Interaction of Acetone with Single Wall Carbon Nanotubes at Cryogenic Temperatures: A Combined Temperature Programmed Desorption and Theoretical Study Dmitry Kazachkin, †,‡ Yoshifumi Nishimura, § Stephan Irle, §,|, Keiji Morokuma, |, Radisav D. Vidic, # and Eric Borguet* ,† Department of Chemistry, Temple UniVersity, Philadelphia, PennsylVania 19122, Department of Chemical Engineering, UniVersity of Pittsburgh, Pittsburgh, PennsylVania 15261, Department of Chemistry and Institute for AdVanced Research, Nagoya UniVersity, Nagoya 464-8602, Japan, Fukui Institute for Fundamental Chemistry, Kyoto UniVersity, Kyoto 606-8103, Japan, Cherry L. Emerson Center for Scientific Computation and Department of Chemistry, Emory UniVersity, Atlanta, Georgia 30322, and Department of CiVil and EnVironmental Engineering, UniVersity of Pittsburgh, Pittsburgh, PennsylVania 15261 ReceiVed January 4, 2008. ReVised Manuscript ReceiVed March 5, 2008 The interaction of acetone with single wall carbon nanotubes (SWCNTs) at low temperatures was studied by a combination of temperature programmed desorption (TPD) and dispersion-augmented density-functional-based tight binding (DFTB-D) theoretical simulations. On the basis of the results of the TPD study and theoretical simulations, the desorption peaks of acetone can be assigned to the following adsorption sites: (i) sites with energy of 75 kJ mol -1 (T des 300 K)sendohedral sites of small diameter nanotubes (7.7 Å); (ii) sites with energy 40–68 kJ mol -1 (T des 240 K)sacetone adsorption on accessible interstitial, groove sites, and endohedral sites of larger nanotubes (14 Å); (iii) sites with energy 25–42 kJ mol -1 (T des 140 K)sacetone adsorption on external walls of SWCNTs and multilayer adsorption. Oxidatively purified SWCNTs have limited access to endohedral sites due to the presence of oxygen functionalities. Oxygen functionalities can be removed by annealing to elevated temperature (900 K) opening access to endohedral sites of nanotubes. Nonpurified, as-received SWCNTs are characterized by limited access for acetone to endohedral sites even after annealing to elevated temperatures (900 K). Annealing of both purified and as-produced SWCNTs to high temperatures (1400 K) leads to reduction of access for acetone molecules to endohedral sites of small nanotubes, probably due to defect self-healing and cap formation at the ends of SWCNTs. No chemical interaction between acetone and SWCNTs was detected for low temperature adsorption experiments. Theoretical simulations of acetone adsorption on finite pristine SWCNTs of different diameters suggest a clear relationship of the adsorption energy with tube sidewall curvature. Adsorption of acetone is due to dispersion forces, with its C-O bond either parallel to the surface or O pointing away from it. No significant charge transfer or polarization was found. Carbon black was used to model amorphous carbonaceous impurities present in as-produced SWCNTs. Desorption of acetone from carbon black revealed two peaks at 140 and 180–230 K, similar to two acetone desorption peaks from SWCNTs. The characteristic feature of acetone desorption from SWCNTs was peak at 300 K that was not observed for carbon black. Care should be taken when assigning TPD peaks for molecules desorbing from carbon nanotubes as amorphous carbon can interfere. 1. Introduction Carbon materials are of interest for fundamental science and technological applications. 1 After their discovery more then 50 years ago, 2 the importance of carbon nanotubes (CNTs) for technological applications was not initially recognized and became clear only recently. 3,4 The dimensions and properties of CNTs make their application as nanosensors attractive. 5–8 Acetone is a simple polar organic solvent and a major chemical commodity. 9 Acetone is reported to be the dominant non-methane organic atmospheric pollutant. 10 Moreover, acetone forms in the body during ketogenesis. 11 Thus, there is ongoing interest in the study of the interaction of acetone molecules with CNTs for the development of sensors 6,12–15 to control the environmental release * Corresponding author. Eric Borguet, Department of Chemistry, Temple University, Philadelphia, PA 19122. Tel: 1-215-204-9696. Fax: 1-215-204- 9530. E-mail: eborguet@temple.edu. Temple University. Department of Chemical Engineering, University of Pittsburgh. § Nagoya University. | Kyoto University. Emory University. # Department of Civil and Environmental Engineering, University of Pittsburgh. (1) Burchell, T. D. Carbon Materials for AdVanced Technologies; 1999; p 540. (2) Radushkevich, L. V.; Luk’yanovich, V. M. Zh. Fiz. Khim. 1952, 26, 88– 95. (3) Iijima, S. Nature 1991, 354(6348), 56–8. (4) Tanaka, K.; Yamabe, T.; Fukui, K. The Science and Technology of Carbon Nanotubes; Elsevier Science Ltd.: Oxford, 1999; p 191. (5) Kong, J.; Franklin, N. R.; Zhou, C. W.; Chapline, M. G.; Peng, S.; Cho, K. J.; Dai, H. J. Science 2000, 287(5453), 622–625. (6) Robinson, J. A.; Snow, E. S.; Badescu, S. C.; Reinecke, T. L.; Perkins, F. K. Nano Lett. 2006, 6(8), 1747–1751. (7) Snow, E. S.; Perkins, F. K.; Houser, E. J.; Badescu, S. C.; Reinecke, T. L. Science 2005, 307(5717), 1942–1945. (8) Li, J.; Lu, Y. J.; Ye, Q.; Cinke, M.; Han, J.; Meyyappan, M. Nano Lett. 2003, 3(7), 929–933. (9) Kirk, R. E.; Othmer, D. F.; Kroschwitz, J. I. Kirk-Othmer Concise Encyclopedia of Chemical Technology, 5th Edition; John Wiley & Sons: New York, 2007. (10) Singh, H. B.; Ohara, D.; Herlth, D.; Sachse, W.; Blake, D. R.; Bradshaw, J. D.; Kanakidou, M.; Crutzen, P. J. J. Geophys. Res., [Atmos.] 1994, 99(D1), 1805–19. (11) VanItallie, T. B.; Nufert, T. H. Nutr. ReV. 2003, 61(10), 327–341. (12) Lu, Y.; Partridge, C.; Meyyappan, M.; Li, J. J. Electroanal. Chem. 2006, 593(1–2), 105–110. (13) Snow, E. S.; Perkins, F. K. Nano Lett. 2005, 5(12), 2414–2417. (14) Parikh, K.; Cattanach, K.; Rao, R.; Suh, D.-S.; Wu, A.; Manohar, S. K. Sens. Actuators, B: Chem. 2006, B113(1), 55–63. 7848 Langmuir 2008, 24, 7848-7856 10.1021/la800030y CCC: $40.75 2008 American Chemical Society Published on Web 07/10/2008