[{"title":"Emergent SO(3) symmetry of the frictionless shear jamming transition","citation":{"chicago":"Baity-Jesi, Marco, Carl Peter Goodrich, Andrea J. Liu, Sidney R. Nagel, and James P. Sethna. “Emergent SO(3) Symmetry of the Frictionless Shear Jamming Transition.” <i>Journal of Statistical Physics</i>. Springer Nature, 2017. <a href=\"https://doi.org/10.1007/s10955-016-1703-9\">https://doi.org/10.1007/s10955-016-1703-9</a>.","ieee":"M. Baity-Jesi, C. P. Goodrich, A. J. Liu, S. R. Nagel, and J. P. Sethna, “Emergent SO(3) symmetry of the frictionless shear jamming transition,” <i>Journal of Statistical Physics</i>, vol. 167, no. 3–4. Springer Nature, pp. 735–748, 2017.","ista":"Baity-Jesi M, Goodrich CP, Liu AJ, Nagel SR, Sethna JP. 2017. Emergent SO(3) symmetry of the frictionless shear jamming transition. Journal of Statistical Physics. 167(3–4), 735–748.","mla":"Baity-Jesi, Marco, et al. “Emergent SO(3) Symmetry of the Frictionless Shear Jamming Transition.” <i>Journal of Statistical Physics</i>, vol. 167, no. 3–4, Springer Nature, 2017, pp. 735–48, doi:<a href=\"https://doi.org/10.1007/s10955-016-1703-9\">10.1007/s10955-016-1703-9</a>.","short":"M. Baity-Jesi, C.P. Goodrich, A.J. Liu, S.R. Nagel, J.P. Sethna, Journal of Statistical Physics 167 (2017) 735–748.","ama":"Baity-Jesi M, Goodrich CP, Liu AJ, Nagel SR, Sethna JP. Emergent SO(3) symmetry of the frictionless shear jamming transition. <i>Journal of Statistical Physics</i>. 2017;167(3-4):735-748. doi:<a href=\"https://doi.org/10.1007/s10955-016-1703-9\">10.1007/s10955-016-1703-9</a>","apa":"Baity-Jesi, M., Goodrich, C. P., Liu, A. J., Nagel, S. R., &#38; Sethna, J. P. (2017). Emergent SO(3) symmetry of the frictionless shear jamming transition. <i>Journal of Statistical Physics</i>. Springer Nature. <a href=\"https://doi.org/10.1007/s10955-016-1703-9\">https://doi.org/10.1007/s10955-016-1703-9</a>"},"year":"2017","oa_version":"None","type":"journal_article","author":[{"full_name":"Baity-Jesi, Marco","first_name":"Marco","last_name":"Baity-Jesi"},{"orcid":"0000-0002-1307-5074","id":"EB352CD2-F68A-11E9-89C5-A432E6697425","full_name":"Goodrich, Carl Peter","first_name":"Carl Peter","last_name":"Goodrich"},{"full_name":"Liu, Andrea J.","first_name":"Andrea J.","last_name":"Liu"},{"last_name":"Nagel","full_name":"Nagel, Sidney R.","first_name":"Sidney R."},{"last_name":"Sethna","first_name":"James P.","full_name":"Sethna, James P."}],"day":"03","article_type":"original","doi":"10.1007/s10955-016-1703-9","publication_identifier":{"issn":["0022-4715","1572-9613"]},"user_id":"2DF688A6-F248-11E8-B48F-1D18A9856A87","date_updated":"2021-01-12T08:15:19Z","language":[{"iso":"eng"}],"issue":"3-4","article_processing_charge":"No","page":"735-748","date_published":"2017-01-03T00:00:00Z","_id":"7756","date_created":"2020-04-30T11:38:38Z","abstract":[{"text":"We study the shear jamming of athermal frictionless soft spheres, and find that in the thermodynamic limit, a shear-jammed state exists with different elastic properties from the isotropically-jammed state. For example, shear-jammed states can have a non-zero residual shear stress in the thermodynamic limit that arises from long-range stress-stress correlations. As a result, the ratio of the shear and bulk moduli, which in isotropically-jammed systems vanishes as the jamming transition is approached from above, instead approaches a constant. Despite these striking differences, we argue that in a deeper sense, the shear jamming and isotropic jamming transitions actually have the same symmetry, and that the differences can be fully understood by rotating the six-dimensional basis of the elastic modulus tensor.","lang":"eng"}],"extern":"1","month":"01","publisher":"Springer Nature","publication_status":"published","volume":167,"intvolume":"       167","status":"public","quality_controlled":"1","publication":"Journal of Statistical Physics"}]