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<record><TEI><teiHeader><fileDesc><titleStmt><title xml:lang="en">Energy efficiency in nanoscale synthesis using nanosecond plasmas</title><author><name sortKey="Pai, David Z" sort="Pai, David Z" uniqKey="Pai D" first="David Z." last="Pai">David Z. Pai</name><affiliation><nlm:aff id="a1"><institution>Department of Advanced Materials Science, Graduate School of Frontier Sciences, The University of Tokyo</institution>, 5-1-5 Kashiwanoha, Kashiwa-shi, Chiba 277 8562,<country>Japan</country></nlm:aff></affiliation><affiliation><nlm:aff id="a2"><institution>Laboratoire EM2C, CNRS UPR288</institution>, Ecole Centrale Paris, Grande Voie des Vignes, 92295 Châtenay-Malabry,<country>France</country></nlm:aff></affiliation><affiliation><nlm:aff id="a5"><institution>Département Fluides, Thermique et Combustion, Institut Pprime (CNRS UPR 3346, Université de Poitiers</institution>, ENSMA), bd Marie et Pierre Curie, Téléport 2, BP 30179F, 86962 Futuroscope,<country>France</country></nlm:aff></affiliation></author><author><name sortKey=" Ken Ostrikov, Kostya" sort=" Ken Ostrikov, Kostya" uniqKey=" Ken Ostrikov K" first="Kostya" last=" Ken Ostrikov">Kostya Ken Ostrikov</name><affiliation><nlm:aff id="a3"><institution>Plasma Nanoscience Centre Australia (PNCA), CSIRO Materials Science and Engineering</institution>, P.O. Box 218, Lindfield, New South Wales 2070 Australia</nlm:aff></affiliation><affiliation><nlm:aff id="a4"><institution>Plasma Nanoscience@Complex Systems, School of Physics, The University of Sydney</institution>, Sydney, New South Wales 2006, Australia</nlm:aff></affiliation></author><author><name sortKey="Kumar, Shailesh" sort="Kumar, Shailesh" uniqKey="Kumar S" first="Shailesh" last="Kumar">Shailesh Kumar</name><affiliation><nlm:aff id="a3"><institution>Plasma Nanoscience Centre Australia (PNCA), CSIRO Materials Science and Engineering</institution>, P.O. Box 218, Lindfield, New South Wales 2070 Australia</nlm:aff></affiliation><affiliation><nlm:aff id="a4"><institution>Plasma Nanoscience@Complex Systems, School of Physics, The University of Sydney</institution>, Sydney, New South Wales 2006, Australia</nlm:aff></affiliation></author><author><name sortKey="Lacoste, Deanna A" sort="Lacoste, Deanna A" uniqKey="Lacoste D" first="Deanna A." last="Lacoste">Deanna A. Lacoste</name><affiliation><nlm:aff id="a2"><institution>Laboratoire EM2C, CNRS UPR288</institution>, Ecole Centrale Paris, Grande Voie des Vignes, 92295 Châtenay-Malabry,<country>France</country></nlm:aff></affiliation></author><author><name sortKey="Levchenko, Igor" sort="Levchenko, Igor" uniqKey="Levchenko I" first="Igor" last="Levchenko">Igor Levchenko</name><affiliation><nlm:aff id="a3"><institution>Plasma Nanoscience Centre Australia (PNCA), CSIRO Materials Science and Engineering</institution>, P.O. Box 218, Lindfield, New South Wales 2070 Australia</nlm:aff></affiliation><affiliation><nlm:aff id="a4"><institution>Plasma Nanoscience@Complex Systems, School of Physics, The University of Sydney</institution>, Sydney, New South Wales 2006, Australia</nlm:aff></affiliation></author><author><name sortKey="Laux, Christophe O" sort="Laux, Christophe O" uniqKey="Laux C" first="Christophe O." last="Laux">Christophe O. Laux</name><affiliation><nlm:aff id="a2"><institution>Laboratoire EM2C, CNRS UPR288</institution>, Ecole Centrale Paris, Grande Voie des Vignes, 92295 Châtenay-Malabry,<country>France</country></nlm:aff></affiliation></author></titleStmt><publicationStmt><idno type="wicri:source">PMC</idno><idno type="pmid">23386976</idno><idno type="pmc">3564032</idno><idno type="url">http://www.ncbi.nlm.nih.gov/pmc/articles/PMC3564032</idno><idno type="RBID">PMC:3564032</idno><idno type="doi">10.1038/srep01221</idno><date when="2013">2013</date><idno type="wicri:Area/Pmc/Corpus">000117</idno><idno type="wicri:explorRef" wicri:stream="Pmc" wicri:step="Corpus" wicri:corpus="PMC">000117</idno></publicationStmt><sourceDesc><biblStruct><analytic><title xml:lang="en" level="a" type="main">Energy efficiency in nanoscale synthesis using nanosecond plasmas</title><author><name sortKey="Pai, David Z" sort="Pai, David Z" uniqKey="Pai D" first="David Z." last="Pai">David Z. Pai</name><affiliation><nlm:aff id="a1"><institution>Department of Advanced Materials Science, Graduate School of Frontier Sciences, The University of Tokyo</institution>, 5-1-5 Kashiwanoha, Kashiwa-shi, Chiba 277 8562,<country>Japan</country></nlm:aff></affiliation><affiliation><nlm:aff id="a2"><institution>Laboratoire EM2C, CNRS UPR288</institution>, Ecole Centrale Paris, Grande Voie des Vignes, 92295 Châtenay-Malabry,<country>France</country></nlm:aff></affiliation><affiliation><nlm:aff id="a5"><institution>Département Fluides, Thermique et Combustion, Institut Pprime (CNRS UPR 3346, Université de Poitiers</institution>, ENSMA), bd Marie et Pierre Curie, Téléport 2, BP 30179F, 86962 Futuroscope,<country>France</country></nlm:aff></affiliation></author><author><name sortKey=" Ken Ostrikov, Kostya" sort=" Ken Ostrikov, Kostya" uniqKey=" Ken Ostrikov K" first="Kostya" last=" Ken Ostrikov">Kostya Ken Ostrikov</name><affiliation><nlm:aff id="a3"><institution>Plasma Nanoscience Centre Australia (PNCA), CSIRO Materials Science and Engineering</institution>, P.O. Box 218, Lindfield, New South Wales 2070 Australia</nlm:aff></affiliation><affiliation><nlm:aff id="a4"><institution>Plasma Nanoscience@Complex Systems, School of Physics, The University of Sydney</institution>, Sydney, New South Wales 2006, Australia</nlm:aff></affiliation></author><author><name sortKey="Kumar, Shailesh" sort="Kumar, Shailesh" uniqKey="Kumar S" first="Shailesh" last="Kumar">Shailesh Kumar</name><affiliation><nlm:aff id="a3"><institution>Plasma Nanoscience Centre Australia (PNCA), CSIRO Materials Science and Engineering</institution>, P.O. Box 218, Lindfield, New South Wales 2070 Australia</nlm:aff></affiliation><affiliation><nlm:aff id="a4"><institution>Plasma Nanoscience@Complex Systems, School of Physics, The University of Sydney</institution>, Sydney, New South Wales 2006, Australia</nlm:aff></affiliation></author><author><name sortKey="Lacoste, Deanna A" sort="Lacoste, Deanna A" uniqKey="Lacoste D" first="Deanna A." last="Lacoste">Deanna A. Lacoste</name><affiliation><nlm:aff id="a2"><institution>Laboratoire EM2C, CNRS UPR288</institution>, Ecole Centrale Paris, Grande Voie des Vignes, 92295 Châtenay-Malabry,<country>France</country></nlm:aff></affiliation></author><author><name sortKey="Levchenko, Igor" sort="Levchenko, Igor" uniqKey="Levchenko I" first="Igor" last="Levchenko">Igor Levchenko</name><affiliation><nlm:aff id="a3"><institution>Plasma Nanoscience Centre Australia (PNCA), CSIRO Materials Science and Engineering</institution>, P.O. Box 218, Lindfield, New South Wales 2070 Australia</nlm:aff></affiliation><affiliation><nlm:aff id="a4"><institution>Plasma Nanoscience@Complex Systems, School of Physics, The University of Sydney</institution>, Sydney, New South Wales 2006, Australia</nlm:aff></affiliation></author><author><name