-
1
-
-
0035826241
-
Supercooled liquids and the glass transition
-
DOI 10.1038/35065704
-
P. G. Debenedetti and F. H. Stilinger, Nature (London) 410, 259 (2001). 10.1038/35065704 (Pubitemid 32218700)
-
(2001)
Nature
, vol.410
, Issue.6825
, pp. 259-267
-
-
Debenedetti, P.G.1
Stillinger, F.H.2
-
2
-
-
0004220260
-
-
Springer Series in Materials Science, Vol. 48 (Springer-Verlag, Berlin).
-
E. Donth, The Glass Transition, Springer Series in Materials Science, Vol. 48 (Springer-Verlag, Berlin, 2001).
-
(2001)
The Glass Transition
-
-
Donth, E.1
-
3
-
-
0024017655
-
-
10.1016/0022-3093(88)90133-0
-
C. A. Angell, J. Non-Cryst. Solids 102, 205 (1988). 10.1016/0022-3093(88) 90133-0
-
(1988)
J. Non-Cryst. Solids
, vol.102
, pp. 205
-
-
Angell, C.A.1
-
7
-
-
33751124528
-
-
10.1063/1.466117
-
R. Bhmer, K. L. Ngai, C. A. Angell, and D. J. Plazek, J. Chem. Phys. 99, 4201 (1993). 10.1063/1.466117
-
(1993)
J. Chem. Phys.
, vol.99
, pp. 4201
-
-
Bhmer, R.1
Ngai, K.L.2
Angell, C.A.3
Plazek, D.J.4
-
9
-
-
79957608664
-
-
for a review see, e.g., W. Kob, e-print arXiv:cond-mat/0212344v1
-
for a review see, e.g., W. Kob, e-print arXiv:cond-mat/0212344v1.
-
-
-
-
10
-
-
0029992608
-
Nonresonant spectral hole burning in the slow dielectric response of supercooled liquids
-
DOI 10.1126/science.274.5288.752
-
B. Schiener, R. Bhmer, A. Loidl, and R. V. Chamberlin, Science 274, 752 (1996). 10.1126/science.274.5288.752 (Pubitemid 26398248)
-
(1996)
Science
, vol.274
, Issue.5288
, pp. 752-754
-
-
Schiener, B.1
Bohmer, R.2
Loidl, A.3
Chamberlin, R.V.4
-
11
-
-
0032575818
-
-
10.1103/PhysRevLett.81.2727
-
U. Tracht, M. Wihelm, A. Heuer, H. Feng, K. Schmidt-Rohr, and H. W. Speiss, Phys. Rev. Lett. 81, 2727 (1998). 10.1103/PhysRevLett.81.2727
-
(1998)
Phys. Rev. Lett.
, vol.81
, pp. 2727
-
-
Tracht, U.1
Wihelm, M.2
Heuer, A.3
Feng, H.4
Schmidt-Rohr, K.5
Speiss, H.W.6
-
12
-
-
0002055106
-
-
10.1146/annurev.physchem.51.1.99
-
M. D. Ediger, Annu. Rev. Phys. Chem. 51, 99 (2000). 10.1146/annurev. physchem.51.1.99
-
(2000)
Annu. Rev. Phys. Chem.
, vol.51
, pp. 99
-
-
Ediger, M.D.1
-
13
-
-
0037124631
-
Heterogeneous dynamics in liquids: Fluctuations in space and time
-
DOI 10.1088/0953-8984/14/23/201, PII S0953898402267211
-
R. Richert, J. Phys.: Condens. Matter 14 R703 (2002). 10.1088/0953-8984/14/23/201 (Pubitemid 34715147)
-
(2002)
Journal of Physics Condensed Matter
, vol.14
, Issue.23
-
-
Richert, R.1
-
14
-
-
0002805179
-
-
10.1016/S0022-3093(98)00831-X
-
H. Sillescu, J. Non-Cryst. Solids 243, 81 (1999). 10.1016/S0022-3093(98) 00831-X
-
(1999)
J. Non-Cryst. Solids
, vol.243
, pp. 81
-
-
Sillescu, H.1
-
15
-
-
0035795873
-
-
10.1209/epl/i2001-00320-5
-
R. Richert, EuroPhys. Lett. 54, 767 (2001). 10.1209/epl/i2001-00320-5
-
(2001)
EuroPhys. Lett.
