scholarly journals The envelope of holomorphy of a classical truncated tube domain

Author(s):  
Marek Jarnicki ◽  
Peter Pflug

2006 ◽  
Vol 16 (1) ◽  
pp. 167-185
Author(s):  
Fatiha Sahraoui


2008 ◽  
Vol 259 (3) ◽  
pp. 697-711 ◽  
Author(s):  
Hideyuki Ishi ◽  
Takaaki Nomura
Keyword(s):  


2013 ◽  
Vol 65 (4) ◽  
pp. 495-514
Author(s):  
Satoru Shimizu


2008 ◽  
Vol 53 (4) ◽  
pp. 307-309
Author(s):  
Linus Carlsson ◽  
Anders Fällström


1986 ◽  
Vol 273 (2) ◽  
pp. 199-207 ◽  
Author(s):  
Sandra Hayes ◽  
Genevi�ve Pourcin


1958 ◽  
Vol 54 (3) ◽  
pp. 377-382 ◽  
Author(s):  
J. G. Taylor

In the last few years it has been found useful to apply known theorems in the theory of functions of several complex variables to solve problems arising in the quantum theory of fields (11). In particular, in order to derive the dispersion relations of quantum field theory from the general postulates of that theory it appears useful to apply known theorems on holomorphic continuation for functions of several complex variables ((2), (10)). The most important theorems are those which enable a determination to be made of the largest domain to which every function which is holomorphic in a domain D may be continued. This domain is called the envelope of holomorphy of D, and denoted by E(D). If D = E(D) then D is termed a domain of holomorphy. E(D) may be defined as the smallest domain of holomorphy containing D. Only in the special cases that D is a tube, semi-tube, Hartogs, or circular domain has it been possible to determine the envelope of holomorphy E(D) ((3), (7)). An iterative method for the computation of envelopes of holomorphy has recently been given by Bremmerman(4). It is also possible to use the continuity theorem (1) in a direct manner, though in most cases this is exceedingly difficult.





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