The continued development of integrated photonic devices requires low-power, small volume all-optical modulators. The weak nonlinear optical response of conventional optical materials requires the use of high intensities and large interaction volumes in order to achieve significant light modulation, hindering the miniaturization of all-optical switches and the development of lightweight transmission optics with nonlinear optical response. These challenges may be addressed using plasmonic nanostructures due to their unique ability to confine and enhance electric fields in sub-wavelength volumes. The ultrafast nonlinear response of free electrons in such plasmonic structures and the fast thermal nonlinear optical response of metal nanoparticles, as well as the plasmon enhanced nonlinear Kerr-type response of the host material surrounding the nanostructures could allow ultrafast all-optical modulation with low modulation energy. In this thesis, we investigate the linear and nonlinear optical response of engineered effective media containing coupled metallic nanoparticles. The fundamental interactions in systems containing coupled nanoparticles with size, shape, and composition dissimilarity, are evaluated analytically and numerically, and it is demonstrated that under certain conditions the achieved field enhancement factors can exceed the single-particle result by orders of magnitude in a process called cascaded plasmon resonance. It is demonstrated that these conditions can be met in systems containing coupled nanospheres, and in systems containing non-spherical metal nanoparticles that are compatible with common top-down nanofabrication methods such as electron beam lithography and nano-imprint lithography. We show that metamaterials based on such cascaded plasmon resonance structures can produce enhanced nonlinear optical refraction and absorption compared to that of conventional plasmonic nanostructures. Finally, it is demonstrated that the thermal nonlinear optical response of metal nanoparticles can be enhanced in carefully engineered heterogeneous nanoparticle clusters, potentially enabling strong and fast thermal nonlinear optical response in system that can be produced in bulk through chemical synthesis.

A novel type of alternating-current (AC) powder electroluminescent (EL) device that relies on nanowire-phosphor heterogeneous junction structure has been developed. It shows promise for manufacturing of highly stable powder EL devices. To pursue this goal, manganese ion (Mn2+)-doped zinc germanate (Zn2GeO4:Mn) oxide phosphor was synthesized and used as EL powder material for the fabrication of the new types of AC powder EL devices. The Zn2GeO4:Mn oxide phosphor powder could eliminate the well-known degradation problem of zinc sulfide (ZnS)-based AC powder EL devices predominant in the current marketplace. In order to realize a high brightness at a relatively low operating voltage, a conductive semiconductor nanowire architecture using zinc oxide (ZnO) and copper oxide (CuO) nanowires with sharp-tip features, was created and integrated into conventional AC powder EL structures. Particularly, vertically-aligned n-type ZnO nanowires arrays were successfully synthesized on a Zn2GeO4:Mn polycrystalline substrate for the first time, and the growth behavior using a chemical vapor deposition (CVD) process was investigated. The density of the ZnO nanowires could be effectively controlled by some experimental parameters, such as the density of gold catalyst nanoparticles, and spatial distance between substrate and CVD source powders. This novel ZnO nanowire-decorated Zn2GeO4:Mn phosphor architecture was used to fabricate top-emission AC powder EL devices. On the other hand, a vertically-aligned ZnO nanowire array was directly synthesized on a thin film indium-tin-oxide (ITO)-coated glass substrate for fabrication of bottom-emission AC powder EL device. The nanowires were adopted to form heterogeneous junction structures between the tips of the nanowires and the Zn2GeO4:Mn EL powders, so that the composites could have a similar electrical field enhancement as in the needle-like CuxS precipitates within widely-used ZnS:Cu EL powder materials. The behavior of these top- and bottom- emission AC powder EL devices was also studied. Alternatively, vertically-aligned p-type CuO nanowires were prepared by a thermal oxidation method. Reliable heterogeneous junction structures were formed by a simple drop-coating method. The CuO nanowire-based AC powder EL device has excellent brightness maintenance with a loss of luminescent intensity under 1 % at over 10 cd/m2 luminance during 360 hours of operation. The integrating of semiconductor nanowires into conventional AC powder EL device structures offers the very promising prospect of fabrication of simple, low-cost, scaled-up EL devices that could fundamentally solve the limited operational lifetime of current ZnS-based AC powder EL devices. / Thesis / Doctor of Philosophy (PhD)

No description available.