, vol.54
, pp. 767
-
-
Richert, R.1
-
17
-
-
20544478364
-
Nonresonant dielectric hole burning in neat and binary organic glass formers
-
DOI 10.1063/1.1931647, 224511
-
T. Blochowicz and E. A. Rssler, J. Chem. Phys. 122, 224511 (2005). 10.1063/1.1931647 (Pubitemid 40844901)
-
(2005)
Journal of Chemical Physics
, vol.122
, Issue.22
, pp. 1-13
-
-
Blochowicz, T.1
Rossler, E.A.2
-
19
-
-
0031269003
-
-
10.1063/1.475089
-
B. Schiener, R. V. Chamberlin, G. Diezemann, and R. Bhmer, J. Chem. Phys. 107, 7746 (1997). 10.1063/1.475089
-
(1997)
J. Chem. Phys.
, vol.107
, pp. 7746
-
-
Schiener, B.1
Chamberlin, R.V.2
Diezemann, G.3
Bhmer, R.4
-
21
-
-
33748356294
-
Nonlinear dielectric response and thermodynamic heterogeneity in liquids
-
DOI 10.1103/PhysRevLett.97.095703
-
R. Richert and S. Weinstein, Phys. Rev. Lett. 97, 095703 (2006). 10.1103/PhysRevLett.97.095703 (Pubitemid 44335282)
-
(2006)
Physical Review Letters
, vol.97
, Issue.9
, pp. 095703
-
-
Richert, R.1
Weinstein, S.2
-
22
-
-
33846781157
-
-
10.1103/PhysRevB.75.064302
-
S. Weinstein and R. Richert, Phys. Rev. B 75, 064302 (2007). 10.1103/PhysRevB.75.064302
-
(2007)
Phys. Rev. B
, vol.75
, pp. 064302
-
-
Weinstein, S.1
Richert, R.2
-
23
-
-
57849153403
-
-
10.1140/epjb/e2008-00416-2
-
W. Huang and R. Richert, Eur. Phys. J. B 66, 217 (2008). 10.1140/epjb/e2008-00416-2
-
(2008)
Eur. Phys. J. B
, vol.66
, pp. 217
-
-
Huang, W.1
Richert, R.2
-
24
-
-
77349110242
-
-
10.1016/j.jnoncrysol.2009.08.047
-
R. Richert and W. Huang, J. Non-Cryst. Solids 356, 787 (2010). 10.1016/j.jnoncrysol.2009.08.047
-
(2010)
J. Non-Cryst. Solids
, vol.356
, pp. 787
-
-
Richert, R.1
Huang, W.2
-
25
-
-
0037405746
-
-
10.1016/S0378-4371(02)01912-X
-
R. Richert, Physica A 322, 143 (2003). 10.1016/S0378-4371(02)01912-X
-
(2003)
Physica A
, vol.322
, pp. 143
-
-
Richert, R.1
-
26
-
-
35948935280
-
Measuring the configurational heat capacity of liquids
-
DOI 10.1103/PhysRevLett.99.185701
-
L.-M. Wang and R. Richert, Phys. Rev. Lett. 99, 185701 (2007). 10.1103/PhysRevLett.99.185701 (Pubitemid 350074465)
-
(2007)
Physical Review Letters
, vol.99
, Issue.18
, pp. 185701
-
-
Wang, L.-M.1
Richert, R.2
-
29
-
-
0035263681
-
-
10.1209/epl/i2001-00195-4
-
G. Diezemann, EuroPhys. Lett. 53, 604 (2001). 10.1209/epl/i2001-00195-4
-
(2001)
EuroPhys. Lett.
