USES OF A CARBON NANOBUD MOLECULE AND DEVICES COMPRIS 1NG THE SAME FIELD OF THE INVENTION 5 The present invention relates to nanotechnol ogy. Especially the present invention relates to opti cal and optoelectrunic devices based on using an opti cally active nanomaterial, and to methods for their production, 10 BACKGROUND OF THE INVENTION Optical and optoelectronic devices finr many applications in e.g. telecommunications networks and metrology. The devices in the aforementioned fields 15 may comprise active devices such as lasers, amplfiers and detectors, and passive devices such as filters, posarzers and absorbers. n general key parameters of these devices are power consumption (for active de vices), stability which dictates the lifetime of the 20 device and various parameters related to the function of the device; the functional parameters may include e.g. saturable absorption of electromagnetic radia tion, polarization dependent absorption of electromag netic radiation, internal and/or external quantum ef 25 ficiencies etc Novel nanomaterials including e.g. nanotubes, nanowires, fullerenes, quantum dots, nanoparticles and nanowhiskers present a new way to tailor the key pa rameters in optical and optoelectronic devices. E.g. 30 nonlinear optical effects may be introduced to and en hanced in a device by using these nanomaterials at a suitable location in the device structure. Although the new nanomazerials and nanostructures show promise in improving key parameters cf optical and optoelec 35 tronic devices, the materials simultaneously present new challenges to the fabrication of these devices.
2 The method for the synthesis of nanostruc tures is strongly dependent on the structure itself Some nanostructures e.g. guantum dots may be synthe sized in a conventional thin-film deposition tool such 5 as an MOCVD tool whereas fibrous network structures comprising e.g. nanowires may require a tool specifi cally designed for the synthesis andr deposition of these high aspect ratio molecules (HARMs) . The fabri cation of deVices comprising the new nanomaterials of 10 ten requires manipulation of iterial at a molecular resolution. This is especially important in optical devices comprising HARMs where the specific orienta tion of a molecule with a high aspect ratio may si nificantly affect the optical properties of the de 5vice An example of such a device is a polarizer (or polarizing filter) whose optical transmission coe_f cient depends on the polarization of incident light. Additionally, of paramount importance in op tiea applications is the purity and homogeneity of 20 the nanomaterial In order to incorporate HARMs in a device the molecules are filtered from e.g. a gas stream :and/or dispersed in a solution. These opera tions risk the incorporation of impurities in the op tical device and the dispersion of HARMs a solution 25 is commonLy -sufficient to result in homogeneous ma teriai Moreover dispersion often requires the use of harsh treatments such as sonification and/or the use of surfactants and functionalizing materials, which may be detrimental to the operation of the de:-vice 30 The performance of many of the cuently known optical and optoelectronic devices based on nanostructures suffers from the difficulties in fabri cation as well as from properties of the functional nanomateria. For example publication W02008/025966 Al 35 discloses a composition comprising nanomateri in an optical coupling gel Or an optical adhesive. The in vention disclosed in publication W2008/025966 Al suf- - 3 fers from inhomogeneous dispersion of the nanomaterial e.g. nanodots in the optical gel or adhesive, It may furthermore be difficult to obtain nanomaterial of sufficient purity for optical or optoelectronic devices 5 from the nanomaterials disclosed in the publication. For the improvement of existing, and for the development of new optical and optoelectronic devices it is important to find new nanomaterials with improved 10 functionality, purity, versatility and homoge-neity, Equally important is to develop new manufacturing methods that do not result in degradation and do not detrimental ly alter the key properties of the materials utilized in these devices. 15 PURPOSE OF THE INVENTION The purpose of the present invention is to reduce the aforementioned technical problems of the prior-art by providing new type of optical and opto-electronic devices 20 based on using fullerene functionalized and covalently bonded fullerene functionalized tubular carbon molecules. SUMMARY OF THE INVENTION A device according to the present invention is 25 characterized by what is presented. in independent claims 1 and 3. According to an embodiment, a carbon nanobud molecule having at least one fullerene part covalently 30 bonded to the side of a tubular carbon molecule is used to interact with electromagnetic radiation in a device, wherein the interaction with 604!269 i (GHMaltes) P5840AU.1 PCABRAL 1112,i4 4 electromagnetic radiation occurs through relaxation and/or excitation of the carbon nanobud molecule. A device according to the present invention comprises a carbon nanobud molecule having at least S one fullerene part covalently bonded to the side of a tubular carbon molecule. The device comprises one or more at east par y p-type electricailly conductive carbon nanobud molecules and one or more at least partly -type electrically conductive carbon nanobud 10 molecules, such that the one or more at least partly p-type electrically conductive carbon nanabud mole cules are in electrical contact wiih the one or more at least partly n-type electrically conductive carbon nanobud molecules to enable radiative electron-hole LS recombination A device according to the present invention comprises a carbon nanobud molecule having at least one fcllerene part covalently bonded to the Side of a tubular carbon molecule, and a chromnphore i s attached 20 to the carbon nanobud molecule, to influence the spec tral charateristics of the device and to enhance non linearity of absorption characteristics of electromag netic radiation to the molecule. In this context interaction cf the carbon 25 nanobud molecule with electromacnetic radiation should be understood as coorisino all processes inviving excitation or relaxation of the nanobud molecule which cause absorption or emission of electromagnetic