| two dimensional | 2D | 157 | 26 | 1.002775 | 0401016,0401030,etc |
| local density approximation | LDA | 292 | 21 | 2.004046 | 0401011,0401066,etc |
| antiferromagnetic | AF | 383 | 21 | 2.006469 | 0401014,0401130,etc |
| density of states | DOS | 171 | 19 | 2.001582 | 0401011,0401012,etc |
| density functional theory | DFT | 105 | 19 | 1.000734 | 0401012,0401073,etc |
| one dimensional | 1D | 100 | 15 | 2.002344 | 0401059,0401068,etc |
| monte carlo | MC | 133 | 13 | 1.002822 | 0401002,0401073,etc |
| quantum monte carlo | QMC | 115 | 13 | 2.002351 | 0401073,0401089,etc |
| dynamical mean field theory | DMFT | 289 | 12 | 2.006274 | 0401060,0401064,etc |
| molecular dynamics | MD | 188 | 12 | 2.002237 | 0401073,0401117,etc |
| random phase approximation | RPA | 49 | 10 | 1.001055 | 0401043,0401160,etc |
| charge density wave | CDW | 120 | 10 | 1.003505 | 0401059,0401079,etc |
| density matrix renormalization group | DMRG | 83 | 10 | 1.006743 | 0401060,0401115,etc |
| generalized gradient approximation | GGA | 21 | 9 | 1.000675 | 0401051,0401318,etc |
| ginzburg landau | GL | 80 | 9 | 1.003603 | 0401077,0401124,etc |
| mean field | MF | 67 | 8 | 1.001962 | 0401002,0401077,etc |
| three dimensional | 3D | 30 | 7 | 1.002205 | 0401002,0401098,etc |
| exact diagonalization | ED | 35 | 7 | 2.001192 | 0401043,0401125,etc |
| spin density wave | SDW | 46 | 7 | 1.002354 | 0401159,0401242,etc |
| lennard jones | LJ | 66 | 7 | 2.001863 | 0401230,0401314,etc |
| angle resolved photoemission spectroscopy | ARPES | 49 | 6 | 2.002977 | 0401034,0401063,etc |
| hartree fock | HF | 49 | 6 | 2.001327 | 0401043,0401079,etc |
| inelastic neutron scattering | INS | 48 | 6 | 2.001884 | 0401064,0401244,etc |
| quantum critical point | QCP | 47 | 6 | 1.001104 | 0401099,0401167,etc |
| local density of states | LDOS | 175 | 6 | 2.00268 | 0401417,0401498,etc |
| numerical renormalization group | NRG | 18 | 5 | 1.000632 | 0401005,0401022,etc |
| highest occupied molecular orbital | HOMO | 45 | 5 | 1.001493 | 0401012,0401066,etc |
| metal insulator transition | MIT | 40 | 5 | 1.002627 | 0401028,0401090,etc |
| nearest neighbor | NN | 79 | 5 | 1.002028 | 0401028,0401368,etc |
| resonating valence bond | RVB | 17 | 5 | 1.000653 | 0401041,0401122,etc |
| jahn teller | JT | 48 | 5 | 2.001275 | 0401104,0401185,etc |
| bose einstein condensation | BEC | 62 | 5 | 1.004041 | 0401109,0401411,etc |
| scanning tunneling microscopy | STM | 12 | 5 | 1.00077 | 0401271,0401467,etc |
| gross pitaevskii | GP | 32 | 4 | 2.001394 | 0401021,0401228,etc |
| electron spin resonance | ESR | 18 | 4 | 2.000796 | 0401022,0401240,etc |
| quantum dot | QD | 85 | 4 | 2.001753 | 0401029,0401043,etc |
| two dimensional electron gas | 2DEG | 46 | 4 | 2.004017 | 0401029,0401085,etc |
| fermi liquid | FL | 21 | 4 | 1.001047 | 0401031,0401099,etc |