sortKey="Laux, Christophe O" sort="Laux, Christophe O" uniqKey="Laux C" first="Christophe O." last="Laux">Christophe O. Laux</name><affiliation><nlm:aff id="a2"><institution>Laboratoire EM2C, CNRS UPR288</institution>, Ecole Centrale Paris, Grande Voie des Vignes, 92295 Châtenay-Malabry,<country>France</country></nlm:aff></affiliation></author></analytic><series><title level="j">Scientific Reports</title><idno type="eISSN">2045-2322</idno><imprint><date when="2013">2013</date></imprint></series></biblStruct></sourceDesc></fileDesc><profileDesc><textClass></textClass></profileDesc></teiHeader><front><div type="abstract" xml:lang="en"><p>We report a nanoscale synthesis technique using nanosecond-duration plasma discharges. Voltage pulses 12.5 kV in amplitude and 40 ns in duration were applied repetitively at 30 kHz across molybdenum electrodes in open ambient air, generating a nanosecond spark discharge that synthesized well-defined MoO<sub>3</sub> nanoscale architectures (i.e. flakes, dots, walls, porous networks) upon polyamide and copper substrates. No nitrides were formed. The energy cost was as low as 75 eV per atom incorporated into a nanostructure, suggesting a dramatic reduction compared to other techniques using atmospheric pressure plasmas. These findings show that highly efficient synthesis at atmospheric pressure without catalysts or external substrate heating can be achieved in a simple fashion using nanosecond discharges.</p></div></front><back><div1 type="bibliography"><listBibl><biblStruct><analytic><author><name sortKey="Ostrikov, K" uniqKey="Ostrikov K">K. Ostrikov</name></author></analytic></biblStruct><biblStruct><analytic><author><name sortKey="Yarris, L" uniqKey="Yarris L">L. Yarris</name></author></analytic></biblStruct><biblStruct><analytic><author><name sortKey="Chen, Z B" uniqKey="Chen Z">Z. B. Chen</name></author></analytic></biblStruct><biblStruct><analytic><author><name sortKey="Brezesinski, T" uniqKey="Brezesinski T">T. Brezesinski</name></author><author><name sortKey="Wang, J" uniqKey="Wang J">J. 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<front><journal-meta><journal-id journal-id-type="nlm-ta">Sci Rep</journal-id><journal-id journal-id-type="iso-abbrev">Sci Rep</journal-id><journal-title-group><journal-title>Scientific Reports</journal-title></journal-title-group><issn pub-type="epub">2045-2322</issn><publisher><publisher-name>Nature Publishing Group</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="pmid">23386976</article-id><article-id pub-id-type="pmc">3564032</article-id><article-id pub-id-type="pii">srep01221</article-id><article-id pub-id-type="doi">10.1038/srep01221</article-id><article-categories><subj-group subj-group-type="heading"><subject>Article</subject></subj-group></article-categories><title-group><article-title>Energy efficiency in nanoscale synthesis using nanosecond plasmas</article-title></title-group><contrib-group><contrib contrib-type="author"><name><surname>Pai</surname><given-names>David Z.</given-names></name><xref ref-type="corresp" rid="c1">a</xref><xref ref-type="aff" rid="a1">1</xref><xref ref-type="aff" rid="a2">2</xref><xref ref-type="aff" rid="a5">5</xref></contrib><contrib contrib-type="author"><name><surname>(Ken) Ostrikov</surname><given-names>Kostya</given-names></name><xref ref-type="aff" rid="a3">3</xref><xref ref-type="aff" rid="a4">4</xref></contrib><contrib contrib-type="author"><name><surname>Kumar</surname><given-names>Shailesh</given-names></name><xref ref-type="aff" rid="a3">3</xref><xref ref-type="aff" rid="a4">4</xref></contrib><contrib contrib-type="author"><name><surname>Lacoste</surname><given-names>Deanna A.</given-names></name><xref ref-type="aff" rid="a2">2</xref></contrib><contrib contrib-type="author"><name><surname>Levchenko</surname><given-names>Igor</given-names></name><xref ref-type="aff" rid="a3">3</xref><xref ref-type="aff" rid="a4">4</xref></contrib><contrib contrib-type="author"><name><surname>Laux</surname><given-names>Christophe O.</given-names></name><xref ref-type="aff" rid="a2">2</xref></contrib><aff id="a1"><label>1</label><institution>Department of Advanced Materials Science, Graduate School of Frontier Sciences, The University of Tokyo</institution>, 5-1-5 Kashiwanoha, Kashiwa-shi, Chiba 277 8562,<country>Japan</country></aff><aff id="a2"><label>2</label><institution>Laboratoire EM2C, CNRS UPR288</institution>, Ecole Centrale Paris, Grande Voie des Vignes, 92295 Châtenay-Malabry,<country>France</country></aff><aff id="a3"><label>3</label><institution>Plasma Nanoscience Centre Australia (PNCA), CSIRO Materials Science and Engineering</institution>, P.O. Box 218, Lindfield, New South Wales 2070 Australia</aff><aff id="a4"><label>4</label><institution>Plasma Nanoscience@Complex Systems, School of Physics, The University of Sydney</institution>, Sydney, New South Wales 2006, Australia</aff><aff id="a5"><label>5</label><institution>Département Fluides, Thermique et Combustion, Institut Pprime (CNRS UPR 3346, Université de Poitiers</institution>, ENSMA), bd Marie et Pierre Curie, Téléport 2, BP 30179F, 86962 Futuroscope,<country>France</country></aff></contrib-group><author-notes><corresp id="c1"><label>a</label><email>david.pai@univ-poitiers.fr</email></corresp></author-notes><pub-date pub-type="epub"><day>05</day><month>02</month><year>2013</year></pub-date><pub-date pub-type="collection"><year>2013</year></pub-date><volume>3</volume><elocation-id>1221</elocation-id><history><date date-type="received"><day>11</day><month>09</month><year>2012</year></date><date date-type="accepted"><day>18</day><month>01</month><year>2013</year></date></history><permissions><copyright-statement>Copyright © 2013, Macmillan Publishers Limited. All rights reserved</copyright-statement><copyright-year>2013</copyright-year><copyright-holder>Macmillan Publishers Limited. All rights reserved</copyright-holder><license license-type="open-access" xlink:href="http://creativecommons.org/licenses/by-nc-nd/3.0/"><pmc-comment>author-paid</pmc-comment>