, vol.53
, pp. 604
-
-
Diezemann, G.1
-
31
-
-
76349097608
-
-
10.1063/1.3290986
-
M. Tarzia, G. Biroli, A. Lefvre, and J.-P. Bouchaud, J. Chem. Phys. 132, 054501 (2010). 10.1063/1.3290986
-
(2010)
J. Chem. Phys.
, vol.132
, pp. 054501
-
-
Tarzia, M.1
Biroli, G.2
Lefvre, A.3
Bouchaud, J.-P.4
-
32
-
-
55349113232
-
-
10.1063/1.2960564
-
C. Thibierge, D. LHte, F. Ladieu, and R. Tourbot, Rev. Sci. Instrum. 79, 103905 (2008). 10.1063/1.2960564
-
(2008)
Rev. Sci. Instrum.
, vol.79
, pp. 103905
-
-
Thibierge, C.1
Lhte, D.2
Ladieu, F.3
Tourbot, R.4
-
33
-
-
77951280740
-
-
10.1103/PhysRevLett.104.165703
-
C. Crauste-Thibierge, C. Brun, F. Ladieu, D. LHte, G. Biroli, and J.-P. Bouchaud, Phys. Rev. Lett. 104, 165703 (2010). 10.1103/PhysRevLett.104.165703
-
(2010)
Phys. Rev. Lett.
, vol.104
, pp. 165703
-
-
Crauste-Thibierge, C.1
Brun, C.2
Ladieu, F.3
Lhte, D.4
Biroli, G.5
Bouchaud, J.-P.6
-
34
-
-
79957589261
-
-
See supplementary material in Ref. E-JCPSA6-134-012120.
-
See supplementary material in Ref. http://dx.doi.org/10.1063/1.3591375 E-JCPSA6-134-012120.
-
-
-
-
35
-
-
79957581372
-
-
The Debye character of each box holds for neat liquids, see, e.g., Refs., and. In the very specific case of mixtures studied in Ref., it was shown that agreement with NHB experiment demands that the dynamics of each box is a stretched exponential and not a simple exponential.
-
The Debye character of each box holds for neat liquids, see, e.g., Refs., and. In the very specific case of mixtures studied in Ref., it was shown that agreement with NHB experiment demands that the dynamics of each box is a stretched exponential and not a simple exponential.
-
-
-
-
36
-
-
0037724980
-
-
10.1063/1.1563247
-
T. Blochowicz, C. Tschirwitz, S. Benkhof, and E. A. Rssler, J. Chem. Phys. 118, 7544 (2003). 10.1063/1.1563247
-
(2003)
J. Chem. Phys.
, vol.118
, pp. 7544
-
-
Blochowicz, T.1
Tschirwitz, C.2
Benkhof, S.3
Rssler, E.A.4
-
37
-
-
35949018243
-
-
10.1103/PhysRevB.34.1631
-
N. O. Birge, Phys. Rev. B 34, 2674 (1986); 10.1103/PhysRevB.34.1631
-
(1986)
Phys. Rev. B
, vol.34
, pp. 2674
-
-
Birge, N.O.1
-
39
-
-
0037663911
-
-
Standard (but tedious) thermal calculations taking into account the thermal circuit connecting the electrodes to the metallic experimental cell do show that the approximation made by considering electrodes as a perfect thermostat produce an error smaller, in any case, than 1 for the nonlinear susceptibility. Besides, we also neglect the possible thermal resistance associated with the interface glycerol/electrode: this is supported by the thorough study of Minakov who has showed, for the Glycerol/Macor interface, that such an effect was responsible of only 5 of the temperature increase [A. A. Minakov, S. A. Adamovsky, and C. Schick, Thermochim. Acta 403, 89 (2003)].
