Aluminum nitride nanotubes

An AlN nanotube (AlNNT) was theoretically predicted in 2003. In comparison with the carbon nanotubes, the AlNNTs are wide-band-gap nanostructures with high reactivity, high thermal stability and sharp electronic sensitivity toward some chemicals.
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  REVIEW Aluminum nitride nanotubes Maziar Noei 1 • Hamed Soleymanabadi 2 • Ali Ahmadi Peyghan 3 Received: 2 August 2016/Accepted: 14 October 2016   Institute of Chemistry, Slovak Academy of Sciences 2016 Abstract  An AlN nanotube (AlNNT) was theoreticallypredicted in 2003. In comparison with the carbon nan-otubes, the AlNNTs are wide-band-gap nanostructures withhigh reactivity, high thermal stability and sharp electronicsensitivity toward some chemicals. The B3LYP predicts anHOMO–LUMO gap of 3.74–4.27 eV for  zigzag  AlNNTs,while the experimental bad gap of bulk AlN is about6.28 eV. The lowest strain energy of AlNNTs relative to itsAlN nanosheet compared to the nanosheets of carbon andBN nanotubes with an equivalent diameter suggests thefeasibility of AlNNT synthesis from its nanosheet. Theo-retical methods predict a Young’s Modulus of about453 GPa for AlNNTs that is smaller than that of carbon(1 TPa), BN (870 GPa) and GaN (796 GPa) nanotubes. In2003, the faceted single-crystalline hexagonal AlNNTswere synthesized and extensively explored by means of density functional theory calculations. Several works havesuggested different potential applications for AlNNTsincluding chemical sensors, hydrogen storage, gas adsor-bent, and electron field emitter. This review is a compre-hensive study on the latest achievements in the structuralanalyses, synthesis, and property evaluations based on thecomputational methods on the AlNNTs in the light of thedevelopment of nanotubes. Keywords  Nanostructures based on AlN    Aluminumnitride nanotube    Computational study    Wide-band-gapsystems    Sensor Introduction From the time when carbon nanotubes (CNTs) have beendiscovered (Iijima 1991) and their extensive possibleapplications (Beheshtian et al. 2012a, b, c, d, e, f , g, h, i, j; Parlayici et al. 2015; Baei et al. 2012a, b, c; Robati et al. 2016; Shamsudin et al. 2013; Sreekala et al. 2013; Saha and Das 2014; Goodarzi et al. 2015), intensive attentions have been devoted to non-carbon nanotubes (Beheshtianand Peyghan 2013; Peyghan and Bagheri 2012; Baei et al. 2012a, b, c, 2013; Beheshtian et al. 2013a, b, c, d, e; Peyghan et al. 2012a, b). Examples are the nanotubes of  B x C y N z  composites, metal oxides such as MgO, ZnO andWS 2 , the halogen compound of NiC l2 , silica and polyani-line nanotubes (Altoe et al. 2003; Stejskal et al. 2009; Kim et al. 2011; Hacohen et al. 1998; Cui et al. 2012). Among these compounds, group III nitride nanostructured materi-als are mostly fascinating because the wurtzite nitridesyield a continuous alloy structure with variable band gapsfrom 1.9 to 6.2 eV (Beheshtian et al. 2012a, b, c, d, e, f , g, h, i, j, 2013a, b, c, d, e; Peyghan et al. 2013a, b, c). The AlN is a wide-band-gap material, exhibiting high hardness, highstability, high thermal conductivity, and low coefficient of thermal expansion, and it is frequently used in thin filmdevices as a substrate (Yim et al. 1973). During the lastdecade, numerous efforts have been dedicated to synthesis,characterization, and potential applications of AlN nan-otubes (AlNNTs) (Balasubramanian et al. 2004; Yin et al.2005). The most promising applications include chemicalsensors, hydrogen storage, and field emitters (Baei et al. &  Ali Ahmadi 1 Department of Chemistry, Mahshahr Branch, Islamic AzadUniversity, Mahshahr, Iran 2 Young Researchers and Elite Club, Yadegar-e-ImamKhomeini (RAH) Shahr-e-Rey Branch, Islamic AzadUniversity, Tehran, Iran 3 Young Researchers and Elite Club, Islamshahr Branch,Islamic Azad University, Islamshahr, Iran  1 3 Chem. Pap.DOI 10.1007/s11696-016-0015-5 Downloaded from  2012a, b, c; Noei et al. 2015; Shi et al. 2005; Wang et al. 2009; Ahmadi et al. 2012). This contribution provides a comprehensive review on the AlNNT field, and systemat-ically summarizes respected successes in synthesis, mor-phology, potential applications and predictions on thevarious properties. Theoretical prediction Zhang and Zhang (2003) have theoretically explored thepossibility of synthesis and different properties of AlNNTsusing different models (Fig. 