Mahdi Maleki*ab,
Ali Beitollahi*a,
Jinwoo Leeb,
Mohammadreza Shokouhimehrc,
Jafar Javadpoura,
Eun Ju Parkd,
Jinyoung Chunb and
Jongkook Hwangb
aCenter of Excellence for Ceramic Materials in Energy and Environment Applications, School of Metallurgy & Materials Engineering, Iran University of Science and Technology (IUST), Narmak, Tehran 16846, Iran. E-mail: malekim@metaleng.iust.ac.ir; beitolla@iust.ac.ir; Fax: +98 21 77240480; Tel: +98 21 77459151
bPohang University of Science and Technology (POSTECH), Chemical Engineering, Pohang, Republic of Korea
cSchool of Chemical and Biological Engineering, Seoul National University, Seoul 151-742, Republic of Korea
dPolymer Design & Reaction Engineering, Institute of Chemical and Engineering Sciences, Agency for Science, Technology and Research (A*STAR), 1 Pesek Road, Jurong Island, 627833, Singapore
First published on 16th December 2014
We report a successful synthesis of Mesoporous BN (MBN) powder through a facile one-pot synthesis strategy. In this respect, laboratory made block copolymer, polystyrene-b-poly(ethylene oxide) (PS-b-PEO) was used as structure directing agent and ammonia borane was used as BN precursor, respectively. Various characterization techniques such as X-ray photoelectron spectroscopy, Fourier-transform infrared spectroscopy, X-ray diffraction (XRD), scanning electron microscopy, transmission electron microscopy (TEM) and N2 sorption analysis were used to characterize different properties of the synthesized MBN powder. The formation of turbostratic boron nitride with wormlike pores (20 nm) was confirmed by XRD and TEM results. N2 sorption analysis of the obtained MBN sample exhibited a high specific surface area of 326 m2 g−1 and a pore volume of 0.5 m3 g−1.
Porous BN due to its wide range of applications such as organic pollutant adsorption, water purification, energy storage, catalyst supports and field emission devices have recently received remarkable attention.8–15 However, for most of these applications, the precise control of pore size/distributions, wall thickness, pore shape, specific surface area and surface chemistry is demanded. To achieve such goals, two major strategies known as hard and soft templates are normally utilized.
Mesoporous BN (MBN) has also been prepared by both of these synthetic routes as well. It is worth to mention that most of the previous studies have used mesoporous carbon or silica as the hard templates for the synthesis of MBN16–19 and less attention has been paid to the soft template route using amphiphilic block copolymers (BCPs). The hard template method utilized for the synthesis of the MBN generally provides appropriate pore size and shape control through the pores of rigid template.19 However, template removal, frequent replication and air sensitive precursors such as tri(methylamino)borazine (MAB) lend themselves as inevitable obstacles for facile synthesis of this material.20,21
Wan et al. reported a successful synthesis of highly ordered MBN by synthesizing a complex BCP, polynorbornene-b-polynorbornene decaborane (PNB-b-PDB).22 Despite of the interesting results obtained by this group, however, the synthesis of such a complicated block copolymer is not an easy task.
Evaporation induced self assembly (EISA) method is appropriate procedure in the synthesis of mesoporous materials. In this respect, lab made BCPs such as PS-b-PEO (PSE) and poly(isoprene-block-ethyleneoxide) have been used for the synthesis of various mesoporous oxides such as TiO2, Nb2O5, SiO2 and carbon.23–25 The composition, block sequence, molecular weight and volume fraction of the lab made BCPs can be tailored to earn suitable mesostructures.26 However, for a successful synthesis of mesoporous materials using PSE, appropriate precursors and solvents should be attentively selected for either hydrophobic (PS) or hydrophilic (PEO) blocks.
In the synthesis of mesoporous SiO2 through EISA method using PSE, the tetraethyl orthosilicate (TEOS) precursor can interact with the PEO segment of the BCPs.27 The self assembly of (PEO-b-PS)/TEOS is occurred during solvent evaporation. In the case of mesoporous carbon, resol has a similar role with TEOS to interact with PEO block with hydrogen bonding to make a self assembled structure.28 Heat treatment of self assembled BCP with resol/TEOS led to decomposition of BCP and formation of mesopores.27,28
Various BN precursors have been utilized by many research groups for the synthesis of porous BN powders such as MAB,29 tri(chloro)borazine,21 boron oxide30–32 and boron tribromide (BBr3).33 Among these precursors, MAB has been frequently used due to appropriate micro-meso pores filling of carbon template and in situ thermal polymerization.21 However, this compound is highly air–moisture sensitive making its handling difficult besides the fact that MAB is not commercially available. In contrast, ammonia borane (AB) or borazane as BN precursor is a nontoxic, non-explosive and stable crystalline compound under normal pressures and temperatures. It can be handled easily and it does not need any special facility compared to borazine compounds and can be solved in many polar solvents.34–39 Furthermore, polymerization ability of AB as a necessary character for the precursors used in soft template route39,40 and its commercially availability makes this compound as an appropriate candidate for the synthesis of MBN.
