| two dimensional | 2D | 297 | 29 | 1.003263 | 0402011,0402018,etc |
| density of states | DOS | 329 | 27 | 2.003046 | 0402031,0402060,etc |
| one dimensional | 1D | 211 | 21 | 2.002041 | 0402041,0402060,etc |
| density functional theory | DFT | 164 | 17 | 1.004099 | 0402088,0402096,etc |
| antiferromagnetic | AF | 257 | 16 | 2.002498 | 0402011,0402064,etc |
| monte carlo | MC | 132 | 16 | 1.002585 | 0402036,0402046,etc |
| renormalization group | RG | 123 | 15 | 1.001294 | 0402024,0402055,etc |
| local density approximation | LDA | 135 | 14 | 1.002263 | 0402088,0402101,etc |
| molecular dynamics | MD | 90 | 13 | 2.001165 | 0402005,0402048,etc |
| two dimensional electron gas | 2DEG | 141 | 11 | 2.002844 | 0402042,0402158,etc |
| bose einstein condensate | BEC | 210 | 11 | 2.007272 | 0402078,0402128,etc |
| quantum well | QW | 147 | 10 | 1.004237 | 0402043,0402093,etc |
| fermi surface | FS | 138 | 10 | 2.005181 | 0402058,0402076,etc |
| charge density wave | CDW | 133 | 9 | 1.003599 | 0402024,0402141,etc |
| density matrix renormalization group | DMRG | 84 | 9 | 2.002669 | 0402250,0402298,etc |
| three dimensional | 3D | 79 | 8 | 1.00237 | 0402018,0402024,etc |
| random phase approximation | RPA | 24 | 8 | 1.000371 | 0402150,0402273,etc |
| local density of states | LDOS | 164 | 7 | 2.00383 | 0402019,0402021,etc |
| nuclear magnetic resonance | NMR | 41 | 7 | 1.001326 | 0402064,0402274,etc |
| quantum monte carlo | QMC | 68 | 7 | 2.00147 | 0402102,0402189,etc |
| inelastic neutron scattering | INS | 25 | 6 | 2.001376 | 0402011,0402048,etc |
| spin density wave | SDW | 84 | 6 | 2.002733 | 0402011,0402141,etc |
| brillouin zone | BZ | 24 | 6 | 1.000807 | 0402093,0402096,etc |
| scanning tunneling microscopy | STM | 23 | 6 | 1.001291 | 0402144,0402233,etc |
| mode coupling theory | MCT | 126 | 6 | 2.003038 | 0402254,0402314,etc |
| bose einstein condensates | BEC | 52 | 5 | 2.001773 | 0402003,0402081,etc |
| ground state | GS | 52 | 5 | 2.001538 | 0402011,0402198,etc |
| nearest neighbor | NN | 35 | 5 | 1.001959 | 0402011,0402132,etc |
| x ray diffraction | XRD | 31 | 5 | 2.002085 | 0402012,0402015,etc |
| heavy fermion | HF | 24 | 5 | 1.001079 | 0402017,0402187,etc |
| metal insulator transition | MIT | 64 | 5 | 2.004407 | 0402018,0402121,etc |
| lennard jones | LJ | 55 | 5 | 1.001505 | 0402030,0402209,etc |
| ferromagnetic | FM | 134 | 5 | 2.004469 | 0402043,0402122,etc |
| coherent potential approximation | CPA | 42 | 5 | 1.002258 | 0402060,0402093,etc |
| ybacuo | YBCO | 19 | 5 | 2.000824 | 0402064,0402131,etc |
| bose einstein condensation | BEC | 37 | 5 | 1.002369 | 0402079,0402276,etc |
| dynamical mean field theory | DMFT | 79 | 5 | 1.001648 | 0402121,0402133,etc |
| quantum dot | QD | 101 | 5 | 2.002783 | 0402244,0402260,etc |
| angle resolved photoemission spectroscopy | ARPES | 35 | 5 | 1.000926 | 0402247,0402457,etc |
| non fermi liquid | NFL | 38 | 4 | 2.001637 | 0402004,0402076,etc |
| mechanical alloying | MA | 56 | 4 | 2.002482 | 0402012,0402013,etc |
| fundamental research on matter | FOM | 6 | 4 | 1.000047 | 0402019,0402090,etc |
| minority game | MG | 153 | 4 | 2.004022 | 0402028,0402300,etc |
| de haas van alphen | dHvA | 17 | 4 | 1.00094 | 0402058,0402076,etc |
| ginzburg landau | GL | 15 | 4 | 2.001639 | 0402064,0402123,etc |
| scanning tunneling microscope | STM | 22 | 4 | 1.00139 | 0402083,0402244,etc |
| superconducting | SC | 65 | 4 | 2.005634 | 0402115,0402199,etc |
| thomas fermi | TF | 29 | 4 | 2.002156 | 0402128,0402208,etc |
| one dimension | 1D | 32 | 4 | 2.001697 | 0402138,0402198,etc |
| hartree fock | HF | 16 | 4 | 1.001697 | 0402150,0402469,etc |
