@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}
}

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