Proprieta elettriche e ottiche di film di ge impiantati con sn.

In questo lavoro di tesi vengono studiate le proprietà ottiche ed elettriche di film sottili di germanio, impiantati con ioni stagno. I campioni, realizzati tramite tecnica CVD (\emph{Chemical Vapor Deposition}), sono stati realizzati in condizioni operative differenti, il che ha permesso di ottenere materiali con proprietà strutturali e fisiche diverse. Si è posta particolare attenzione alla presenza di strutture nanoporose, presenti in alcuni di questi campioni, che possono dar vita ad effetti di confinamento quantico, associato ad uno spostamento dell'energy gap rispetto al materiale bulk. Le analisi sono state effettuate sia tramite misure SPV (\emph{Surface Photovoltage}), che hanno permesso di indagare le proprietà ottiche, sia tramite tecnica IV (\emph{corrente-tensione}), volta ad evidenziare le proprietà elettriche dei diversi campioni. I risultati ottenuti sono, infine, stati confrontati con un campione di riferimento di film di germanio non impiantato, mettendone in luce le differenze strutturali e fisiche. Lo studio di questo materiale, oltre ad avere un'importanza di carattere fondamentale, è di interesse anche per le possibili ricadute applicative. Infatti, i materiali nanoporosi possono essere impiegati in vari campi, come ad esempio nell'elettronica, nello sviluppo di pannelli fotovoltaici e nella purificazione di gas e liquidi.

Einzelmolekülspektroskopie an einer homologen Reihe von Rylendiimiden und an einem bichromophoren Modellsystem für elektronischen Energietransfer

In dieser Arbeit wurden Untersuchungen zur Fluoreszenzdynamik und zum Mechanismus des Photobleichens einzelner Farbstoffmoleküle einer homologen Reihe von Rylentetracarbonsäurediimiden durchgeführt. Mit der Erweiterung des elektronischen π-Systems verringert sich die HOMO/LUMO-Energiedifferenz, so dass strahlungslose Relaxationsprozesse gemäß des Energielückengesetzes zunehmen. Die konfokale Einzelmolekülspektroskopie in Kombination mit zeitkorrelierter Einzelphotonenzählung ermöglicht es, Fluktuationen der inneren Konversionsrate zu detektieren. Der limitierende Faktor jedes Einzelmolekülexperiments ist die Photostabilität der Moleküle. Für die homologe Reihe konnten mindestens zwei Photobleichmechanismen identifiziert werden. Wenn Singulett-Sauerstoff durch Selbstsensibilisierung erzeugt werden kann, ist unter Luft die Photooxidation der wahrscheinlichste Mechanismus. Unter Ausschluss von Luftsauerstoff spielt die Bildung langlebiger Dunkelzustände eine entscheidende Rolle, die bevorzugt über höher angeregte Triplett- und Singulett-Zustände abläuft. Es wird angenommen, dass es sich hierbei um einen reversiblen Ionisierungsprozess handelt, bei dem das Radikal-Kation der Rylendiimide gebildet wird. Es konnte gezeigt werden, dass durch eine geeignete Wahl der Anregungsbedingungen die Dunkelzustandspopulierung verhindert und zugleich die Photostabilität der Fluorophore deutlich erhöht wird. Durch die Verknüpfung der beiden niedrigsten Homologen erhält man ein Donor-Akzeptor-Modellsystem, bei dem die Anregungsenergie mit hoher Effizienz vom Donor- auf den Akzeptor-Chromophor übertragen wird. In der Fluoreszenz einzelner Bichromophore wurden bei selektiver Anregung des Donors kollektive Auszeiten beobachtet, die durch effiziente Singulett-Triplett-Annihilation verursacht werden.