<license-p>This work is licensed under a Creative Commons Attribution-NonCommercial-NoDerivs 3.0 Unported License. To view a copy of this license, visit <ext-link ext-link-type="uri" xlink:href="http://creativecommons.org/licenses/by-nc-nd/3.0/">http://creativecommons.org/licenses/by-nc-nd/3.0/</ext-link></license-p></license></permissions><abstract><p>We report a nanoscale synthesis technique using nanosecond-duration plasma discharges. Voltage pulses 12.5 kV in amplitude and 40 ns in duration were applied repetitively at 30 kHz across molybdenum electrodes in open ambient air, generating a nanosecond spark discharge that synthesized well-defined MoO<sub>3</sub> nanoscale architectures (i.e. flakes, dots, walls, porous networks) upon polyamide and copper substrates. No nitrides were formed. The energy cost was as low as 75 eV per atom incorporated into a nanostructure, suggesting a dramatic reduction compared to other techniques using atmospheric pressure plasmas. These findings show that highly efficient synthesis at atmospheric pressure without catalysts or external substrate heating can be achieved in a simple fashion using nanosecond discharges.</p></abstract></article-meta></front><body><p>Efficiency in energy and matter consumption during synthesis is one of the Grand Science Challenges presently facing nanotechnology, which is expected to play a key role in the development of energy technologies critical for a sustainable future<xref ref-type="bibr" rid="b1">1</xref><xref ref-type="bibr" rid="b2">2</xref>. This is in addition to the drive to develop new nanofabrication processes that are economical at the industrial scale, environmentally friendly, and of high quality. Such innovation will ultimately require effective control of the energy and matter involved in nanoscale materials synthesis, which is the primary motivation for using the synthesis method introduced in this work. This technique is demonstrated here for the case of MoO<sub>x</sub> nanostructures, which have potential applications in catalysis<xref ref-type="bibr" rid="b3">3</xref>, charge storage<xref ref-type="bibr" rid="b4">4</xref>, gas sensing<xref ref-type="bibr" rid="b5">5</xref>, and field emission<xref ref-type="bibr" rid="b6">6</xref>.</p><p>The existing methods for the production of MoO<sub>x</sub> nanomaterials include hydrothermal processing<xref ref-type="bibr" rid="b7">7</xref> that can involve the use of templates<xref ref-type="bibr" rid="b8">8</xref>, electrodeposition in solution<xref ref-type="bibr" rid="b9">9</xref>, thermal evaporation followed by chemical vapor deposition (CVD)<xref ref-type="bibr" rid="b6">6</xref>, thermal oxidation<xref ref-type="bibr" rid="b10">10</xref>, flame synthesis<xref ref-type="bibr" rid="b11">11</xref>, and plasma-based synthesis<xref ref-type="bibr" rid="b12">12</xref>. Wet chemistry processes are usually low-temperature and quite energy efficient but produce significant chemical waste, involve complicated steps for isolating products, and are more suited for the production of loose, unsupported nanoparticles<xref ref-type="bibr" rid="b13">13</xref>. Thermal evaporation methods typically must take place in vacuum environments or requires catalysts. Thermal and plasma CVD are more environmentally friendly but are less energy efficient due to higher temperatures and reduced pressures. Essentially, unnecessarily large quantities of energy and/or matter are mustered to synthesize small objects.</p><p>To address this problem, here we use the deterministic “building unit” approach<xref ref-type="bibr" rid="b14">14</xref>, whereby only the required atoms should be produced from precursors before rapid delivery and incorporation into a nanoscale assembly with minimum loss and energy consumption. To be clear, we are concerned here with self-organized processes, as opposed to atom-by-atom manipulation, which is very inefficient in terms of time and cost. <xref ref-type="fig" rid="f1">Figure 1(a)</xref> shows the deterministic approach in relation to the results to be presented in this work, namely metal-oxide nanostructures generated in open air. Ideally, metal and oxygen atoms would be produced and then consumed stoichiometrically. One efficient means of generating both species is to conduct electric current between two metal electrodes via a gas discharge in the inter-electrode gap. Metal atoms come via evaporation from the electrodes and the oxygen atoms via dissociation of O<sub>2</sub> in the gas phase. Thus, targeting the discharge energy towards efficient dissociation of O<sub>2</sub> is of primary interest. To produce a pure metal vapor, a high-current discharge can be efficiently used in which the current is localized in high-temperature spots on the electrode surface. In this case mainly pure metal ions are usually produced<xref ref-type="bibr" rid="b15">15</xref><xref ref-type="bibr" rid="b16">16</xref>.</p><p>The use of plasma discharges for nanoscale synthesis is a rapidly developing field<xref ref-type="bibr" rid="b1">1</xref><xref ref-type="bibr" rid="b14">14</xref>. In particular, non-thermal plasmas (for which the mean electron energy <<italic>ε</italic>> is significantly higher than the energy of neutral gas particles) at atmospheric pressure are attractive because of several factors conducive to efficiency<xref ref-type="bibr" rid="b17">17</xref><xref ref-type="bibr" rid="b18">18</xref>. Operating at atmospheric pressure eliminates the need for vacuum equipment and enables fast chemistry due to high species densities, thus speeding up growth compared to low-pressure synthesis. Non-thermal plasmas efficiently channel energy towards generating plasma chemical species such as electrons, ions, excited neutral species, and radicals typically not found in other synthesis environments that can serve as vehicles for the specific transfer of energy towards growth processes. So far, little attention has been paid to efficiency until recently<xref ref-type="bibr" rid="b19">19</xref><xref ref-type="bibr" rid="b20">20</xref>.</p><p>Among non-thermal atmospheric-pressure plasma sources, nanosecond repetitive pulsed (NRP) discharges possess particularly high mean electron energy <<italic>ε</italic>> and therefore may be well suited for efficient synthesis because significant fractions of the discharge energy are channeled to the electron-impact processes of ionization, electronic excitation, and dissociation when <<italic>ε</italic>> is much greater than 1 eV. This subject has been explored previously in a perspectives article<xref ref-type="bibr" rid="b19">19</xref>. NRP discharges are generated by applying high-voltage nanosecond-duration pulses at high pulse repetition frequency (PRF), as shown in <xref ref-type="fig" rid="f2">Figure 2</xref>. A short rise time minimizes electron-heavy species collisions at low <<italic>ε</italic>> before high <<italic>ε</italic>> is attained once the voltage reaches its maximum value. A recent model shows that <<italic>ε</italic>> at atmospheric pressure increases up to a maximum value within several nanoseconds of the instantaneous application of a high-voltage pulse and then remains close to the maximum for several tens of ns<xref ref-type="bibr" rid="b21">21</xref>. However, <<italic>ε</italic>> then decreases significantly once a quasi-neutral plasma column forms. Thus, we aim to choose the pulse duration to maximize <<italic>ε</italic>> while allowing sufficient time for synthesis. To maintain an active medium between pulses, the PRF is chosen to match the recombination time of the discharge. In practice, the above criteria can be met in air at atmospheric pressure using pulses with nanosecond-scale duration and rise time, with PRF of about 10 – 100 kHz, at applied voltages on the order of 10 kV for inter-electrode gaps on the order of 1 cm.