In this work, we report a novel procedure for the synthesis of MBN through self assembly of PSE as a structure directing agent and AB as BN precursor through a simple one-pot EISA method.
11B NMR spectra were recorded on Solid/Micro-Imaging High Resolution NMR AVANCE 400 WB operating at 128.28 MHz. Chemical shifts were referenced to BF3(OEt)2 (δ = 0 ppm). X-ray photoelectron spectroscopy (XPS) measurements were carried out for the prepared MBN using AXIS Ultra DLD, Kratos Inc, employing Mg Kα lines (1486.6 eV) as an excitation source. The carbonaceous C 1s line (284.6 eV) was used as the reference to calibrate the binding energies.
Nitrogen physisorption was measured using Micromeritics Tristar II system at −196 °C. The samples were degassed at 150 °C before measurements. The Brunauer–Emmett–Teller (BET) method was utilized to calculate the specific surface area (SBET) using the adsorption branch. The pore size distribution (PSD) was derived from the adsorption branch by using the Barrett–Joyner–Halenda (BJH) model. The total pore volume (Vtotal) was estimated from the adsorbed amount at P/P0 = 0.995. In order to determine micropore volume, the Dubinin–Raduskevitch (DR) theory was used.18
The microstructural analyses were carried out using a scanning electron microscopy (SEM) JEOL JSM-6330F and a transmission electron microscopy (TEM) Philips Tecnai 20. The prepared powders were dispersed in EtOH and deposited on to carbon coated grid and left to dry at room temperature before the TEM analysis.
In order to understand the possible set up of interaction between AB and PSE, the samples were characterized by solid state 11B NMR. The 11B NMR spectra of AB and AB/PSE are shown in Fig. 2. Compared to AB 11B NMR peak (−29 ppm), 11B NMR spectrum of AB/PSE hybrid has an extra peak at −24.6 ppm.
W. J. Shaw et al.42 has also reported the appearance of rather similar extra peak for AB subjected to thermal decomposition at 80 °C. This was attributed to the formation of highly mobile (BH3NH3) molecules. Furthermore, they have also noticed the existence of such peak for AB scaffolded in MCM-41.42 This was related to highly mobile molecule due to breaks up the 3-dimensional dihydrogen bonding network.42 Further, similar phase was also observed due to interaction between AB and polyetheral promoters.43 The observed peak at −24.6 ppm (Fig. 2) for AB/PSE samples studied could be possibly due to the formation of such new mobile molecules.
FTIR spectroscopy was used to further investigate the interactions between AB and PSE. Fig. 3a–d shows the FTIR spectra of the AB, PSE and AB/PSE samples (with two different weight ratios: 1:
1 and 1
:
15) after evaporation of the solvent for the latter at 50 °C.
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Fig. 3 FTIR spectra of (a) AB, (b) PSE, (c) AB/PSE: 1/1 and (d) AB/PSE: 1/15 (weight ratio) after evaporation of solvent at 50 °C. |
Fig. 3a shows peaks at 3318, 2344, 1610, 1379, 1163, 1065, 782, 729 cm−1 for AB. The observed peak at 3318 cm−1 is assigned to NH stretching modes and peak near 2344 cm−1 is assigned to BH stretching mode.44 The detected peaks at 1610 cm−1 and 1379 cm−1 are due to NH3 deformations, and peak at 1165 cm−1 is assigned to BH3 deformations.44 The peaks at 1065 cm−1 and 729 cm−1 have been attributed to NBH rocking modes. The peak at 782 cm−1 is due to B–N bond in AB.44 The appeared peaks in Fig. 3b at 3026, 1601, 1493, 1452, 843 and 698 cm−1 are related to polystyrene and the emerged peaks at 1148 and 1108 cm−1 are assigned to PEO block in PSE BCP made by ATRP method.28,45,46
FTIR peaks comparison of the AB, PSE and AB/PSE samples showed that PS peaks have minimum chemical shift after AB/PSE hybrid formation as it was also confirmed by Kurban finding about interaction between AB and PS.47 The presence of a peak in a similar position for B–N bond (781 cm−1) in AB and AB/PSE (782 cm−1) confirms the existence of such bond in AB/PSE as well. B–H peaks of AB/PSE compared to AB have shifted to higher wave numbers from 1064 cm−1 to 1057 cm−1 and 2344 cm−1 to 2352 cm−1 (Fig. 2c). As it can be noticed from Fig. 2d, the N–H peak of AB has shifted from 3317 cm−1 to lower wave number (3304 cm−1) due to the weakening of the N–H stretching bond. On the other hand, the observed increase of N–H3 bending mode bond peak position from 1379 cm−1 to 1385 cm−1 can be possibly due to change of AB configuration and N–H3 bending bonds.
