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Undercooling driven growth of Q-carbon, diamond, and graphite

Published online by Cambridge University Press:  26 April 2018

Siddharth Gupta
Affiliation:
Department of Materials Science and Engineering, Centennial Campus, North Carolina State University, Raleigh, NC 27695-7907, USA
Ritesh Sachan
Affiliation:
Department of Materials Science and Engineering, Centennial Campus, North Carolina State University, Raleigh, NC 27695-7907, USA Materials Science Division, Army Research Office, Research Triangle Park, NC 27709, USA
Anagh Bhaumik
Affiliation:
Department of Materials Science and Engineering, Centennial Campus, North Carolina State University, Raleigh, NC 27695-7907, USA
Punam Pant
Affiliation:
Department of Materials Science and Engineering, Centennial Campus, North Carolina State University, Raleigh, NC 27695-7907, USA
Jagdish Narayan*
Affiliation:
Department of Materials Science and Engineering, Centennial Campus, North Carolina State University, Raleigh, NC 27695-7907, USA
*
Address all correspondence to Jagdish Narayan at [email protected]
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Abstract

We provide insights pertaining the dependence of undercooling in the formation of graphite, nanodiamonds, and Q-carbon nanocomposites by nanosecond laser melting of diamond-like carbon (DLC). The DLC films are melted rapidly in a super-undercooled state and subsequently quenched to room temperature. Substrates exhibiting different thermal properties—silicon and sapphire, are used to demonstrate that substrates with lower thermal conductivity trap heat flow, inducing larger undercooling, both experimentally and theoretically via finite element simulations. The increased undercooling facilitates the formation of Q-carbon. The Q-carbon is used as nucleation seeds for diamond growth via laser remelting and hot-filament chemical vapor deposition.