-
(2003)
Thermochim. Acta
, vol.403
, pp. 89
-
-
Minakov, A.A.1
Adamovsky, S.A.2
Schick, C.3
-
40
-
-
79957618728
-
-
note
-
2 of the heating, defined just before Eq., but it is in general not valid for computing the dc temperature increase. The difference lies in the fact that, because of the skin effect, the temperature oscillations are efficiently damped in the thick electrodes, while the dc component is not damped at all. The dc heat flux is thus fully transmitted by the electrodes, and the unavoidable insulating piece between the electrode and the experimental cell is responsible for the major part of the dc temperature increase. The only way to get rid of the dc heating is to perform extremely fast experiments, in the spirit of what is made in Ref., so as to measure the sample properties in a time scale much lower than the thermal diffusion time between the sample and the experimental cell.
-
-
-
-
41
-
-
77953533227
-
-
See the comment:, 10.1103/PhysRevLett.104.239602
-
See the comment: R. Pick, Phys. Rev. Lett. 104, 239602 (2010) 10.1103/PhysRevLett.104.239602
-
(2010)
Phys. Rev. Lett.
, vol.104
, pp. 239602
-
-
Pick, R.1
-
42
-
-
77953525391
-
-
the reply:, 10.1103/PhysRevLett.104.239603
-
and the reply: L.-M. Wang and R. Richert, Phys. Rev. Lett. 104, 239603 (2010). 10.1103/PhysRevLett.104.239603
-
(2010)
Phys. Rev. Lett.
, vol.104
, pp. 239603
-
-
Wang, L.-M.1
Richert, R.2
-
43
-
-
78650687518
-
-
10.1063/1.3507252
-
C. Brun, C. Crauste-Thibierge, F. Ladieu, and D. LHte, J. Chem. Phys. 133, 234901 (2010). 10.1063/1.3507252
-
(2010)
J. Chem. Phys.
, vol.133
, pp. 234901
-
-
Brun, C.1
Crauste-Thibierge, C.2
Ladieu, F.3
Lhte, D.4
-
44
-
-
79957604282
-
-
0, dh because of the interferences effects depicted in Sec..
-
0, dh because of the interferences effects depicted in Sec..
-
-
-
-
45
-
-
79957615845
-
-
note
-
0, ph.
-
-
-
-
46
-
-
79957593533
-
-
1, the latter quantity is taken as a constant when solving Eq.. The same approximation was made independently in, e.g., the Appendix of Ref..
-
1, the latter quantity is taken as a constant when solving Eq.. The same approximation was made independently in, e.g., the Appendix of Ref..
-
-
-
-
47
-
-
79957605341
-
-
note
-
2, klin, k, see Eq., we are led to the conclusion that our estimate should, again, be slightly overestimated.
-
-
-
-
48
-
-
79957615635
-
-
note
-
0, tot, k, is exactly the same, in modulus and phase, as the one found by using Eqs..
-
-
-
-
50
-
-
79957608858
-
-
note
-
3(, T) better than 1.
-
-
-
-
51
-
-
79957594794
-
-
note
-
The values of the temperatures in the calculations were tuned to yield the same values of the relaxation frequencies f as those found in the experiments of Ref.. Hence, the small differences (less than 1K) between the two sets of temperatures for Figs..