Previous studies43,48 have also considered interaction between AB with other polymers. For instance, the results of Zhao group48 demonstrated that AB binds to methyl methacrylate polymer through hydrogen bonding between hydrogen in B–H bond and oxygen of polymer. Further, Kim et al. declared that hydrogen of the N–H bond is the agent of hydrogen bonding between AB and oxygen atom of ethereal polymer.43
For the investigated samples in this work, in addition to XRD and 11B NMR studies, the N–H stretching bond weakening and B–H strengthening bonds suggest that AB could be possibly connected to oxygen atom of PEO through the N–H bond of AB.48 However, this demanded further study by more details analysis.
As it was mentioned before, key controlling factor in the synthesis of mesoporous materials such as TiO2, SiO2 and carbon through EISA methods using BCPs is the compatibility between hydrophilic blocks of BCPs and inorganic precursors. W. Luo reported that hydroxyl groups of resol can form hydrogen-bonding with EO-containing block polymers and are arranged around block copolymer micelles.49 In the synthesis of MBN with PNB-b-PDB, also tried to connect the BN precursor (decaborane) to polynorbornene block before BCP preparation.22 Pyrolysis of self assembled PNB-b-PDB under ammonia atmosphere led to decomposition of the PNB and formation of mesopores.
As AB does not have interaction with PS, AB selectively incorporates in hydrophilic PEO block of BCP and swells hydrophilic part to form corona while the PS forms rigid core. Casting the solution in the petri-dish leads to evaporation of solvent (Scheme 1). Evaporation induced self assembly of PSE/AB precursors leads to form a white film. Pyrolysis at high temperature (1150 °C) for the as-made film under ammonia atmosphere further involves the substitution of carbon with nitrogen, eventually leading to the formation of MBN with white color.22
Fig. 4b exhibits a typical FTIR spectrum of the prepared MBN powder with two main characteristic absorption peaks around 1384 cm−1 and 798 cm−1. The former peak can be attributed to the stretching vibration of the B–N bond, while the latter one is corresponding to the out-of-plane bending vibrations of B–N–B bond.19 The weak bands around 3430 cm−1 and 3250 cm−1 can be also assigned to ν(N–H) and ν(BOH) vibrations.50
The XPS survey scan spectrum and deconvoluted XPS spectra of B 1s and N 1s from MBN powder are depicted in Fig. 5. Deconvolution of B 1s spectrum gives two peaks centered at 190.27 eV and 192.38 eV. The dominant peak of the B 1s spectrum is located at 190.27 eV (Fig. 5), which is attributable to B 1s of B–N bonds. The small peak at high energy (192.38 eV) is assigned to B–O bonds and can be due to air exposure of the sample or surface contamination.31,51–53 The observed peak at 39 8.09 eV is attributed to N 1s spectrum (398.1 eV) of B–N bond.54 Both B 1s and N 1s spectra indicate that the main configuration of B and N atoms are related to the B–N bonds. The atomic percentage of B, N, C and O from XPS spectra were 42.1%, 37.3%, 7.9% and 12.7%, respectively. The B/N atomic ratio from our XPS survey was about 1.1 which is near to the BN stoichiometry.
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Fig. 7 Nitrogen adsorption–desorption isotherm and PSD (BJH) of the MBN prepared by PSE block copolymer. |
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Fig. 8 (a) SEM and (b) TEM images of the MBN prepared by one pot method. The inset shows a TEM image of micropores in the prepared MBN. |
For the prepared MBN powder in this work, the thermal decomposition of interpenetrating of PEO in AB network is considered as one of the micropores resources.
Furthermore, precursor polymerization could be one of the micropores sources.57 It was indicated that the polymerization of polymeric BN precursors leads to microporosity in BN ceramic.58–60 In order to investigate the contribution of AB thermal decomposition in the micropores formation, AB was polymerized at 80 °C for 16 h. Then the polymerized AB was heat treated using a similar heating program used for AB/PSE hybrid under ammonia atmosphere at 1150 °C for 2 h. Fig. 9 shows the nitrogen sorption isotherm of polymerized AB after heat treatment under ammonia atmosphere. Surprisingly, the surface area was 480 m2 g−1 and micropore volume was 0.177 cm3 g−1. Moreover, as it can be seen from Fig. 9, beginning of absorption isotherm from low relative pressure demonstrates presence of micropores.61 Therefore, the set up of micropores for the MBN powders synthesized here could be possibly originated from AB and PEO thermal decomposition.
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Fig. 9 Nitrogen adsorption–desorption isotherm and BJH pore size distribution of polymerized AB after heat treatment at 1150 °C under ammonia atmosphere. |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c4ra11431k |
This journal is © The Royal Society of Chemistry 2015 |