Le but de cette thèse est d’étudier le processus de la génération d’harmoniques d’ordre élevé (HHG, de l’anglais high-order harmonic generation) dans des solides et la possibilité d’augmenter l’efficacité de la génération en exploitant l’exaltation locale du champ incident dans des nanostructures. La HHG dans les gaz est connue depuis plusieurs décennies et a été étudiée en détails, par contre la HHG dans les solides a été démontrée pour la première fois en 2011. Différents processus comme les oscillations interbandes et intrabandes y jouent un rôle fondamental. Le processus exact est toujours en cours d’investigation et est discuté dans la communauté. Dans ce manuscrit, nous étudions la génération d’harmoniques dans différents cristaux, comme ZnO, CaCO₃ et CdWO₄. Nous confirmons que la HHG dépend de la longueur d’onde génératrice et de l’orientation cristalline. Outre les cristaux 3D nous étudions la HHG dans des matériaux 2D comme le graphène. Grâce à sa grande mobilité électronique et sa structure de bande spécifique la HHG dans graphène est plus efficaces que dans des cristaux 3D.Typiquement des intensités de 10¹² TW/cm² ou plus sont nécessaires pour susciter la HHG. Ces intensités élevées sont généralement atteintes par des méthodes comme l’amplification par dérive de fréquence qui génère des impulsions femtosecondes à des énergies µJ ou mJ. Grâce aux progrès récents des techniques de nanofabrication, il est possible d’exalter un champ électrique laser de plusieurs ordres de grandeurs dans des nanostructures. Alors que la HHG dans les gaz assistée par la plasmonique a été démontrée comme n’étant pas réalisable, des travaux récents démontrent l’amplification de la HHG dans des solides. Dans ce travail, nous étudions l’amplification de la HHG dans différentes configurations. D’abord, nous analysons différents types de nanostructures, à savoir des bow ties, des nano-trous, des réseaux et des résonateurs. Nous comparons ces structures suivant plusieurs critères tels que le volume d’exaltation et l’exaltation crête. Différentes longueurs d’onde et cristaux sont utilisés. Une large amplification de plusieurs ordres de grandeur est démontrée pour la troisième harmonique. En plus, nous discutons l’endommagement des nanostructures causé par l’irradiation laser. Des nanostructures semiconductrices confinant la lumière par guidage sub-longueur d’onde ont plusieurs avantages par rapport aux nanostructures métalliques. Des nanocones semiconducteurs, par exemple, présentent un grand volume d’amplification, supérieur de plusieurs ordres de grandeur à ce qui a été démontré récemment, et évitent la fusion observée dans des nanostructures métalliques. Nous présentons plusieurs itérations de l’expérience avec des nanocones de ZnO en améliorant le système de détection et la géométrie des nanocones entre chaque étape. Nous utilisons différents lasers et différentes géométries de nanocones. Nous avons observé les harmoniques d’un laser à 3.1 µm dans des nanocones de ZnO jusqu’à l’ordre 15. L’amplification de plusieurs ordres de grandeur d’harmoniques perturbatives et non perturbatives, générées à partir des impulsions d’un oscillateur nanojoule à une cadence MHz et une longueur d’onde de 2.1 µm, est démontrée pour la première fois jusqu’à H9. Le facteur d’amplification dépend de l’éclairement du faisceau pompe. Nous étudions également la forte amplification de la luminescence et proposons des méthodes pour séparer sa contribution de la contribution cohérente. En outre, nous démontrons plusieurs applications de la HHG dans les solides. Premièrement, nous proposons une nouvelle méthode pour déduire la distribution spatiale du champ électrique dans des nanostructures en analysant les dommages induits par laser. Deuxièmement, nous utilisons l’émission du nanocone, qui est cohérente spatialement, pour imager des objets avec une résolution à l’échelle nanométrique. Enfin, nous générons des harmoniques portant un moment orbital angulaire contrôlé. / The aim of this dissertation is to study the process of high-order harmonic generation (HHG) in solids and the possibility to amplify solid HHG by exploiting local field enhancements in nanostructures. While HHG in gases has been known for several decades and has been extensively studied, HHG in solids was first reported in 2011. Different processes such as interband and intraband oscillations were identified to play an important role in solid HHG. However, the process is still under investigation and debated in the community. Here, we study the generation of high harmonics in different crystals, such as ZnO, CaCO₃ and CdWO₄. We confirm that HHG depends on the driving wavelengths and on crystalline orientation. Beside 3D bulk crystals, we investigate HHG in 2D materials such as graphene. Due to its high electron mobility and its special band structure HHG in graphene is more efficient than in bulk crystals. Typically, intensities of 10¹² TW/cm² or more are needed to trigger HHG. The high intensity is reached by employing schemes like chirped pulse amplification which generates femtosecond pulses with µJ- or mJ-energies. Thanks to recent advances in nanofabrication techniques, nanostructures can enhance a laser electric field by several orders of magnitude. While plasmonically enhanced HHG in gases was shown not to be feasible, recent works reported on the amplification of HHG in solids. In this work, we explore the amplification of crystal HHG under various configurations. We first study different types of plasmonic nanostructures, namely bow ties, nanoholes, gratings and resonators. We compare them with respect to different parameters such as