</p><p>To test the ideas proposed in Refs. <xref ref-type="bibr" rid="b1">1</xref> and <xref ref-type="bibr" rid="b19">19</xref> that plasmas and NRP discharges in particular can be potentially used for targeted and efficient use of energy and matter in nanoscale synthesis, here we employ NRP spark discharges for controlling the production of metal and oxygen atoms in open ambient air, resulting in the synthesis of high quality MO<sub>3</sub> nanostructures suitable for various applications. When metal electrodes for plasma generation also serve as the source for metal precursor atoms, it is convenient to use spark discharges because they generate temperatures high enough for evaporating metal<xref ref-type="bibr" rid="b22">22</xref><xref ref-type="bibr" rid="b23">23</xref><xref ref-type="bibr" rid="b24">24</xref>. NRP spark-based nanofabrication consumes potentially much less energy than other methods while operating in open ambient air without catalysts or additional heating of the substrate. Furthermore, it is possible to synthesize on plastic, which is useful for hybrid organic-inorganic energy conversion and electronic devices. The high <<italic>ε</italic>> of NRP discharges is a basic plasma property that may be generally useful in nanoscale synthesis and materials processing.</p><p>In this work, NRP spark discharges have been generated in open ambient air using two different vertical discharge configurations, as shown in <xref ref-type="fig" rid="f1">Figure 1</xref> as well as in <xref ref-type="supplementary-material" rid="s1">Figure SI1</xref> in <xref ref-type="supplementary-material" rid="s1">Supplementary information</xref>. Details of the experimental setup are discussed in the Methods section.</p><sec disp-level="1" sec-type="results"><title>Results</title><sec disp-level="2"><title>Metal-oxide nanoarchitectures – morphological, compositional, and structural characterization</title><p><xref ref-type="fig" rid="f3">Figure 3</xref> is a selection of scanning electron microscopy (SEM) images showing a variety of nanostructures that have been synthesized using NRP spark discharges. <xref ref-type="fig" rid="f3">Figures 3(a)–(e)</xref> show the nanostructures grown using the pin-to-pin setup (<xref ref-type="fig" rid="f1">Fig. 1(b)</xref>) using an applied voltage of 5 kV and a pulse width of 45 ns. These nanostructures were collected via “remote deposition” on different areas of copper strips attached to the inside surface of the plastic tube. As one can see from these images, the spark discharge forms hierarchical architectures with nanometer-scale flakes covering sub-micron scale features, which in turn form micron scale clusters. When the applied voltage was increased to 12 kV, the nanowall-like structures shown in <xref ref-type="fig" rid="f3">Fig. 3(e)</xref> were formed. <xref ref-type="fig" rid="f3">Figure 3(f)–(h)</xref> are the progressively enlarged views of the nanostructures grown using the pin-to-plate configuration shown in <xref ref-type="fig" rid="f1">Fig. 1(c)</xref> at an applied voltage of 7.7 kV and a pulse width of 45 ns. In this case, hierarchical structures consisting of nanoscale dots studding the surfaces of micron-scale structures were also formed. <xref ref-type="fig" rid="f3">Figure 3(i)</xref> shows a nanoporous network produced under the same conditions but at a location on the plane that is approximately 100 μm away from the spot at which the discharge contacts the cathode. In all cases, the produced nanostructures possess well-defined architectures (i.e. flakes, dots, walls, or a porous network), a reasonable uniformity in terms of their distribution over the micron-scale surfaces, and a well-defined structural hierarchy from the nanometer to micron scales.</p><p><xref ref-type="fig" rid="f4">Figure 4</xref> shows more extensive results from materials characterization measurements. The energy-dispersive x-ray spectroscopy (EDS) spectrum from <xref ref-type="fig" rid="f4">Figure 4(a)</xref> reveals the presence of Mo and O but the absence of N, indicating that oxides have been produced selectively by the discharge. As will be discussed later, NRP spark discharges can achieve up to 50% dissociation of O<sub>2</sub>, and therefore it is reasonable to suspect that the abundance of O atoms leads to high oxide content. However, it is not possible to conclude that the lack of nitrides is due to the absence of N atoms, whose production may also be quite significant due to the dissociation of N<sub>2</sub> via electron impact<xref ref-type="bibr" rid="b25">25</xref>.</p><p><xref ref-type="fig" rid="f4">Figure 4(b)</xref> shows a typical Raman spectrum for the nanoflakes shown in <xref ref-type="fig" rid="f3">Figure 3(a)</xref> acquired using a probe beam size of ~ 1 μm. The presence of sharp bands is consistent with crystallinity, whereas the broad features upon which these sharp bands sit can be attributed to an amorphous phase<xref ref-type="bibr" rid="b26">26</xref><xref ref-type="bibr" rid="b27">27</xref>. The bands at 994, 821, and 664 cm<sup>−1</sup> can be readily assigned to M = O and O–M–O stretch modes of α-MoO<sub>3</sub><xref ref-type="bibr" rid="b28">28</xref><xref ref-type="bibr" rid="b29">29</xref>. Smaller peaks at 774 and 849 cm<sup>−1</sup> may be attributed to the same modes but for β-MoO<sub>3</sub><xref ref-type="bibr" rid="b29">29</xref>. The bands at 285 and 337 cm<sup>−1</sup> can be assigned to the δ O = M = O wag mode common to both α- and β-MoO<sub>3</sub> and δ O–M–O bend mode of α-MoO<sub>3</sub>, respectively. These bands are found not only in bulk MoO<sub>3</sub> but also in MoO<sub>3</sub> nanostructures<xref ref-type="bibr" rid="b10">10</xref><xref ref-type="bibr" rid="b30">30</xref>. Also, β-MoO<sub>3</sub> transforms to α-MoO<sub>3</sub> above 450°C<xref ref-type="bibr" rid="b29">29</xref>, thus giving an idea of how hot the substrate surface must have been at some point during the synthesis process. Synthesis occurred on the polyamide substrate in this case, which did not suffer any noticeable thermal damage. This implies that the heat flux from the remote discharge was sufficient to create temperatures exceeding 450°C at the substrate surface but not throughout the bulk. Given the pulse train scheme used and the short duration of the NRP spark, it is possible that transient heating leads to such differences in bulk and surface temperatures of the substrate. Band positions may be shifted from those reported in the literature due to various effects, including different materials supporting the MoO<sub>x</sub> nanostructures<xref ref-type="bibr" rid="b31">31</xref>. The absence of characteristic peaks for MoO<sub>2</sub> at 740 and 569/585 cm<sup>−1</sup> is notable<xref ref-type="bibr" rid="b32">32</xref>. Finally, the band at 149 cm<sup>−1</sup> corresponds to the strongest band of Cu<sub>2</sub>O, which can be expected given that the substrate is Cu<xref ref-type="bibr" rid="b33">33</xref>.