neutrophil oxidative metabolism: A pharmacophore model for 3-phenylcoumarin derivatives using GRIND-based 3D-QSAR and 2D-QSAR procedures

In this study, twenty hydroxylated and acetoxylated 3-phenylcoumarin derivatives were evaluated as inhibitors of immune complex-stimulated neutrophil oxidative metabolism and possible modulators of the inflammatory tissue damage found in type III hypersensitivity reactions. By using lucigenin- and luminol-enhanced chemiluminescence assays (CL-luc and CL-lum, respectively), we found that the 6,7-dihydroxylated and 6,7-diacetoxylated 3-phenylcoumarin derivatives were the most effective inhibitors. Different structural features of the other compounds determined CL-luc and/or CL-lum inhibition. The 2D-QSAR analysis suggested the importance of hydrophobic contributions to explain these effects. In addition, a statistically significant 3D-QSAR model built applying GRIND descriptors allowed us to propose a virtual receptor site considering pharmacophoric regions and mutual distances. Furthermore, the 3-phenylcoumarins studied were not toxic to neutrophils under the assessed conditions. (C) 2007 Elsevier Masson SAS. All rights reserved.

Results of high dose-rate brachytherapy boost before 2D or 3D external beam irradiation for prostate cancer

Background and purpose: To evaluate biochemical control and treatment related toxicity of patients with localized adenocarcinoma of the prostate treated with high dose-rate brachytherapy (HDRB) combined with conventional 2D or 3D-conformal external beam irradiation (EBI). Material and methods: Four-hundred and three patients treated between December 2000 and March 2004. HDRB was delivered with three fractions of 5.5-7 Gy with a single implant, followed by 45 Gy delivered with 2D or 3D conformal EBI. Results: The median follow-up was 48.4 months. Biochemical failure (BF) occurred in 9.6% according to both ASTRO and Phoenix consensus criteria. Mean time to relapse was 13 and 26 months, respectively. The 5-year BF free survival using the ASTRO criteria was 94.3%, 86.9% and 86.6% for the low, intermediate and high risk groups, respectively; using Phoenix criteria, 92.4%, 88.0% and 85.3%, respectively. The only predictive factor of BF in the multivariate analysis by both ASTRO and Phoenix criteria was the presence of prostate nodules detected by digital palpation, and patients younger than 60 years presented a higher chance of failure using Phoenix criteria only. Conclusions: Treatment scheme is feasible and safe with good efficacy. (C) 2011 Elsevier Ireland Ltd All rights reserved. Radiotherapy and Oncology 98 (2011) 169-174

Assessment of Laparoscopic Skills Performance: 2D Versus 3D Vision and Classic Instrument Versus New Hand-Held Robotic Device for Laparoscopy

Introduction and Objectives. Laparoscopic surgery has undeniable advantages, such as reduced postoperative pain, smaller incisions, and faster recovery. However, to improve surgeons’ performance, ergonomic adaptations of the laparoscopic instruments and introduction of robotic technology are needed. The aim of this study was to ascertain the influence of a new hand-held robotic device for laparoscopy (HHRDL) and 3D vision on laparoscopic skills performance of 2 different groups, naïve and expert. Materials and Methods. Each participant performed 3 laparoscopic tasks—Peg transfer, Wire chaser, Knot—in 4 different ways. With random sequencing we assigned the execution order of the tasks based on the first type of visualization and laparoscopic instrument. Time to complete each laparoscopic task was recorded and analyzed with one-way analysis of variance. Results. Eleven experts and 15 naïve participants were included. Three-dimensional video helps the naïve group to get better performance in Peg transfer, Wire chaser 2 hands, and Knot; the new device improved the execution of all laparoscopic tasks (P < .05). For expert group, the 3D video system benefited them in Peg transfer and Wire chaser 1 hand, and the robotic device in Peg transfer, Wire chaser 1 hand, and Wire chaser 2 hands (P < .05). Conclusion. The HHRDL helps the execution of difficult laparoscopic tasks, such as Knot, in the naïve group. Three-dimensional vision makes the laparoscopic performance of the participants without laparoscopic experience easier, unlike those with experience in laparoscopic procedures.

