-
1
-
-
19944396853
-
-
Luryi, S., Xu, J., Zaslavsky, A., Eds.; Wiley: New York
-
Solomon, P.; Kagan, C. R. in Future Trends in Microelectronics: The Nano, the Giga, and the Ultra; Luryi, S., Xu, J., Zaslavsky, A., Eds.; Wiley: New York, 2004; p 168.
-
(2004)
Future Trends in Microelectronics: The Nano, the Giga, and the Ultra
, pp. 168
-
-
Solomon, P.1
Kagan, C.R.2
-
2
-
-
2342471251
-
-
Other recent discussions of this have been given by Ghosh, A. W.; Rakshit, T.; Datta, S. Nano Lett. 2004, 4, 565
-
(2004)
Nano Lett.
, vol.4
, pp. 565
-
-
Ghosh, A.W.1
Rakshit, T.2
Datta, S.3
-
3
-
-
0000042026
-
-
Di Ventra, M.; Pantelides, S. T.; Lang, N. D. Appl. Phys. Lett. 2000, 76, 3448
-
(2000)
Appl. Phys. Lett.
, vol.76
, pp. 3448
-
-
Di Ventra, M.1
Pantelides, S.T.2
Lang, N.D.3
-
5
-
-
0344511650
-
-
and Yang, Y.; Lang, N. D.; Di Ventra, M. Appl. Phys. Lett. 2003, 82, 1938.
-
(2003)
Appl. Phys. Lett.
, vol.82
, pp. 1938
-
-
Yang, Y.1
Lang, N.D.2
Di Ventra, M.3
-
6
-
-
2642569912
-
-
Experimental studies of gating of carbon nanotubes are given, e.g., by Lin, Y.-M.; Appenzeller, J.; Avouris, Ph. Nano Lett. 2004, 4, 947
-
(2004)
Nano Lett.
, vol.4
, pp. 947
-
-
Lin, Y.-M.1
Appenzeller, J.2
Avouris, Ph.3
-
7
-
-
1642487759
-
-
Javey, A.; Guo, J.; Farmer, D. B.; Wang, Q.; Wang, D.; Gordon, R. G.; Lundstrom, M.; Dai, H. Nano Lett. 2004, 4, 447
-
(2004)
Nano Lett.
, vol.4
, pp. 447
-
-
Javey, A.1
Guo, J.2
Farmer, D.B.3
Wang, Q.4
Wang, D.5
Gordon, R.G.6
Lundstrom, M.7
Dai, H.8
-
8
-
-
0842287345
-
-
Biercuk, M. J.; Mason, N.; Marcus, C. M. Nano Lett. 2004, 4, 1
-
(2004)
Nano Lett.
, vol.4
, pp. 1
-
-
Biercuk, M.J.1
Mason, N.2
Marcus, C.M.3
-
9
-
-
2342527945
-
-
Li, S.; Yu, Z.; Yen, S.-F; Tang, W. C.; Burke, P. J. Nano Lett. 2004, 4, 753
-
(2004)
Nano Lett.
, vol.4
, pp. 753
-
-
Li, S.1
Yu, Z.2
Yen, S.-F.3
Tang, W.C.4
Burke, P.J.5
-
10
-
-
0005836651
-
-
Martel, R.; Schmidt, T.; Shea, H. R.; Hertel, T.; Avouris, Ph. Appl. Phys. Lett. 1998, 73, 2447
-
(1998)
Appl. Phys. Lett.
, vol.73
, pp. 2447
-
-
Martel, R.1
Schmidt, T.2
Shea, H.R.3
Hertel, T.4
Avouris, Ph.5
-
11
-
-
0032492884
-
-
and Tans, S.; Verschueren, A.; Dekker, C. Nature (London) 1998, 393, 49.
-
(1998)
Nature (London)
, vol.393
, pp. 49
-
-
Tans, S.1
Verschueren, A.2
Dekker, C.3
-
12
-
-
19944374518
-
-
note
-
These H atoms are expected to be removed when the molecule bonds to a metal.