enhancement volume and peak enhancement. Different driving wavelengths and crystals are used. Strong amplification by several orders of magnitude is demonstrated for the third harmonic. Furthermore, we discuss radiation-induced damage of plasmonic nanostructures. Semiconductor nanostructures which confine light by subwavelength waveguiding have several advantages with respect to metallic nanostructures. Semiconductor nanocones for example exhibit a large amplification volume, several orders of magnitudes larger than previously reported and avoid melting observed in metallic nanostructures. We carry out several iterations of experiments with ZnO nanocones where the detection system and the nanocone geometry are improved in each cycle. We use different driving lasers and different optimized nanocone geometries. HHG in ZnO nanocones up to 15th order from a 3.1 µm driving laser is demonstrated. Amplification by several orders of magnitude of both perturbative and non-perturbative harmonics from nanojoule-oscillator pulses at MHz repetition rate and 2.1 µm wavelength is demonstrated, for the first time up to H9. The amplification factor depends on the pump intensity. We also explore the strong amplification of luminescence and propose ways to disentangle its contribution from the coherent one. Furthermore, we explore several applications of crystal HHG. First, we propose a new way to deduce the electric field spatial distribution in nanostructures by analyzing the radiation-induced damage. Secondly, we use the spatially coherent emission from the nanocone to image nanoscale objects with nanometer scale resolution. In addition, we generate solid harmonics that carry an orbital angular momentum.

No description available.

The foundation of vacuum nanoelectronics was laid as early as in 1961 when Kenneth Shoulders proposed the development of vertical field-emission micro-triodes. After years of conspicuous stagnancy in the field much interest has reemerged for the vacuum nanoelectronics in recent years. Electron field emission under high electric field from conventional and exotic nanoemitters, which have now been made possible with the use of modern day technology, has been the driving force behind this renewal of interest in vacuum nanoelectronics. In the research reported in this thesis self-assembled silicon nanostructures were studied as a potential source of field emission for vacuum nanoelectronic device applications. Whiskerlike protruding silicon nanostructures were grown on untreated n- and p-type silicon surfaces using electron-beam annealing under high vacuum. The electrical transport characteristics of the silicon nanostructures were investigated using conductive atomic force microscopy (C-AFM). Higher electrical conductivities for the nanostructured surface compared to that for the surrounding planar silicon substrate region were observed. Non-ideal diode behaviour with high ideality factors were reported for the individual nanostructure-AFM tip Schottky nanocontacts. This demonstration, indicative of the presence of a significant field emission component in the analysed current transport phenomena was also detailed. Field emission from these nanostructures was demonstrated qualitatively in a lift-mode interleave C-AFM study. A technique to fabricate integrated field emission diodes using silicon nanostructures in a CMOS process technology was developed. The process incorporated the nanostructure growth phase at the closing steps in the process flow. Turn-on voltages as low as ~ 0.6 V were reported for these devices, which make them good candidates for incorporation into standard CMOS circuit applications. Reproducible I V characteristics exhibited by these fabricated devices were further studied and field emission parameters were extracted. A new consistent and reliable method to extract field emission parameters such as effective barrier height, field conversion factor, and total emitting area at the onset of the field emission regime was developed and is reported herein. The developed parameter extraction method used a unified electron emission approach in the transition region of the device operation. The existence of an electron-supply limited current saturation region at very high electric field was also confirmed. Both the C-AFM and the device characterization studies were modelled and simulated using the finite element method in COMSOL Multiphysics. The experimental results – the field developed at various operating environments – are explained in relation to these finite element analyses. Field enhancements at the atomically sharp nanostructure apexes as suggested in the experimental studies were confirmed. The nanostructure tip radius effect and sensitivity to small nanostructure height variation were investigated and mathematical relations for the nanostructure regime of our interest were established. A technique to optimize the cathode-opening area was also demonstrated. Suggestions related to further research on field emission from silicon nanostructures, optimization of the field emission device fabrication process, and fabrication of field emission triodes are elaborated in the final chapter of this thesis. The experimental, modelling, and simulation works of this thesis indicate that silicon field emission devices could be integrated into the existing CMOS process technology. This integration would offer goods from both the worlds of vacuum and solid-sate nanoelectronics – fast ballistic electron transport, temperature insensitivity, radiation hardness, high packing density, mature technological backing, and economies of scale among other features.