Sintesi e caratterizzazione di oligo e politiofeni tioalchil sostituiti per applicazioni fotovoltaiche

Nell'ultimo decennio sono stati sviluppati numerosi materiali π-coniugati contenenti unità tiofeniche per applicazioni in dispositivi organici a film sottile. Nel campo delle celle solari, la possibilità di creare dispositivi basati sull’utilizzo di materiali organici, rispetto ai dispositivi attualmente in commercio a base di silicio, ha suscitato grande interesse soprattutto per la possibilità di realizzare dispositivi su larga area con basso costo di produzione e su substrati flessibili. Gli oligo- e i politiofeni sono eccellenti candidati grazie alle ottime proprietà di trasporto di carica e alle caratteristiche di assorbimento di luce. In celle solari di tipo Bulk-Heterojunction (BHJ), ad esempio, il poli(3-esiltiofene) è uno tra i materiali più studiati. Ad oggi, con il P3HT sono state raggiunte efficienze certificate superiori all’8%, variando sia parametri dipendenti dalla struttura molecolare, come ad esempio il peso molecolare, la regioregolarità delle catene alchiliche, il grado di polidispersità, il grado di polimerizzazione, sia parametri da cui dipende l’organizzazione della blend donatore-accettore. Per superare l’efficienza di conversione ottenuta con i polimeri classici come il P3HT è necessario progettare e sintetizzare materiali con precise caratteristiche: basso energy gap per aumentare l’assorbimento di luce, elevata mobilità di carica per avere una rapida estrazione delle cariche, posizione ottimale degli orbitali di frontiera per garantire una efficiente dissociazione dell’eccitone ed infine buona solubilità per migliorare la processabilità. Il presente lavoro di tesi si è articolato nei seguenti punti: sintesi di oligo- e politiofeni tioalchil sostituiti con inserzione di unità benzotiadiazolo per massimizzare l’assorbimento ed abbassare il gap energetico; studio dell’effetto della ramificazione del gruppo tioalchilico sull’organizzazione supramolecolare allo stato solido e successiva ottimizzazione della morfologia del film solido variando metodi di deposizione e solventi; applicazione degli oligomeri e dei polimeri sintetizzati come materiali donatori in celle fotovoltaiche di tipo Bulk-Heterojunction in presenza di fenil-C61-butirrato di metile (PCBM) come materiale accettore.

Proprietà ottiche di film sottili a base di silicio per applicazioni fotovoltaiche

Questa tesi ha come obiettivo quello di misurare la dipendenza spettrale di alcune proprietà ottiche, come trasmittanza e riflettanza, al fine di ricavare l’energy gap di film sottili costituiti da nanocrystalline silicon oxynitride (nc-SiOxNy) per applicazioni in celle solari HIT (Heterojunction Intrinsic Thin layer). Questi campioni sono stati depositati presso l’Università di Konstanz (Germania) tramite tecnica PECVD (Plasma-Enhanced Chemical Vapor Deposition). Questo materiale risulta ancora poco conosciuto per quanto riguarda le proprietà optoelettroniche e potrebbe presentare una valida alternativa a silicio amorfo (a-Si) e ossido di silicio idrogenato amorfo (a-SiOx:H) che sono attualmente utilizzati in questo campo. Le misure sono state effettuate presso i laboratori del Dipartimento di Fisica e Astronomia, settore di Fisica della Materia, dell’Università di Bologna. I risultati ottenuti mostrano che i campioni che non hanno subito alcun trattamento termico (annealing) presentano un energy gap che cresce linearmente rispetto alla diluizione di protossido di azoto in percentuale. Nei campioni analizzati sottoposto ad annealing a 800°C si è osservato un aumento dell’Eg dopo il trattamento. Un risultato ottimale consiste in un gap energetico maggiore di quello del silicio amorfo (a-Si) e del silicio amorfo idrogenato (a-Si:H), attualmente utilizzati in questa tipologia di celle, per evitare che questo layer assorba la luce solare che deve invece essere trasmessa al silicio sottostante. Per questo motivo i valori ottenuti risultano molto promettenti per future applicazioni fotovoltaiche.