tion. Examples of devices where one or more carbon 30 nanohud molecues mnay be used to perform functions re lated to emission, absorption and/or other interaction with electromagnetic radiation include e.g. emitters, displays, lasers, amplifiers, filters, polarizers, photodetectors, detector arrays (eg. for cameras, 35 bio-chemical sensors, markers for use: in scectroscopic or fluorescence-related applications, signal regenera tors, waveform shapers, dispersion ccompensators, wave- Length converters. optically powered actuators (e.g. laser-driven nanomotor) , optical switches, structuri zation-enhancing materials for lithographic processes, antirftlective (AR) coatings or selectively reflec 5 tire ooat:ngs with superior chemical, mechanical or irradiration resistance 9 photographic or hoographic materials for increased information storage density and phase or amplitude modulators The one or more carbon nanobud molecules in these devices may take the 10 form of e.g. a network, a deposit or a film or they may be incorporated in a matrix material, such as glass, quartz, crystalline material, polymer optical gel or optical adhesive. Components comprising carbon nanobud mole 5 cules which, according to the present invention, are used to interact with electromagnetic raciation are especially suitable for various optical or optoelec tronic devices. A reason for this is that the synthe sis processes for carbon nanobud moecules is able to 20 produce purer, more crystalline and more homogeneous material than e.g. conventional synthesis processes for carbon nancubes. This is a result of the specific geometry of the nanobud molecule enabling synthesis processes without the need for additional, potentially 25 damaging, purification steps. The production methods result in material that neets the high purity, quality and homogeneity requirements for many optical applica tions. The carbon nanobud molecules furthermore combine the functional features of tubular carbon mere 30 cules and of fullerene molecules in a stable and ro bust structure which can be functionalized to modify the properties and behaviour of the material in which the nanobud molecules are incorporated This may be especially useful in nonlinear optical applications 35 performing functions such as saturable absorption? re verse saturable absorption, light amplification and polarization. Additionally, the fullerene part of the 6 carbon nanobud molecule provides a means for separat ing the tubular part of the nanobud molecule from its neighbours, either by simple geometric considerations or by functionalization of the fulleree par so as 5 to avoid or otherw:ise control tube-tube interactions ich can alter the optical characteristics of the ma terial comprising carbon nanobud molerules- It is noted that the fullerene part of the carbon nanobud molecuLe can be a ful erene molecule or other 10 fuIlerene-iike structure possibly comprising a fullerene molecule. Furthermore, the fullerene part or the fullerene-like structure bonded to the tubular part of the carbon nanobud mirlecuie can be utilized to change 1 5 the band-gap (the conductivity or semiconductivity) of the material comprising the carbon nanobud molecules. This allows :absorption, emission or other electromag netic interaction in the material to be tuned as a function of wavelength, temperature, chemical environ 20 ment or other local conditions. Te fullerene li e structure bonded to the tubular part of the carbon nanobud molecule can additionally be used as a bridg ing molecule between two nanobud molecules? either di rectly or via another bridging molecule such as an es 25 ter group, This may, for instance, be utilized to en hance relaxarion o carriers within the nanobud mole cules and/or to decrease the recovery time of the ma terial comprising carbon nanobud molecules and/or to increase the mechanical robustness of a deposit or a 30 film, In one embodiment of the invention a chrome phore is attached to the carbon nanobud molecule, to enhance non 1 4 nearity of absorption characteristics of electromagnetic radiation to the nanobud molecule. 35 in another embodiment of the invention tne chromophore is attached to the fullerene part of the carbon nanobud molecule, to enhance non-linearity of absorption characteristics of electromagnetic radia tion to the nanobud molecule. By attaching a chromophore to a reactive site in the carbon nanobud molecule in the tuiular part or 5 in the fullerene part, a non-linear optical material may be realized. This type of material exhibits im proved stability compared to non-linear optical mate rials of the prior art as a result of the stability of the carbon nanobud molecules. A chromophore in this 10 context can be understood as any molecular structure generating a desired optical effect when interacting with electromagnetic radiation. Examples of chiromopho res inducing non-linear optical effects in carbon nanobud molecules include organic molecules such as 15 polymers, oligomers, monomers and dimers. Specifically dye molecules e.g. phenosa tranin (PSF) induce strong non-:inear absorption dharacteristics to carbon nano bud molecules. A chromophore can also act as a bridg ing molecule referred to above. 20 Carbon nanobud molecules can be deposited onto a device structure e.g. directly from the gas phase, without using dispersion of the nanobud mole cules from a liquid solution, to improve the optical quality of the carbon nanobud molecules. Other produc- 25 tion methods are also possible, such as spin coating or dispersing in a matrix material. The deposition of carbon nanobud molecules directly from the gas phase on a substrate such as an optical component structure, according to the method described in detail in 30 vW2007/05701 Al, enables a more uniform distribution of the molecules compared to methods in which nanoma terial is dispersed in a matrix material. Deposition directly from the gas phase additionally decreases the risk of contamination by impurities and the risk of 35 alteration of properties due to intermediate process ing steps as long as the carbon nancbud molecules are efficiently separated from other molecles or carti- 8 cles in the gas. An additional benefit of depositing the carbon nanobud molecules directly from the gas phase with the referenced method is that the optical properties of an individual