LEADER 02266nam 2200529 a 450 001 9910810009103321 005 20230725024526.0 010 $a90-485-1312-X 035 $a(CKB)2670000000034702 035 $a(EBL)564074 035 $a(OCoLC)657112389 035 $a(SSID)ssj0000418321 035 $a(PQKBManifestationID)12130778 035 $a(PQKBTitleCode)TC0000418321 035 $a(PQKBWorkID)10369969 035 $a(PQKB)10866440 035 $a(MiAaPQ)EBC564074 035 $a(Au-PeEL)EBL564074 035 $a(CaPaEBR)ebr10405014 035 $a(EXLCZ)992670000000034702 100 $a20100823d2010 uy 0 101 0 $aeng 135 $aur|n|---||||| 181 $ctxt 182 $cc 183 $acr 200 10$aFundamentals of the pure spinor formalism$b[electronic resource] /$fJoost Hoogeveen 210 $aAmsterdam $cAmsterdam University Press$d2010 215 $a1 online resource (180 p.) 225 1 $aUvA-proefschriften 300 $aDescription based upon print version of record. 311 $a90-5629-641-8 320 $aIncludes bibliographical references. 327 $aContents; Preface; 1. String theory; 2. Pure spinor formalism; 3. Basic techniques; 4. BRST quantisation of the pure spinor superstring; 5. Decoupling of unphysical states; 6. Discussion and conclusion; Appendix A; Bibliography; Samenvatting; Acknowledgments 330 $aThis thesis presents recent developments within the pure spinor formalism, which has simplified amplitude computations in perturbative string theory, especially when spacetime fermions are involved. Firstly the worldsheet action of both the minimal and the non-minimal pure spinor formalism is derived from first principles, i.e. from an action with two dimensional diffeomorphism and Weyl invariance. Secondly the decoupling of unphysical states in the minimal pure spinor formalism is proved. 410 0$aUvA-proefschriften 606 $aSpinor analysis 615 0$aSpinor analysis. 676 $a531/.14 700 $aHoogeveen$b Joost$01620342 801 0$bMiAaPQ 801 1$bMiAaPQ 801 2$bMiAaPQ 906 $aBOOK 912 $a9910810009103321 996 $aFundamentals of the pure spinor formalism$93953053 997 $aUNINA