Article

Charge transfer in steam purified arc discharge single walled carbon nanotubes filled with lutetium halides

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Abstract

In the present work, the effect of doping on electronic properties in bulk purified and filled arc-discharge single-walled carbon nanotubes samples is studied for the first time by in situ Raman spectroelectrochemical method. A major challenge to turn the potential of SWCNTs into customer applications is to reduce or eliminate their contaminants by means of purification techniques. Besides, the endohedral functionalization of SWCNTs with organic and inorganic materials (i.e. metal halides) allows the development of tailored functional hybrids. Here, we report the purification and endohedral functionalization of SWCNTs with doping affecting the SWCNTs. Steam-purified SWCNTs have been filled with selected lutetium(III) halides, LuCl3, LuBr3, LuI3, and sealed using high-temperature treatment, yielding closed-ended SWCNTs with the filling material confined in the inner cavity. The purified SWCNTs were studied using TGA, EDX, STEM and Raman spectroscopy. The lutetium(III) halide-filled SWCNTs (LuX3@SWCNTs) were characterized using STEM, EDX, Raman spectroscopy and in situ Raman spectroelectrochemistry. It was found that there is a charge transfer between the SWCNTs and the encapsulated LuX3 (X = Cl, Br, I). The obtained data testify to the acceptor doping effect of lutetium(III) halides incorporated into the SWCNT channels, which is accompanied by the charge transfer from nanotube walls to the introduced substances.

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... The electronic properties of SWCNTs filled with manganese halogenides [175], iron halogenides [170], cobalt halogenides [190], nickel halogenides [167], zink halogenides, [169], cadmium halogenides [173], luthetium halogenides [184], mercury halogenies [172], and lead halogenides [177] were studied by Raman spectroscopy, near-edge X-ray absorption fine structure spectroscopy, photoemission spectroscopy, and optical absorption spectroscopy and p-doping with the Fermi level shift of −0.05-0.5 eV was revealed. ...
... However, the direction of the charge transfer cannot be deduced from the OAS data ( Figure 6) [212]. The electronic properties of SWCNTs filled with manganese halogenides [175], iron halogenides [170], cobalt halogenides [190], nickel halogenides [167], zink halogenides, [169], cadmium halogenides [173], luthetium halogenides [184], mercury halogenies [172], and lead halogenides [177] were studied by Raman spectroscopy, near-edge X-ray absorption fine structure spectroscopy, photoemission spectroscopy, and optical absorption spectroscopy and p-doping with the Fermi level shift of −0.05-0.5 eV was revealed. ...
... Raman spectroscopy was also used to study the electronic properties of filled SWCNTs in Refs. [155,156,163,164,167,169,170,172,173,175,177,[182][183][184]190,200,207,211]. Raman spectra revealed the changes in the radial breathing mode and G-mode, such as shifts in the peaks and modification of the band profile. ...
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This review discusses the phemenology of filling, the investigation of kinetics, and the electronic properties for applications of filled single-walled carbon nanotubes (SWCNTs), and summarizes five main achievements that were obtained in processing the spectroscopic data of SWCNTs filled with metal halogenide, metal chalcogenide, metal and metallocenes. First, the methods of processing kinetic data were developed to reveal precise trends in growth rates and activation energies of the growth of SWCNTs. Second, the metal-dependence of kinetics was revealed. Third, metallicity-sorted (metallic and semiconducting) SWCNTs were filled with a range of substances and the electronic properties were investigated. Fourth, new approaches to processing the data of spectroscopic investigations of filled SWCNTs were developed, which allowed more reliable and precise analysis of the experimental results. Fifth, the correlation between the physical and chemical properties of encapsulated substances and the electronic properties of SWCNTs were elucidated. These points are highlighted in the review.
