2017
DOI: 10.1088/1674-1056/26/1/014503
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Granular packing as model glass formers

Abstract: Static granular packings are model hard-sphere glass formers. The nature of glass transition has remained a hotly debated issue. We review recent experimental progresses in using granular materials to study glass transitions. We focus on the growth of glass order with five-fold symmetry in granular packings and relate the findings to both geometric frustration and random first-order phase transition theories.

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Cited by 9 publications
(7 citation statements)
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References 116 publications
(216 reference statements)
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“…From a homogeneous excited-state, the system enters into an initial period of homogeneous energy loss, and later grains can spontaneously cluster. [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17] Theoretical modeling, [18][19][20][21][22][23][24][25][26][27][28][29] and simulation investigations [20][21][22]24,28,[30][31][32][33][34][35][36][37][38][39] are based on simplifications and assumptions of grain properties. Quantitative experiments are very much needed for better understanding of fundamental features of such ensembles.…”
Section: Introductionmentioning
confidence: 99%
“…From a homogeneous excited-state, the system enters into an initial period of homogeneous energy loss, and later grains can spontaneously cluster. [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17] Theoretical modeling, [18][19][20][21][22][23][24][25][26][27][28][29] and simulation investigations [20][21][22]24,28,[30][31][32][33][34][35][36][37][38][39] are based on simplifications and assumptions of grain properties. Quantitative experiments are very much needed for better understanding of fundamental features of such ensembles.…”
Section: Introductionmentioning
confidence: 99%
“…For further estimations, [14][15][16][17] we can take the coordinate number Z = 2 √ 3φ / (1−φ ) and its value at the random loose pack Z lp = 4 = 2 √ 3φ lp / 1−φ lp . Parameters for glass are as follows: ρ glass = 2600 kg/m 3 , ν g = 0.2, and µ g = 10 GPa.…”
Section: Theorymentioning
confidence: 99%
“…Dynamical heterogeneity is considered to be one of the key features of structural relaxation in supercooled liquids and glasses. [1][2][3] As the temperature of a glass-forming liquid is rapidly lowered, the motion of particles within the liquid becomes spatially and temporally heterogeneous. [2,[4][5][6] While the overall motions within the liquid slow down, particles in some regions exhibit faster dynamics than the rest, and over time these mobile regions can appear and disappear throughout the system.…”
Section: Introductionmentioning
confidence: 99%