carbon nanobud molecule, 5 e.g. crystallinity and defect density, are Afmproved. Furthermore, the nanobud molecules can be surfacted and debundled during the process, which promotes their dispersion in liquids or on solid substrates. in order to minimize the risk of contamination of the carbon 10 nanobud molecules the sustrate used for deposition of the carbon nanobud molecules can be different to the final substrate. A network comprising carbon nanobud molecules may be transferred from a preliminary sub strate onto a final substrate. which may be part of 15 e.g. an optical component, using the method described in patent application FI 20075482 In one embodiment of the invention the device comprises two or more carbon nanobud molecules wherein the two or more carbon nanonud molecules are 20 separated from each other to increase the light cap turing cross section of a single carbon nanobud mole cule. The average light capturing cross section of carbon nanobud molecules in a device may be increased 25 by ensuring that the molecules are separated from each other in the device, as opposed to a situation where the carbon nanabud molecules reside close or even in contact with each other in the device. In the latter situation the carbon nanobud molecules may screen each 30 other such thati their average light capturing cross section is reduced. One way to enhance the separation. of carbon nanobud molecules is to separate them from bundles of these molecules already at the deposition stage. This may be accomplished by eg, exploiting the 35 charge difference between bundled carbon nanobuds and individual carbon nanobud molecules. An increased light capturing cross section results in enhancement 9 of the optical processes in the material comrising carbon nanobud molecules Another way to enhance the separation is to bind individual nanobud molecules to gether by joining the fullerene or the fulierene-like 5 parts of the nanobud molecule together by, for in stance, bridging molecules so that the carbon nanobud molecules are less likely to bundle or rebundle during Processing, Yet another way to enhance the separation is to bInd individual nanobud molecules to a matrix or 10 surface material by joiniug the fullerene or the fullerene-like arts of the nanobud molecule to the matrix material via, for instance, appropriate matrix molecules such as polymers, so that the carbon nano bud m molecules are less likely to bundle In one embodiment of the invention the carbon nanocud molecule is used to saturably absorb electro maanetic radiation In aranother embodimen: of the invention the carbon nanobud molecule is used to reverse saturably 20 absorb electromagnetic radiation. in another embodiment of the. invent-i on the tubular carbon molecule is used to saurably absorb electromagnetic radiation, and the fullerene part co valently bonded to the tubular carbon molecule is Used 25 to reverse saturably absorb electromagnetic radiation. In yet another embodiment of the invention two or more mutually aigned carbon nanobud molecules are used to enable anisotropic absorption of electro magnetic radiation in the device. 30 Due to the asymmetica shape of the carbon nanobud molecule these molecules may be easily elec trostatically or otherwise polarized and aligned at wll by posItioning them e.g. in an electric or a ma netic field The possibility to accurately align the 35 absorbing molecules enables anisotropic absorption or ndulazion patterns for materials comprising carbon nanobud molecules. This feature together with the 10 saturable and reverse saturable absorption character istics of carbon nanobud molecules presents interest ing opportunities for eg waveform shaping appliica tions which can be used in pulse regeneration in opti 5 cal telecommunication networks. In one embodiment of the invention the carbon nanobud molecule is used for nolarized optica emis sion. In one embodiment of the invention the device 10 comprises a first electrode in electrical contact with the one or more at least partly n-type electrically conductive carbon nancbud Inolecules, a second elec trode in electrical contact with the one or more at least partly p-type electrically conductive carbon 15 nanobud molecules, a gate electrode, and an insulating layer in between the gate esectrode and the carbon nanobud molecules to electrically insulate the gate electrode from the carbon nanobud molecules. The embOdinents of the invention described 20 hereinbefore may be used in any combination with each other. Several of the embodiments may be combined .o gether to form a further embodiment of the invention. A use or a device, to which the invention is related, may comprise at least one of the embodiments of the 25 invention described hereinbefore. DETAILED DESCRIPTION OF THE INVENTION in the following, the present invention will be described in more detail. References wili be made 30 to the accompanying figures, in which Fig. 1. (Pior Art) presents five different molecular models for a carbon nanobud molecule in which at least one fullerene molecule or a fullerene like molecular structure is covalently bonded to a tu 35 bular carbon molecule, 11 Fig. 2 schematically presents a light emit ting diode according to one embodiment of the present invention, Pig. 3 schenatically presents a laser accord 5 ing to one embodiment of the present invention, Fig. 4 schematically presents a light emit ting FET structure according to one embodiment of the present invention, Fig. 5 schematically presents a device setup 10 according to one embodiment of the present invention, Fig. 6 schematically presents another device setup according to one embodiment of the present in vention, Pig. 7a schematically presents a longitudinal 15 cross section of a semiconducto r laser ceording to one embodiment of the present invention, Sig g 7b schematically presents a transverse cross section of a semiconductor laser according to one embodiment of the present invention, 20 Fig. 8 schematically presents a cross section of a fiber laser according to one embodiment of the present invention, Fig. 9 schematically presents a ring laser configuration according to one emodiment of the pre 25 sent invention, Pig. 10 schematically presents another device setup according to one embodiment of the present in vention, Fig. 11 schematically presents a