</p><p>The conclusions drawn from the Raman spectrum are consistent with the x-ray photoelectron spectroscopy (XPS) spectrum shown in <xref ref-type="fig" rid="f4">Figure 4(c)</xref>. This spectrum shows peaks at 233 and 236 eV common to MoO<sub>3</sub> and MoO<sub>2</sub>, but without the peak at 229 eV characteristic of MoO<sub>2</sub><xref ref-type="bibr" rid="b34">34</xref>. The high-resolution TEM image shown in <xref ref-type="fig" rid="f4">Figure 4(d)</xref> demonstrates that a fraction of the domain is made of small nanocrystals, where the lattice spacing of 0.369 nm corresponds to the (001) plane of MoO<sub>3</sub><xref ref-type="bibr" rid="b30">30</xref>. Although not shown in <xref ref-type="fig" rid="f4">Figure 4(d)</xref>, lattice spacing of 0.345 nm corresponding to the (210) plane of MoO<sub>3</sub> is also observed<xref ref-type="bibr" rid="b35">35</xref>. A typical selected area electron diffraction (SAED) pattern collected from the sample is shown in <xref ref-type="fig" rid="f4">Figure 4(e)</xref> and consists of concentric rings of resolved diffraction spots with few discrete spots lying outside the rings. Such a pattern indicates the presence of a single dominant phase consisting of relatively large polycrystalline grains that are randomly oriented<xref ref-type="bibr" rid="b36">36</xref>. This differs from the presence of both α- and β-MoO<sub>3</sub> indicated by Raman spectroscopy, which can be explained by the fact that the area probed by Raman spectroscopy is much larger than that probed by SAED. The first ring on the SAED pattern reveals the (002) plane of α-MoO<sub>3</sub>.</p></sec><sec disp-level="2"><title>Energy consumed in nanoscale synthesis</title><p><xref ref-type="fig" rid="f5">Figure 5</xref> shows examples of single-shot measurements of the applied voltage, current, and discharge energy of the NRP spark discharges generated during synthesis. Unlike in previous work on NRP spark discharges<xref ref-type="bibr" rid="b37">37</xref>, the total current here is considered to be the conduction current because the capacitance of the discharge circuit is much smaller in this work, such that we can consider the displacement current to be negligible. Single-shot measurements of the discharge energy <italic>E</italic> found by integrating the product of the current and voltage waveforms ranged from 1 to 8 mJ per pulse. This shot-to-shot variation is due to the discharge instability that can result from a variety of factors such as electrode erosion with each discharge event, and the fact that the NRP spark can require several pulses before initiating and then reaching stable behavior<xref ref-type="bibr" rid="b37">37</xref>.</p><p>We can now estimate the energy cost per atom incorporated into the synthesized nanostructures (<italic>ε<sub>atom</sub></italic>). In addition to the aforementioned energy measurement, it was also observed that 2 ± 0.1 mm of the Mo anode was consumed using the direct deposition configuration. Note that in our experiment the peak current of up to 40 A well exceeds a threshold of 10–15 A required for hot spot formation, which means that a pure metal vapor was predominantly produced in the spots formed on the electrode surface. Given that 600 pulse trains of 500 pulses each were applied, and assuming 1 – 8 mJ of energy was dissipated with each pulse, we have 300 – 2400 J of energy dissipated. Given that the Mo electrodes were 250 μm in diameter with 2 mm in length consumed, and that the mass density of solid Mo at room temperature is 10.28 g/cm<sup>3</sup>, with an atomic weight of 95.94 g/mol, we thus assume here that 1 mg or 10 μmol of Mo has been incorporated into nanostructures. This amounts to about 300 – 2400 eV/atom of Mo. The nanostructures have been determined to be MoO<sub>3</sub> in the previous section, which yields <italic>ε<sub>atom</sub></italic> = 75 – 600 eV/atom.</p></sec></sec><sec disp-level="1" sec-type="discussion"><title>Discussion</title><p>Now we consider <italic>ε<sub>atom</sub></italic> as a figure of comparison for the energy efficiency of various methods of nanomaterials synthesis. Globally speaking, it is the energy needed for producing atoms of building material (e.g. by dissociation or evaporation), transporting them to the stacking point, and overcoming energy barriers to incorporation into the assembly. On <xref ref-type="table" rid="t1">Table 1</xref>, we show the minimum possible <inline-formula id="m3"><inline-graphic id="d32e502" xlink:href="srep01221-m3.jpg"></inline-graphic></inline-formula> calculated for several studies of nanofabrication using atmospheric pressure plasma sources without external substrate heating, where <italic>P</italic> is the discharge power and <inline-formula id="m4"><inline-graphic id="d32e508" xlink:href="srep01221-m4.jpg"></inline-graphic></inline-formula> is the nanomaterial mass production rate. Details on how these quantities have been determined from the data in the references can be found in Ref. <xref ref-type="bibr" rid="b19">19</xref>. For the case of the NRP sparks studied here, <italic>P</italic> and <inline-formula id="m5"><inline-graphic id="d32e518" xlink:href="srep01221-m5.jpg"></inline-graphic></inline-formula> are average values over 610 s in real time of applying discharges in the previously mentioned pulse-train fashion, although it should be noted that the instantaneous power during a pulse can reach over 100 kW. We caution that <inline-formula id="m6"><inline-graphic id="d32e521" xlink:href="srep01221-m6.jpg"></inline-graphic></inline-formula> for all of the cases shown in <xref ref-type="table" rid="t1">Table 1</xref> was determined by assuming that all of the material collected or evaporated from electrodes was comprised of or transformed into the reported nanomaterial. To compare <italic>ε<sub>atom</sub></italic> for plasma processing to conventional non-plasma synthesis, we also performed a carbon nanotube growth experiment using a typical thermal furnace process on a Fe-catalyzed silicon substrate, with a furnace heating-up time of 5 min at 6 kW and a growth time of 10 min at 500 W (Furnace OTF-1200X, MTI Corporation).</p><p>Of all of the methods shown in <xref ref-type="table" rid="t1">Table 1</xref>, nanofabrication using NRP discharges is the most energy efficient with the caveat that the values for <italic>ε<sub>atom</sub></italic> shown are the minimum for their respective processes. For NRP discharges, <italic>ε<sub>atom</sub></italic> = 75 – 600 eV/atom represents the range of values obtained from single-shot measurements, as discussed in the previous section and in <xref ref-type="supplementary-material" rid="s1">Supplementary information</xref>. This represents a significant and possibly dramatic improvement over the current benchmark of 1000 eV/atom, although further measurements on the average value of <italic>ε<sub>atom</sub></italic> will be necessary.