... The most popular among them are metal halogenides. SWCNTs were filled with metal fluorides (SnF2 [122]), metal chlorides (sodium/cesium/copper/silver/tantal)Cl [113,[123][124][125][126][127][128][129][130][131][132][133], (manganese/iron/cobalt/nickel/zinc/cadmium/mercury/palladium/lead)Cl2 [108,126,127,[134][135][136][137][138][139][140][141][142][143][144][145], (iron/yttrium/ruthenium/gold/lanthan/neodym/samarium/europium/gadolinium/terbium/thulium/praseodymium/holmium/erbium/ytterbium/luthetium)Cl3, Al2Cl6 [102,103,107,108,121,126,127,134,139,142,[146][147][148][149][150][151][152], (zirkonium/hafnium/platinum/thorium)Cl4 [108,127,139,[153][154][155][156], MoCl5 [126], WCl6 [126,127], (KCl)x(UCl4)y [113,157], metal bromides (cesium/copper/silver)Br [113,123,124,127], (manganese/iron/cobalt/nickel/zinc/cadmium/lead)Br2 [135][136][137][138]141,143,145,158,159]), TbBr3 [151], LuBr3 [152], metal iodides (lithium/sodium/potassium/rubidium/cesium/copper/silver)I [123,124,127,[154][155][156][157][160][161][162][163][164][165][166][167][168], (calcium/strontium/barium/iron/cobalt/zinc/cadmium/lead)I2 [137,138,141,145,[154][155][156][169][170][171], (lanthan/terbium/luthetium)I3, Al2I6 [139,151,152,172,173], SnI4 [126,127]), their mixtures [113,126,127,154,157,160,174,175], and other substances [176][177][178][179][180]. ...
... The most popular among them are metal halogenides. SWCNTs were filled with metal fluorides (SnF2 [122]), metal chlorides (sodium/cesium/copper/silver/tantal)Cl [113,[123][124][125][126][127][128][129][130][131][132][133], (manganese/iron/cobalt/nickel/zinc/cadmium/mercury/palladium/lead)Cl2 [108,126,127,[134][135][136][137][138][139][140][141][142][143][144][145], (iron/yttrium/ruthenium/gold/lanthan/neodym/samarium/europium/gadolinium/terbium/thulium/praseodymium/holmium/erbium/ytterbium/luthetium)Cl3, Al2Cl6 [102,103,107,108,121,126,127,134,139,142,[146][147][148][149][150][151][152], (zirkonium/hafnium/platinum/thorium)Cl4 [108,127,139,[153][154][155][156], MoCl5 [126], WCl6 [126,127], (KCl)x(UCl4)y [113,157], metal bromides (cesium/copper/silver)Br [113,123,124,127], (manganese/iron/cobalt/nickel/zinc/cadmium/lead)Br2 [135][136][137][138]141,143,145,158,159]), TbBr3 [151], LuBr3 [152], metal iodides (lithium/sodium/potassium/rubidium/cesium/copper/silver)I [123,124,127,[154][155][156][157][160][161][162][163][164][165][166][167][168], (calcium/strontium/barium/iron/cobalt/zinc/cadmium/lead)I2 [137,138,141,145,[154][155][156][169][170][171], (lanthan/terbium/luthetium)I3, Al2I6 [139,151,152,172,173], SnI4 [126,127]), their mixtures [113,126,127,154,157,160,174,175], and other substances [176][177][178][179][180]. ...
... The most popular among them are metal halogenides. SWCNTs were filled with metal fluorides (SnF2 [122]), metal chlorides (sodium/cesium/copper/silver/tantal)Cl [113,[123][124][125][126][127][128][129][130][131][132][133], (manganese/iron/cobalt/nickel/zinc/cadmium/mercury/palladium/lead)Cl2 [108,126,127,[134][135][136][137][138][139][140][141][142][143][144][145], (iron/yttrium/ruthenium/gold/lanthan/neodym/samarium/europium/gadolinium/terbium/thulium/praseodymium/holmium/erbium/ytterbium/luthetium)Cl3, Al2Cl6 [102,103,107,108,121,126,127,134,139,142,[146][147][148][149][150][151][152], (zirkonium/hafnium/platinum/thorium)Cl4 [108,127,139,[153][154][155][156], MoCl5 [126], WCl6 [126,127], (KCl)x(UCl4)y [113,157], metal bromides (cesium/copper/silver)Br [113,123,124,127], (manganese/iron/cobalt/nickel/zinc/cadmium/lead)Br2 [135][136][137][138]141,143,145,158,159]), TbBr3 [151], LuBr3 [152], metal iodides (lithium/sodium/potassium/rubidium/cesium/copper/silver)I [123,124,127,[154][155][156][157][160][161][162][163][164][165][166][167][168], (calcium/strontium/barium/iron/cobalt/zinc/cadmium/lead)I2 [137,138,141,145,[154][155][156][169][170][171], (lanthan/terbium/luthetium)I3, Al2I6 [139,151,152,172,173], SnI4 [126,127]), their mixtures [113,126,127,154,157,160,174,175], and other substances [176][177][178][179][180]. ...