saturable 30 absorption function, Fig. 12 schematically presents a reverse saturable absorption function, Fig. 13 schematically presents a combined saturable absorption and reverse saturable absorption 35 function, Fig. 1 4 a presents the effect of the saturable absorption, the reverse saturable absorption and the 12 combine saturable and reverse saturable absorption functions on a stream. of optical pulses, Fig, 1h preents how narrower pulses in an optical pulse stream enable an increased pulse rate, Fig 14c presents an optical pulse sequence before reforming with a carbon nanobud-based saturable and reverse saturable absorber and Fig 1.4d presents an optical pulse sequence after reforming with a carbon nanobud-based saturable 10 and reverse saturable absorber. Carbon nanobud molecules schematically illus trated in Fig. I can be synthesized from for in stance, a carbon source e.g. carbon monoxide using catalyst precursors such as ferrocene, or catalysts 15 generated from a hot wire generator, such as metal particles and additional agents which, in addition to promoting the growth of nanobud molecules, increase the purity of the product. Details of the synthesis process can be found in publication W02007/057501 Al, 20 which is added as a reference herein. A light emitter structure based on light emission from carbon nanobud molecules is presented in Fi, 2. This structure comprises an n-type Si region I and a p-type Si region 2. In between these regions 25 there is an insulating region comprising semiconduct ing carbon nanobud molecules 3 with a direct band gap embedded in an insulating matrix 4 material such as undoped Si or a thin (thickness 5 10 nm) layer of silicon oxide (SiC 2 ). TUnder operation a negative volt 20 age -V/2 is apiied to the electrical contact 5 on the n-type Si I side of the structure and a positive volt age V/2 is applied to the electrical contact 6 on the p-type S 2 side of the structure. This injects elec tron from the n-type Si iI side and holes from the p 35 type Si 2 side towards the insulating region, When a hole and an electron encounter a carbon nanobud mole cule 3 inside the insulating region they will undergo 13 recombination which, with a finite probability, will be radiative, The band gap of a carbon nanobud molecule can be tailored by adjusting the process used for the syn 5 thesis of these molecules. The band gap of carbon nanobud molecules may be e.g. modified by functionali ration of the moalecules with additional atoms or by adjusting the chirality. A carbon nanobud molecule 3 with a smaller band gap than the surrounding insulat 10 ing matrix 4 may operate like a quantum dot confining charge carriers tunnelled in the insulating region, to the carbon nanobud molecules 3 to enhance the in ternal quantum efficiency of the light emitter. in one embodiment of the present invention 135 the structure of Fic. 2 nay be modified to function as a laser, The modified structure is presented in Fic. 3. It comprises Bragg-reflectors on both sides of the structure presented in Fig. 2. The Bragg-reflectors confine a Fabry-Perot miorocavitv wre the active me 20 dium comprises carbon nanobud molecules as the light emitting material. The Bragg-reflectors may comprise e.g. alternating layers of Si 7 and SiO 2 8 that form a highly reflective interference structure. When elec tron and hoes are injected into the active medium at 25 sufficiently high rate to achieve population inver sion in the active medium, easing begins. The lasing wavelength in the structure of Fig. 3 is dictated by the interplay between the length of the Fabry-Perot cavity and the fundamental band gap of the light emit 30 ter i.e. the carbon nanobud molecules 3 The thick ness of the Si 7 and Si0 2 8 layers in the Bragg reflectors should be adjusted so that a sufficiently high reflectivity is achieved for the lasing wave length. In order to achieve a high level of charge In S section into the active medium highly doped n-ype Si 1 and p-type Si 2 regions may be beneficiaL 14 There may eist many variations to the light emitting structures of Fig. 2 and Fig 3, which oper ate according to the corresponding principle. The n type Si I and the ptype Si 2 regions may e.g. alter 5 natively be formed by a network of p- and/or n-type carbon nanobud molecules that respcrtiveey form the p and/or the n-type side of the structure, Additionally, in the laser structure of Fig. 3 the Bragg-reflectors may comprise carbon nanobud molecules within the re 10 flector structure, or a Si 7 or a SiC 2 S layer may be replaced by a layer comprising carbon nanobud mole cules. The light emitting structures (the LWD of Fig. 2 and the laser of Fig. 3) may be fabricated by depositing Si02 and Si by CVD or PECVD on a silicon substrate and by using a suitable annealing process for n- or p-type doping. Alternately, if nanobuds are used, suitably doped n- or p-type nanobud molecules can b deposited . The carbon anobud molecules 3 are 20 embedded into the active region of the light emitting device by overgrowing them with Si. or a suitable thin layer of insulating material such as SiO). A device according to one embodiment of the invention is a colarized light Source. The device is 25 schematically presented in Fig. 4 The device struc ture resembles a field effect transistor (FET) and it compries a carbon nanobud moec e in between a source 10 and a drain 11 electrode a gate electrode 12, a gate dielectric 13 and a capping layer 14 on top 30 of the drain 11 and the source 10 electrodes. By ap plying a voltage to the gate electrode 12, such that the potential of the qate is between the potential of the source and the drain, simultaneous electron and hole injection into the carbon nanobud molecule 9 is 35 achieved, In this way a p-n junction is generated within a single carbon nanobud molecule 9. Nhen an electron and a hole recombine in the carbon nanobud 1.5 molecule 9 within the presented device, emission of polarized light has surprisingly been observed. The operation of the device, the ambipoLar FET, in Pig. 4 relies on the generation of thin Schot 5 tky barriers at each end of the carbon nanobud mole cite 9 at the boundary of the source 10 and drain 11 contacts. When the device is suitably biased as de scribed above, both electrons and holes are able to tunnel through the Schottkv barriers into the carbon 