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Volumn 82, Issue 2, 2010, Pages

Suspensions of repulsive colloidal particles near the glass transition: Time and frequency domain descriptions

Author keywords

[No Author keywords available]

Indexed keywords

BREAK-UP; COLLOIDAL PARTICLE; DYNAMIC PARAMETERS; ERGODICITY; ERGODICS; HARD-SPHERE; MODE COUPLING; RELAXATION DYNAMICS; TIME AND FREQUENCY DOMAINS;

EID: 77956095651     PISSN: 15393755     EISSN: 15502376     Source Type: Journal    
DOI: 10.1103/PhysRevE.82.021406     Document Type: Article
Times cited : (1)

References (32)
  • 3
    • 30344481716 scopus 로고    scopus 로고
    • 10.1080/00018730500414570
    • F. Sciortino and P. Tartaglia, Adv. Phys. 54, 471 (2005). 10.1080/00018730500414570
    • (2005) Adv. Phys. , vol.54 , pp. 471
    • Sciortino, F.1    Tartaglia, P.2
  • 8
    • 4243591791 scopus 로고
    • 10.1103/PhysRevLett.75.2770
    • T. G. Mason and D. A. Weitz, Phys. Rev. Lett. 75, 2770 (1995). 10.1103/PhysRevLett.75.2770
    • (1995) Phys. Rev. Lett. , vol.75 , pp. 2770
    • Mason, T.G.1    Weitz, D.A.2
  • 13
    • 18144429899 scopus 로고    scopus 로고
    • 10.1103/PhysRevLett.94.158301
    • L. Ramos and L. Cipelletti, Phys. Rev. Lett. 94, 158301 (2005). 10.1103/PhysRevLett.94.158301
    • (2005) Phys. Rev. Lett. , vol.94 , pp. 158301
    • Ramos, L.1    Cipelletti, L.2
  • 14
    • 70350482357 scopus 로고    scopus 로고
    • 10.1063/1.3240345
    • E. Di Cola, J. Chem. Phys. 131, 144903 (2009). 10.1063/1.3240345
    • (2009) J. Chem. Phys. , vol.131 , pp. 144903
    • Di Cola, E.1
  • 16
    • 0030188212 scopus 로고    scopus 로고
    • 10.1016/0370-1573(95)00078-X
    • G. Nägele, Phys. Rep. 272, 215 (1996). 10.1016/0370-1573(95)00078-X
    • (1996) Phys. Rep. , vol.272 , pp. 215
    • Nägele, G.1
  • 17
    • 84947641899 scopus 로고
    • 10.1080/09500349114551951
    • K. Schätzel, J. Mod. Opt. 38, 1849 (1991). 10.1080/09500349114551951
    • (1991) J. Mod. Opt. , vol.38 , pp. 1849
    • Schätzel, K.1
  • 18
    • 0000193629 scopus 로고    scopus 로고
    • 10.1103/PhysRevE.60.5670
    • A. Moussaïd and P. N. Pusey, Phys. Rev. E 60, 5670 (1999). 10.1103/PhysRevE.60.5670
    • (1999) Phys. Rev. e , vol.60 , pp. 5670
    • Moussaïd, A.1    Pusey, P.N.2
  • 19
    • 0004706699 scopus 로고
    • 10.1016/0378-4371(89)90063-0
    • P. Pusey and W. van Megen, Physica A 157, 705 (1989). 10.1016/0378-4371(89)90063-0
    • (1989) Physica A , vol.157 , pp. 705
    • Pusey, P.1    Van Megen, W.2
  • 20
    • 77956128841 scopus 로고    scopus 로고
    • For our ergodic systems, statistics at long times (final α -decay) is not reliable since we adapted the duration of our measurements to reach only a consistent description of the first and second beta decays. However, the MCT solutions show the predicted stretched exponential decay f ( qp,τ) exp (-(τ) β ), where β=0.82±0.02.
    • For our ergodic systems, statistics at long times (final α -decay) is not reliable since we adapted the duration of our measurements to reach only a consistent description of the first and second beta decays. However, the MCT solutions show the predicted stretched exponential decay f ( qp,τ) exp (-(τ) β ), where β=0.82±0.02.
  • 21
    • 77956112986 scopus 로고    scopus 로고
    • We found that our nonergodic systems aged only in the first few hours after tumbling. Then, after a waiting time of one day, we performed independent measurements separated by one day finding no evolution due to aging effects within the time window of the measurements.
    • We found that our nonergodic systems aged only in the first few hours after tumbling. Then, after a waiting time of one day, we performed independent measurements separated by one day finding no evolution due to aging effects within the time window of the measurements.
  • 23
    • 0038400103 scopus 로고    scopus 로고
    • 10.1103/PhysRevE.67.021502
    • W. Götze and Th. Voigtmann, Phys. Rev. E 67, 021502 (2003). 10.1103/PhysRevE.67.021502
    • (2003) Phys. Rev. e , vol.67 , pp. 021502
    • Götze, W.1    Voigtmann, Th.2
  • 27
    • 33748324534 scopus 로고    scopus 로고
    • 10.1209/epl/i2006-10156-y
    • K. N. Pham, EPL 75, 624 (2006). 10.1209/epl/i2006-10156-y
    • (2006) EPL , vol.75 , pp. 624
    • Pham, K.N.1
  • 28
    • 33749254111 scopus 로고    scopus 로고
    • 10.1209/epl/i2006-10203-9
    • K. Miyazaki, EPL 75, 915 (2006). 10.1209/epl/i2006-10203-9
    • (2006) EPL , vol.75 , pp. 915
    • Miyazaki, K.1
  • 29
    • 0037049529 scopus 로고    scopus 로고
    • 10.1103/PhysRevLett.89.248304
    • M. Fuchs and M. E. Cates, Phys. Rev. Lett. 89, 248304 (2002). 10.1103/PhysRevLett.89.248304
    • (2002) Phys. Rev. Lett. , vol.89 , pp. 248304
    • Fuchs, M.1    Cates, M.E.2
  • 31
    • 67149107332 scopus 로고    scopus 로고
    • 10.1126/science.1174217
    • D. Bonn and M. M. Denn, Science 324, 1401 (2009). 10.1126/science.1174217
    • (2009) Science , vol.324 , pp. 1401
    • Bonn, D.1    Denn, M.M.2
  • 32
    • 77956130825 scopus 로고    scopus 로고
    • The emergence of tσ in both the time and frequency domain descriptions is accounted for by the very nature of the Fourier transformation. On one hand, tσ is the characteristic time associated to the beta decays: f (qp, τ)-f (qp,∞) (τ/tσ)-a and f (qp, τ)-f (qp ,∞) (τ/tσ)b. On the other hand, via Fourier transformation, the frequency tσ -1 appears as the characteristic counterpart in the frequency domain description given by Eqs.
    • The emergence of tσ in both the time and frequency domain descriptions is accounted for by the very nature of the Fourier transformation. On one hand, tσ is the characteristic time associated to the beta decays: f (qp, τ)-f (qp,∞) (τ/tσ)-a and f (qp, τ)-f (qp,∞) (τ/tσ)b. On the other hand, via Fourier transformation, the frequency tσ -1 appears as the characteristic counterpart in the frequency domain description given by Eqs.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.