</p><p>Thus, <xref ref-type="table" rid="t1">Table 1</xref> implies that NRP spark discharges are capable of setting a new standard for energy efficiency in nanoscale synthesis. As discussed in the introduction, this possibility was anticipated in Ref. <xref ref-type="bibr" rid="b19">19</xref> because NRP discharges at atmospheric pressure feature high <<italic>ε</italic>> greater than 2 eV for pulse widths under 100 ns<xref ref-type="bibr" rid="b21">21</xref>. Synthesizing MoO<sub>x</sub> nanostructures in air requires the production of O atoms, which can occur via several mechanisms in an air plasma<xref ref-type="bibr" rid="b38">38</xref>. One example that contributes significantly in NRP sparks is a two-step mechanism<xref ref-type="bibr" rid="b39">39</xref><xref ref-type="bibr" rid="b40">40</xref> in which free electrons elevate ground-state N<sub>2</sub> to various electronically excited states N<sub>2</sub>* (reaction (1)), which in turn dissociate O<sub>2</sub> upon impact (reaction (2)): <disp-formula id="m1"><inline-graphic id="d32e585" xlink:href="srep01221-m1.jpg"></inline-graphic></disp-formula><disp-formula id="m2"><inline-graphic id="d32e588" xlink:href="srep01221-m2.jpg"></inline-graphic></disp-formula></p><p>Reactions (1)–(2) illustrate the importance of high electron energy for efficiently producing O atoms. As <<italic>ε</italic>> increases, a higher proportion of the electrons are found in the high-energy tail of the electron energy distribution function (EEDF), towards energies at which the cross-sections for useful processes is higher. As discussed in the introduction, NRP discharges achieve such control of the EEDF by first rapidly increasing <<italic>ε</italic>> using a short rise time and maintaining high <<italic>ε</italic>> for a short duration on the order of 10 ns before decreasing due to the screening of the applied field by space charge.</p><p>The time evolution of the EEDF of nanosecond discharges has been modeled for the case of a fast ionization wave at 4 torr and shows the development of a significant high-energy tail<xref ref-type="bibr" rid="b41">41</xref>. The corresponding time profile of <<italic>ε</italic>> closely follows that of the reduced electric field <italic>E</italic>/<italic>N</italic>, where <italic>E</italic> is the electric field and <italic>N</italic> is the gas density, with a lag of 0.5 ns. The characteristic time for electron energy relaxation varies directly with the gas density. At atmospheric pressure, <<italic>ε</italic>> would therefore respond yet faster for the same <italic>E</italic>/<italic>N</italic>. Although the decrease of <<italic>ε</italic>> closely tracks that of <italic>E</italic>/<italic>N</italic> during the fall time of the pulse, the high-energy tail relaxes more slowly because this portion of the EEDF is no longer in equilibrium with the field. As a result, reaction rates at a given <italic>E</italic>/<italic>N</italic> for excitation, dissociation, and ionization can differ between unsteady and stationary applied field conditions.</p><p>The high-energy tail of the EEDF characteristic of nanosecond discharges with high <<italic>ε</italic>> shifts the channeling of discharge energy towards reactions (1) and (2) and away from processes that generally are too low in energy to dissociate O<sub>2</sub>. One key example of such wasteful processes in air is the vibrational excitation of N<sub>2</sub>, which consumes over 99% of the discharge energy at low <<italic>ε</italic>> of about 1 eV<xref ref-type="bibr" rid="b38">38</xref>. Such a low <<italic>ε</italic>> is typical of dc discharges in air at atmospheric pressure, for example<xref ref-type="bibr" rid="b42">42</xref>. The vibrational energy generally cascades down to heat the gas via vibrational-translational energy transfer and does not contribute to ionization or electronic excitation. On the other hand, the fraction of the discharge energy expended on all ionization, electronic excitation, and dissociation processes in air can exceed 90% at high values of the reduced electric field<xref ref-type="bibr" rid="b25">25</xref>, which correspond to high <<italic>ε</italic>> conditions. The above arguments are supported by measurements showing that NRP spark discharges in air at atmospheric pressure achieve up to about 50% dissociation of O<sub>2</sub> via the mechanism described by reactions (1) and (2)<xref ref-type="bibr" rid="b43">43</xref>.</p><p>In conclusion, the deterministic approach to energy-efficient nanoscale synthesis has been achieved using NRP spark discharges in ambient air. MoO<sub>3</sub> nanostructures have been synthesized in an open, ambient air environment without using a gas chamber or additional heating of the substrates. Furthermore, the energy expended per atom incorporated into the nanostructure has been shown to be very low compared to many typical plasma and thermal nanoscale synthesis techniques such as CVD. Nanosecond discharges can achieve such energy efficiency because the average electron temperature is maximized with short pulsed excitation. As a result, the discharge energy is focused towards plasma-chemical processes that are useful for synthesis, such as the dissociation of O<sub>2</sub>. These advantages of using NRP discharges for nanomaterials synthesis mark an advance towards the goals of energy efficiency and sustainability outlined in the Grand Energy Challenge by the U.S. Department of Energy<xref ref-type="bibr" rid="b2">2</xref>.</p><p>There are also other interesting aspects to NRP spark-based synthesis. Fast heating and cooling may be responsible for the formation of nonequilibrium material phases, as discussed in Refs. <xref ref-type="bibr" rid="b19">19</xref>,<xref ref-type="bibr" rid="b19">20</xref>. Although the nanostructures have formed in a variety of architectures, they are all composed of MoO<sub>3</sub>. No MoO<sub>2</sub> or nitrides have been detected, which indicates a high degree of chemical selectivity for synthesis. Furthermore, it was possible to grow nanostructures on a polyamide substrate placed only a few millimeters away from the discharge, without melting it. Note that although the pulse train scheme and air cooling were chosen to prevent overheating of the polyamide, the heat flux from the discharge during remote deposition would nonetheless be expected to be much less than when the NRP spark is in direct contact with the substrate.</p><p>There are a number of ways to build upon the results of this work. The pulse duration and amplitude can be tuned to produce desired rates of metal evaporation and oxygen dissociation. In this work, the pulses were applied in trains with pauses in between as a precaution against overheating the polyamide substrate. If the pulses were applied continuously instead, or if the pulse repetition frequency were increased, then the growth rate could be increased above that reported in this work. Furthermore, arrays of discharges could be used to scale up production.