-
2
-
-
0037009148
-
-
10.1016/S0042-207X(02)00185-9;
-
D. R. T. Zahn, S. Park, and T. U. Kampen, Vacuum 67, 101 (2002) 10.1016/S0042-207X(02)00185-9
-
(2002)
Vacuum
, vol.67
, pp. 101
-
-
Zahn, D.R.T.1
Park, S.2
Kampen, T.U.3
-
4
-
-
3342974684
-
-
10.1016/j.apsusc.2004.05.258
-
T. Kampen, A. Bekkali, I. Thurzo, D. R. T. Zahn, A. Bolognesi, T. Ziller, A. Di Carlo, and P. Lugli, Appl. Surf. Sci. 234, 313 (2004). 10.1016/j.apsusc.2004.05.258
-
(2004)
Appl. Surf. Sci.
, vol.234
, pp. 313
-
-
Kampen, T.1
Bekkali, A.2
Thurzo, I.3
Zahn, D.R.T.4
Bolognesi, A.5
Ziller, T.6
Di Carlo, A.7
Lugli, P.8
-
7
-
-
0030150242
-
-
10.1016/0038-1101(95)00158-1;
-
Y. Onganer, M. Saǧlam, A. Türüt, H. Efeoǧlu, and S Tüzemen, Solid-State Electron. 39, 677 (1996) 10.1016/0038-1101(95)00158- 1
-
(1996)
Solid-State Electron.
, vol.39
, pp. 677
-
-
Onganer, Y.1
Saǧlam, M.2
Türüt, A.3
Efeoǧlu, H.4
Tüzemen, S.5
-
8
-
-
39549112521
-
-
10.1016/j.apsusc.2007.10.082
-
Ö. Güllü, Ö. Bariş, M. Biber, and A. Türüt, Appl. Surf. Sci. 254, 3039 (2008). 10.1016/j.apsusc.2007.10.082
-
(2008)
Appl. Surf. Sci.
, vol.254
, pp. 3039
-
-
Güllü, Ö.1
Bariş, Ö.2
Biber, M.3
Türüt, A.4
-
10
-
-
11344290288
-
-
10.1002/adma.200400923
-
H. Haick, M. Ambrico, T. Ligonzo and D. Cahen, Adv. Mater. (Weinheim, Ger.) 16, 2145 (2004). 10.1002/adma.200400923
-
(2004)
Adv. Mater. (Weinheim, Ger.)
, vol.16
, pp. 2145
-
-
Haick, H.1
Ambrico, M.2
Ligonzo, T.3
Cahen, D.4
-
11
-
-
52649083451
-
-
10.1021/jp802685j
-
M. A. Kuikka, W. Li, K. L. Kavanagh, and H.-Z. Yu, J. Phys. Chem. C 112, 9081 (2008). 10.1021/jp802685j
-
(2008)
J. Phys. Chem. C
, vol.112
, pp. 9081
-
-
Kuikka, M.A.1
Li, W.2
Kavanagh, K.L.3
Yu, H.-Z.4
-
12
-
-
33847657425
-
-
10.1063/1.2710211
-
S. Özcan, J. Smoliner, M. Andrews, and G. Strasser, T. Dienel, R. Franke, and T. Fritz, Appl. Phys. Lett. 90, 092107 (2007). 10.1063/1.2710211
-
(2007)
Appl. Phys. Lett.
, vol.90
, pp. 092107
-
-
Özcan, S.1
Smoliner, J.2
Andrews, M.3
Strasser, G.4
Dienel, T.5
Franke, R.6
Fritz, T.7
-
14
-
-
36149025707
-
-
10.1103/PhysRev.71.717
-
J. Bardeen, Phys. Rev. 71, 717 (1947). 10.1103/PhysRev.71.717
-
(1947)
Phys. Rev.
, vol.71
, pp. 717
-
-
Bardeen, J.1
-
15
-
-
3743067479
-
-
10.1103/PhysRev.138.A1689
-
V. Heine, Phys. Rev. 138, A1689 (1965). 10.1103/PhysRev.138.A1689
-
(1965)
Phys. Rev.
