@article{
 title = {Interacting composite fermions},
 type = {article},
 year = {2001},
 pages = {117-122},
 volume = {117},
 websites = {http://dx.doi.org/10.1016/S0038-1098(00)00440-3},
 id = {4eecb665-3fbb-3fba-9e95-35f14876ca73},
 created = {2017-12-12T20:22:27.843Z},
 file_attached = {true},
 profile_id = {004c1ae0-7ed4-35f3-b39b-28665b4ab9a2},
 last_modified = {2017-12-12T20:23:37.056Z},
 read = {false},
 starred = {false},
 authored = {true},
 confirmed = {true},
 hidden = {false},
 citation_key = {Jain2001},
 source_type = {JOUR},
 private_publication = {false},
 abstract = {Even though much of the dramatic physics of two-dimensional electrons in a high magnetic field is explicable in terms of weakly interacting composite fermions (CFs), the inter-CF interaction is responsible for many interesting, non-trivial phenomena. Here, we discuss four examples. (i) At small filling factors, a softening of the roton mode destroys the fractional Hall effect, giving way to the Wigner crystal. (ii) In higher Landau levels, the fractional Hall effect is destroyed due to a collapse of the energy of the neutral exciton. (iii) At ν = 5/2, the Fermi sea of CFs is unstable to Cooper pairing of CFs, thereby opening up a gap and producing a fractional Hall effect. (iv) Prior to the transition into the Wigner crystal, the CF liquid exhibits the Bloch instability into a magnetically ordered, spontaneously broken symmetry phase.},
 bibtype = {article},
 author = {Jain, J. K. and Kamilla, R. K. and Park, K. and Scarola, V. W.},
 doi = {10.1016/S0038-1098(00)00440-3},
 journal = {Solid State Communications},
 number = {3}
}

{"_id":"KqqJgs7A8JB5ayHc7","bibbaseid":"jain-kamilla-park-scarola-interactingcompositefermions-2001","downloads":1,"creationDate":"2017-11-18T02:13:58.805Z","title":"Interacting composite fermions","author_short":["Jain, J., K.","Kamilla, R., K.","Park, K.","Scarola, V., W."],"year":2001,"bibtype":"article","biburl":"https://bibbase.org/service/mendeley/004c1ae0-7ed4-35f3-b39b-28665b4ab9a2","bibdata":{"title":"Interacting composite fermions","type":"article","year":"2001","pages":"117-122","volume":"117","websites":"http://dx.doi.org/10.1016/S0038-1098(00)00440-3","id":"4eecb665-3fbb-3fba-9e95-35f14876ca73","created":"2017-12-12T20:22:27.843Z","file_attached":"true","profile_id":"004c1ae0-7ed4-35f3-b39b-28665b4ab9a2","last_modified":"2017-12-12T20:23:37.056Z","read":false,"starred":false,"authored":"true","confirmed":"true","hidden":false,"citation_key":"Jain2001","source_type":"JOUR","private_publication":false,"abstract":"Even though much of the dramatic physics of two-dimensional electrons in a high magnetic field is explicable in terms of weakly interacting composite fermions (CFs), the inter-CF interaction is responsible for many interesting, non-trivial phenomena. Here, we discuss four examples. (i) At small filling factors, a softening of the roton mode destroys the fractional Hall effect, giving way to the Wigner crystal. (ii) In higher Landau levels, the fractional Hall effect is destroyed due to a collapse of the energy of the neutral exciton. (iii) At ν = 5/2, the Fermi sea of CFs is unstable to Cooper pairing of CFs, thereby opening up a gap and producing a fractional Hall effect. (iv) Prior to the transition into the Wigner crystal, the CF liquid exhibits the Bloch instability into a magnetically ordered, spontaneously broken symmetry phase.","bibtype":"article","author":"Jain, J. K. and Kamilla, R. K. and Park, K. and Scarola, V. W.","doi":"10.1016/S0038-1098(00)00440-3","journal":"Solid State Communications","number":"3","bibtex":"@article{\n title = {Interacting composite fermions},\n type = {article},\n year = {2001},\n pages = {117-122},\n volume = {117},\n websites = {http://dx.doi.org/10.1016/S0038-1098(00)00440-3},\n id = {4eecb665-3fbb-3fba-9e95-35f14876ca73},\n created = {2017-12-12T20:22:27.843Z},\n file_attached = {true},\n profile_id = {004c1ae0-7ed4-35f3-b39b-28665b4ab9a2},\n last_modified = {2017-12-12T20:23:37.056Z},\n read = {false},\n starred = {false},\n authored = {true},\n confirmed = {true},\n hidden = {false},\n citation_key = {Jain2001},\n source_type = {JOUR},\n private_publication = {false},\n abstract = {Even though much of the dramatic physics of two-dimensional electrons in a high magnetic field is explicable in terms of weakly interacting composite fermions (CFs), the inter-CF interaction is responsible for many interesting, non-trivial phenomena. Here, we discuss four examples. (i) At small filling factors, a softening of the roton mode destroys the fractional Hall effect, giving way to the Wigner crystal. (ii) In higher Landau levels, the fractional Hall effect is destroyed due to a collapse of the energy of the neutral exciton. (iii) At ν = 5/2, the Fermi sea of CFs is unstable to Cooper pairing of CFs, thereby opening up a gap and producing a fractional Hall effect. (iv) Prior to the transition into the Wigner crystal, the CF liquid exhibits the Bloch instability into a magnetically ordered, spontaneously broken symmetry phase.},\n bibtype = {article},\n author = {Jain, J. K. and Kamilla, R. K. and Park, K. and Scarola, V. W.},\n doi = {10.1016/S0038-1098(00)00440-3},\n journal = {Solid State Communications},\n number = {3}\n}","author_short":["Jain, J., K.","Kamilla, R., K.","Park, K.","Scarola, V., W."],"urls":{"Website":"http://dx.doi.org/10.1016/S0038-1098(00)00440-3"},"biburl":"https://bibbase.org/service/mendeley/004c1ae0-7ed4-35f3-b39b-28665b4ab9a2","bibbaseid":"jain-kamilla-park-scarola-interactingcompositefermions-2001","role":"author","metadata":{"authorlinks":{"scarola, v":"https://bibbase.org/service/mendeley/004c1ae0-7ed4-35f3-b39b-28665b4ab9a2"}},"downloads":1},"search_terms":["interacting","composite","fermions","jain","kamilla","park","scarola"],"keywords":[],"authorIDs":["zqzBMncc4o9w2om2w"],"dataSources":["3hvXS94a6LrrsHXsS","ya2CyA73rpZseyrZ8","q9AemAnoxjKBeqdKn"]}