10 nanobud molecule 9 resulting in polarized light emis sion. The device of Fig. 4 may be fabricated by e.g. depositing 502 on a P-Si substrate wafer and dispersing carbon nanobud molecules on the insulating 15 Si02 gate dielectric 13. The Ti drain 11 and source 10 electrodes may be e.g. deposited using PVD and then patte rne by Iithography to produce contact regions at suitable locations on the substrate. At this stage an nealing in Ar atmosphere at eg. 900c "Cmay be used to 20 improve electrical contacting between the carbon nano bud molecule 9 and the Ti drain and Ti source 10 contact. The structure may be capped with a thin SiO0 capping layer 14. The carbon nanobud molecule may be replaced by two or more carbon nanobud molecuaes in 25 the device of Fig. 4 to form a further embodiment of the present invention. In addition to the aforementioned devices which are based on electroluminescence of carbon nano bud molecules, these molecules can additionally or ex 30 delusively be optically excited to perform various functions. Embodiments of the invent on performing these functions ill be described subsequently In one embodiment of the present invention one or more carbon nanobud molecules can no usec in a 35 device setup schematically and generically illustrated in Fig. 5. This setup comprise's an input light source 15, an input beam 16 of electromagnetic radiation, a slab 17 of transparent or semi-transparent material 17 comprising one or more carbon nanobud molecules I8, two output beams of electromagnetic radiation (the transmitted beam 19 and the emitted beam 20) and a de 5 tection device. 21. in this context transparency should be understood as transparency at the wavelengths of the beams of electromagnetic radiation presented in Fig. 5. The input light source 15 may be e.g. a laser or a broadband light source and it may be modulated. GO The detection device 21 may be e.g. a photodiode or other photosensitive device with the ability to detect radiation at the wavelengths of the two output beams 19, 20, The transmitted beam 19 in Fig. 5 is the part 15 of the input beam 16 that is transmitted through the slab 17 comprising carbon nanobud molecules 18 essen tially without interaction with the slab 17. The emitted beam 20 is a beam of electromagnetic radiation emerging from the slab 17 as a result of the input 20 beam 16 interacting with the carbon nanobud molecules 18 in the slab 17. The carbon nanobud molecules 18 embedded in the slab 17 may absorb electromagnetic radiation at the wavelength, or at several wavelengths, of the in 25 rut beam 16. This absorption may vary depending on many parameters such as direction, polarization, in tensity and wavelength or wavelength spectral charac teristics of the input beam 16. These dependencies en able the slab 17 to perform different functions which 30 may be utilized in e.g. communication and measurement technology. It is noted that the slab 17 of Fig. 5 may take any geometrical shape. When electromagnetic radiation is absorbed in the carbon nanobud molecule (s) 18 these molecules get 35 excited as electrons move to higher energy states in the molecules. Wihen relaxation of the same mlecules occurs electrons move back to the lower energy states I7 in the molecules and energy may be emitted at one or more wavelengths characteristic to the carboni nanobud molecules 18. It has surprisingly been observed, that carbon nanobud molecules I8 exhibit non-linear photo 5 luminescence which can be used to e.g, perform logic operations, optical switching and modulation entirely in the optical domain. As a result of the non-linear photolumines cence the intensity of the luminescent light emitted 10 20 from the slab 17 of Fig. 5 varies as a non-linear <nction of the intensity of the electromagnetic ra diation, which is used to excite the carbon nanobud molecules 18 in the slab 17, i e. the intensity of the input beam 16. Therefore, in the setup of Fig. 5 the 15 output intensity of the emitted beam 20 can be dynami cally controlled as a function of the intensity of the input beam 16. The signal processing and modulation may therefore be performed in a purely optical compo nent as opposed to more conentional electro-optical 20 modulator. This enables purely optical interconnec tion, signal processing and eventually logic opera tions with high switching speeds associated with opti cal signal processing. An abrupt increase in light emission may be 25 observed from the slab 17 when the intensity of the input beam 16 increases above a certain threshold value. The switching control parameter used is there fore the power Pi of the relevant spectral components of the input beam 16. Control of this power may be re 30 alized by e.g. electro-optically modulating the input light source 15. The resulting intensity of the emit ted beam 20 obeys the relation P&=c5P; The one or more carbon nanobud molecules 18 exhibiting the non-linear photoluminescence character 35 istics described above may be synthesized, for in stance, by the aforementioned synthesis method dis alOSed in WO2007/057501 Al. To fabricate the slab 17 18 of Fig. 5 these one or more carbon nanobud molecules 18 are deposited on a transparent or semi-transparent substrate composed of e.g. quartz, borosilicate or soft glass. This transparent substrate may be inserted 5 iro, cr csitoned after, the reactor in which the carbon nanobud molecules 18 are synthesized in order to deposit the carbon nanobud molecd es 18 onto the substrate directly from the gas phase, Alternatively the carbon nanobud molecules may first be deposited on 10 a preliminary substrate and a network comprising car bon nanobud molecules may then be transferred from the preliminary substrate onto the final substrate, which may be e.g. the aforementioned transparent or semi transparent substrate, using the method described in 15 patent application FI 20075482, The threshold value for the non-linear ampli fication depends on the process parameters used in the synthesis of the carbon nanobud molecules. The most critical parameters affecting the threshold value are 20 the synthesis temperature which may be e.g. 900 *C and the concentration of additional reagents such as 1-2O and C02. The carbon atoms in the tubular part of the nanobud molecule should be linked to each other by sp*2 bonds to form hexagonal rings. The