LEADER 02470nam 2200625 a 450 001 9910959314203321 005 20251117082352.0 010 $a1-61668-658-8 035 $a(CKB)2550000000010765 035 $a(EBL)3020086 035 $a(SSID)ssj0000413080 035 $a(PQKBManifestationID)12144922 035 $a(PQKBTitleCode)TC0000413080 035 $a(PQKBWorkID)10381913 035 $a(PQKB)11390565 035 $a(MiAaPQ)EBC3020086 035 $a(Au-PeEL)EBL3020086 035 $a(CaPaEBR)ebr10675094 035 $a(OCoLC)923662501 035 $a(BIP)23678585 035 $a(EXLCZ)992550000000010765 100 $a20081112d2009 uy 0 101 0 $aeng 135 $aur|n|---||||| 181 $ctxt 182 $cc 183 $acr 200 10$aBosons after symmetry breaking in quantum field theory /$fTakehisa Fujita, Makoto Hiramoto and Hidenori Takahashi 205 $a1st ed. 210 $aHauppauge N.Y. $cNova Science Publishers$dc2009 215 $a1 online resource (102 p.) 300 $aDescription based upon print version of record. 311 08$a1-60692-110-X 320 $aIncludes bibliographical references and index. 327 $aGoldstone theorem and its applicability -- Goldstone boson in boson field theory -- No Goldstone boson in fermion field theory -- Bethe ansatz solutions in thirring model -- Schwinger boson in two dimensional QED -- Bosons in two dimensional QCD. 330 $aThe authors present a unified description of the spontaneous symmetry breaking and its associated bosons in fermion field theory. The defect of the Goldstone theorem is clarified, and the 'massless boson' predicted by the theorem is virtual and corresponds to just a free massless fermion and antifermion pair. 606 $aInteracting boson-fermion models 606 $aBroken symmetry (Physics) 606 $aQuantum chromodynamics 606 $aQuantum electrodynamics 615 0$aInteracting boson-fermion models. 615 0$aBroken symmetry (Physics) 615 0$aQuantum chromodynamics. 615 0$aQuantum electrodynamics. 676 $a530.14/3 700 $aFujita$b T$01599584 701 $aHiramoto$b Makoto$01861937 701 $aTakahashi$b Hidenori$01861938 801 0$bMiAaPQ 801 1$bMiAaPQ 801 2$bMiAaPQ 906 $aBOOK 912 $a9910959314203321 996 $aBosons after symmetry breaking in quantum field theory$94468167 997 $aUNINA