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Temperature dependence of the hole mobility

Figure 12-27. Temperature dependence of the hole mobility in DPOP-PPV at different electric fields Dale for T= 0 have been obtained by extrapolation. The inset shows the intersection of Arrhenius plots at T()=465 K (Ref. 1831). Figure 12-27. Temperature dependence of the hole mobility in DPOP-PPV at different electric fields Dale for T= 0 have been obtained by extrapolation. The inset shows the intersection of Arrhenius plots at T()=465 K (Ref. 1831).
Fig. 9 Temperature dependence of the hole mobility of a polyfluorene copolymer inferred from space-charge-limited current measurements on samples of thicknesses 122 nm, 1 pm, and 10 pm. The full curve is an extrapolation to the low carrier density limit using the extended Gaussian disorder model. From [90] with permission. Copyright (2008) by the American Institute of Physics... Fig. 9 Temperature dependence of the hole mobility of a polyfluorene copolymer inferred from space-charge-limited current measurements on samples of thicknesses 122 nm, 1 pm, and 10 pm. The full curve is an extrapolation to the low carrier density limit using the extended Gaussian disorder model. From [90] with permission. Copyright (2008) by the American Institute of Physics...
In this context it is appropriate to recall the work of Mozer et al. [91] on hole transport in regio(3-hexylthiophene). These authors compared the field and temperature dependencies of the hole mobility measured via the ToF and CELIV methods. Quite remarkably, the temperature dependence deduced from ToF signals plotted on a In p vs scale deviate significantly from linearity while the CELIV data follow a In p law down to lowest temperatures (180 K) (see Fig. 10). The reason is that... [Pg.27]

Fig. 11 Temperature dependence of the hole mobility in PMPSi at different electric fields. Full curves are calculated using the theory by Fishchuk et al. [70], The fit parameters are the width a of the density of states distribution, the activation energy (which is p/2), the electronic exchange integral J, and the intersite separation a. From [70] with permission. Copyright (2003) by the American Institute of Physics... Fig. 11 Temperature dependence of the hole mobility in PMPSi at different electric fields. Full curves are calculated using the theory by Fishchuk et al. [70], The fit parameters are the width a of the density of states distribution, the activation energy (which is p/2), the electronic exchange integral J, and the intersite separation a. From [70] with permission. Copyright (2003) by the American Institute of Physics...
Fig. 17 Temperature dependence of the hole mobility measured in an FET with (a) pentacene and (b) P3HT as active layers. Parameter Is the gate voltage. Data fitting using the Fishchuk et al. theory in [102] yields values for the mobility and the disorder potential extrapolated to zero electric field and zero carrier concentration. To is the Meyer-Nedel temperature (see text). From [102] with permission. Copyright (2010) by the American Institute of Physics... Fig. 17 Temperature dependence of the hole mobility measured in an FET with (a) pentacene and (b) P3HT as active layers. Parameter Is the gate voltage. Data fitting using the Fishchuk et al. theory in [102] yields values for the mobility and the disorder potential extrapolated to zero electric field and zero carrier concentration. To is the Meyer-Nedel temperature (see text). From [102] with permission. Copyright (2010) by the American Institute of Physics...
Gambino S, Samuel IDW, Barcena H, Bum PL (2008) Electric field and temperature dependence of the hole mobility in a bis-fluorene cored dendrimer. Org Electron 9 220... [Pg.59]