Misure di trasmittanza ottica di nanoparticelle di Ti(1-x)V(x)O(2)

Negli ultimi tempi sta assumendo grande importanza la ricerca sulla produzione di idrogeno dall’acqua tramite celle foto-elettrolitiche. In questa tesi vengono descritte le analisi condotte su un materiale che può essere coinvolto in questa applicazione: il TiO2 drogato con atomi di V. In particolare è stato valutato l’effetto del drogaggio sull’energy gap tramite misure di trasmittanza ottica effettuate in laboratorio su campioni con diverse concentrazioni di V e trattati termicamente a varie temperature. Nel primo capitolo vengono descritte le caratteristiche dei semiconduttori legate all’ottica, soffermandosi in particolare sul TiO2. Nel secondo capitolo sono illustrati l’apparato e il metodo sperimentale; viene inoltre fornita una descrizione dettagliata dei campioni analizzati. Nel terzo capitolo vengono esposti i risultati delle analisi dei dati.

Temperatur- und ortsabhängige Zustandsdichte des organischen Supraleiters Kappa-(BEDT-TTF) 2 Cu[N(CN) 2]Br

Im Rahmen dieser Arbeit wurde die temperatur- und ortsabhängige Zustandsdichte des organischen Supraleiters kappa-(BEDT-TTF)2Cu[N(CN)2]Br mit Rastertunnelspektroskopie bei tiefen Temperaturen untersucht.rnZusätzlich zur bereits bekannten supraleitenden Energielücke wird dabei eine logarithmische Unterdrückung der Zustandsdichte an der Fermikante beobachtet, die auch oberhalb der kritischen Temperatur erhalten bleibt. In der vorliegenden Arbeit wird gezeigt, dass sich dieses Verhalten durch ein für ungeordnete elektronische Systeme entwickeltes Modell unter Berücksichtigung von Coulomb-Wechselwirkungen beschreiben lässt. Die daraus resultierenden Fluktuationen der elektronischen Struktur führen zu einer Verbreiterung der gemessenen supraleitenden Energielücke, die sich durch sehr kleine Kohärenzmaxima im entsprechenden Quasiteilchenanregungsspektrum äußert. Dieses Verhalten wurde bereits beobachtet, konnte jedoch bisher nicht erklärt werden. Die theoretische Beschreibung der logarithmischen Unterdrückung trägt somit zusätzlich zum Verständnis des supraleitenden Beitrags bei, sodass die gesamte Zustandsdichte vollständig beschrieben werden kann. Die Analyse der gemessenen supraleitenden Energielücke wurde für verschiedene Symmetrien des Ordnungsparameters durchgeführt, wobei die beste Übereinstimmung für die Annahme einer d-wellenartigen Symmetrie mit zwei unterschiedlich stark ausgeprägten Energielücken gefunden wurde. Der Paarbildungsmechanismus, der zur Bindung zweier Elektronen zu einem Cooper-Paar führt, kann mit einer $d$-wellenartigen Symmetrie nicht durch die in konventionellen Supraleitern gefundene Elektron-Phonon-Kopplung erklärt werden. Stattdessen wird in Analogie zur Hochtemperatur-Supraleitung eine durch antiferromagnetische Spin-Wechselwirkungen induzierte Kopplung der Elektronen vermutet. Dies wird zum einen durch die oberhalb der kritischen Temperatur auftretende, zweite Energielücke und zum anderen durch die zwischen 4,66 und 5,28 liegende Kopplungsstärke 2Delta/(kB Tc) unterstützt, die deutlich größer als für konventionelle Supraleiter mit Elektron-Phonon-Kopplung ist.

Tuning of magnetic exchange interactions between organic radicals through bond and space