| lasrcuo | LSCO | 48 | 4 | 2.000972 | 0401034,0401063,etc |
| ybacuo | YBCO | 41 | 4 | 2.000322 | 0401034,0401328,etc |
| energy loss spectroscopy | EELS | 20 | 4 | 1.001516 | 0401051,0401095,etc |
| landau level | LLL | 18 | 4 | 2.001457 | 0401079,0401173,etc |
| asymmetric simple exclusion process | ASEP | 33 | 4 | 2.001182 | 0401080,0401341,etc |
| kardar parisi zhang | KPZ | 40 | 4 | 2.001385 | 0401110,0401229,etc |
| mode coupling theory | MCT | 38 | 4 | 1.004719 | 0401117,0401401,etc |
| spin orbit | SO | 43 | 4 | 2.002149 | 0401130,0401187,etc |
| linear muffin tin orbital | LMTO | 19 | 4 | 1.000545 | 0401133,0401235,etc |
| bose einstein condensate | BEC | 46 | 4 | 2.003284 | 0401172,0401228,etc |
| double exchange | DE | 11 | 4 | 1.000617 | 0401185,0401275,etc |
| non fermi liquid | NFL | 12 | 4 | 1.000474 | 0401375,0401412,etc |
| single electron transistor | SET | 138 | 4 | 2.006885 | 0401387,0401391,etc |
| shubnikov de haas | SdH | 29 | 3 | 1.001759 | 0401007,0401396,etc |
| self consistent born approximation | SCBA | 17 | 3 | 1.001113 | 0401007,0401398,etc |
| berezinskii kosterlitz thouless | BKT | 39 | 3 | 2.001816 | 0401030,0401101,etc |
| quantum point contact | QPC | 66 | 3 | 2.002403 | 0401058,0401204,etc |
| fundamental research on matter | FOM | 3 | 3 | 1.000111 | 0401058,0401305,etc |
| gross pitaevskii equation | GP | 32 | 3 | 2.000924 | 0401070,0401219,etc |
| potential energy surface | PES | 11 | 3 | 1.000519 | 0401073,0401095,etc |
| finite size scaling | FSS | 17 | 3 | 1.000722 | 0401097,0401259,etc |
| thomas fermi | TF | 26 | 3 | 2.000783 | 0401107,0401298,etc |
| su schrieffer heeger | SSH | 26 | 3 | 1.002281 | 0401125,0401261,etc |
| one step replica symmetry breaking | 1RSB | 46 | 3 | 2.00163 | 0401139,0401602,etc |
| dzyaloshinskii moriya | DM | 53 | 3 | 1.003378 | 0401158,0401614,etc |
| aharonov bohm | AB | 34 | 3 | 2.001734 | 0401169,0401182,etc |
| non crossing approximation | NCA | 5 | 3 | 1.000073 | 0401180,0401539,etc |
| stochastic resonance | SR | 37 | 3 | 1.005636 | 0401213,0401263,etc |
| coherent potential approximation | CPA | 15 | 3 | 1.00268 | 0401215,0401553,etc |
| long range order | LRO | 11 | 3 | 2.000556 | 0401235,0401264,etc |
| linearized augmented planewave | LAPW | 7 | 3 | 1.000741 | 0401246,0401563,etc |
| two dimensional electron system | 2DES | 36 | 3 | 2.001584 | 0401325,0401462,etc |
| full counting statistics | FCS | 58 | 3 | 2.00102 | 0401361,0401577,etc |
| minority game | MG | 110 | 3 | 2.002879 | 0401363,0401372,etc |
| potential energy landscape | PEL | 22 | 3 | 1.000665 | 0401435,0401449,etc |
| high temperature superconductors | HTSC | 25 | 3 | 2.001225 | 0401452,0401474,etc |
| bond order wave | BOW | 96 | 3 | 2.003231 | 0401472,0401494,etc |
| gw approximation | GWA | 65 | 3 | 2.002211 | 0401620,0401626,etc |