This thesis examines and exploits the optical properties of pairs of MNPs. Pairs of MNPs offer two further parameters not existent at single MNPs, which both affect the local optical fields in their vicinity: the distance between them, and their relative orientation with respect to the polarisation of the excitation light. These properties are subject of three chapters: One section examines the distance-dependent and orientation-sensitive scattering cross section (SCS) of two equally sized MNPs. Both near- and far-field interactions affect the spectral position and spectral width of the SCS. Far-field coupling affects the SCS even in such a way that a two-particle system may show both a blue- and redshifted SCS, depending only on the distance between the two MNPs. The maximum distance for this effect is the coherence length of the illumination source – a fact of importance for SCS-based experiments using laser sources. Another part of this thesis examines the near-field between two MNPs and the dependence of the locally enhanced field on the relative particle orientation with respect to the polarisation of the excitation light. To attain a figure of merit, the intensity of fluorescence light from dye molecules in the surrounding medium was measured at various directions of polarisation. The field enhancement was turned into fluorescence enhancement, even providing a means for sensing the presence of very small MNPs of 12 nm in diameter. In order to quantify the near-field experimentally, a different technique is devised in a third section of this thesis – scanning particle-enhanced Raman microscopy (SPRM). This device comprises a scanning probe carrying an MNP which in turn is coated with a molecule of known Raman signature. By manoeuvring this outfit MNP into the vicinity of an illuminated second MNP and by measuring the Raman signal intensity, a spatial mapping of the field enhancement was possible. / Diese Dissertation untersucht und nutzt die optischen Eigenschaften von Paaren von Metall-Nanopartikeln (MNP). MNP-Paare bieten gegenüber einzelnen MNP zwei weitere Parameter, welche beide auf das optische Nahfeld der zwei MNPs wirken: zum Einen der Abstand der zwei MNPs zueinander, zum Anderen die relative Ausrichtung des Paares bezüglich der Polarisation des anregenden Lichts. Diese Eigenschaften sind Thema der Arbeit: Ein Abschnitt untersucht den abstands- und orientierungsabhängigen Streuquerschnitt (SQS) zweier gleichgroßer MNPs. Die spektrale Position und die Breite des SQS wird von Wechselwirkungen sowohl im Nah- als auch im Fernfeld beeinflusst. Der Einfluß der Fernfeld-Wechselwirkung geht so weit, daß ein Zwei-MNP-System sowohl einen blau- als auch einen rotverschobenen SQS haben kann – dies hängt lediglich vom Abstand der zwei MNPs ab. Die Reichweite dieser Fernfeld-Wechselwirkung wird durch die Kohärenzlänge der Beleuchtungsquelle bestimmt – eine wichtige Tatsache für SQS-Untersuchungen, welche Laserquellen verwenden. Ein weiterer Teil der Dissertation untersucht das Nahfeld zwischen zwei MNPs. Insbesondere wird dargestellt, inwieweit die Überhöhung des Nahfelds von der Orientierung des Partikelpaares bezüglich der Polarisation des Anregungslichts abhängt. Um den Effekt quantifizieren zu können, wurde die Intensität der Fluoreszenz des umgebenden Mediums für verschiedene Polarisationsrichtungen gemessen. Die lokale Feldverstärkung konnte in eine Fluoreszenzverstärkung gewandelt werden, mit deren Hilfe sich sogar die Anwesenheit sehr kleiner MNPs von nur 12 nm Durchmesser nachweisen ließ. Wie Nahfeld-Intensitäten experimentell quantifiziert werden können, stellt ein dritter Abschnitt dieser Dissertation vor – per MNP-verstärkter Raman-Rastersonden-Mikroskopie. Diese Technik besteht aus einer Rastersonde, welcher ein MNP anheftet, welches wiederum mit einem Molekül bekannter Ramansignatur überzogen ist. Indem solch eine Sonde in die unmittelbare Nähe eines zweiten, beleuchteten MNPs gebracht wurde und dabei die Intensität des Raman-Signals aufgezeichnet wurde, ließ sich die räumliche Verteilung der Ramanverstärkung vermessen.