| electron paramagnetic resonance | EPR | 9 | 4 | 1.000645 | 0402152,0402398,etc |
| aharonov bohm | AB | 25 | 4 | 1.000626 | 0402165,0402168,etc |
| kosterlitz thouless | KT | 45 | 4 | 2.003253 | 0402177,0402186,etc |
| luttinger liquid | LL | 120 | 4 | 2.002057 | 0402244,0402332,etc |
| double exchange | DE | 34 | 4 | 1.002156 | 0402279,0402344,etc |
| directed percolation | DP | 79 | 4 | 2.002067 | 0402283,0402430,etc |
| momentum distribution curve | MDC | 26 | 4 | 1.000456 | 0402304,0402457,etc |
| resonating valence bond | RVB | 69 | 3 | 2.004814 | 0402011,0402497,etc |
| quantum critical point | QCP | 22 | 3 | 2.001646 | 0402016,0402017,etc |
| finite size scaling | FSS | 10 | 3 | 1.000382 | 0402018,0402596,etc |
| lasrcuo | LSCO | 9 | 3 | 1.000889 | 0402025,0402141,etc |
| effective medium approximation | EMA | 44 | 3 | 2.001636 | 0402046,0402047,etc |
| inelastic x ray scattering | IXS | 19 | 3 | 2.002163 | 0402048,0402067,etc |
| series expansion | SSE | 18 | 3 | 1.000735 | 0402051,0402189,etc |
| ultra high vacuum | UHV | 5 | 3 | 1.000335 | 0402057,0402488,etc |
| shubnikov de haas | SdH | 10 | 3 | 1.001812 | 0402058,0402139,etc |
| flux line lattice | FLL | 27 | 3 | 2.000953 | 0402064,0402400,etc |
| bisrcacuo | BSCCO | 16 | 3 | 2.001483 | 0402064,0402141,etc |
| zero range process | ZRP | 20 | 3 | 2.001022 | 0402071,0402305,etc |
| israel science foundation | ISF | 3 | 3 | 1.000041 | 0402071,0402252,etc |
| monte carlo steps | MCS | 11 | 3 | 1.000294 | 0402075,0402521,etc |
| antiferromagnet | AFM | 66 | 3 | 2.008449 | 0402076,0402109,etc |
| fast fourier transform | FFT | 5 | 3 | 1.00016 | 0402081,0402386,etc |
| ferroelectric | FE | 20 | 3 | 2.00032 | 0402100,0402465,etc |
| long range order | LRO | 50 | 3 | 2.001681 | 0402102,0402109,etc |
| nuclear quadrupole resonance | NQR | 5 | 3 | 1.000513 | 0402102,0402503,etc |
| atomic force microscopy | AFM | 7 | 3 | 1.000281 | 0402106,0402496,etc |
| kohn sham | KS | 27 | 3 | 2.0007 | 0402108,0402514,etc |
| generalized gradient approximation | GGA | 9 | 3 | 2.000296 | 0402108,0402409,etc |
| numerical renormalization group | NRG | 17 | 3 | 1.000814 | 0402121,0402184,etc |
| paramagnetic | PM | 24 | 3 | 1.000509 | 0402122,0402243,etc |
| gross pitaevskii equation | GPE | 25 | 3 | 1.001672 | 0402128,0402225,etc |
| low energy electron diffraction | LEED | 4 | 3 | 1.000116 | 0402144,0402410,etc |
| variable range hopping | VRH | 18 | 3 | 1.000648 | 0402145,0402327,etc |
| landau level | LLL | 23 | 3 | 1.000316 | 0402167,0402292,etc |
| exact diagonalization | ED | 52 | 3 | 2.002326 | 0402184,0402514,etc |
| highest occupied molecular orbital | HOMO | 5 | 3 | 1.000183 | 0402197,0402257,etc |
| lowest unoccupied molecular orbital | LUMO | 8 | 3 | 1.000515 | 0402197,0402257,etc |
| quasiparticle | QP | 18 | 3 | 1.000742 | 0402197,0402263,etc |
| gross pitaevskii | GP | 28 | 3 | 2.00149 | 0402208,0402281,etc |
| tight binding | TB | 10 | 3 | 1.000326 | 0402210,0402568,etc |
| scanning tunnelling microscopy | STM | 21 | 3 | 2.000645 | 0402229,0402398,etc |
| replica symmetric | RS | 104 | 3 | 2.000784 | 0402243,0402504,etc |
| angle resolved photoemission | ARPES | 32 | 3 | 2.003887 | 0402304,0402340,etc |
| single wall carbon nanotube | SWNT | 13 | 3 | 1.001329 | 0402332,0402359,etc |
| boltzmann gibbs | BG | 25 | 3 | 1.003774 | 0402343,0402635,etc |
| bardeen cooper schrieffer | BCS | 29 | 3 | 1.003952 | 0402375,0402448,etc |
| fundamenteel onderzoek der materie | FOM | 3 | 3 | 1.000081 | 0402388,0402465,etc |
| field cooling | FC | 8 | 3 | 1.00048 | 0402483,0402503,etc |
| superconducting quantum interference device | SQUID | 9 | 3 | 1.000829 | 0402655,0402678,etc |