-
-
-
-
52
-
-
29244447380
-
Physics: Direct experimental evidence of a growing length scale accompanying the glass transition
-
DOI 10.1126/science.1120714
-
L. Berthier, G. Biroli, J.-P. Bouchaud, L. Cipelletti, D. El Masri, D. LHte, F. Ladieu, and M. Pierno, Science 310, 1797 (2005). 10.1126/science. 1120714 (Pubitemid 41818947)
-
(2005)
Science
, vol.310
, Issue.5755
, pp. 1797-1800
-
-
Berthier, L.1
Biroli, G.2
Bouchaud, J.-P.3
Cipelletti, L.4
El Masri, D.5
L'Hote, D.6
Ladieu, F.7
Pierno, M.8
-
53
-
-
34248575106
-
Spontaneous and induced dynamic fluctuations in glass formers. I. General results and dependence on ensemble and dynamics
-
DOI 10.1063/1.2721554
-
L. Berthier, G. Biroli, J.-P. Bouchaud, W. Kob, K. Miyazaki, and D. R. Reichman, J. Chem. Phys. 126, 184503 (2007). 10.1063/1.2721554 (Pubitemid 46745219)
-
(2007)
Journal of Chemical Physics
, vol.126
, Issue.18
, pp. 184503
-
-
Berthier, L.1
Biroli, G.2
Bouchaud, J.-P.3
Kob, W.4
Miyazaki, K.5
Reichman, D.R.6
-
54
-
-
35648950044
-
Spatial correlations in the dynamics of glassforming liquids: Experimental determination of their temperature dependence
-
DOI 10.1103/PhysRevE.76.041510
-
C. Dalle-Ferrier, C. Thibierge, C. Alba-Simionesco, L. Berthier, G. Biroli, J.-P. Bouchaud, F. Ladieu, D. LHte, and G. Tarjus, Phys. Rev. E 76, 041510 (2007). 10.1103/PhysRevE.76.041510 (Pubitemid 350023311)
-
(2007)
Physical Review E - Statistical, Nonlinear, and Soft Matter Physics
, vol.76
, Issue.4
, pp. 041510
-
-
Dalle-Ferrier, C.1
Thibierge, C.2
Alba-Simionesco, C.3
Berthier, L.4
Biroli, G.5
Bouchaud, J.-P.6
Ladieu, F.7
L'Hote, D.8
Tarjus, G.9
-
55
-
-
79957623188
-
-
0 following Eq. (18) of Ref..
-
0 following Eq. (18) of Ref..
-
-
-
-
56
-
-
34547869819
-
g probed by rotational diffusion of ensembles and single dye molecules
-
DOI 10.1073/pnas.0610521104
-
R. Zondervan, F. Kulzer, G. C. G. Berkhout, and M. Orrit, Proc. Natl. Acad. Sci. U.S.A. 104, 12628 (2007). 10.1073/pnas.0610521104 (Pubitemid 47255205)
-
(2007)
Proceedings of the National Academy of Sciences of the United States of America
, vol.104
, Issue.31
, pp. 12628-12633
-
-
Zondervan, R.1
Kulzer, F.2
Berkhout, G.C.G.3
Orrit, M.4
-
57
-
-
79957587726
-
Experimental approaches to heterogeneous dynamics
-
in, edited by L. Berthier, L. Cipeletti, G. Biroli, and W. van Saarloos (Oxford University Press, New York) (Sec. 6.1).
-
R. Richert, N. Israeloff, C. Alba-Simionesco, F. Ladieu, and D. LHte, Experimental approaches to heterogeneous dynamics. in Dynamical Heterogeneities in Glasses, Colloids and Granular Media, edited by, L. Berthier, L. Cipeletti, G. Biroli, J.-P. Bouchaud, and, W. van, Saarloos (Oxford University Press, New York, 2011) (Sec. 6.1).
-
(2011)
Dynamical Heterogeneities in Glasses, Colloids and Granular Media
-
-
Richert, R.1
Israeloff, N.2
Alba-Simionesco, C.3
Ladieu, F.4
Lhte, D.5
Bouchaud, J.-P.6
-
58
-
-
79957585681
-
-
3 and the measured one is even larger than in Fig., since the calculated phase never coincides with the experimental one, whatever the frequency.
-
3 and the measured one is even larger than in Fig., since the calculated phase never coincides with the experimental one, whatever the frequency.
-
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