Type
Research Letters
Copyright
Copyright © Materials Research Society 2018 

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References

1.Narayan, J., Godbole, V., and White, C.: Laser method for synthesis and processing of continuous diamond films on nondiamond substrates. Science 252, 416 (1991).Google Scholar
2.Narayan, J. and Bhaumik, A.: Novel phase of carbon, ferromagnetism, and conversion into diamond. J. Appl. Phys. 118, 215303 (2015).CrossRefGoogle Scholar
3.Gupta, S., Bhaumik, A., Sachan, R., and Narayan, J.: Structural Evolution of Q-Carbon and Nanodiamonds. JOM 70, 450 (2018). https://doi.org/10.1007/s11837-017-2714-y.CrossRefGoogle Scholar
4.Heremans, J., Olk, C., Eesley, G., Steinbeck, J., and Dresselhaus, G.: Observation of metallic conductivity in liquid carbon. Phys. Rev. Lett. 60, 452 (1988).Google Scholar
5.Narayan, J., and Bhaumik, A.: Q-carbon discovery and formation of single-crystal diamond nano-and microneedles and thin films. Mater. Res. Lett. 4, 118 (2016).Google Scholar
6.Narayan, J. and Bhaumik, A.: Research update: direct conversion of amorphous carbon into diamond at ambient pressures and temperatures in air. Appl. Phys. Lett. Mater. 3, 100702 (2015).Google Scholar
7.Bhaumik, A., Sachan, R., Gupta, S., and Narayan, J.: Discovery of high-temperature superconductivity (T c = 55 K) in B-Doped Q-Carbon. ACS Nano 11, 11915 (2017).Google Scholar
8.Narayan, J., Gupta, S., Bhaumik, A., Sachan, R., Cellini, F., and Reido, E.: Q-carbon is harder than diamond. MRS Comm., 1 (2018). doi: 10.1557/mrc.2018.35.Google Scholar
9.Gupta, S., Sachan, R., Bhaumik, A., and Narayan, J.: Superhard Q-carbon nanocomposites J. Appl. Phys. (2018) under review.Google Scholar
10.Bhaumik, A., Nori, S., Sachan, R., Gupta, S., Kumar, D., Majumdar, A.K., and Narayan, J.: Room-temperature ferromagnetism and extraordinary hall effect in nanostructured Q-carbon: implications for potential spintronic devices. ACS Appl. Nano Mater. 1, 807 (2018). doi: 10.1021/acsanm.7b00253.Google Scholar
11.Bhaumik, A., Sachan, R., and Narayan, J.: High-temperature superconductivity in boron-doped Q-carbon. ACS Nano 11, 11915 (2017). doi: 10.1021/acsnano.7b06888.Google Scholar
12.Bhaumik, A., Sachan, R., and Narayan, J.: A novel high-temperature carbon-based superconductor: B-doped Q-carbon. J. Appl. Phys. 122, 045301 (2017).Google Scholar
13.Narayan, J. and Bhaumik, A.: Novel synthesis and properties of pure and NV-doped nanodiamonds and other nanostructures. Mater. Res. Lett. 5, 242 (2016).CrossRefGoogle Scholar
14.Kumomi, H.: Location control of crystal grains in excimer laser crystallization of silicon thin films. Appl. Phys. Lett. 83, 434 (2003).Google Scholar
15.Shamsa, M., Liu, W., Balandin, A., Casiraghi, C., Milne, W., and Ferrari, A.: Thermal conductivity of diamond-like carbon films. Appl. Phys. Lett. 89, 161921 (2006).Google Scholar
16.Steinbeck, J., Dresselhaus, G., and Dresselhaus, M.: The properties of liquid carbon. Int. J. Therm. 11, 789 (1990).Google Scholar
17.Ho, C.Y., Powell, R.W., and Liley, P.E.: Thermal conductivity of the elements: a comprehensive review, (NATIONAL STANDARD REFERENCE DATA SYSTEM1974).Google Scholar
18.Sachan, R., Yadavali, S., Shirato, N., Krishna, H., Ramos, V., Duscher, G., Pennycook, S.J., Gangopadhyay, A., Garcia, H., and Kalyanaraman, R.: Self-organized bimetallic ag–co nanoparticles with tunable localized surface plasmons showing high environmental stability and sensitivity. Nanotechnology 23, 275604 (2012).CrossRefGoogle ScholarPubMed
19.Sachan, R., Ramos, V., Malasi, A., Yadavali, S., Bartley, B., Garcia, H., Duscher, G., and Kalyanaraman, R.: Oxidation-resistant silver nanostructures for ultrastable plasmonic applications. Adv. Mater. 25, 2045 (2013).Google Scholar
20.Sachan, R., Malasi, A., Ge, J., Yadavali, S., Krishna, H., Gangopadhyay, A., Garcia, H., Duscher, G., and Kalyanaraman, R.: Ferroplasmons: intense localized surface plasmons in metal-ferromagnetic nanoparticles. ACS Nano 8, 9790 (2014).Google Scholar
21.Trice, J., Thomas, D., Favazza, C., Sureshkumar, R., and Kalyanaraman, R.: Pulsed-laser-induced dewetting in nanoscopic metal films: theory and experiments. Phys. Rev. B 75, 235439 (2007).Google Scholar
22.Bhaumik, A., and Narayan, J.: Wafer scale integration of reduced graphene oxide by novel laser processing at room temperature in air. J. Appl. Mater. 10, 105304 (2016).Google Scholar
23.Bhaumik, A., and Narayan, J.: Synthesis and characterization of quenched and crystalline phases: Q-carbon, Q-BN, diamond and phase-pure c-BN. JOM 70, 456 (2018).Google Scholar
24.Narayan, J.: Dislocations, twins, and grain boundaries in CVD diamond thin films: atomic structure and properties. J. Mater. Res. 5, 2414 (1990).Google Scholar
25.Jackson, K.: Crystal Growth and Phase Formation. In Surface Modification and Alloying, edited by Poate, J.M., Foti, G. and Jacobson, D.C. (Springer, Boston, MA, 1983) p. 51.CrossRefGoogle Scholar
26.Narayan, J.: Interface structures during solid-phase-epitaxial growth in ion implanted semiconductors and a crystallization model. J. Appl. Phys. 53, 8607 (1982).Google Scholar
27.Spaepen, F., Turnbull, D., Poate, J., and Mayer, J.: Laser annealing of semiconductors. In Laser Annealing of Semiconductors, edited by Poate, J.M. and Mayor, J.W. (Academic, New York, 1982), p. 15.Google Scholar
28.Cullis, A., Chew, N., Webber, H., and Smith, D.J.: Orientation dependence of high speed silicon crystal growth from the melt. J. Crys. Grow. 68, 624 (1984).Google Scholar
29.Singh, R.K. and Narayan, J.: A novel method for simulating laser-solid interactions in semiconductors and layered structures. Mater. Sci. Engg.: B 3, 217 (1989).Google Scholar
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