-
3
-
-
85037874612
-
-
(unpublished)
-
Z.W. Pan (unpublished).
-
-
-
Pan, Z.W.1
-
5
-
-
85037909043
-
-
and Zhang Dian-lin (unpublished)
-
L. Lu, W. Yi, and Zhang Dian-lin (unpublished).
-
-
-
Lu, L.1
Yi, W.2
-
9
-
-
43949163762
-
-
R.A. Jishi, L. Venkataraman, M.S. Dresselhaus, and G. Dresselhaus, Chem. Phys. Lett. 209, 77 (1993).
-
(1993)
Chem. Phys. Lett.
, vol.209
, pp. 77
-
-
Jishi, R.A.1
Venkataraman, L.2
Dresselhaus, M.S.3
Dresselhaus, G.4
-
11
-
-
0001527526
-
-
R. Saito, T. Takeya, T. Kimura, G. Dresselhaus, and M.S. Dresselhaus, Phys. Rev. B 57, 4145 (1998).
-
(1998)
Phys. Rev. B
, vol.57
, pp. 4145
-
-
Saito, R.1
Takeya, T.2
Kimura, T.3
Dresselhaus, G.4
Dresselhaus, M.S.5
-
13
-
-
85037914522
-
-
It is less likely that a complicated (Formula presented) could “happen” to result in a linear (Formula presented) after the integration; in this case one would usually get a complicated T dependence of (Formula presented)
-
It is less likely that a complicated (Formula presented) could “happen” to result in a linear (Formula presented) after the integration; in this case one would usually get a complicated T dependence of (Formula presented)
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-
-
-
14
-
-
85037887919
-
-
This approximation sounds better if considering the fact that the outer walls, which have more weight on the total (Formula presented) than the inner walls, undergo dimensional crossover at even lower temperatures.
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This approximation sounds better if considering the fact that the outer walls, which have more weight on the total (Formula presented) than the inner walls, undergo dimensional crossover at even lower temperatures.
-
-
-
-
19
-
-
26744475447
-
-
Y. Saito, et al., Phys. Rev. B 48, 1907 (1993).
-
(1993)
Phys. Rev. B
, vol.48
, pp. 1907
-
-
Saito, Y.1
-
20
-
-
0000694674
-
-
X. Sun, et al., Phys. Rev. B 54, 12 629 (1996).
-
(1996)
Phys. Rev. B
, vol.54
, pp. 12 629
-
-
Sun, X.1
-
21
-
-
0001132276
-
-
C.-H. Kiang, et al., Phys. Rev. Lett. 81, 1869 (1998).
-
(1998)
Phys. Rev. Lett.
, vol.81
, pp. 1869
-
-
-
23
-
-
0004283499
-
-
Applied Science Publishers, London
-
B.T. Kelly, Physics of Graphite (Applied Science Publishers, London, 1981).
-
(1981)
Physics of Graphite
-
-
Kelly, B.T.1
-
24
-
-
15444347981
-
-
A.M. Rao, et al., Science 275, 187 (1997).
-
(1997)
Science
, vol.275
, pp. 187
-
-
Rao, A.M.1
-
25
-
-
0001098336
-
-
We define the averaged electrical resistivity by assuming that all walls in a MWNT conduct electric current; the characteristic value is about (Formula presented) at 300 K. This value, together with the weak negative temperature-dependent coefficient, are similar to those of disordered semimetallic graphite, and are comparable to previously reported data on MWNT bundles [see S.N. Song, et al., Phys. Rev. Lett. 72, 697 (1994);
-
(1994)
Phys. Rev. Lett.
, vol.72
, pp. 697
-
-
Song, S.N.1
-
27
-
-
16344378712
-
-
H. Dai, et al., Science 275, 1922 (1996)].
-
(1996)
Science
, vol.275
, pp. 1922
-
-
Dai, H.1
-
29
-
-
0000980461
-
-
B. Nysten, J.-P. Issi, R. Barton, Jr., D.R. Boyington, and J.G. Lavin, Phys. Rev. B 44, 2142 (1991).
-
(1991)
Phys. Rev. B
, vol.44
, pp. 2142
-
-
Nysten, B.1
Barton, R.2
Boyington, D.R.3
Lavin, J.G.4
-
30
-
-
0000416063
-
-
)] could contribute to a linear term of specific heat additive to the ordinary term and even surpass the latter at very low temperatures. Obviously, such a mechanism, if it exists, cannot account for a total linear (Formula presented) of the MWNT over the entire temperature range measured.
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For a disordered system, a two-level mechanism [for a review article see W.A. Phillips, Rep. Prog. Phys. 50, 1657 (1987)] could contribute to a linear term of specific heat additive to the ordinary term and even surpass the latter at very low temperatures. Obviously, such a mechanism, if it exists, cannot account for a total linear (Formula presented) of the MWNT over the entire temperature range measured.
-
(1987)
Rep. Prog. Phys.
, vol.50
, pp. 1657
-
-
Phillips, W.A.1
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