In the quest for reliable, repeatable and stable field electron emission that has commercial potential, whilst many attempts have been made, none yet has been truly distinguishable as being successful. Whilst I do not claim within this thesis to have uncovered the secret to success, fundamental issues have been addressed that concern the future directions towards achieving its full potential. An exhaustive comparison is made across the diverse range of materials that have, over the past 40-50 years, been postulated and indeed tested as field emitters. This has not previously been attempted. The materials are assessed according to the important metrics of turn on voltage, Eon, and maximum current density, Jmax, where low Eon and high Jmax are seen as desirable. The nano-carbons, carbon nanotubes (CNTs), in particular, perform well in both these metrics. No dependency was seen between the material work function and its performance as an emitter, which might have been suggested by the Fowler Nordheim equations. To address the issues underlying the definition of the local enhancement factor, β, a number of variations of surface geometry using CNTs were fabricated. The field emission of these emitters was measured using two different approaches. The first is a Scanning Electrode Field Emission Microscope, SAFEM, which maps the emission at individual locations across the surface of the emitter, and the parallel plate that is more commonly encountered in field emission measurements. Finally, an observed hysteretic behaviour in CNT field emission was explored. The field emitters were subjected to a number of tests. These included; in-situ residual gas analysis of the gas species in the emitter environment, a stability study in which the emitters were exposed to a continuing voltage loop for 50 cycles, differing applied voltage times to analyse the effects on the emitted current, and varying maximums of applied field in a search for hysteresis onset information. These studies revealed the candidate in causing the hysteresis is likely to be water vapour that adsorbs on the CNT surface. A six step model if the emission process was made that details how and when the hysteresis is caused.

L’irradiation des matériaux par des impulsions laser ultrabrèves déclenche un agencement anisotrope de la matière à l’échelle nanométrique: des structures de surface périodiques induites par laser (LIPSS). L'énergie laser déposée et distribuée de manière inhomogène dans le matériau induit des contraintes thermiques locales et des changements de phase transitoires entraînant ainsi des modifications microstructurales. Cette thèse porte sur le rôle de l'altération de la surface irradiée ainsi que les modifications microstructurales en profondeur dans la contribution à la formation des LIPSS, en établissant une corrélation entre l'auto-organisation de la matière et la génération de défauts en tenant en compte de l'orientation cristalline. Comme les LIPSS sont générés au seuil de transition de phase, l’étude de la corrélation avec les défauts induits est alors pertinente. Une étude expérimentale couplée à des simulations de dynamique moléculaire effectuées à l’Université de Virginie suggère que l'altération de surface générée par une irradiation d'échantillons monocristallins de Chrome dans le régime de spallation est susceptible de jouer un rôle majeur dans le déclenchement de génération de LIPSS de haute fréquence spatiale. La microscopie à force atomique ainsi que les résultats de simulations attestent que les caractéristiques de rugosité de surface à l'échelle nanométrique dépendent de l'orientation cristalline. La forte rugosité de surface générée par la première impulsion laser active la diffusion de la lumière laser et l’exaltation du champ local lors des irradiations ultérieures, ce qui génère des structures LIPSS de haute fréquence plus prononcés du côté (100) que celle du (110). Une étude expérimentale approfondie, utilisant la microscopie électronique rétrodiffusés et transmission, a révélé que le Cr (110) est plus susceptible d'être endommagé que les autres orientations cristallines de surface. On constate que les défauts induits par le laser peuvent altérer la topographie de surface et la région sous-jacente, ce qui peut avoir un impact sur les caractéristiques des centres de rugosité favorisant la formation de structures de fréquence spatiale élevée. Afin d’accéder à la transition de phase subie dans la région de formation des LIPSS, une approche d'analyse microstructurale à haute résolution couplée à des calculs hydrodynamiques est utilisée, comprenant la croissance épitaxiale et la nanocavitation. La formation de structures de fréquence spatiale élevée est le résultat de nanocavités périodiques piégés sous la surface, ainsi que des nanocavités apparues à la surface des matériaux cubiques faces centrées.De plus, étant