1). The nanotube structure whichwas studied in their work was single-walled with an  armchair  chirality, and the geometries were relaxed at the Hartree–Fock (HF) level of theory with 3-21G* basis set. Theydeduced that AlNNTs are thermodynamically favorable witha uniform diameter and smooth tubular surface, in compar-ison to the experimentally observed CNTs and AlN nano-wires. Aluminum and nitrogen atoms arrange in a hexagonalnetwork in the tube wall, adopting an sp 2 hybridization. Thecalculated eigenvalues of HOMO and LUMO were about - 0.34226 ( - 9.31 eV) and 0.05823 a. u. (1.58 eV); thus, theHOMO–LUMO gap is 10.89 eV. It should be noted thatwhat they have calculated is HOMO–LUMO gap, not bandgap, as mentioned in the srcinal paper (Zhang and Zhang2003). Band gap in the solid-state physics refers to the dif-ference in energy between the bottom of the conduction bandand the top of the valence band, corresponding to the energydifference between the electron affinity and ionizationpotential of the material (Cui et al. 2012).The unusually large HOMO–LUMO gap is srcinatedfrom the disadvantage of HF theory in predicting theHOMO, and LUMO levels, and also the size influence of nanotubes (Zhang et al. 1996). In the HF model, theLUMO sees one electron more (N instead of N  -  1) thanthe HOMO; therefore, the LUMO is shifted to muchhigher energy, overestimating the HOMO–LUMO gap.The model nanotubes were finite-sized and their endswere saturated with H atoms to decrease the boundaryeffect (Bredas 2014). It should be noted that the realnanotubes are much longer and did not have any hydro-gen atoms. A nanotube with a greater diameter and lengthis expected to have lower strain energy and, therefore,higher stability. Finally, it has been suggested that thesynthesis of AlNNTs may be a potential achievement infuture (Bredas 2014).However, unlike BN nanotubes (BNNTs) which possesshoneycomb graphitic framework on the single walls of thetube (Golberg et al. 1996), so far, no experimental syn-thesis of analogous geometries in AlNNTs has beenreported. Undoubtedly, this difference is because of theexistence of BN graphene-like nanosheets which can berolled up in BN nanotubes, while AlN nanosheets are rathermetastable or unstable. The stability of an infinite hexag-onal AlN (h-AlN) sheet and its structural and electronicproperties have been studied within the framework of DFTat the GGA-PBE level of theory, demonstrating, qualita-tively, synthesizability of individual h-AlN sheets(Almeida et al. 2012). Although, graphite-like h-AlNmultilayers have been experimentally observed and theo-retically modeled (Santos et al. 2016), the synthesis of monolayer graphene-like h-AlN has not been reported yet. Fig. 1  Models demonstrating the various models used in (Stejskalet al. 2009), where the  circled atoms  are chosen as the representativeatoms of each of the model systems: a diamond nanowire  c -C 54  ( 1 ),an AlN nanowire  c -Al 27  N 27  ( 2 ), a carbon nanotube  h -C 54  nanotube( 3 ) and AlN nanotube  h -nitridea AlN nanotube  h – h -Al27 N27 ( 4 )Chem. Pap.  1 3 Downloaded from  Synthesis Wu et al. (2003) synthesized the faceted single-crystallinehexagonal AlNNTs by nitriding the Al powder, impreg-nating with CoSO 4  (1.0 mmol Co per gram of Al) inadvance, with NH 3  /N 2  (NH 3  4 vol%). The transmissionelectron microscopic (TEM) images (Fig. 2) show that theproduct is a blend of nanowires and nanotubes. MostAlNNTs have both ends open and their lengths are fewmicrometers and the diameters are in the range of 30–80 nm. It has been detected that the ends of the tubeshave the pseudohexagonal shape (Fig. 2). However, theresults provided an alternative AlNNT with N and Alatoms [compared to the theoretical results of (Bredas2014)] still positioning in hexagonal crystalline arrange-ment, analogous to the case for bulk h-AlN, and a non-layered construction is detected. In this construction, eachatom has one dangling bond; thus, surface passivation iscommonly unavoidable.Balasubramanian et al. (2004) have synthesized theAlNNTs using solid–vapor equilibrium by gas-phase con-densation. The tubes were dispersed on an extremely ori-ented pyrolytic graphite sheet. The scanning tunnelingmicroscopy measurements have been performed in a vac-uum chamber at room temperature by an OMICRON STM/ AFM system. Diverse structures including nanotubes andnanoparticles have been observed (Fig. 3). The AlNNTsare a mixture of a single tube and also tubes as groups of three or four ones as wide as a few micrometers. They aremostly in helicoidal or twisted arrangement with diameterof about 0.8–3.0 nm. It has been predicted that the AlNNTconstruction consists of, chiefly, hexagons of N and Alatoms which adopt sp 2 hybridization, thereby confirmingthe computational predictions (Bredas 2014). This expla-nation is deep-rooted by comparing the computed inter-atomic distance (0.32 nm) and the average distancebetween two N (0.306 nm), or two Al atoms with theresults of Ref. (Bredas 2014).Yin et al. (2005) have reported the first synthesis of coaxial C–AlN–C combined nanotubes created in bulk  Fig. 2 a  TEM image of theAlN product containingnanotubes and nanowires.  b , c  Pseudohexagonal open ends of two AlN nanotubes in differentlying fashions as schematicallyshown in the figures. For facetedtubular structure, different lyingfashions will result in differentnumbers of distinguishablecontrast regions as seen here Fig. 3  STM image (160  9  160 nm) showing bundles of twisted AlNnanotubes and nanoparticles. The flat surface is highly orientedpyrolytic graphite. A line profile is also reported to show the height of the nanotubes. The white line is only a guideline for the eye to followthe curling direction of the tube along its axis ( white arrow )Chem. Pap.  1 3 Downloaded from  quantities through a reaction of chemical substitution in amanageable two-step process using CNTs as templates.They showed that the C–AlN–C nanotubes are slightlyfaceted because of a confinement effect of the CNT tem-plates. Therefore, only faceted single-crystalline AlNNTswith a non-layered structure were finally formed. Thelength of the AlNNTs was about several micrometers, andthe outer diameter was approximately between 45 and50 nm, with walls of 13-nm thickness. The synthesizedAlNNTs were straight (in contract to the results of Ref.(Wu 2009)) and the TEM images (Fig. 4) show that most of them are open-ended. Chemically, the coaxial C–AlN–Cnanotube formation is a carbonitridation route, in whichCNTs act as reducing material and templates for theAlNNT creation. The coaxial C–AlN–C composite nan-otube formation is shown in Fig. 5. Stability and strain energy The p orbital character of HOMO of an AlNNT like that of CNT predicts the probability of AlNNT formation (Bredas2014). The strain energies needed to generate nanotubesfrom their graphene-like nanosheets, and their thermalstability are main factors in anticipating the formation of tubular geometries (Tenne and Zettl 1996). In a theoreticalwork, Zhao et al. (2003) have assessed the strain energyneeded to roll up an AlN nanosheet into an AlNNT usingDFT calculations, comparing it with the results of carbon,GaN, and BN nanotubes. They used ab initio code of SIESTA with the exchange–correlation functional of Per-dew, Burke and Ernzerhof and the basis set of double- f plus polarization orbitals (Zhao et al. 2003). Theyemployed periodical boundary condition along the AlNNTaxis. The average Al–N bond length has been computed tobe 1.83 A˚which is slightly smaller than that of the cubicAlN which is about 1.89 A˚(Pentaleri et al. 1997).It was found that the buckling in AlNNTs is smaller,compared to that of GaN and BN nanotubes with compa-rable diameters. To evaluate the thermal stability, theymodeled the annealing route of an (5,5)  armchair   AlNNTfor 2 ps at 1000 K, using first-principles moleculardynamics (Zhao et al. 2003). The tubular construction wasmaintained even at high temperature, and the tube wallbucking was very small so that the structural deformationcan be recovered by re-optimization. They suggested thisphenomenon as a reason for the high thermal stability of AlNNTs.Figure 6 (Zhao et al. 2003) shows the computed strain energy per atom needed to roll up an AlN nanosheet into an Fig. 4 a ,  b  Low-magnification TEM images of the synthesized AlNnanotubes Fig. 5  Schematic illustration of the formation process of C–AlN–C composite nanotubes. a  Al 2 O 3  powders are coated onthe surface of carbon nanotubes. b  Al 2 O 3  adsorbed on the surfaceof MWCNTs reacts with themto form Al 2 O through achemical reaction.  