Amygdala activation in response to 2D and 3D emotion-inducing stimuli

Studying changes in brain activation according to the valence of emotion-inducing stimuli is essential in the research on emotions. Due to the ecological potential of virtual reality, it is also important to examine whether brain activation in response to emotional stimuli can be modulated by the three-dimensional (3D) properties of the images. This study uses functional Magnetic Resonance Imaging to compare differences between 3D and standard (2D) visual stimuli in the activation of emotion-related brain areas. The stimuli were organized in three virtual-reality scenarios, each with a different emotional valence (pleasant, unpleasant and neutral). The scenarios were presented in a pseudo-randomized order in the two visualization modes to twelve healthy males. Data were analyzed through a GLM-based fixed effects procedure. Unpleasant and neutral stimuli activated the right amygdala more strongly when presented in 3D than in 2D. These results suggest that 3D stimuli, when used as “building blocks” for virtual environments, can induce increased emotional loading, as shown here through neuroimaging.

Comparação entre a ecocardiografia 2D e 3D na avaliação do remodelamento reverso após a TRC

FUNDAMENTO: A ecocardiografia consiste em método muito útil para seleção e avaliação de resposta à terapia de ressincronização cardíaca (TRC). O eco 3D já tem seu papel estabelecido na avaliação dos volumes ventriculares e fração de ejeção ventricular esquerda (FEVE) com excelente correlação de resultados quando comparado à RNM. OBJETIVO: Comparar a avaliação dos volumes ventriculares (VDVE, VSVE), FEVE e massa do VE antes e após a TRC pela ecocardiografia bi (Eco 2D) e tridimensional (Eco 3D). MÉTODOS: Foram avaliados 24 pacientes com IC CFIII ou IV (NYHA), ritmo sinusal QRS > 150 ms, em vigência de terapêutica otimizada para IC submetidos a TRC. Foram realizados eletrocardiograma (ECG), avaliação clínica, Eco 2D e 3D antes, três e seis meses após a TRC. A comparação entre as técnicas foi realizada utilizando-se a correlação de Pearson (r). RESULTADOS: No momento basal, a correlação entre os métodos foi de 0,96 para avaliação do VDVE, 0,95 para avaliação do VSVE, 0,87 para FEVE, e 0,72 para massa do VE. Após três meses da TRC, a correlação entre os métodos para análise do VDVE foi de 0,96, 0,95 para VSVE, 0,95 para FEVE, e 0,77 para massa do VE. Após seis meses da TRC, a correlação entre o Eco 2D e 3D para análise do VDVE foi de 0,98, 0,91 para VSVE, 0,96 para FEVE, e 0,85 para massa do VE. CONCLUSÃO: Neste estudo foi observada redução dos VDVE,VSVE, além de melhora da FEVE após a TRC. Houve excelente correlação entre o Eco 2D e o 3D para avaliação dos volumes ventriculares e FEVE, e boa correlação entre os métodos para avaliação da massa ventricular esquerda antes e após a TRC.

Extraction of topological structures in 2D and 3D vector fields

feature extraction, feature tracking, vector field visualization

Trabecular bone score (TBS) the new parameter of 2D texture analysis for the evaluation of 3D bone micro architecture status