donné que le feedback dans la formation des LIPSS est souvent évoquée, le comportement dynamique des surfaces a été sondé par microscopie électronique à photoémission et étayé par des calculs électromagnétiques. Un caractère périodique des photoélectrons émis par les creux des LIPSS a été mis en évidence, ce qui a permis de vérifier la modulation du dépôt d'énergie.Le travail effectué contribue non seulement à progresser vers l'objectif général d’élucider le phénomène complexe multi-échelles de la formation des LIPSS, mais ouvre une nouvelle voie expérimentale pour générer des structures non conventionnelles avec des périodicités extrêmes (~60nm), offrant ainsi de nouvelles opportunités pour le traitement laser ultrarapide des métaux. / Irradiation of materials by ultrashort laser pulses triggers anisotropically structured arrangement of matter on the nanoscale, the so-called laser-induced periodic surface structures (LIPSS), or ‘ripples’. Ultrashort laser energy deposited and distributed inhomogeneously in the material launches local thermal stresses and transient phase changes yielding microstructural modifications. This thesis focuses on the role of irradiated surface alteration as well as in-depth microstructural modifications in promoting LIPSS formation, by establishing a correlation between self-organization of matter and defect generation taking into account crystalline orientation. Since LIPSS are generated at the threshold of phase transition, then the correlation with defects formation is relevant. An experimental study coupled with molecular dynamic MD simulations performed in the University of Virginia suggest that surface alteration generated by a single pulse irradiation of monocrystalline Cr samples in the spallation regime is likely to play a main role in triggering high-spatial frequency LIPSS generation upon irradiation by multiple laser pulses. Atomic force microscopy as well as computational results suggested that the nanoscale surface features are crystalline orientation dependent. The higher surface roughness generated by the first laser pulse activates scattering of the laser light and the local field enhancement upon irradiation by the second laser pulse, leading to the formation of much more pronounced high-spatial frequency structures on the (100) surface as compared to (110) one. An extended in-depth experimental study, using electron backscattered and transmission microscopy, combined with large-scale two-temperature model TTM-MD simulations revealed that Cr (110) is more likely to get damaged. It is found that laser-induced defects can alter the surface topography and the region beneath it which can impact in turn the roughness center features promoting high-spatial frequency structures formation. In order to infer the phase transition undergone in the LIPSS region, a high resolution microstructural analysis approach coupled with hydrodynamic calculations is employed, including epitaxial regrowth and nanocavitation. High-spatial frequency structures formation is found to be the result of periodic nanovoids trapped beneath the surface as well as nanocavities emerged at the surface on fcc materials. Furthermore, since optical feedback in LIPSS is often evoked, the behavior of dynamical surfaces was probed by photoemission electron microscopy and supported by electromagnetic calculations. A periodic character of photoelectrons emitted from nanoholes was unveiled, which in turn verified a modulated energy deposition. The performed work not only contributes to the progress towards the general goal of untangling the complex multiscale phenomenon of the LIPSS formation, but unlocks a new experimental setup to generate unconventional structures with extreme periodicities (~60 nm), which offers new opportunities in ultrafast laser processing of metals.

This diploma thesis deals with the design and optimization of the device for measurement of field emission from gallium nitride (GaN) nanocrystals surface. The first part of the thesis is the topic review, which contains the introduction to the problematics of field emissio focused on GaN. Then there were designed, constructed and optimized two versions of the device for the measurement of field emission. Through the optimization phase, the first successful test has been performed with zinc oxide (ZnO) nanowires. Simultaneously GaN nanocrystals were fabricated on the silicon substrate Si(111) with 2 nm of silicon dioxide SiO2 and also on the copper foil covered by graphene by molecular beam epitaxy (MBE). In the last chapter, there are presented the results of the measurement for emission of GaN nanocrystals. Finally, this study is comparing results with the current research in the area of field emission, which displays the improved characteristics for field emission of GaN nanocrystals on the copper foil covered by graphene.