deposited car 25 bon nanobud molecule or layer of carbon nanobud mole cules 18 on a transparent substrate may be embedded inside a transparent structure (such as the slab 17) by e.g. coating the one or more carbon nanobud mole cules 18 by a transparent or a semi -transparent film. 30 Another non-linear function called saturable absorption may be realized using the simple setup of Fig. 5. With this function e.g. the waveform of the transmitted beam 19 may be shaped or modulated, which may be useful e.g. in pulse regeneration in optical 35 telecommunication networks or in laser components in the generation of short laser pulses. When the carbon nanobud molecules 18 in the slab 17 behave as satur- 19 able absorbers they absorb the electromagnetic radia tion of the input beam 16 as a function of the inte-n sity of the input beam 16. When the intenait of the ineu: beam 16 is lower than the saturation threshold, S absorption is high and a very small proportion of the intensity of the input beam 16 is transmitted through the slab 17. When the intensity exceeds the threshold the carbon nanobud iolecules 18 are no longer able to absorb the radiation of the input beam 16 and the part 10 of the intensity exceeding the saturation threshold (also called the bleaching threshold) gets transmitted through the slab 17. The saturable absorption function is illustrated. in Fi. 11, Saturable absorption may be realized by car 15 hon nanobud molecules directly, or modified or en hanced by e.g. attaching chromophores to reactive sites on the tubular part, on the ends of the tubular part or on the fullerene (or fullerene-like) part of the carbon nanobud molecule . The activity of these 20 chromophores in non-linear optics is based on their hyperpolarizability. Especially phenosafranin (PSF) is a molecule that can be used to create dipoles in the opticalyv actie materin comuriing carbon nanobud molecules. The generation of these dipoles strongly 25 enhances the non-linear properties of the optically active material. As the carbon nanobud molecules are physically and chemically very stable molecules the non-linear optical material obtained by functionaliz ing carbon nanobuds with chromophores allows the use 30 of strong optical fields without risk of degradation of the optical material. An application utilizing a saturable absorber device based on the saturable absorption function of carbon nanobud molecules is a saturable absorber r 35 rmr. These mirrors comprise a reflective surface be hind a slab (such as the slab 17) or a layer performing the saturable absorption function Saturable ab- 20 sorber mirrors may be utilized in e g. lasers as cav ity mirrors for ultrashort pulse generation A satur able absorber rnrrer eased on carbon nanobud molecules may be fabricated by erg. direct deposition from the 5 gas phase, transfer deposition from a primary sub strate or spin coating the synthesized carbon nanobud molecules in a suitable transparent matrix material (e.g. polymer) on a reflecting surface. Carbon nanobud molecules exhibit non-linear 10 saturable absorption characteristics even on their own without chroophore attachments enhancing these non linearities. The non-inearly absorbing carbon ranobud molecules with or without chromophore attachments may bc incorporated in a gel or in an optical adhesive to 15 form a nanocomposite material The matrix material (ie. the eel or the adhesive in this composite may be chosen to possess certain application specific op tical properties. E.g. the refractive index of the ma trix material may be chosen to optically match two 20 sections of an optical fiber, In this case the slab 17 of Fig. 5 corresponds to a piece of the nanocomposite which can take on any geometrical form, This piece may join together the medium in which the input beam 16 proagate s and the medium in which the transmitted 19 25 and the emitted 20 beams propagate The carbon nanobud molecules can alternatively simply be deposited on one or more surfaces in a cut or a break in the medium as presented schematically in Fig, 6. The cut may be par tial (as shown in Fig 6) or complete . In the figure a 30 piece of nanocomposite 17 comprising carbon nanobud molecules 18 is deposited into a via in a solid medium 28 The solid medium may be, for instance, a gain me dium in a laser or in an optical fiber, The optical nanocomposite described above may 35 be fabricated by e.gp taking up synthesized carbon nanobud molecules n a matrix material. . The solution is then e.g. sonicated to generate a carbon nanobud 21 suspension in the matrix material which may be e.-g,. liquid optical coupling gel or optical adhesive. The suspension is then mixed by e.g. ultracantrifugation. Alternatively, the nanocomposite can be produced by, 5 for instance, the method of application F1 20075482 in which the nanobuds are first deposited on a primary substrate and then transferred and inmpregnated into a. secondary substrate. Saturably absorbing films based on carbon 10 nanobud molecules can also be used for passive mode lockino i e.g. pulsed fiber lasers, pulsed wavequide lasers or pulsed ring lasers. In these devices the carbon nanobud based saturable absorbers are used to passively modulate lasing modes inside the laser cav 15 ity to generate ultrashort laser pulses. The saturable absorber may be placed inside the optical cavity, to operate in transmiSsion mode, or outside the optical cavity to operate by interaction with an evanescent wave of the lasing modes. in the latter case interac 20 tion with the evanescent wave can be accomplished by e.g. coating a tapered or a non-tapered fiber laser with a film comprising carbon nanobud molecules or de positing a layer comprising carbon nanobud molecules on a channel or on a planar waveguide of a seiconduc 25 tor laser. The aforementioned pulsed laser devices take advantage of the fast recovery rate ano excellent stability of the carbon nanobud molecules to generate ultrashort laser pulses e.g. in the femtosecond range with great reliability. 