c  Under acontinuous NH 3  flow, Al 2 Oreacts with NH 3  and C to formAlN nanotubes through achemical reaction. The carbonlayers form on both the outerand inner surfaces of AlN tubesduring the reverse reaction. d  Cross-el of C–AlN–Ccomposite nanotubesChem. Pap.  1 3 Downloaded from  AlNNT of a specified diameter. For comparison, the energycosts for the formation of carbon, BN, and GaN nanotubesare also given in Fig. 6. As it can be seen, by increasing thediameter of the tubes, the strain energy decreases. Also, thestrain energies are independent of chirality, in the case of BN (Pentaleri et al. 1997) and GaN (23 Lee et al. 1999) nanotubes. This is in good contrast with the results of (Ohand Lee 1998) which indicate that  armchair   CNTs aremore stable than  zigzag  ones. The lowest strain energy of AlNNTs relative to its nanosheet in comparison to those of BN and CNTs with a comparable diameter proposes thefeasibility of AlNNT synthesis from a graphene-like AlN.Stan et al. (2008) have reported the synthesis of facetedAlNNTs through an ‘epitaxial casting’ process like thatreported for the GaN nanotube synthesis (Goldberger et al.2003). First, they used triangular faceted GaN nanowiressynthesized by Ni-catalyzed metal–organic chemical vapordeposition (MOCVD) at 800   C, and then, AlN shells weregrown around the GaN nanowires by MOCVD at 1000   C.Subsequently, the GaN cores were removed by annealing at1120   C in hydrogen atmosphere, leaving behind theempty AlN shells.The MOCVD method is a highly complex procedure forgrowing crystalline layers, employed in the manufacturingof transistors, light-emitting diodes (LEDs), solar cells,lasers, and different electronic devices (Nishizawa andKurabayashi 1983; Liu et al. 2000; Kakanakova-Georgieva et al. 2006; Choi et al. 2012). Also, sublimation epitaxy of  AlN has been performed on 4H-SiC (Kakanakova-Ge-orgieva et al. 2004), resulting in AlN pattern consisting of individual single wurtzite AlN crystallites with plate-likeshape aligned along [1   1 0 0] direction. In contrast toepitaxy method, the growth of crystals in MOCVD is bychemical reaction and not physical deposition. TheMOCVD method is more favorable for formation of devices that are thermodynamically metastable. Mechanical properties ‘‘A reaction to an applied load’’ may be a proper definitionfor mechanical properties of materials. These propertiesmay delineate the range of utility of a substance andestablish the service life can be anticipated. There exist afew studies on the mechanical properties of AlNNTs of which most of them are theoretical studies. Young’s moduli The  Y   indicates the ratio of stress (force per unit area) andstrain (proportional deformation) in a material and is ameasure of the stiffness. The typical equation for Young’smodulus is: Y   ¼ ð F  = a Þ = ð D l = l 0 Þ  ;  ð 1 Þ where  a  is the cross-sectional area and  l 0  is the nanotubelength. Kang and Hwang (2004) have calculated theYoung’s moduli of single-wall (5,5)  armchair   AlNNTs,BN and GaN nanotubes (BNNTs and GaNNTs) usingsimulations. Their calculations showed that the Young’smodulus of AlNNTs is about 453 GPa. An experimentalwork has reported this value to be about 250–400 GPa forfaceted AlNNTs (Stan et al. 2008). This is smaller thanYoung’s moduli of CNT which is about 1 TPa, and, also, issmaller than that of BN (870 GPa) and GaN (796 GPa)nanotubes. Kumar et al. (2015) have investigated thisparameter for several  zigzag  and  armchair   single-walledAlNNTs, BNNTs and GaNNTs, using the second-genera-tion reactive empirical bond order potential with modifiedparameters. They showed that for smaller radii of AlNNTs,the Young’s modulus rises with diameter and then reachesa constant value being lower than that of CNTs, BNNTsand GaNNTs. Poisson’s ratio Poisson’s ratio  m  is another interesting mechanical propertythat is defined by the nanotube radius variation due toexpressing an axial strain on the nanotube: m  ¼  Lateral strainLongitudinal strain ¼ D r r  0 D ll 0 ;  ð 2 Þ where  D r   is the difference between the radius of thestrained and that of the unstrained tube, and  D ll 0 is the axialstrain. The calculated Poisson’s ratio for (3,3) and (5,5) armchair   AlNNTs is about 0.184 and 0.216 and that for Fig. 6  Strain energy vs diameter for the formation of AlN  armchair  and  zigzag  nanotubes relative to their sheet structures. The strainenergies of BN, GaN, and carbon nanotubes are also presented forcomparison. The curves are fitted by the least-square methodChem. Pap.  1 3 Downloaded from
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