X-ray is a technology that is used for numerous applications in the medical field. The process of X-ray projection gives a 2-dimension (2D) grey-level texture from a 3- dimension (3D) object. Until now no clear demonstration or correlation has positioned the 2D texture analysis as a valid indirect evaluation of the 3D microarchitecture. TBS is a new texture parameter based on the measure of the experimental variogram. TBS evaluates the variation between 2D image grey-levels. The aim of this study was to evaluate existing correlations between 3D bone microarchitecture parameters - evaluated from μCT reconstructions - and the TBS value, calculated on 2D projected images. 30 dried human cadaveric vertebrae were acquired on a micro-scanner (eXplorer Locus, GE) at isotropic resolution of 93 μm. 3D vertebral body models were used. The following 3D microarchitecture parameters were used: Bone volume fraction (BV/TV), Trabecular thickness (TbTh), trabecular space (TbSp), trabecular number (TbN) and connectivity density (ConnD). 3D/2D projections has been done by taking into account the Beer-Lambert Law at X-ray energy of 50, 100, 150 KeV. TBS was assessed on 2D projected images. Correlations between TBS and the 3D microarchitecture parameters were evaluated using a linear regression analysis. Paired T-test is used to assess the X-ray energy effects on TBS. Multiple linear regressions (backward) were used to evaluate relationships between TBS and 3D microarchitecture parameters using a bootstrap process. BV/TV of the sample ranged from 18.5 to 37.6% with an average value at 28.8%. Correlations' analysis showedthat TBSwere strongly correlatedwith ConnD(0.856≤r≤0.862; p<0.001),with TbN (0.805≤r≤0.810; p<0.001) and negatively with TbSp (−0.714≤r≤−0.726; p<0.001), regardless X-ray energy. Results show that lower TBS values are related to "degraded" microarchitecture, with low ConnD, low TbN and a high TbSp. The opposite is also true. X-ray energy has no effect onTBS neither on the correlations betweenTBS and the 3Dmicroarchitecture parameters. In this study, we demonstrated that TBS was significantly correlated with 3D microarchitecture parameters ConnD and TbN, and negatively with TbSp, no matter what X-ray energy has been used. This article is part of a Special Issue entitled ECTS 2011. Disclosure of interest: None declared.

Functional calibration procedure for 3D knee joint angle description using inertial sensors.

Measurement of three-dimensional (3D) knee joint angle outside a laboratory is of benefit in clinical examination and therapeutic treatment comparison. Although several motion capture devices exist, there is a need for an ambulatory system that could be used in routine practice. Up-to-date, inertial measurement units (IMUs) have proven to be suitable for unconstrained measurement of knee joint differential orientation. Nevertheless, this differential orientation should be converted into three reliable and clinically interpretable angles. Thus, the aim of this study was to propose a new calibration procedure adapted for the joint coordinate system (JCS), which required only IMUs data. The repeatability of the calibration procedure, as well as the errors in the measurement of 3D knee angle during gait in comparison to a reference system were assessed on eight healthy subjects. The new procedure relying on active and passive movements reported a high repeatability of the mean values (offset<1 degrees) and angular patterns (SD<0.3 degrees and CMC>0.9). In comparison to the reference system, this functional procedure showed high precision (SD<2 degrees and CC>0.75) and moderate accuracy (between 4.0 degrees and 8.1 degrees) for the three knee angle. The combination of the inertial-based system with the functional calibration procedure proposed here resulted in a promising tool for the measurement of 3D knee joint angle. Moreover, this method could be adapted to measure other complex joint, such as ankle or elbow.

Pre-procés i segmentació en imatges d’ultrasons 2D i 3D de la pròstata

Aquest projecte s'ha dut a terme amb el Grup de visió per computador del departamentd'Arquitectura i Tecnologia de Computadors (ATC) de la Universitat de Girona. Està enfocat a l'anàlisi d'imatges mèdiques, en concret s'analitzaran imatges de pròstata en relació a desenvolupaments que s'estan realitzant en el grup de visió esmentat. Els objectius fixats per aquest projecte són desenvolupar dos mòduls de processamentm d'imatges els quals afrontaran dos blocs important en el tractament d'imatges, aquests dos mòduls seran un pre-processat d'imatges, que constarà de tres filtres i un bloc de segmentació per tal de cercar la pròstata dintre de les imatges a tractar. En el projecte es treballarà amb el llenguatge de programació C++, concretament amb unes llibreries que es denominen ITK (Insight Toolkit ) i són open source enfocades al tractament d'imatges mèdiques. A part d'aquesta eina s'utilitzaran d'altres com les Qt que és una biblioteca d'eines per crear entorns gràfics