Figure 5 The temperature dependencies of the hole mobility of TPM-E doped PS. Figure 5 The temperature dependencies of the hole mobility of TPM-E doped PS.
Figure 22 The temperature dependence of the hole mobility of EFTP doped PC. Figure 22 The temperature dependence of the hole mobility of EFTP doped PC.
Figure 66 The temperature dependencies of the hole mobility of the hydrazone compound designated as CT6 in Fig. 65 in PC. The field dependence of the activation energy is shown in the inset. Figure 66 The temperature dependencies of the hole mobility of the hydrazone compound designated as CT6 in Fig. 65 in PC. The field dependence of the activation energy is shown in the inset.
FIGURE 2.1.22 Temperature dependence of the hole mobility in ultrapure pentacene crystals extracted from the SCLC measurements. The open symbols correspond to the valnes of p calculated under an assumption of uniform current flow across the crystal thickness solid symbols take into account the anisotropy of conductivity in pentacene. Below room temperature, the mobility increases with decreasing T as p T T where y 2.4. (From Jurchescu, O. D. et ah, Appl. Phys. Lett., 84, 3061, 2004.)... [Pg.56]

Fig. 8.2 The temperature dependence of the hole mobility jLt in an 8.7 /xm thick disordered film of MPMP molecules at different field strengths F. MPMP = bis(4-N,N-diethylamino-2-methylphenyl)-4-methylphenylmethane. The film was prepared by vapour-deposition (sublimation) [49]. Tg is the glass point (for details see Sect. 8.6). After [49]. Fig. 8.2 The temperature dependence of the hole mobility jLt in an 8.7 /xm thick disordered film of MPMP molecules at different field strengths F. MPMP = bis(4-N,N-diethylamino-2-methylphenyl)-4-methylphenylmethane. The film was prepared by vapour-deposition (sublimation) [49]. Tg is the glass point (for details see Sect. 8.6). After [49].
Fig. 8.47 The temperature dependence of the hole mobility fji = djF tx) in DEH (see Fig. 8.44). o and are the experimental values for two different sample thicknesses, d = 2.3 iim and 5.6 iirr. The lines give the simulation results with or = 0.101 eV. From [46]. Fig. 8.47 The temperature dependence of the hole mobility fji = djF tx) in DEH (see Fig. 8.44). o and are the experimental values for two different sample thicknesses, d = 2.3 iim and 5.6 iirr. The lines give the simulation results with or = 0.101 eV. From [46].
Fig. 2.12 Doping of an inert polymer, bisphenol A polycarbonate, with triphenyl-amine (TPA). Temperature dependence of the hole mobility. Plot of log // vs. 1/T for various TPA contents denoted as weight... Fig. 2.12 Doping of an inert polymer, bisphenol A polycarbonate, with triphenyl-amine (TPA). Temperature dependence of the hole mobility. Plot of log // vs. 1/T for various TPA contents denoted as weight...
Figure 18 Temperature dependence of the hole mobility in liquid xenon included are some values for solid Xe. (Redrawn from the data of Hilt, O. and Schmidt, W.F., Chem. Phys., 183, 147, 1994a.)... Figure 18 Temperature dependence of the hole mobility in liquid xenon included are some values for solid Xe. (Redrawn from the data of Hilt, O. and Schmidt, W.F., Chem. Phys., 183, 147, 1994a.)...
Figure 9.20 Temperature dependence of the hole mobility in TAPC (glass), TAPC/PS and TAPC/PC plotted on a In p vs. T- scale. (From Borsenberger, P. M. and Weiss, D. S., Organic Photo-Receptors for Imaging Systems, Marcel Dekker, New York, 1993. With permission.)... Figure 9.20 Temperature dependence of the hole mobility in TAPC (glass), TAPC/PS and TAPC/PC plotted on a In p vs. T- scale. (From Borsenberger, P. M. and Weiss, D. S., Organic Photo-Receptors for Imaging Systems, Marcel Dekker, New York, 1993. With permission.)...

See other pages where Temperature dependence of the hole mobility is mentioned: [Pg.11]    [Pg.28]    [Pg.33]    [Pg.393]    [Pg.403]    [Pg.418]    [Pg.460]    [Pg.578]    [Pg.55]    [Pg.285]    [Pg.301]    [Pg.1801]    [Pg.481]    [Pg.159]   
See also in sourсe #XX -- [ Pg.285 ]




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Temperature dependence of the mobility

Temperature mobilities

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