The dissertation entitled "Tuning of magnetic exchange interactions between organic radicals through bond and space" comprises eight chapters. In the initial part of chapter 1, an overview of organic radicals and their applications were discussed and in the latter part motivation and objective of thesis was described. As the EPR spectroscopy is a necessary tool to study organic radicals, the basic principles of EPR spectroscopy were discussed in chapter 2. rnAntiferromagnetically coupled species can be considered as a source of interacting bosons. Consequently, such biradicals can serve as molecular models of a gas of magnetic excitations which can be used for quantum computing or quantum information processing. Notably, initial small triplet state population in weakly AF coupled biradicals can be switched into larger in the presence of applied magnetic field. Such biradical systems are promising molecular models for studying the phenomena of magnetic field-induced Bose-Einstein condensation in the solid state. To observe such phenomena it is very important to control the intra- as well as inter-molecular magnetic exchange interactions. Chapters 3 to 5 deals with the tuning of intra- and inter-molecular exchange interactions utilizing different approaches. Some of which include changing the length of π-spacer, introduction of functional groups, metal complex formation with diamagnetic metal ion, variation of radical moieties etc. During this study I came across two very interesting molecules 2,7-TMPNO and BPNO, which exist in semi-quinoid form and exhibits characteristic of the biradical and quinoid form simultaneously. The 2,7-TMPNO possesses the singlet-triplet energy gap of ΔEST = –1185 K. So it is nearly unrealistic to observe the magnetic field induced spin switching. So we studied the spin switching of this molecule by photo-excitation which was discussed in chapter 6. The structural similarity of BPNO with Tschitschibabin’s HC allowed us to dig the discrepancies related to ground state of Tschitschibabin’s hydrocarbon(Discussed in chapter 7). Finally, in chapter 8 the synthesis and characterization of a neutral paramagnetic HBC derivative (HBCNO) is discussed. The magneto liquid crystalline properties of HBCNO were studied by DSC and EPR spectroscopy.rn

Pyrene derivatives as donors and acceptors

Pyrene derivatives as donors and acceptorsrnrnAlmost 200 years have passed since pyrene was first discovered, and to this day it garners unbroken interest by chemists around the world. One of the most fascinating areas of pyrene chemistry is its selective functionalization, since it is still currently a challenge to specifically functionalize different positions on the molecule.[1]rnIn this work, two new patterns of pyrene substitution have been developed. Under suitable conditions, a fourfold bromination of 4,5,9,10 tetramethoxypyrene is possible to yield eightfold functionalized pyrenes. Based on these molecules a novel series of 1,3,4,5,6,8,9,10-substituted pyrene derivatives was achieved. Synthetic approaches to a non-quinoidal, strong pyrene-4,5,9,10-tetraone based acceptor have been discussed. It emerged that the chosen synthetic approach is suitable for intermediate acceptors, yet it failed very electron deficient pyrene derivatives. Donors based on 4,5,9,10-tetramethoxypyrene (2,7- and 1,3,6,8-substitued) have been prepared and studied as CT complexes. In the SFB/TR 49 these complexes were analyzed in the solid state. For the first time charge transfer in a non-TTF CT-complex was studied by HAXPES and NEXAFS.rnBased on the works of ZÖPHEL et al.[2] it was possible to obtain an asymmetric 4,9,10 substituted pyrene derivative. This was used as a building block to prepare a non-planar acceptor molecule as well as electron-rich rylene-type molecules. rnFinally, two separate series of molecules intended as emitters for OLEDs were presented. Thermally activated delayed fluorescence (TADF) in OLEDs attracted significant academic interest as it is considered a promising approach to improve the efficiency of fluorescent OLEDs.[3] Our molecules were designed to have a deep blue emission spectrum and a minimal singlet triplet energy gap (∆ES1->T1) while retaining a high fluorescence quantum yield ϕPL. The initial OD series has a small ∆ES1->T1, yet had an insufficient ϕPL for the use in OLEDs. The Py series emitters, in contrast, combine both desired properties and were successfully implemented in efficient OLED devices.rn[1]. T. M. Figueira-Duarte and K. Müllen, Chem. Rev., 2011, 111, 7260-7314.rn[2]. L. Zöphel, V. Enkelmann and K. Müllen, Org. Lett., 2013, 15, 804-807.rn[3]. H. Uoyama, K. Goushi, K. Shizu, H. Nomura and C. Adachi, Nature, 2012, 492, 234-238.