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Here, we present a review of the major achievements in kinetics, electronic properties, and engineering in the Fermi level of single-walled carbon nanotubes (SWCNTs). Firstly, the kinetics of metal-filled SWCNTs were revealed with precision over several minutes. Secondly, the growth rates of nanotubes were calculated. Thirdly, the activation energies of nanotubes were measured. Fourthly, the methods of the quantitative analysis of the doping level were developed. Indeed, only qualitative analysis has been previously performed. The quantitative analysis allowed us to obtain quantitative data on charge transfer. Fifthly, the correlation between the physical properties, chemical properties, electronic properties of SWCNTs was elucidated.
... In this case, the Raman scattering intensities can be enhanced by several orde magnitude [27]. Raman spectroscopy was applied to investigate the modified electronic structur SWCNTs filled with MnCl2, MnBr2 [35,36], FeCl2, FeBr2, FeI2 [12], CoBr2 [13], NiCl2, N [37], ZnCl2 [20], ZnCl2, ZnBr2, ZnI2 [14], AgCl, AgBr, AgI [15], AgCl [38,39], CuCl [17], [40,41], CuCl, CuBr, CuI [18], CdCl2 [20,42], CdCl2, CdBr2, CdI2 [16], PbCl2, PbBr2, PbI2 SnF2 [44], RbI [45], RbAg4I5 [46], TbCl3 [20,47,48], TbBr3, TbI3 [48], TmCl3 [24,47], P Raman spectroscopy was applied to investigate the modified electronic structure of SWCNTs filled with MnCl 2 , MnBr 2 [35,36], FeCl 2 , FeBr 2 , FeI 2 [12], CoBr 2 [13], NiCl 2 , NiBr 2 [37], ZnCl 2 [20], ZnCl 2 , ZnBr 2 , ZnI 2 [14], AgCl, AgBr, AgI [15], AgCl [38,39], CuCl [17], CuI [40,41], CuCl, CuBr, CuI [18], CdCl 2 [20,42], CdCl 2 , CdBr 2 , CdI 2 [16], PbCl 2 , PbBr 2 , PbI 2 [43], SnF 2 [44], RbI [45], RbAg 4 I 5 [46], TbCl 3 [20,47,48], TbBr 3 , TbI 3 [48], TmCl 3 [24,47], PrCl 3 [19,47], LuCl 3 , LuBr 3 , LuI 3 [49], HgCl 2 [50], GaSe, GaTe [21,22], SnS, SnTe [22,23], Bi 2 Se 3 [22] and Bi 2 Te 3 [24], Ag [24,[51][52][53], Cu [53,54], ferrocene [55][56][57][58], cobaltocene [59,60] and nickelocene [61][62][63]. ...
... MnCl 2 , MnBr 2 Shifts and changes in relative intensities of peaks in the RBM and G-bands [35,36] FeCl 2 , FeBr 2 , FeI 2 Shifts and changes in relative intensities of peaks in the RBM and G-bands [12] CoBr 2 Shifts and changes in relative intensities of peaks in the RBM and G-bands [13] NiCl 2 , NiBr 2 Shifts and changes in relative intensities of peaks in the RBM and G-bands [37] ZnCl 2 Shifts and changes in relative intensities of peaks in the RBM and G-bands [20] ZnCl 2 , ZnBr 2 , ZnI 2 Shifts and changes in relative intensities of peaks in the RBM and G-bands [14] AgCl, AgBr, AgI Shifts and changes in relative intensities of peaks in the RBM and G-bands [15] AgCl Shifts and changes in relative intensities of peaks in the RBM and G-bands [38,39] CuCl Shifts and changes in relative intensities of peaks in the RBM and G-bands [17] CuI Shifts and changes in relative intensities of peaks in the RBM and G-bands [40,41] CuCl, CuBr, CuI Shifts and changes in relative intensities of peaks in the RBM and G-bands [18] CdCl 2 Shifts and changes in relative intensities of peaks in the RBM and G-bands [20,42] CdCl 2 , CdBr 2 , CdI 2 Shifts and changes in relative intensities of peaks in the RBM and G-bands [16] PbCl 2 , PbBr 2 , PbI 2 Shifts and changes in relative intensities of peaks in the RBM and G-bands [43] SnF 2 No modifications [44] RbI Shifts and changes in relative intensities of peaks in the RBM and G-bands [45] RbAg 4 I 5 Shifts and changes in relative intensities of peaks in the RBM and G-bands [46] TbCl 3 Shifts and changes in relative intensities of peaks in the RBM and G-bands [20,47,48] TbBr 3 , TbI 3 Shifts and changes in relative intensities of peaks in the RBM and G-bands [48] TmCl 3 Shifts and changes in relative intensities of peaks in the RBM and G-bands [24,47] PrCl 3 Shifts and changes in relative intensities of peaks in the RBM and G-bands [19,47] LuCl 