</p></sec><sec disp-level="1" sec-type="methods"><title>Methods</title><sec disp-level="2"><title>Electrical circuit and measurement</title><p>In both cases, a solid-state switch-based generator (FID Technology FPG20-30MKS50) supplied positive-polarity pulses of 12.5-kV amplitude and 40-ns duration at a pulse repetition frequency (PRF) of 30 kHz. These high-voltage nanosecond pulses propagated down a 100-Ω coaxial cable terminated by a 2-mm discharge gap in parallel with a matching box. The anode was Mo wire of 250-μm diameter that also served as the precursor material. In the case of “remote” deposition (<xref ref-type="fig" rid="f1">Figure 1(b)</xref>), the cathode was a wire identical to the anode, with a Cu foil strip placed 3 mm away from the discharge serving as the substrate. This Cu foil strip was supported inside a 6-mm diameter polyamide tube, which was cooled by forced air. As an additional measure against heating the polyamide tube, the pulses were applied in trains of 500 pulses each for a total 600 trains, with a 1-s pause between trains. In the case of “direct” deposition (<xref ref-type="fig" rid="f1">Figure 1(c)</xref>), the cathode was a polished Cu plate that also served as the substrate upon which nanostructures were grown and analyzed. A slow downward airflow coming from above the anode aided the downward trajectory of evaporated particulates towards the substrate. For consistency, the pulse train scheme was also applied for the direct deposition experiments, even though no polyamide tube was used. See <xref ref-type="supplementary-material" rid="s1">Supplementary information</xref> for a detailed schematic of the synthesis apparatus as well as details of the measurement techniques for materials characterization and energy.</p><p>A 100-MHz bandwidth high-voltage probe (Lecroy PPE20 kV) was used to measure the voltage across the discharge gap. The discharge current was measured with a Prodyn coil current monitor (Model I 125 2 HF) with a 0.7 rise time.</p></sec><sec disp-level="2"><title>Characterization of nanomaterials</title><p>The surface morphologies, composition analyses and the crystalline features of MoO<sub>3</sub> nanostructures were investigated using SEM (Zeiss Auriga SEM, operated at 4 kV), an Oxford X-max large area EDS SDD detector attached to the SEM, confocal micro-Raman spectroscopy (Renishaw inVia Raman microscope, with a 514 nm laser excitation source), X-ray photoelectron spectroscopy (Specs SAGE 150, Mg Kα source), and HRTEM (JEOL 3000F, operated at 300 kV). EDS analysis was performed on the sample size area ~ 1600 μm<sup>2</sup>.</p><p>The mass of synthesized nanomaterials was determined by the consumption of the wire anode, as follows. The electrode (Mo wire of 0.25-mm diameter) was uniformly consumed from the flat end-face (circular area of 0.25-mm diameter). No erosion of the cylindrical side surface was noticed. The consumption was estimated by measuring the wire length before the experiment and after the application of 3 × 10<sup>5</sup> discharges (600 trains of 500 repetitive discharges). The typical consumption after 3 × 10<sup>5</sup> pulses was 2 mm in length, with a measurement error of 5%. The experiments were repeated several times with very similar consumption levels.</p></sec></sec><sec disp-level="1"><title>Author Contributions</title><p>D.Z.P. and K.O. conceived the project and co-wrote the manuscript. D.Z.P. led the project, designed and performed the synthesis experiments, and analyzed all the data. K.O. supported the work and provided guidance and ideas. S.K. performed the materials characterization and analyzed the corresponding data. D.A.L. performed additional discharge characterization experiments. I.L. contributed to the results interpretation and manuscript preparation. C.O.L. supported the work and contributed to manuscript preparation. All authors discussed the results and read the manuscript.</p></sec><sec sec-type="supplementary-material" id="s1"><title>Supplementary Material</title><supplementary-material id="d32e34" content-type="local-data"><caption><title>Supplementary Information</title><p>Energy Efficiency in Nanoscale Synthesis Using Nanosecond Plasmas</p></caption><media xlink:href="srep01221-s1.pdf" mimetype="application" mime-subtype="pdf"></media></supplementary-material></sec></body><back><ack><p>The authors thank the following sources of funding support: the Agence Nationale de la Recherche IPER (grant ANR-05-BLAN-0090-01) and PREPA (grant ANR-09-BLAN-0043-03) projects, the Ministère de l'Enseignement Supérieur et de la Recherche Chaire d'Excellence program, Australian Research Council, and CSIRO's Science Leadership Program.</p></ack><ref-list><ref id="b1"><mixed-citation publication-type="journal"><name><surname>Ostrikov</surname><given-names>K.</given-names></name><article-title>Control of energy and matter at nanoscales: challenges and opportunities for plasma nanoscience in a sustainability age</article-title>. <source>J. 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Res.</source><volume>9</volume>, <fpage>203</fpage>–<lpage>213</lpage> (<year>2007</year>).</mixed-citation></ref></ref-list></back><floats-group><fig id="f1"><label>Figure 1</label><caption><title>Schematics of the experimental setups for the deposition of MoO<sub>x</sub> nanostructures (NS) by nanosecond repetitively pulsed (NRP) spark discharges in open ambient air.</title><p>(a) The deterministic approach for energy-efficient nanoscale synthesis using atmospheric-pressure plasmas in air (b) The pin-to-pin electrode configuration for “remote deposition” in which the Mo electrodes act as a source of Mo, and the tube enclosing the electrodes is the substrate for the deposition of MoO<sub>x</sub>, and (c) the pin-to-plate electrode configuration for “direct deposition” in which the pin electrode is the source of Mo, and the copper plate is the substrate.</p></caption><graphic xlink:href="srep01221-f1"></graphic></fig><fig id="f2"><label>Figure 2</label><caption><title>Schematic of the characteristic times of nanosecond repetitively pulsed (NRP) discharges.</title><p><italic>ε</italic> – average electron energy; <italic>τ<sub>rise</sub></italic> – pulse rise time; <italic>τ<sub>f</sub></italic> – pulse fall time; <italic>τ<sub>pd</sub></italic> – pulse duration; <italic>τ<sub>ε</sub></italic> – time for electron energy relaxation due to quasi-neutral plasma formation and the loss of high-energy electrons to the anode; <italic>τ<sub>rec</sub></italic> – recombination time of O atoms.</p></caption><graphic xlink:href="srep01221-f2"></graphic></fig><fig id="f3"><label>Figure 3</label><caption><title>SEM images of MoO<sub>3</sub> nanostructures.</title><p>(a–e) Deposited in the pin-to-pin electrode configuration, (f–h) deposited in the pin-to-plate electrode configuration; (i) porous networks of MoO<sub>3 </sub>deposited in the pin-to-plate configuration.</p></caption><graphic xlink:href="srep01221-f3"></graphic></fig><fig id="f4"><label>Figure 4</label><caption><title>Characterization measurements of the crystalline structure and chemical composition of the NRP spark-produced nanostructures shown in <xref ref-type="fig" rid="f3">Figure 3(a)</xref>.</title><p>(a) Energy-dispersive X-ray (EDS) spectrum (b) Raman spectrum, (c) X-ray photoelectron (XPS) spectrum, (d) high-resolution TEM image, and (e) the corresponding selected area electron diffraction (SAED) pattern.