30 A schematic example of a passively mode locked laser diode structure utilizing a saturable ab sorber, based on an evanescent wave interacting with carbon nanobud molecules is presented by the longitu dinal cross section of Fig. 7a and by the transverse 35 cross section of Fig. 7b. The structure comprises car bon nanobud mlOOules 29 which are deposi ted on the planar waveguide outside of the active region 30 of a 22 conventiona semiconductor laser The device further comprises an n-type substrate 31 sg. n-GaAs) o which semiconductor films, comprising the active re gion 30 are deposited, The active region 30 may be 5 conventionally fabricated from eg, doped IIl-V semi conductors such as n and -tpe GaAs and MlGaAs in e,cr. an MCCV) reactor and the active region 30 (the gain medium) of the device r comprise mutiple quan tum wells The n-type 32 and the p--type 33 electrical 10 contacts are also visible in Fig. 7a and Fig. 7h. The laser cavity is defined in the longitudinal direction by bleaved facets 34 of the laser chip, which serve the purpose of cavity mirrors. In the lateral direc tion carrier injection may be limited by suitably dop 15 Ing the active region 30 to fabricate insulating car rier guiding regions 35. When the lasting modes are generated in the active region 30 of the device of Fig. 7a and Fig. Tb the modes propagate in the optical cavity defined by 20 the cleaved facets 34 and a portion of the optical flower distribution concentrated into the modes, the evanescent wave, overlaps with the carbon nanobud molecules 29. The saturable sorption of the carbon nanobud molecules 29 passively modulates the optical 25 power of the laser modes resulting in mode locking of the laser, Fig. 8 schematically presents how carbon nanohud molecules 36 may be placed inside the cavity 37 of a mnode locked fiber laser to act as a saturable 30 absorber in transmission mode. In Fig. R the carbon nanobud molecules 36 are placed at the end of the cav ity 37, close to une of the fiber Bragg gratings 38 odfining the length of the laser cavity 37. In this geometry the optical modes guided n the laser cavity 35 37 are modulated by saturable absorption as they pass through the region comprising carbon nanobud molecules 36. In one embodiment of the invention the carbon 23 nanobud molecules may a 1 so be embedded as part of a cavity mirror in a laser to perform the saturable ab sorpticn function for mode locking Fig. 9 schematically presents how the carbon 5 nanobud molecules may be utilized in a saturable ab sorber in a ring laser configuration, to achieve mode locking. The configuration comprises the saturablv ab sorbing element such as the slab 17 comprising carbon nanobud molecules 18 suitably connected to a ring of 10 optical fiber 39 at the input and at the output side of the .slab with erg, optical couplers. The configura tion further comprises a 50:50 coupler 40, a first op tical isolator 41, a second optical isolator 42 and an erbium-doped fiber amplifier (EDFA) 43. The EDFA 43 is 15 p Ily pumped with a pump laser (not shown) in the mode-locked ring laser structure of Fig, 9 the EDFA 43 serves the purpose of gain medium, the first optical isolator 41 prevents back (counter clockwise) propagation of light an the rii 39 and the 20 second optical isolator 42 prevents back propagation of light in the output path 44. The 50:50 coupler cou ples half of the intensity of light propagating in the ring 39 to the output oath 44 and the other half back to the EDFPA 43. The wavelength of the lasing moces 25 supported by the ring laser of Fig. 9 is determined by the op t ical length of the propagation path for these modes around the ring 39, The supported wave lengths have to be such that constructive interference of light is achieved for each wave propagated around the 30 fiber ring 39. This enables Stimulated emission of liQht into the corresponding modes in the FDFA 43. Whe a slab 7 comprising saturably absorbing carbon nanobud molecules 18 is placed within the ring cavity as presented in ig. 9, the saturable absorption func 35 tion performed by he slab 17 modulates the lasing modes resulting in passive mode locking of the ring .aser.
24 Carbon nanobud molecules with saturable ab sorption characteristics aay be synthesized th the method disclosed in W02007/0501 Al-. To attach chro mophores e.g. PSF to these molecules the carbon nano 5 bud molecules can be first treated in acid, e.g. in H:SO4/HNO 3 , to form carboxyl groups on the tubular and/cr the full iene part of the carbon nanobud moie cule, PSF molecules can then be attached to these car boxyl groups by putting the carboxylated carbon nano 10 buds in deionized water containing PSF. Another device setup according to one emzodi ment of the present invention is presented in FIC. 10, This setup comprises a layer 22 comprising non linearly absorbing carbon nanobud molecules 23 in be 15 tween two mirrors, a back mirror 24 and a front mirror 25. The interferometric structure may be used to en hance the interaction of the input light 26 with the carbon nanobud molecules 23. The mirror behinJd the nanobud layer (as viewed from the side of the incident 20 light 26), the back mirror 24, has a vry high reflec tivity so that incident light 26 is not able to escape the structure from the back side. As light impinges the structure it penetrates the less reflective front mIrror 25 and goes through multiple reflections be 25 tween the two mirrors 24. 25 before escaping the structure from the side of the front mirror 25. During each passage through the layer 22 comprisilng carbon nanobud molecules 23 a portion of the incident light 26 interacts with the nanobud layer 22, which in 30 creases the total interaction volume. This type of in terferometer furthermore exhibits spectral selectively as the optical cavity in between the two mirrs 24, 25 only supports certain wavelengths depend ng on the length of the cavity. The device setup of Fig 10 fur 35 thor comprises electrical contat 27 such that a voltage V may he applied over the ayer 22 comprising carbon nanobud molecules 23. This voltage V may be 25 used to e.g. electrical> m1odiate the optical proper ties of the layer 22, In order for the slab 17 of Fig 5 or the aver 22 of Fig. 10 to efficiently act as a non-linear S optical component the light absorbing volume of the slab 17 or the layer 22 should be maximized. To this end the average Tight capturing cross section of the carbon nanobud molecules per one carbon nanobud mole cule should be maximized. The average light capturing 10 cross section maw be increased by ensuring that the molecules are separated from each other in the slab i1 or the layer 