-
-
-
-
14
-
-
0002305877
-
-
that in solid biphenyl, the equilibrium configuration has a twist angle of 13.3° between the two carbon rings, but that at room temperature, the average configuration is planar. For the gas phase, electron diffraction measurements [Almenningen, A.; et al. J. Mol. Struct. 1985, 128, 59]
-
(1985)
J. Mol. Struct.
, vol.128
, pp. 59
-
-
Almenningen, A.1
-
15
-
-
0035894316
-
-
show a twist angle of 44.4°. A density-functional calculation for the geometry of biphenyl in the gas phase is given by Arulmozhiraja, S.; Fujii, T. J. Chem. Phys. 2001, 115, 10589.
-
(2001)
J. Chem. Phys.
, vol.115
, pp. 10589
-
-
Arulmozhiraja, S.1
Fujii, T.2
-
16
-
-
0037399058
-
-
Ronald Breslow (private communication) has pointed out that another way to ensure that the rings are in fact coplanar is to consider instead dihydrophenanthrene. The geometry dependence of the current has been studied by Ghosh et al. (ref 2); cf. also Troisi, A.; Ratner, M. A.; Nitzan, A. J. Chem. Phys. 2003, 118, 6072
-
(2003)
J. Chem. Phys.
, vol.118
, pp. 6072
-
-
Troisi, A.1
Ratner, M.A.2
Nitzan, A.3
-
17
-
-
0842278601
-
-
and Pecchia, A.; Gheorghe, M.; Di Carlo, A.; Lugli, P.; Niehaus, T. A.; Frauenheim, Th.; Scholz, R. Phys. Rev. B 2003, 68, 235321.
-
(2003)
Phys. Rev. B
, vol.68
, pp. 235321
-
-
Pecchia, A.1
Gheorghe, M.2
Di Carlo, A.3
Lugli, P.4
Niehaus, T.A.5
Frauenheim, Th.6
Scholz, R.7
-
19
-
-
0035883571
-
-
The various bond distances used are given in ref 16 of Lang, N. D.; Avouris, Ph. Phys. Rev. B 2001, 64, 125323. This paper reported the conductance of the BPH molecule in the absence of a gate.
-
(2001)
Phys. Rev. B
, vol.64
, pp. 125323
-
-
Lang, N.D.1
Avouris, Ph.2
-
20
-
-
19944365278
-
-
note
-
The separation of the two electrodes that comprise the gate was taken to be 12.4 b; the width of the electrodes was taken to be 9.85 b.
-
-
-
-
21
-
-
19944408409
-
-
note
-
G, are referenced to the source.
-
-
-
-
24
-
-
19944379189
-
-
note
-
This was seen clearly in figures showing changes in the spatial distribution of total charge in response to changes in gate voltage. These figures are not reproduced here for lack of space.
-
-
-
-
25
-
-
19944405511
-
-
note
-
By state density we mean the difference in density of energy eigenstates between two systems: the electrodes together with the molecule, and the same electrodes (with the same spacing) without the molecule. The eigenstates are those of the single-particle equations of the density functional formalism.
-
-
-
-
26
-
-
0141451990
-
-
The separate polarizabilities of the σ and π systems were also seen in Lang, N. D.; Avouris, Ph. Nano Lett. 2003, 3, 737.
-
(2003)
Nano Lett.
, vol.3
, pp. 737
-
-
Lang, N.D.1
Avouris, Ph.2
-
29
-
-
84971101851
-
-
Cheng, C. L.; Murthy, D. S. N.; Ritchie, G. L. D. Aust. J. Chem. 1972, 25, 1301.
-
(1972)
Aust. J. Chem.
, vol.25
, pp. 1301
-
-
Cheng, C.L.1
Murthy, D.S.N.2
Ritchie, G.L.D.3
|