-
4
-
-
41149114007
-
-
The reader will note that here the word ''relaxation'' is given a specific meaning, which contrasts with the term ''retardation'' defined before. On the other hand, the word ''relaxation'' is also used in its general sense for both cases in combinations like relaxation function, relaxation time, and relaxation process.
-
The reader will note that here the word ''relaxation'' is given a specific meaning, which contrasts with the term ''retardation'' defined before. On the other hand, the word ''relaxation'' is also used in its general sense for both cases in combinations like relaxation function, relaxation time, and relaxation process.
-
-
-
-
5
-
-
0030844190
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POLMAG 0032-3861 10.1016/S0032-3861(96)00524-1
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H. Wagner and R. Richert, Polymer POLMAG 0032-3861 10.1016/S0032-3861(96) 00524-1 38, 255 (1997).
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6
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0036642891
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JNCSBJ 0022-3093 10.1016/S0022-3093(02)00960-2
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R. Richert, J. Non-Cryst. Solids JNCSBJ 0022-3093 10.1016/S0022-3093(02) 00960-2 305, 29 (2002).
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Richert, R.1
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7
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0037439727
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JCPSA6 0021-9606 10.1063/1.1529193
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Duvvuri, K.1
Richert, R.2
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8
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0042956534
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-
JCPSA6 0021-9606 10.1063/1.452460
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M. Maroncelli and G. R. Fleming, J. Chem. Phys. JCPSA6 0021-9606 10.1063/1.452460 86, 6221 (1987).
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Maroncelli, M.1
Fleming, G.R.2
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10
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12344271673
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JUPSAU 0031-9015 10.1143/JPSJ.12.570
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R. Kubo, J. Phys. Soc. Jpn. JUPSAU 0031-9015 10.1143/JPSJ.12.570 12, 570 (1957).
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Kubo, R.1
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11
-
-
41149109182
-
-
f (±0) stands for limδ→0;δ>0 f (±δ) for any function f (t).
-
f (±0) stands for limδ→0;δ>0 f (±δ) for any function f (t).
-
-
-
-
12
-
-
41149085143
-
-
The relation may also be found by Fourier transforming equation 6 for V (t) to obtain M (ω), and the corresponding equation for Q (t) to obtain ε (ω), using the reciprocity relation M (ω) =1/ ε (ω).
-
The relation may also be found by Fourier transforming equation 6 for V (t) to obtain M(ω), and the corresponding equation for Q (t) to obtain ε (ω), using the reciprocity relation M(ω) =1/ ε (ω).
-
-
-
-
13
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0031647841
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SSIOD3 0167-2738 10.1016/S0167-2738(97)00461-X
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R. Richert and H. Wagner, Solid State Ionics SSIOD3 0167-2738 10.1016/S0167-2738(97)00461-X 105, 167 (1998).
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Richert, R.1
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14
-
-
41149087355
-
-
Taking the limit Δt→0 of Eq. 24 an integral equation for the current dQ (t) /dt is obtained, which, however, is not useful in the present context.
-
Taking the limit Δt→0 of Eq. 24 an integral equation for the current dQ (t) /dt is obtained, which, however, is not useful in the present context.
-
-
-
-
15
-
-
0034319356
-
-
PHYADX 0378-4371 10.1016/S0378-4371(00)00451-9
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Richert, R.1
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0000711870
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17
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25144446248
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JCPSA6 0021-9606 10.1063/1.2036972
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18
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0024736142
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D. Kivelson and H. Friedman, J. Phys. Chem. JPCHAX 0022-3654 10.1021/j100356a029 93, 7026 (1989).
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Kivelson, D.1
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19
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0000473886
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-
ARPLAP 0066-426X 10.1146/annurev.physchem.47.1.109
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G. R. Fleming and M. Cho, Annu. Rev. Phys. Chem. ARPLAP 0066-426X 10.1146/annurev.physchem.47.1.109 47, 109 (1996).
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Fleming, G.R.1
Cho, M.2
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22
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4243104032
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Jäckle, J.1
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23
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0034323173
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JCPSA6 0021-9606 10.1063/1.1319174
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R. Richert, J. Chem. Phys. JCPSA6 0021-9606 10.1063/1.1319174 113, 8404 (2000).
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Richert, R.1
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24
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0033074343
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JAPIAU 0021-8979 10.1063/1.369318
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