-
5
-
-
80054890798
-
-
NMAACR
-
G.N. Greaves, A.L. Greer, R.S. Lakes, and T. Rouxel, Nat. Mater. 10, 823 (2011). NMAACR 1476-1122 10.1038/nmat3134
-
(2011)
Nat. Mater.
, vol.10
, pp. 823
-
-
Greaves G, N.1
Greer A, L.2
Lakes R, S.3
Rouxel, T.4
-
6
-
-
84935914239
-
-
arXiv:1501.04227v1
-
M.M. Driscoll, B.G.-G. Chen, T.H. Beuman, S. Ulrich, S.R. Nagel, and V. Vitelli, arXiv:1501.04227v1.
-
-
-
Driscoll M, M.1
Chen B, G.-G.2
Beuman T, H.3
Ulrich, S.4
Nagel S, R.5
Vitelli, V.6
-
7
-
-
34247580877
-
-
RMPHAT
-
T. Witten, Rev. Mod. Phys. 79, 643 (2007). RMPHAT 0034-6861 10.1103/RevModPhys.79.643
-
(2007)
Rev. Mod. Phys.
, vol.79
, pp. 643
-
-
Witten, T.1
-
8
-
-
20144385588
-
-
SCIEAS
-
L. Mahadevan and S. Rica, Science 307, 1740 (2005). SCIEAS 0036-8075 10.1126/science.1105169
-
(2005)
Science
, vol.307
, pp. 1740
-
-
Mahadevan, L.1
Rica, S.2
-
9
-
-
84918567807
-
-
PRLTAO
-
T. Castle, Y. Cho, X. Gong, E. Jung, D.M. Sussman, S. Yang, and R.D. Kamien, Phys. Rev. Lett. 113, 245502 (2014). PRLTAO 0031-9007 10.1103/PhysRevLett.113.245502
-
(2014)
Phys. Rev. Lett.
, vol.113
, pp. 245502
-
-
Castle, T.1
Cho, Y.2
Gong, X.3
Jung, E.4
Sussman D, M.5
Yang, S.6
Kamien R, D.7
-
10
-
-
2442518273
-
-
PRESCM
-
C.S. O'Hern, L.E. Silbert, A.J. Liu, and S.R. Nagel, Phys. Rev. E 68, 011306 (2003). PRESCM 1063-651X 10.1103/PhysRevE.68.011306
-
(2003)
Phys. Rev. e
, vol.68
, pp. 011306
-
-
O'Hern C, S.1
Silbert L, E.2
Liu A, J.3
Nagel S, R.4
-
12
-
-
28844441964
-
-
PRESCM
-
M. Wyart, L.E. Silbert, S.R. Nagel, and T.A. Witten, Phys. Rev. E 72, 051306 (2005). PRESCM 1539-3755 10.1103/PhysRevE.72.051306
-
(2005)
Phys. Rev. e
, vol.72
, pp. 051306
-
-
Wyart, M.1
Silbert L, E.2
Nagel S, R.3
Witten T, A.4
-
14
-
-
24444464013
-
-
PRBMDO
-
E.J. Garboczi, Phys. Rev. B 39, 2472 (1989). PRBMDO 0163-1829 10.1103/PhysRevB.39.2472
-
(1989)
Phys. Rev. B
, vol.39
, pp. 2472
-
-
Garboczi, E.J.1
-
16
-
-
84935906054
-
-
See the Supplemental Material at for additional figures and discussion, including numerical details
-
See the Supplemental Material at http://link.aps.org/supplemental/10.1103/PhysRevLett.114.225501 for additional figures and discussion, including numerical details.
-
-
-
-
17
-
-
84865583985
-
-
PRLTAO
-
S. Dagois-Bohy, B.P. Tighe, J. Simon, S. Henkes, and M. van Hecke, Phys. Rev. Lett. 109, 095703 (2012). PRLTAO 0031-9007 10.1103/PhysRevLett.109.095703
-
(2012)
Phys. Rev. Lett.