Morphological and optical properties of SiON thin films for photovoltaic applications

In the last years technologies related to photovoltaic energy have rapidly developed and the interest on renewable energy power source substantially increased. In particular, cost reduction and appropriate feed-in tariff contributed to the increase of photovoltaic installation, especially in Germany and Italy. However, for several technologies, the observed experimental efficiency of solar cells is still far from the theoretical maximum efficiency, and thus there is still room for improvement. In this framework the research and development of new materials and new solar devices is mandatory. In this thesis the morphological and optical properties of thin films of nanocrystalline silicon oxynitride (nc-SiON) have been investigated. This material has been studied in view of its application in Si based heterojunction solar cells (HIT). Actually, a-Si:H is used now in these cells as emitter layer. Amorphous SiO_x N_y has already shown excellent properties, such as: electrical conductivity, optical energy gap and transmittance higher than the ones of a-Si:H. Nc-SiO_x N_y has never been investigated up to now, but its properties can surpass the ones of amorphous SiON. The films of nc-SiON have been deposited at the University of Konstanz (Germany). The properties of these films have been studied using of atomic force microscopy and optical spectroscopy methods. This material is highly complex as it is made by different coexisting phases. The main purpose of this thesis is the development of methods for the analyses of morphological and optical properties of nc-SiON and the study of the reliability of those methods to the measurement of the characteristics of these silicon films. The collected data will be used to understand the evolution of the properties of nc-SiON, as a function of the deposition parameters. The results here obtained show that nc-SiON films have better properties with respect to both a-Si:H and a-SiON, i. e. higher optical band-gap and transmittance. In addition, the analysis of the variation of the observed properties as a function of the deposition parameters allows for the optimization of deposition conditions for obtaining optimal efficiency of a HIT cell with SiON layer.

Realizzazione di un amplificatore lock-in digitale

Tra tutte le tecniche sviluppate per il recupero di segnali, i metodi basati sul principio di rilevazione sincrona, utilizzati dagli amplificatori lock-in, sono largamente i più usati in tutti i campi della ricerca scientifica. Gli amplificatori lock-in sono strumenti utilizzati per rilevare e misurare segnali in ambienti in cui il rumore di fondo può essere di diversi ordini di grandezza più grande del segnale che si intende misurare. In questo lavoro viene presentato un metodo per realizzare un amplificatore lock-in digitale su scheda hardware NI ELVIS II+ e software LabVIEW. In seguito viene descritto come, attraverso test opportuni, sono state analizzate le performance del sistema realizzato e sono state confrontate con i sistemi disponibili commercialmente. Infine, l’amplificatore lock-in realizzato è stato poi utilizzato in un esperimento di misura spettroscopica dell’energia di gap di un campione di Germanio per mezzo dell’effetto fotoelettrico interno.

Structure and properties of graphene nano disks (GND) with and without edge-dopants

Graphene is one of the most important materials. In this research, the structures and properties of graphene nano disks (GND) with a concentric shape were investigated by Density Functional Theory (DFT) calculations, in which the most effective DFT methods - B3lyp and Pw91pw91 were employed. It was found that there are two types of edges - Zigzag and Armchair in concentric graphene nano disks (GND). The bond length between armchair-edge carbons is much shorter than that between zigzag-edge carbons. For C24 GND that consists of 24 carbon atoms, only armchair edge with 12 atoms is formed. For a GND larger than the C24 GND, both armchair and zigzag edges co-exist. Furthermore, when the number of carbon atoms in armchair-edge are always 12, the number of zigzag-edge atoms increases with increasing the size of a GND. In addition, the stability of a GND is enhanced with increasing its size, because the ratio of edge-atoms to non-edge-atoms decreases. The size effect of a graphene nano disk on its HOMO-LUMO energy gap was evaluated. C6 and C24 GNDs possess HOMO-LUMO gaps of 1.7 and 2.1eV, respectively, indicating that they are semi-conductors. In contrast, C54 and C96 GNDs are organic metals, because their HOMO-LUMO gaps are as low as 0.3 eV. The effect of doping foreign atoms to the edges of GNDs on their structures, stabilities, and HOMO-LUMO energy gaps were also examined. When foreign atoms are attached to the edge of a GND, the original unsaturated carbon atoms become saturated. As a result, both of the C-C bonds lengths and the stability of a GND increase. Furthermore, the doping effect on the HOMO-LUMO energy gap is dependent on the type of doped atoms. The doping H, F, or OH into the edge of a GND increases its HOMO-LUMO energy gap. In contrast, a Li-doped GND has a lower HOMO-LUMO energy gap than that without doping. Therefore, Li-doping can increase the electrical conductance of a GND, whereas H, F, or OH-doping decreases its conductance.