3 , LuBr 3 , LuI 3 Shifts and changes in relative intensities of peaks in the RBM and G-bands [49] HgCl 2 Shifts and changes in relative intensities of peaks in the RBM and G-bands [50] GaSe, GaTe Shifts and changes in relative intensities of peaks in the RBM and G-bands [21,22] SnS, SnTe No modifications [22,23] Bi 2 Se 3 Slight modifications [22] Bi 2 Te 3 Slight modifications [24] Ag Shifts and changes in relative intensities of peaks in the RBM and G-bands [24,[51][52][53] Cu Shifts and changes in relative intensities of peaks in the RBM and G-bands [53,54] Ferrocene No modifications [55][56][57][58] Cobaltocene No modifications [59,60] Nickelocene No modifications [61][62][63] The G -LO -mode (Breit-Wigner-Fano mode) in the G-line of metallic SWCNTs is also affected by doping, but the underlying mechanism differs greatly. In the pristine metallic SWCNTs, there is a Kohn anomaly in the phonon dispersion, which results in a sizable phonon softening of the LO mode [74,75]. ...
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... Several groups are working on the topic. The groups of Jeremy Sloan in the UK [4,5], Marianna V. Kharlamova in Austria and Slovakia [6,7], Hisanori Shinohara in Japan [8,9], Antonio Setaro and Stephanie Reich in Germany [10,11], and Gerard Tobias in Spain [12,13]. ...
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... Due to the hollow morphology, CNTs are used in the design of so-called endohedral complexes with inorganic substances, i.e. "carbon nanotube -encapsulate in the nanotube cavity" composites, where encapsulates can be represented by individual atoms or nanofibers of simple substances (phosphorus [11,12], iodine [13], gold [14], iron and cobalt [15], copper [16]) and by compounds such as metal chalcogenides and halides [17][18][19][20][21]. Such composites were proposed as containers for the delivery of drugs [22][23][24] and contrast agents [25][26][27][28][29] to cells and organs, for the production of supercapacitors [30], as nanoreactors for the synthesis of novel materials [31,32], nanothermometers [33], and in thermoelectrics [34]. ...
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... Several groups work on filled carbon nanotubes in various countries across Europe, including Austria. Besides investigations of different molecules [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18][19], for the modification of the electronic properties, the SWCNTs were filled with halogenides of 3d-metal MX2 (M = Fe, Co, Ni, Mn, Zn, Cu, X = Cl, Br, I) [20][21][22][23][24][25][26][27][28][29][30][31][32][33], 4d-metal MX2 (M = Cd, Ag, X = Cl, Br, I) [34][35][36][37][38][39], 5dmetals MX2 (M = Hg, X = Cl) [40] and 4f-metal MX3 (M = Pr, Tb, Tm, Lu, X = Cl, Br, I) [41][42][43][44][45], 6p-metal MX2 (M = Pb, X = Cl, Br, I) [46], 5s-metal MX (M = Rb, X = I) [47] [77,78]. ...
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In this paper we show the advantages of transparent high conductive films based on filled single-wall carbon nanotubes. The nanotubes with internal channels filled with acceptor molecules (copper chloride or iodine) form networks demonstrating significantly improved characteristics. Due to the charge transfer between the nanotubes and filler, the doped-nanotube films exhibit the electrical sheet resistance drop by an order of magnitude together with a noticeable rise of films transparency in the visible and near-infrared spectral range. The thermoelectric power measurements show a significant improvement of air-stability of nanotube network in course of the filling procedure. For the nanotube films with the initial transparency of 87% at 514 nm and the electrical sheet resistance of 862 Ohm/sq we observed the improvement of transparency up to 91% and the decrease of sheet resistance down to 98 Ohm/sq. The combinations of nanotube synthesis technique and molecules for encapsulation have been optimized for applications in optoelectronics.