, vol.109
, pp. 095703
-
-
Dagois-Bohy, S.1
Tighe B, P.2
Simon, J.3
Henkes, S.4
Van Hecke, M.5
-
18
-
-
84907847243
-
-
PRESCM
-
C.P. Goodrich, S. Dagois-Bohy, B.P. Tighe, M. van Hecke, A.J. Liu, and S.R. Nagel, Phys. Rev. E 90, 022138 (2014). PRESCM 1539-3755 10.1103/PhysRevE.90.022138
-
(2014)
Phys. Rev. e
, vol.90
, pp. 022138
-
-
Goodrich C, P.1
Dagois-Bohy, S.2
Tighe B, P.3
Van Hecke, M.4
Liu A, J.5
Nagel S, R.6
-
19
-
-
33845722693
-
-
PRLTAO
-
W.G. Ellenbroek, E. Somfai, M. van Hecke, and W. van Saarloos, Phys. Rev. Lett. 97, 258001 (2006). PRLTAO 0031-9007 10.1103/PhysRevLett.97.258001
-
(2006)
Phys. Rev. Lett.
, vol.97
, pp. 258001
-
-
Ellenbroek W, G.1
Somfai, E.2
Van Hecke, M.3
Van Saarloos, W.4
-
21
-
-
79051470950
-
-
EULEEJ
-
W.G. Ellenbroek, Z. Zeravcic, W. van Saarloos, and M. van Hecke, Europhys. Lett. 87, 34004 (2009). EULEEJ 0295-5075 10.1209/0295-5075/87/34004
-
(2009)
Europhys. Lett.
, vol.87
, pp. 34004
-
-
Ellenbroek W, G.1
Zeravcic, Z.2
Van Saarloos, W.3
Van Hecke, M.4
-
22
-
-
84929598105
-
-
PRLTAO
-
W.G. Ellenbroek, V.F. Hagh, A. Kumar, M.F. Thorpe, and M. van Hecke, Phys. Rev. Lett. 114, 135501 (2015). PRLTAO 0031-9007 10.1103/PhysRevLett.114.135501
-
(2015)
Phys. Rev. Lett.
, vol.114
, pp. 135501
-
-
Ellenbroek W, G.1
Hagh, F.2
Kumar, A.3
Thorpe M, F.4
Van Hecke, M.5
-
24
-
-
84935906345
-
-
Higher order corrections to the elastic constants are negligible for the range of (Equation presented) discussed here
-
Higher order corrections to the elastic constants are negligible for the range of (Equation presented) discussed here.
-
-
-
-
25
-
-
84999396836
-
-
For the cases where the largest (Equation presented) or (Equation presented) bonds are removed, zero modes do not appear until (Equation presented). For the random case and the case where the bond with the smallest (Equation presented) is removed, the first zero mode can appear when there are still a few bonds above the isostatic value
-
For the cases where the largest (Equation presented) or (Equation presented) bonds are removed, zero modes do not appear until (Equation presented). For the random case and the case where the bond with the smallest (Equation presented) is removed, the first zero mode can appear when there are still a few bonds above the isostatic value.
-
-
-
-
28
-
-
84883288944
-
-
BONEDL
-
J.H. Keyak, S. Sigurdsson, G.S. Karlsdottir, D. Oskarsdottir, A. Sigmarsdottir, J. Kornak, T.B. Harris, G. Sigurdsson, B.Y. Jonsson, K. Siggeirsdottir, G. Eiriksdottir, V. Gudnason, and T.F. Lang, Bone 57, 18 (2013). BONEDL 8756-3282 10.1016/j.bone.2013.07.028
-
(2013)
Bone
, vol.57
, pp. 18
-
-
Keyak J, H.1
Sigurdsson, S.2
Karlsdottir G, S.3
Oskarsdottir, D.4
Sigmarsdottir, A.5
Kornak, J.6
Harris T, B.7
Sigurdsson, G.8
Jonsson B, Y.9
Siggeirsdottir, K.10
Eiriksdottir, G.11
Gudnason, V.12
Lang T, F.13
-
29
-
-
84862197022
-
-
PRLTAO
-
M. Lenz, T. Thoresen, M.L. Gardel, and A.R. Dinner, Phys. Rev. Lett. 108, 238107 (2012). PRLTAO 0031-9007 10.1103/PhysRevLett.108.238107
-
(2012)
Phys. Rev. Lett.
, vol.108
, pp. 238107
-
-
Lenz, M.1
Thoresen, T.2
Gardel M, L.3
Dinner A, R.4
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