PROPERTIES AND STRUCTURES OF Li-N BASED HYDROGEN STORAGE MATERIALS

Traditional transportation fuel, petroleum, is limited and nonrenewable, and it also causes pollutions. Hydrogen is considered one of the best alternative fuels for transportation. The key issue for using hydrogen as fuel for transportation is hydrogen storage. Lithium nitride (Li3N) is an important material which can be used for hydrogen storage. The decompositions of lithium amide (LiNH2) and lithium imide (Li2NH) are important steps for hydrogen storage in Li3N. The effect of anions (e.g. Cl-) on the decomposition of LiNH2 has never been studied. Li3N can react with LiBr to form lithium nitride bromide Li13N4Br which has been proposed as solid electrolyte for batteries. The decompositions of LiNH2 and Li2NH with and without promoter were investigated by using temperature programmed decomposition (TPD) and X-ray diffraction (XRD) techniques. It was found that the decomposition of LiNH2 produced Li2NH and NH3 via two steps: LiNH2 into a stable intermediate species (Li1.5NH1.5) and then into Li2NH. The decomposition of Li2NH produced Li, N2 and H2 via two steps: Li2NH into an intermediate species --- Li4NH and then into Li. The kinetic analysis of Li2NH decomposition showed that the activation energies are 533.6 kJ/mol for the first step and 754.2 kJ/mol for the second step. Furthermore, XRD demonstrated that the Li4NH, which was generated in the decomposition of Li2NH, formed a solid solution with Li2NH. In the solid solution, Li4NH possesses a similar cubic structure as Li2NH. The lattice parameter of the cubic Li4NH is 0.5033nm. The decompositions of LiNH2 and Li2NH can be promoted by chloride ion (Cl-). The introduction of Cl- into LiNH2 resulted in the generation of a new NH3 peak at low temperature of 250 °C besides the original NH3 peak at 330 °C in TPD profiles. Furthermore, Cl- can decrease the decomposition temperature of Li2NH by about 110 °C. The degradation of Li3N was systematically investigated with techniques of XRD, Fourier transform infrared (FT-IR) spectroscopy, and UV-visible spectroscopy. It was found that O2 could not affect Li3N at room temperature. However, H2O in air can cause the degradation of Li3N due to the reaction between H2O and Li3N to LiOH. The produced LiOH can further react with CO2 in air to Li2CO3 at room temperature. Furthermore, it was revealed that Alfa-Li3N is more stable in air than Beta-Li3N. The chemical stability of Li13N4Br in air has been investigated by XRD, TPD-MS, and UV-vis absorption as a function of time. The aging process finally leads to the degradation of the Li13N4Br into Li2CO3, lithium bromite (LiBrO2) and the release of gaseous NH3. The reaction order n = 2.43 is the best fitting for the Li13N4Br degradation in air reaction. Li13N4Br energy gap was calculated to be 2.61 eV.

The Domestic Natural Gas Shortage in China

This thesis analyzes the domestic shortage in the Chinese natural gas market. Both the domestic supply and demand of natural gas are growing fast in China. However, the supply cannot catch up with the demand. Under the present pricing mechanism, the Chinese natural gas market cannot get the equilibrium by itself. Expensive imports are inadequate to fill the increasing gap between the domestic demand and supply. Therefore, the shortage problem occurs. Since the energy gap can result in the arrested development of economics, the shortage problem need to be solved. This thesis gives three suggestions to solve the problem: the use of Unconventional Gas, Natural Gas Storage and Pricing Reform.

