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Highly interesting solutions in mathematical physics
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la p SLG IC (^) GL 2 E (^) Ato A und
SLG a^ GLC2 A to A^ SCAB AB (^) PCA (^) PCB and^ f CAB AT
i (^) k A^ B lb det^
(^213) yd I^ D^213 1 2 13 It^15 Take (^) for example in A Ri
t (^) P2 I t^2 1 But
Using (^10) CP Q 7 CF Q2^ ftp.E
P
must be^
(^1913 ) BQ 2103 151oz^2 Choose (^19 0 ) so
l T cgkn.IR
aijbjk aijbjk 0 if K^ j o i j and 0 if i^ j so if ke^ i^ V Dwp Vn^ is^ closed Pwof His (^) closed component
coast (^) and (^0) below and^
2b (^) Lic (^) Vn T Vz (^) y C I^ l^ Vn Ko (^1) So we X O^ Idf Xy I^ o
path Jt
It At^ O (^) i f so all (^) strict (^) triangular Since (^) this also works (^) for any (^) path we
the above
log Nth (^) finite Sum So^ there (^) exists a^ logarithm and^ theres
3ap SU (^3) GUV p dat Ito plexptx dat It exptu
exp C tu^ Ux^ Xu EU X
Sueur Guna and decoup into (^) parts
