_id,doi,title
2120,10.1142/S0219025708003245,On the domain of non-symmetric Ornstein-Uhlenbeck operators in banach spaces
2121,,A Clark-Ocone formula in UMD Banach spaces
2146,10.1063/1.2948392,An analytic model of rotationally inelastic collisions of polar molecules in electric fields
2147,,"Kvantový Zenonův jev aneb co nesejde z očí, nezestárne"
2148,10.1180/minmag.2008.072.2.667 ,In situ X-ray absorption spectroscopy measurement of vapour-brine fractionation of antimony at hydrothermal conditions
224,10.1112/plms/pdm032,On the representation of integers by quadratic forms
225,10.1112/S0010437X08003692,Binary linear forms as sums of two squares
2331,10.1142/9789812832382_0009, Spectral properties of the BCS gap equation of superfluidity
2332,10.1142/9789812832382_0017,Vortices and Spontaneous Symmetry Breaking in Rotating Bose Gases
2374,10.1007/s00220-008-0428-2,Free energy of a dilute Bose gas: Lower bound
2376,10.1103/PhysRevB.77.184517,Critical temperature and energy gap for the BCS equation
2377,10.1007/s11005-008-0242-y,The BCS critical temperature for potentials with negative scattering length
2378,10.1007/s10955-008-9527-x,Ground state energy of the low density hubbard model
2379,10.1090/S0894-0347-07-00582-6,Hardy-Lieb-Thirring inequalities for fractional Schrödinger operators
2380,10.1007/s00220-008-0489-2,The BCS functional for general pair interactions
2381,10.1016/j.jfa.2008.05.015,Non-linear ground state representations and sharp Hardy inequalities
2382,10.1007/s00220-008-0521-6,The Lieb-Liniger model as a limit of dilute bosons in three dimensions
2383,10.1142/S0129055X08003547,A nonlinear model for relativistic electrons at positive temperature
2415,10.1090/conm/453,k-Sets and k-facets
2432,10.1007/978-3-540-69733-6_36,On center regions and balls containing many points