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Short carbon nanotubes (CNTs) are desired for a variety of applications. As a consequence, several strategies have been reported to cut and shorten the length of as-produced CNTs via chemical and physical routes. The efficiency of a given strategy largely depends on the physico-chemical characteristics of the CNTs employed. In order to be able to directly compare the advantages and disadvantages of commonly used protocols, a single batch of chemical vapor deposition single-walled CNTs (SWCNTs) and a batch of multi-walled CNTs (MWCNTs) were subjected to four cutting/shortening strategies, namely acid cutting, piranha treatment, steam shortening and ball milling. The length distribution was assessed by means of scanning electron microscopy. Sample purity and CNT wall structure were determined by Raman spectroscopy, thermogravimetric analysis and magnetic measurements. Within the employed experimental conditions, piranha treatment turned out to be the most efficient to achieve short SWCNTs with a narrow length distribution in a good yield, whereas a mixture of sulfuric/nitric acid was preferred in the case of MWCNTs. A subsequent short steam treatment allowed to remove functional groups present in the samples, leading to median length distributions of 266 nm and 225 nm for SWCNTs and MWCNTs respectively after the combined protocols.
Article
Filled carbon nanotubes are of interest for a wide variety of applications ranging from sensors to magnetoelectronic devices and going through the development of smart contrast and therapeutic agents in the biomedical field. In general, regardless of the method employed, bulk filling of carbon nanotubes results in the presence of a large amount of external non-encapsulated material. Therefore further processing is needed to achieve a sample in which the selected payload is present only in the inner cavities of the nanotubes. Here, we report on a straightforward approach that allows the removal of non-encapsulated compounds in a time efficient and environmentally friendly manner, using water as a ‘green’ solvent, whilst minimizing the residual waste. The results presented herein pave the way towards the production of large amounts of high-quality closed-ended filled nanotubes, also referred to as carbon nanocapsules, readily utilizable in the foreseen applications.
Article
In this work, single-walled carbon nanotubes (SWCNTs) were filled with manganese chloride and manganese bromide by a capillary filling method. The electronic properties of the filled SWCNTs were investigated by Raman spectroscopy and X-ray photoelectron spectroscopy. It was found that the encapsulated manganese halogenides led to hole doping of the SWCNTs due to the charge transfer from the nanotubes to the encapsulated compounds. The embedded MnCl2 had stronger doping effect on the SWCNTs than MnBr2.
Article
A major challenge to turn the potential of carbon nanotubes (CNTs) into customer applications is to reduce or eliminate their toxicity. Taking into account health and safety concerns, intensified research efforts have been conducted to improve the biocompatibility of CNTs, including the development of new shortening and purification strategies. Ideally, the methods used for improving the biocompatibility of CNTs should not alter the electronic properties of CNTs. Herein, we report on the shortening of a sample containing single-walled and double-walled CNTs using steam and obtain new insights in the properties of the steam-treated CNTs. The present study shows that short CNTs (median length ca. 200 nm) can be obtained under the reported conditions. Raman analysis reveals that wider and outer nanotubes undergo more significant changes than the narrower and inner ones, especially after a prolonged steam treatment.
Article
In the vast field of functionalization routes to carbon nanoforms, the fulfillment of such critical requirements as quick and nonharsh methods, good dispersibility, introduction of reactive groups, short reaction time, and low cost can be quite challenging. Traditional thermally induced diazonium chemistry on single-walled carbon nanotubes (SWCNTs) is revisited by using commercial anilines and providing useful insight into the versatility of this approach. Functionalized SWCNTs with multiple controllable features, such as degree (and ratio) of coverage, orthogonalization, doping, and high water dispersibility, are obtained by introducing benzenesulfonic acid and benzylamine moieties. The scenario opens up an avenue to address relevant applications in which most functionalization methods could not be applied in a straightforward way.
Article
Although chemical functionalization of single-walled carbon nanotubes was extensively studied, in many cases detailed information about the influence of the nanotube metallicity and diameter is missing. Here, we present an X-ray photoemission and absorption spectroscopy study of endohedrally functionalized carbon nanotubes with different diameters, where Ni(II)acetylacetonate molecules are reacted to tailor the nanotubes’ electronic properties. The filling factor is found to be dependent on the SWCNT base material used. We trace the reaction process of the filling material at several annealing steps and reveal their dependence on annealing temperature, which allows doping of nanotubes to be controlled.
