LEADER 04047nam 2200601 a 450 001 9910452372803321 005 20200520144314.0 010 $a1-299-46283-9 010 $a981-4478-81-4 035 $a(CKB)2550000001019266 035 $a(EBL)1168192 035 $a(OCoLC)840496752 035 $a(SSID)ssj0001425604 035 $a(PQKBManifestationID)11834232 035 $a(PQKBTitleCode)TC0001425604 035 $a(PQKBWorkID)11380359 035 $a(PQKB)11598746 035 $a(MiAaPQ)EBC1168192 035 $a(WSP)00003015 035 $a(Au-PeEL)EBL1168192 035 $a(CaPaEBR)ebr10691867 035 $a(CaONFJC)MIL477533 035 $a(EXLCZ)992550000001019266 100 $a20130507d2013 uy 0 101 0 $aeng 135 $aur|n|---||||| 181 $ctxt 182 $cc 183 $acr 200 00$aThree-particle physics and dispersion relation theory$b[electronic resource] /$fA.V. Anisovich ... [et al.] 210 $a[Hackensack] N.J. $cWorld Scientific$dc2013 215 $a1 online resource (342 p.) 300 $aDescription based upon print version of record. 311 $a981-4478-80-6 320 $aIncludes bibliographical references. 327 $aPreface; References; Contents; 8.4.5 Overlapping of baryon resonances; 1. Introduction; 1.1 Non-relativistic three-nucleon and three-quark systems; 1.1.1 Description of three-nucleon systems; 1.1.2 Three-quark systems; 1.2 Dispersion relation technique for three particle systems; 1.2.1 Elements of the dispersion relation technique for two-particle systems; 1.2.2 Interconnection of three particle decay amplitudes and two-particle scattering ones in hadron physics; 1.2.3 Quark-gluon language for processes in regions I, III and IV; 1.2.4 Spectral integral equation for three particles 327 $a1.2.5 Isobar models1.2.5.1 Amplitude poles; 1.2.5.2 D-matrix propagator for an unstable particle and the K matrix amplitude; 1.2.5.3 K-matrix and D-matrix masses and the amplitude pole; 1.2.5.4 Accumulation of widths of overlapping resonances; 1.2.5.5 Loop diagrams with resonances in the intermediate states; 1.2.5.6 Isobar model for high energy peripheral production processes; 1.2.6 Quark-diquark model for baryons and group theory approach; 1.2.6.1 Quark-diquark model for baryons; References; 2. Elements of Dispersion Relation Technique for Two-Body Scattering Reactions 327 $a2.2.2 Scattering amplitude and energy non-conservation in the spectral integral representation2.2.3 Composite system wave function and its form factors; 2.2.4 Scattering amplitude with multivertex representation of separable interaction; 2.2.4.1 Generalization for an arbitrary angular momentum state, L = J; 2.3 Instantaneous interaction and spectral integral equation for two-body systems; 2.3.1 Instantaneous interaction; 2.3.1.1 Coordinate representation; 2.3.1.2 Instantaneous interaction - transformation into a set of separable vertices 330 $aThe necessity of describing three-nucleon and three-quark systems have led to a constant interest in the problem of three particles. The question of including relativistic effects appeared together with the consideration of the decay amplitude in the framework of the dispersion technique. The relativistic dispersion description of amplitudes always takes into account processes connected with the investigated reaction by the unitarity condition or by virtual transitions; in the case of three-particle processes they are, as a rule, those where other many-particle states and resonances are produc 606 $aParticles (Nuclear physics) 606 $aDispersion relations 608 $aElectronic books. 615 0$aParticles (Nuclear physics) 615 0$aDispersion relations. 676 $a539.725 701 $aAnisovich$b A. V$0956301 801 0$bMiAaPQ 801 1$bMiAaPQ 801 2$bMiAaPQ 906 $aBOOK 912 $a9910452372803321 996 $aThree-particle physics and dispersion relation theory$92165265 997 $aUNINA LEADER 00913nam a2200265 i 4500 001 991001640539707536 005 20020502203527.0 008 950403s1985 it ||| | ita 035 $ab11542470-39ule_inst 035 $aPRUMB65007$9ExL 040 $aDip. 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