22. One way to enhance the separation of carbon nanobud molecules is to separate them from bun dles of these MC 1 ecules already at the deposition 15 stage. This ima be accomplished by eg. exploiting the electric charge difference between bundled carbon nanobuds and individual carbon nanobud riolecules. An increased light capturing cross section results in en hancement of the optii'cal processes in the material 20 comprising carbon nanobud molecules, In one embodiment of the invention the device utili zes a reverse saturable absorption function of the carbon nanobud molecule, In the case of esg ig. 5, reverse saturable absorption means that absorption 25 of the input beam 16 increases as a function of the intensity of the input beam 16. Hence the carbon nano bud molecules I or a piece of material comprising carbon nanobud molecules" such a th slab 17 in Fig 5, may be utilized as an otice i er in protective 30 devices. These devices may find applications in e.g. optical sensors and eye protecrion equipment, The re verse saturable absorption function s illustrated in Fig, 12. T- has surprisingly been observed that the fullerene part of the carbon nanobud molecule effi 35 ciently acts as a reverse saturable absorberst has especially been observed that a fullerene-like strutc ture or a fullerene, eg the buckminsterfullerene Co 26 is an efficient reverse saturable absorber in the car bon nanobud molecule. Additionally, as the tubular part of the carbon nanobud molecule 'y itself or via functionalization bv chromohores exhibits saturable 5 absorption characteristics as described above the carbon nanobud molecules provide an exceptional plat form for anisotropically functioning opticl or opto electronic devices. Additionally, the reverse saturable absorp IC tion function of the fullerene parts of the nanobud molecule can be used, in combination with the satur able absorption function, to limit the intensity of the electromagnetic radiation transmitted through a region caprisng the carbon nanobud molecules in any 15 of the aforementioned embodiments of the invention, By controlling the concentration of fullerene parts in the nanobuds, the reverse saturable absorption effect can be controlled. This function can be used to, for instance, limit the cutout intensity .f a device or 20 protect portions of a device from damage due to excess electromagnetic energy. Since the carbon nanobud molecules exhibit both satuable absorption (the tubular part of the nanobud moleculey and reverse saturable absorption 25 (the fullerene part of the nanobud molecule) charac teristics, these molecules may be easily used to gen erate an input-cutout relation according to Fig. 13 comcionn the saturable absorption and the reverse saturable absorption functionsa This relation may b 20 observed e.g. in the device setup of Fig. 5 between toe input beam 16 and the transmitted beam. 19, This type of a versatile inpt-output function can be effi ciently used in e.g. optical signal processing, pulse regeneration waveform shaping and. optical switching 35 applications. As shown in Fig. 14a, the reverse saturable absorption function combined with the saturable absorption function allows an electromagnetic pulse to be shaped. Fig. 14a illustrates bow the original pulse sequence 45 is modified by the saturable absorption function alone 46, by the reverse saturable absorption 5 function alone 47, and by combined sat.urable and re verse saturable absorption functions 48 according to one embodiment of the invention to produce, for in stance, a more square-shaped pulse having shorter rise and fall times from the wide, poorly formed original 10 pulse sequence 45 having longer rise and fall times. Such a modified pulse is narrower and easier to iso tare by a detection device, thus allowing an increase in the pulse rate and bandwidth of an optical informa tion stream, for instance, in an optical fiber. Im 12 proved pulse separation is shown in Fig, l4 and dog l4d for a pulse before (Fig. 14c) and after (Fig. 14d) reforming with the described method., The ability to increase the pulse rate as a result of narrower pulses becomes evident from Fig, 14b illustrating four dif 20 fervent pulse sequences with differently dashed lines. In these pulse sequences the separate pulses can be readily isolated. Adjustment, for instance, of the concentra tion of fullerene parts in the carbon nanobud mole 25 cules, of the concentration of nanobud molecules in a matrix material, of the diameter of the nanobud moe cules and of the type and amount of functionaLization of the nanobud molecules, ei . with chromophores, can be used to determine the modulation function the car 30 bon nanobuds superimpose on electromagnetic radiation and thus to determine the resulting pulse shape and intensity. By using the polarization resulting from the asymmetrical shape of the carbon nanobud molecule, the 35 carbon nanobud mole.:"cules may be aligned in a specified direction by exposing them to an external electric field, As this alignment dictates the relative oren- 28 tatiJ on of the-S --everse satiab osoibng fullerene pant and the saturabiy absorbing tubular pat of the carbon nanobud molecule it is pss ible to design devices in which an input bean' (e g the input beam 1i of Fig S of electromagnetic 5 radiation experiences saturable or reverse saturable absorption depending on the angle of incidence of the inut beam wi th the carbon nanobud moleciles. As is clear for a Person skilled in the art, t-he 10 invention Is not limited to the examples described haove hut he- emnbdiinents can freely vary within the scope of the claims It is to be understood that, if any prior art 15 publication is referred to herein, such reference does not constitute an admission that the publication forms a part of the common general knowledge in the art, in Australia or any other country. 20 In the claims which follow and in the preceding description of the invention, except where the context requires otherwise due to express language or necessary implication, the word "comprise" or variations such as "comprises" or "comprising" is used in an inclusive sense, 25 ie. to specify the presence of the stated features but not to preclude the presence or addition of further features in various embodiments of the invention. 6042S1 (GHMatters) P8684O.A11.1 PCA8RAL 1i112M4