J. Phys. Soc. Jpn. 74 (2005) pp. 515-518  |Next Article|  |Table of Contents|
|Full Text PDF (97K)| |Buy This Article|

Letters

Nonlinear Charging and Transport Times in Doped Nanotubes Junctions

Keivan Esfarjani, Amir A. Farajian1, Yoshiyuki Kawazoe1 and Siu Tat Chui2

Department of Physics, Sharif University of Technology, Tehran 11365-9161, Iran
1IMR, Tohoku University, Sendai 980-8577
2BRI, University of Delaware, Newark, DE 19716, U.S.A.

(Received September 1, 2004)

The nonlinear capacitance in doped nanotube junctions is calculated self consistently. A negative differential capacitance is observed when the applied bias becomes larger than the pseudogap of the metallic armchair nanotube. For this device, one can deduce a relaxation time of approximately 0.1 fs. Because of its negative differential resistance (NDR), a switching time of less than a femtosecond, i.e., at least three orders smaller than present-day switching times, can also be estimated. This effect is important in designing ultrafast nano-electronic components. ©2005 The Physical Society of Japan

KEYWORDS: nanotube, junction, transport, device, response time
URL: http://jpsj.ipap.jp/link?JPSJ/74/515/
DOI: 10.1143/JPSJ.74.515


|Full Text PDF (97K)| |Buy This Article| Citation:


References | Citing Article (1)

  1. M. Büttiker: J. Low Temp. Phys. 118 (2000) 519[CrossRef].
  2. M. Büttiker, A. Prêtre and H. Thomas: Phys. Rev. Lett. 70 (1993) 4114[APS].
  3. M. Büttiker, H. Thomas and A. Prêtre: Phys. Lett. A 180 (1993) 364[CrossRef].
  4. X. Zhao, J. Wang and H. Guo: Phys. Rev. B 60 (1999) 16730[APS].
  5. Y.-P. Zhao, B. Q. Wei, P. M. Ajayan, G. Ramanath, T.-M. Lu and G.-C. Wang: Phys. Rev. B 64 (2001) 201402[APS](R).
  6. J. G. Hou, B. Wang, J. Yang, X. R. Wang, H. Q. Wang, Q. Zhu and X. Xiao: Phys. Rev. Lett. 86 (2001) 5321[APS].
  7. G. Cuniberti, M. Sassetti and B. Kramer: Phys. Rev. B 57 (1998) 1515[APS].
  8. G. Cuniberti, M. Sassetti and B. Kramer: J. Phys.: Condens. Matter 8 (1996) L21[IoP STACKS].
  9. K. Esfarjani, A. A. Farajian, Y. Hashi and Y. Kawazoe: Appl. Phys. Lett. 74 (1999) 79[AIP Scitation].
  10. A. A. Farajian, K. Esfarjani and Y. Kawazoe: Phys. Rev. Lett. 82 (1999) 5084[APS].
  11. A. A. Farajian, K. Esfarjani and M. Mikami: Phys. Rev. B 65 (2002) 165415[APS].
  12. R. G. Pearson: Inorg. Chem. 27 (1988) 734.
  13. K. Esfarjani and Y. Kawazoe: J. Phys.: Condens. Matter 10 (1998) 8257[IoP STACKS].
  14. The effect of the substrate or dopants is to transfer some charge to the tube. This modifies the on-site energies which we assume to be known for the two semi-infinite tubes. From this, the additional charge can be easily deduced without the need to perform a self-consistent calculation, if the on-site energies are uniform. At the junction, however, a self-consistent calculation needs to be performed in order to determine the charge and potential profiles, even if the two separated half tubes are treated non-self-consistently.
  15. M. P. Lopez Sancho, J. M. Lopez Sancho and J. Rubio: J. Phys. F 14 (1984) 1205[IoP STACKS].
  16. M. P. Lopez Sancho, J. M. Lopez Sancho, J. M. L. Sancho and J. Rubio: J. Phys. F 15 (1985) 851[IoP STACKS].
  17. P. A. Lee and D. S. Fisher: Phys. Rev. Lett. 47 (1981) 882[APS].
  18. A. MacKinnon: Z. Phys. B 59 (1985) 385[CrossRef].
  19. M. C. Munoz, V. R. Velasco and F. Garcia-Moliner: Prog. Surf. Sci. 26 (1987) 117.
  20. F. Garcia-Moliner and V. R. Velasco: Theory of Single and Multiple Interfaces (World Scientific, Singapore, 1992).
  21. S. Datta: Electronic Transport in Mesoscopic Systems (Cambridge University Press, Cambridge, U.K., 1995).
  22. L. Chico, L. X. Benedict, S. G. Louie and M. L. Cohen: Phys. Rev. B 54 (1996) 2600[APS].
  23. L.-C. Qin, X. Zhao, K. Hirahara, Y. Miyamoto, Y. Ando and S. Iijima: Nature 408 (2000) 50; The electronic structure of the (3,3) tube, however, is not correctly predicted by the one-orbital TB method, due to neglecting the hybrdization of σ* and π* orbitals; however we have considered it because of computational convenience and as an illustration of the results.
  24. Cequivalent-1=Cgeometrical-1+Cquantum-1= εA/d+e2 DOS(µ). This relation, already explained in the introduction, explains why the real value of the capacitance of a nanodevice is always smaller than its geometrical value.
  25. M. S. Dresselhaus, G. Dresselhaus and P. C. Eklund: Science of Fullerenes and Carbon Nanotubes (Academic Press, San Diego, CA, 1996).
  26. The exact value of the junction resistance turns out to be very close to its ballistic value due to the small charge accumulation across the junction and the neglect of any disorder. The RC relaxation time is obtained from this exact calculation.
  27. T. Hertel and G. Moos: Phys. Rev. Lett. 84 (2000) 5002[APS].

|TOP|  |Next Article|  |Table of Contents| |JPSJ Home|
Copyright © 2010 The Physical Society of Japan
Contact Information