Article
Considerable progress has been made in the last several years in the fields of investigation and understanding of the influence of encapsulated substances on the electronic properties of single-walled carbon nanotubes (SWCNTs). Relevant data on the modified electronic properties of filled SWCNTs were obtained. The possibility of achieving both acceptor and donor doping and precise changes of the SWCNT doping level by the filling of channels and transformation of incorporated substances was demonstrated. This article presents a comprehensive review of the current status of the research on the electronic properties of filled SWCNTs. The review begins with a brief description of basic aspects of the band theory of solids and peculiarities of the band structure and electronic properties of SWCNTs. The next part of the review is dedicated to a systematization and description of different methods for modification of the SWCNT electronic properties. Then, the review introduces filling methods of SWCNT inner channels. The main part of the review is dedicated to an analysis, systematization and generalization of the up-to-date reported results on experimental and theoretical investigations of the electronic properties of filled SWCNTs and nanostructures obtained as result of chemical reactions inside the SWCNT channels. Finally, the possible applications of filled nanotubes are highlighted.
Article
Praseodymium chloride (PrCl3) was encapsulated into channels of 1.4 nm diameter single-walled carbon nanotubes (SWCNTs) by a capillary filling method. The high-resolution transmission electron microscopy data demonstrated a high filling factor of the nanotubes and the formation of one-dimensional (1D) PrCl3 nanocrystals. The optical absorption, Raman spectroscopy, and X-ray photoelectron spectroscopy data testified to the filling-induced lowering of the Fermi level of the nanotubes as a result of the electron transfer from the SWCNTs to the embedded PrCl3. The density functional theory modeling showed the absence of local chemical interactions between the nanotubes and the 1D crystals. It was found that the incorporated PrCl3 has stronger influence on the electronic properties of metallic nanotubes than semiconducting SWCNTs.
Article
In the present work, a detailed Raman spectroscopy investigation on the single-walled carbon nanotubes (SWCNTs) filled with praseodymium chloride, terbium chloride and thulium chloride was performed. The salts were incorporated inside the SWCNTs by a capillary filling method using melts, and the high-resolution transmission electron microscopy data proved the high filling degree of the nanotube channels. A thorough analysis of the radial breathing mode and G-band of the Raman spectra of the pristine and filled SWCNTs showed that the encapsulated salts cause acceptor doping of the host nanotubes, and the doping efficiency depends on the compound. The incorporated thulium chloride has the strongest doping effect on the SWCNTs, whereas praseodymium chloride has the weakest effect. It was found that the encapsulated salts modify more significantly the electronic structure of metallic nanotubes than semiconducting SWCNTs.
Article
Raman excitation profiles for 55 homogeneously deformed single- walled carbon nanotubes with diameters from 0.7 to 1.2 nm are calculated and systematically analyzed. Torsion and uniaxial strain produce a number of interesting observable effects, important in designing electromechanical devices. The deformations shift phonon energies. The torsion alone causes mixing of high energy modes, while the uniaxial compression generates interchange of their vibrating directions. It is found that electronic transition energies depend almost linearly on deformation; for some tubes, they cover the entire visible spectrum, making them perfectly tunable light absorbers. On the other hand, this shift causes a number of interference effects. The type of interference and its influence on the excitation profiles is completely determined by electron−phonon coupling matrix elements. Collapse of Raman intensity in resonant scattering experiments is explained either by destructive interference or by moving away from the resonant window. Finally, the deformation causes increase of the lower high energy mode resonant intensity, which should further produce the appreciable change in the G mode profil
Article
In this work the internal channels of the single-walled carbon nanotubes (SWCNTs) were filled with cadmium chloride, cadmium bromide, and cadmium iodide by a capillary method using melts of these salts. The influence of incorporated chemical compounds on the electronic properties of the carbon nanotubes was investigated by optical absorption spectroscopy, Raman spectroscopy, near edge X-ray absorption fine structure spectroscopy, and X-ray photoelectron spectroscopy. It was found that there is the chemical bonding between carbon atoms of nanotube walls and metal atoms of encapsulated CdX2 nanocrystals. The obtained data testify acceptor doping effect of cadmium halogenides incorporated into the SWCNT channels, which is accompanied by the charge transfer from nanotube walls to introduced substances.