Excitonic Splitting, Delocalization, and Vibronic Quenching in the Benzonitrile Dimer

The excitonic S1/S2 state splitting and the localization/delocalization of the S1 and S2 electronic states are investigated in the benzonitrile dimer (BN)2 and its 13C and d5 isotopomers by mass-resolved two-color resonant two-photon ionization spectroscopy in a supersonic jet, complemented by calculations. The doubly hydrogen-bonded (BN-h5)2 and (BN-d5)2 dimers are C2h symmetric with equivalent BN moieties. Only the S0 → S2 electronic origin is observed, while the S0 → S1 excitonic component is electric-dipole forbidden. A single 12C/13C or 5-fold h5/d5 isotopic substitution reduce the dimer symmetry to Cs, so that the heteroisotopic dimers (BN)2-(h5 – h513C), (BN)2-(h5 – d5), and (BN)2-(h5 – h513C) exhibit both S0 → S1 and S0 → S2 origins. Isotope-dependent contributions Δiso to the excitonic splittings arise from the changes of the BN monomer zero-point vibrational energies; these range from Δiso(12C/13C) = 3.3 cm–1 to Δiso(h5/d5) = 155.6 cm–1. The analysis of the experimental S1/S2 splittings of six different isotopomeric dimers yields the S1/S2 exciton splitting Δexc = 2.1 ± 0.1 cm–1. Since Δiso(h5/d5) ≫ Δexc and Δiso(12C/13C) > Δexc, complete and near-complete exciton localization occurs upon 12C/13C and h5/d5 substitutions, respectively, as diagnosed by the relative S0 → S1 and S0 → S2 origin band intensities. The S1/S2 electronic energy gap of (BN)2 calculated by the spin-component scaled approximate second-order coupled-cluster (SCS-CC2) method is Δelcalc = 10 cm–1. This electronic splitting is reduced by the vibronic quenching factor Γ. The vibronically quenched exciton splitting Δelcalc·Γ = Δvibroncalc = 2.13 cm–1 is in excellent agreement with the observed splitting Δexc = 2.1 cm–1. The excitonic splittings can be converted to semiclassical exciton hopping times; the shortest hopping time is 8 ps for the homodimer (BN-h5)2, the longest is 600 ps for the (BN)2(h5 – d5) heterodimer.

Self-assembled MgxZn1−xO quantum dots (0 ≤ x ≤ 1) on different substrates using spray pyrolysis methodology

By using the spray pyrolysis methodology in its classical configuration we have grown self-assembled MgxZn1−xO quantum dots (size [similar]4–6 nm) in the overall range of compositions 0 ≤ x ≤ 1 on c-sapphire, Si (100) and quartz substrates. Composition of the quantum dots was determined by means of transmission electron microscopy-energy dispersive X-ray analysis (TEM-EDAX) and X-ray photoelectron spectroscopy. Selected area electron diffraction reveals the growth of single phase hexagonal MgxZn1−xO quantum dots with composition 0 ≤ x ≤ 0.32 by using a nominal concentration of Mg in the range 0 to 45%. Onset of Mg concentration about 50% (nominal) forces the hexagonal lattice to undergo a phase transition from hexagonal to a cubic structure which resulted in the growth of hexagonal and cubic phases of MgxZn1−xO in the intermediate range of Mg concentrations 50 to 85% (0.39 ≤ x ≤ 0.77), whereas higher nominal concentration of Mg ≥ 90% (0.81 ≤ x ≤ 1) leads to the growth of single phase cubic MgxZn1−xO quantum dots. High resolution transmission electron microscopy and fast Fourier transform confirm the results and show clearly distinguishable hexagonal and cubic crystal structures of the respective quantum dots. A difference of 0.24 eV was detected between the core levels (Zn 2p and Mg 1s) measured in quantum dots with hexagonal and cubic structures by X-ray photoemission. The shift of these core levels can be explained in the frame of the different coordination of cations in the hexagonal and cubic configurations. Finally, the optical absorption measurements performed on single phase hexagonal MgxZn1−xO QDs exhibited a clear shift in optical energy gap on increasing the Mg concentration from 0 to 40%, which is explained as an effect of substitution of Zn2+ by Mg2+ in the ZnO lattice.