"Neuvedeno."@en . "0"^^ . . "756"^^ . "3"^^ . . "0"^^ . "3"^^ . . . "According to current wisdom the deconfined QCD matter at very low temperatures exists in one of several color super-conducting phases. We wish to contribute to the art of describing, understanding and, in the best case, of predicting the behavior of these phases by including the effects so far neglected for simplicity: 1) Cooper pairing in s-state with spin one. 2) Condensates which do not transform covariantly under Lorentz transformation. 3) Condensates which transform as sextet under color SU(3).In the real world of three colors these effects might manifest in the behavior of the neutron stars and, optimistically, also in behavior of the relativistic heavy ion collisions. We wish to apply the principles of quantum fluids also to the confined low-temperature phase of QCD with two colors far from the chiral limit. We expect that the matter of many bosons carrying the baryon charge should be at very low baryon densities a super fluid, similar to the weakly interacting Bose gas with"@en . . "1"^^ . . "N\u00EDzkoteplotn\u00ED uspo\u0159\u00E1dan\u00E9 f\u00E1ze kvantov\u00E9 chromodynamiky p\u0159i kone\u010Dn\u00FDch baryonov\u00FDch hustot\u00E1ch"@cs . "Low-temperature ordered phases of quantum chromodynamics (QCD) at finite baryon densities"@en . . "Podle sou\u010Dasn\u00FDch p\u0159edstav se dekonfinovan\u00E1 QCD hmota p\u0159i velmi n\u00EDzk\u00FDch teplot\u00E1ch nach\u00E1z\u00ED v n\u011Bkter\u00E9 z barevn\u011B-supravodiv\u00FDch f\u00E1z\u00ED. Chceme p\u0159isp\u011Bt k um\u011Bn\u00ED tyto f\u00E1ze popisovat, ch\u00E1pat a v nejlep\u0161\u00EDm p\u0159\u00EDpad\u011B p\u0159edpov\u00EDdat jejich chov\u00E1n\u00ED t\u00EDm, \u017Ee do formalismu zahrneme efekty, zat\u00EDm pro jednoduchost zanedb\u00E1van\u00E9: (l)Cooperovo p\u00E1rov\u00E1n\u00ED v s-stavu se spinem 1; (2) kondenz\u00E1ty, kter\u00E9 se netransformuj\u00ED kovariantn\u011B Lorentzov\u011B transformaci; (3) kondenz\u00E1ty, kter\u00E9 se transformuj\u00ED jako sextet barevn\u00E9 grupy SU(3). V re\u00E1ln\u00E9m sv\u011Bt\u011B t\u0159\u00ED barev by se m\u011Bly uveden\u00E9 efekty projevovat v chov\u00E1n\u00ED neutronov\u00FDch hv\u011Bzd a optimisticky tak\u00E9 v chov\u00E1n\u00ED relativistick\u00FDch sr\u00E1\u017Eek t\u011B\u017Ek\u00FDch iont\u016F. Principy fyziky kvantov\u00FDch kapalin chceme aplikovat tak\u00E9 na konfinovanou n\u00EDzkoteplotn\u00ED f\u00E1zi QCDs dv\u011Bma barvami daleko od chir\u00E1ln\u00ED limity. O\u010Dek\u00E1v\u00E1me, \u017Ee syst\u00E9m mnoha boson\u016F nesouc\u00EDch baryonov\u00E9 \u010D\u00EDslo by m\u011Bl b\u00FDt pro velmi n\u00EDzk\u00E9 baryonov\u00E9 hustoty supratekut\u00FD, podobn\u00FD slab\u011B interaguj\u00EDc\u00EDmu Boseho plynu s Bose-Einsteinov\u00FDm kondenz\u00E1tem. Efektivn\u00ED"@cs . "2106"^^ . . . .