Article
The D band in the Raman spectra of single walled carbon nanotubes is considered as an indicator of defects in carbon nanotubes. However, its dependence on charge-transfer doping is generally ignored, despite the studied samples are often naturally doped. We studied the intensity of the D band, the ratio of the intensities of the D band and TG band (ID/ITG) and the ratio of the intensities of the D and G′ band (ID/IG′) in the Raman spectra of the single walled carbon nanotubes in dependence on a doping level. We tested two laser excitation energies viz 2.41 and 1.92eV, which are in resonance with semiconducting and metallic tubes, respectively in our sample. It is shown that the D band intensity is significantly attenuated in doped carbon nanotubes sample for both semiconducting and metallic tubes. The ID/ITG ratio is weakly dependent on doping for semiconducting tubes but for metallic tubes the ID/ITG ratio exhibits strong dependence on doping. The ID/IG′ ratio is suggested for evaluation of the defects in carbon nanotubes samples since it is less sensitive to doping both for semiconducting and metallic tubes. Nevertheless, for highly doped samples even the ID/IG′ ratio exhibits significant dependence on doping level.
Article
We show that D-mode Raman scattering in single-walled carbon nanotubes is due to a double-resonant Raman process. The unusual shift of the D-mode frequency with excitation energy is even expected for a single nanotube. The magnitude of the shift and the D-mode frequency depend strongly on the tube’s diameter and chirality. Only tubes with (n1-n2)/3n integer contribute to the D-mode spectrum because of the particular electronic structure of carbon nanotubes.
Article
Over the last 10 years, carbon nanotubes have offered a unique system for the study of Raman spectra in one-dimensional systems, and at the same time Raman spectroscopy has provided a widely used and powerful tool for the characterization of single walled carbon nanotubes (SWNTs). The 10 year history of Raman scattering in SWNTs is reviewed here and future prospects for the field are discussed.
Article
The structural and electronic charge distributions of single-wall carbon nanotubes (SWNTs) chemically modified with Ag and CrO3 were investigated by ab initio methods. Using first-principles spin-polarized calculations, we studied the structural and electronic behavior of Ag atoms and CrO3 molecules interacting with an (8, 0) semiconducting SWNT. We have found that the Ag atom behaves as an electron donor and the CrO3 as an electron acceptor in the presence of the SWNT. Resonance Raman experiments performed on Ag and CrO3-adsorbed SWNTs confirm the donor and acceptor behavior, respectively.
Chapter
The electrochemistry of carbon nanotubes is reviewed with the aim of summarizing what we can learn using these techniques, and what are the potential applications of nanotubes as electrode materials. Electrochemical charging changes the electronic structure. Consequently, electrochemistry and in-situ spectroelectrochemistry provide versatile tools for the investigation of fundamental effects related to the electronic structure of carbon nanotubes. This approach is compatible with chemical doping, but the electrochemical charging of nanotubes allows for precise control of the doping conditions. Salient (spectro)electrochemical data accumulated during the last ten years on SWNTs, DWNTs and fullerene peapods are here reviewed.
Article
In the last decade, many theoretical and experimental achievements have been made in the photophysics of single wall carbon nanotubes (SWNTs). Such accomplishments allowed us to gain a deep understanding of the photophysics behind the transition energy (Eii) and the radial breathing mode frequency (ωRBM) dependence on nanotube chirality (n, m). This work is devoted to assemble and discuss what has been done on the research of the SWNT electronic and vibrational properties, based on the radial breathing mode (RBM) resonance Raman spectroscopy. Attention is directed to the understanding of how a change in the environment changes the correlation between (Eii,ωRBM) and (n, m). From the analysis of several data in the literature, we derive a simple routine for the (Eii,ωRBM)→(n,m) assignment.
Article
A review is presented on the resonance Raman spectra from one isolated single wall carbon nanotube. The reasons why it is possible to observe the spectrum from only one nanotube are given and the important structural information that is provided by single nanotube spectroscopy is discussed. Emphasis is given to the new physics revealed by the various phonon features found in the single nanotube spectra and their connection to spectra observed for single wall nanotube bundles. The implications of this work on single wall carbon nanotube research generally are also indicated.
Article
This Minireview is a critical survey of results accumulated during the last decade on the characterization of carbon nanotubes using a combination of electrochemical and spectroscopic methods. The article updates earlier reviews on the topic with special emphasis to recent progress in the field.