</p></caption><graphic xlink:href="srep01221-f4"></graphic></fig><fig id="f5"><label>Figure 5</label><caption><title>Example of single-shot measurements of the applied voltage and current for the NRP spark discharge during the synthesis of the MoO<sub>3</sub> nanostructures shown in <xref ref-type="fig" rid="f3">Figure 3</xref>, as well as the discharge energy calculated using these voltage and current waveforms.</title><p>Note that although the pulse generator was set to deliver high-voltage pulses of 12.5-kV amplitude and 40-ns duration at PRF = 30 kHz, the low discharge resistance causes the voltage pulse to collapse upon spark development. See <xref ref-type="supplementary-material" rid="s1">Figure SI2</xref> in <xref ref-type="supplementary-material" rid="s1">Supplementary information</xref> for a profile of an undistorted pulse.</p></caption><graphic xlink:href="srep01221-f5"></graphic></fig><table-wrap position="float" id="t1"><label>Table 1</label><caption><title>Energy cost of incorporating each atom into the nanostructure <inline-formula id="m7"><inline-graphic id="d32e837" xlink:href="srep01221-m7.jpg"></inline-graphic></inline-formula> using different atmospheric-pressure synthesis processes, where <italic>P</italic> is the average power coupled into the system and <inline-formula id="m8"><inline-graphic id="d32e843" xlink:href="srep01221-m8.jpg"></inline-graphic></inline-formula> is the average mass production rate. In all cases, no external substrate heating was used. Quantities marked by (*) have been calculated in Ref. <xref ref-type="bibr" rid="b19">19</xref> based on data given in the listed references</title></caption><table frame="hsides" rules="groups" border="1"><colgroup><col align="left"></col><col align="center"></col><col align="center"></col><col align="center"></col><col align="center"></col><col align="center"></col><col align="center"></col><col align="center"></col></colgroup><tbody valign="top"><tr><td align="left" valign="top" charoff="50">Source</td><td align="center" valign="top" charoff="50">Carrier gas</td><td align="center" valign="top" charoff="50">Excitation</td><td align="center" valign="top" charoff="50">Nanomaterial</td><td align="center" valign="top" charoff="50"><italic>P</italic> [W]</td><td align="center" valign="top" charoff="50">Max. <inline-formula id="m9"><inline-graphic id="d32e874" xlink:href="srep01221-m9.jpg"></inline-graphic></inline-formula> [μg/s]</td><td align="center" valign="top" charoff="50">Min. ε<italic><sub>atom</sub></italic> [eV]</td><td align="center" valign="top" charoff="50">Ref.</td></tr><tr><td align="center" valign="top" charoff="50">Thermal furnace</td><td align="center" valign="top" charoff="50">Ar</td><td align="center" valign="top" charoff="50">-</td><td align="center" valign="top" charoff="50">Carbon nanotubes</td><td align="center" valign="top" charoff="50">5,000</td><td align="center" valign="top" charoff="50">1</td><td align="center" valign="top" charoff="50">1.2 × 10<sup>8</sup></td><td align="center" valign="top" charoff="50">This work</td></tr><tr><td align="center" valign="top" charoff="50">Microplasma</td><td align="center" valign="top" charoff="50">Ar</td><td align="center" valign="top" charoff="50">144 MHz</td><td align="center" valign="top" charoff="50">Si nanocrystals</td><td align="center" valign="top" charoff="50">35</td><td align="center" valign="top" charoff="50">0.017</td><td align="center" valign="top" charoff="50">600000*</td><td align="center" valign="top" charoff="50"><xref ref-type="bibr" rid="b17">17</xref><xref ref-type="bibr" rid="b44">44</xref></td></tr><tr><td align="center" valign="top" charoff="50">Microplasma</td><td align="center" valign="top" charoff="50">Ar</td><td align="center" valign="top" charoff="50">450 MHz</td><td align="center" valign="top" charoff="50">MoO<sub>3</sub> nanosheets</td><td align="center" valign="top" charoff="50">31</td><td align="center" valign="top" charoff="50">1*</td><td align="center" valign="top" charoff="50">42000*</td><td align="center" valign="top" charoff="50"><xref ref-type="bibr" rid="b12">12</xref></td></tr><tr><td align="center" valign="top" charoff="50">Microplasma</td><td align="center" valign="top" charoff="50">Ar</td><td align="center" valign="top" charoff="50">450 MHz</td><td align="center" valign="top" charoff="50">WO<sub>3</sub> nanoparticles</td><td align="center" valign="top" charoff="50">20</td><td align="center" valign="top" charoff="50">35*</td><td align="center" valign="top" charoff="50">1400*</td><td align="center" valign="top" charoff="50"><xref ref-type="bibr" rid="b45">45</xref></td></tr><tr><td align="center" valign="top" charoff="50">Microsecond spark</td><td align="center" valign="top" charoff="50">Ar</td><td align="center" valign="top" charoff="50">2-μs spark following voltage ramp</td><td align="center" valign="top" charoff="50">Au nanoparticles</td><td align="center" valign="top" charoff="50">1.5*</td><td align="center" valign="top" charoff="50">2*</td><td align="center" valign="top" charoff="50">1500*</td><td align="center" valign="top" charoff="50"><xref ref-type="bibr" rid="b23">23</xref></td></tr><tr><td align="center" valign="top" charoff="50">mw torch</td><td align="center" valign="top" charoff="50">Ar</td><td align="center" valign="top" charoff="50">2.45 GHz</td><td align="center" valign="top" charoff="50">Graphene</td><td align="center" valign="top" charoff="50">250</td><td align="center" valign="top" charoff="50">33</td><td align="center" valign="top" charoff="50">1000*</td><td align="center" valign="top" charoff="50"><xref ref-type="bibr" rid="b46">46</xref></td></tr><tr><td align="center" valign="top" charoff="50">mw torch</td><td align="center" valign="top" charoff="50">Ar</td><td align="center" valign="top" charoff="50">2.45 GHz</td><td align="center" valign="top" charoff="50">Carbon nanotubes</td><td align="center" valign="top" charoff="50">400</td><td align="center" valign="top" charoff="50">7</td><td align="center" valign="top" charoff="50">7200*</td><td align="center" valign="top" charoff="50"><xref ref-type="bibr" rid="b47">47</xref></td></tr><tr><td align="center" valign="top" charoff="50">DC arc</td><td align="center" valign="top" charoff="50">Ar</td><td align="center" valign="top" charoff="50">DC</td><td align="center" valign="top" charoff="50">Ag nanoparticles</td><td align="center" valign="top" charoff="50">120*</td><td align="center" valign="top" charoff="50">3</td><td align="center" valign="top" charoff="50">50000*</td><td align="center" valign="top" charoff="50"><xref ref-type="bibr" rid="b48">48</xref></td></tr><tr><td align="center" valign="top" charoff="50">NRP spark</td><td align="center" valign="top" charoff="50">Air</td><td align="center" valign="top" charoff="50">40-ns pulse at PRF = 30 kHz</td><td align="center" valign="top" charoff="50">MoO<sub>3</sub> nanoflakes/nanowalls</td><td align="center" valign="top" charoff="50">0.5–4</td><td align="center" valign="top" charoff="50">1.6</td><td align="center" valign="top" charoff="50">75</td><td align="center" valign="top" charoff="50">This work</td></tr></tbody></table></table-wrap></floats-group></pmc></record>Pour manipuler ce document sous Unix (Dilib)
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