, vol.138
, pp. 1689
-
-
Heine, V.1
-
16
-
-
0018523693
-
-
10.1116/1.570215
-
W. E. Spicer, P. W. Chye, P. R. Skeath, C. Y. Su, and I. Lindau, J. Vac. Sci. Technol. 16, 1422 (1979). 10.1116/1.570215
-
(1979)
J. Vac. Sci. Technol.
, vol.16
, pp. 1422
-
-
Spicer, W.E.1
Chye, P.W.2
Skeath, P.R.3
Su, C.Y.4
Lindau, I.5
-
19
-
-
23944444818
-
-
10.1063/1.2008371
-
T. Shimada, H. Nogawa, T. Hasegawa, R. Okada, H. Ichikawa, K. Ueno, and K. Saiki, Appl. Phys. Lett. 87, 061917 (2005). 10.1063/1.2008371
-
(2005)
Appl. Phys. Lett.
, vol.87
, pp. 061917
-
-
Shimada, T.1
Nogawa, H.2
Hasegawa, T.3
Okada, R.4
Ichikawa, H.5
Ueno, K.6
Saiki, K.7
-
20
-
-
67650310240
-
-
The condition for the thickness of the dielectric film for which the electrochemical energies in the heterojunction can still line up is in practice a difficult one to write down. Here we consider the case where no bias is applied across the device (as is the case in BEES). The condition is connected to the practical time scales that samples are prepared and then measured. We can estimate (order of magnitude) the time taken to equilibrate as τ eA ψ1/2 mr 1/2 δ, where A=1.025 -1 eV-1/2, ψ is the potential barrier, and mr is the relative effective mass in the dielectric. For the pentacene effective mass of mr =0.3, we find that 2 nm thickness takes just under 8 h to equilibrate. However, 4 nm takes more than 20 years. We emphasize that these are order of magnitude estimates.
-
The condition for the thickness of the dielectric film for which the electrochemical energies in the heterojunction can still line up is in practice a difficult one to write down. Here we consider the case where no bias is applied across the device (as is the case in BEES). The condition is connected to the practical time scales that samples are prepared and then measured. We can estimate (order of magnitude) the time taken to equilibrate as τ eA ψ1/2 mr 1/2 δ, where A=1.025-1 eV-1/2, ψ is the potential barrier, and mr is the relative effective mass in the dielectric. For the pentacene effective mass of mr =0.3, we find that 2 nm thickness takes just under 8 h to equilibrate. However, 4 nm takes more than 20 years. We emphasize that these are order of magnitude estimates.
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-
-
-
21
-
-
67650291514
-
-
The values used in Eq. 13 were ψbi =0.83 V- ξn - Δ image δ=0, ξn =0.3 V, kT/e=0.025 V, sr =11.9, and org r =4.0. The value chosen for ψbi corresponds Au/n-Si (111) barrier measured. We can use this value for ψbi as a first-order approximation together with the thickness of the pentacene as δ. This makes the calculation cleaner as it is less dependant on measurements in the literature of m -χ. We find that the higher-order corrections are significantly (a few orders of magnitude) smaller than the first-order approximation that we used.
-
The values used in Eq. 13 were ψbi =0.83 V- ξn - Δ image δ=0, ξn =0.3 V, kT/e=0.025 V, sr =11.9, and org r =4.0. The value chosen for ψbi corresponds Au/n-Si (111) barrier measured. We can use this value for ψbi as a first-order approximation together with the thickness of the pentacene as δ. This makes the calculation cleaner as it is less dependant on measurements in the literature of m -χ. We find that the higher-order corrections are significantly (a few orders of magnitude) smaller than the first-order approximation that we used.
-
-
-
-
22
-
-
0001021351
-
-
10.1016/0370-1573(94)00082-E
-
M. Prietsch, Phys. Rep. 253, 163 (1995). 10.1016/0370-1573(94)00082-E
-
(1995)
Phys. Rep.
, vol.253
, pp. 163
-
-
Prietsch, M.1
-
24
-
-
17244365811
-
-
10.1103/PhysRevLett.61.2368
-
L. D. Bell and W. J. Kaiser, Phys. Rev. Lett. 61, 2368 (1988). 10.1103/PhysRevLett.61.2368
-
(1988)
Phys. Rev. Lett.
, vol.61
, pp. 2368
-
-
Bell, L.D.1
Kaiser, W.J.2
-
25
-
-
4143136990
-
-
10.1016/0039-6028(86)90857-5
-
J. Tersoff, Surf. Sci. 168, 275 (1986). 10.1016/0039-6028(86)90857-5
-
(1986)
Surf. Sci.
, vol.168
, pp. 275
-
-
Tersoff, J.1
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