Article
The influence of the electrode potential on the electronic structure of individual single-walled carbon nanotubes is studied using Raman spectroscopy. By analyzing the radial breathing mode intensity versus electrode potential profiles in the Raman spectra at many different laser excitation energies, we show that the charging of individual carbon nanotubes causes a broadening of the resonant Raman profiles (resonance window). This effect is observed for both a semiconducting and a metallic tube. The broadening of the resonance Raman profiles already begins at potentials where the first electronic states of a particular tube are filled or depleted. The important consequence of this effect is a striking difference between the Raman intensity versus potential profiles of metallic and semiconducting tubes. While for a metallic tube the intensity of the Raman signal is attenuated at potentials which deviate slightly from 0 V, for a semiconducting tube, the Raman intensity is significantly attenuated only after the electrode potential reaches the first van Hove singularity. Furthermore, for the metallic tube, a strong asymmetry is found in the bleaching of the Raman signal with respect to positive and negative potentials, which results from the different energy bandwidth for the pi* band and the pi band.
Article
A detailed analysis of the in situ Raman spectroelectrochemical behavior of individual semiconducting single-walled carbon nanotubes (SWCNTs) is presented. Special attention has been paid to the development of the tangential (TG) mode frequency, which shifts when the externally applied potential Ve is shifted away from Ve=0. The magnitude and direction (upshift or downshift) of the tangential mode band has been found to be dependent on the diameter of the semiconducting tubes. For negative charging, the small-diameter tubes exhibit a downshift while the large-diameter tubes exhibit an upshift. This behavior is explained by a competition between two effects which cause opposite shifts in the TG mode frequency during negative charging: a phonon renormalization effect and a C-C bond weakening during the charging process. Positive charging always causes an upshift of the TG mode frequency. However, the magnitude of the upshift is dependent on the tube diameter.
Article
Purification and shortening of single-walled carbon nanotubes (SWNTs) is carried out by treatment with steam. During the steam purification the graphitic shells coating the catalytic metal particles are removed. Consequently, the exposed catalytic particles can be easily dissolved by treatment with hydrochloric acid. No damage to the carbon nanotube tubular structure is observed, even after prolonged treatment with steam. Samples are characterized by HRTEM, TGA, magnetic measurements, Raman spectroscopy, AFM, and XPS.
Article
Single-walled carbon nanotubes (SWNTs) have strong potential for molecular electronics, owing to their unique structural and electronic properties. However, various outstanding issues still need to be resolved before SWNT-based devices can be made. In particular, large-scale, air-stable and controlled doping is highly desirable. Here we present a method for integrating organic molecules into SWNTs that promises to push the performance limit of these materials for molecular electronics. Reaction of SWNTs with molecules having large electron affinity and small ionization energy achieved p- and n-type doping, respectively. Optical characterization revealed that charge transfer between SWNTs and molecules starts at certain critical energies. X-ray diffraction experiments revealed that molecules are predominantly encapsulated inside SWNTs, resulting in an improved stability in air. The simplicity of the synthetic process offers a viable route for the large-scale production of SWNTs with controlled doping states.
Article
Purification and opening of carbon nanotubes has been carried out by treatment of as-made single-wall carbon nanotubes (SWNTs) with pure steam at 1 atm pressure. Treated samples have been characterized by high-resolution transmission electron microscopy and IR and Raman spectroscopy. Comparison between the steam purification and the standard nitric acid purification treatment shows that steam is less aggressive toward damage to the tubular nanotube wall structure and forms fewer functional groups.
Article
The detailed analysis of the in situ Raman spectroelectrochemical behavior of single walled carbon nanotube (SWCNT) bundles is presented. The Raman modes of metallic SWCNTs exhibit striking changes even before the potential of the first van Hove singularity is achieved. Special attention has been paid to the development of the tangential (TG) mode broadening, which subsequently vanishes if the potential is shifted away from V = 0. The tangential mode band has been fitted by four components. During the electrochemical doping, three components of the tangential mode follow the predictions of a theoretical model for the LO modes of metallic tubes based on the Kohn anomaly. On the other hand, the behavior of the fourth component is consistent with a model based on electron-plasmon coupling. The TO mode of metallic tubes has been identified only at a doping level corresponding to 1.0 V or above. Our results also indicate an asymmetry in the behavior of the TG mode for positive electrode potentials relative to negative ones.
  • S Sandoval
  • M Kierkowicz
  • E Pach
  • B Ballesteros
  • G Tobias
S. Sandoval, M. Kierkowicz, E. Pach, B. Ballesteros, G. Tobias. MethodsX 5 (2018) 1465-1472