Regularized trace formula of magic Gribov operator on Bargmann space
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In this article, we obtain a regularized trace formula for magic Gribov operator ve&_eid=1-s2.0-S0022247X15011920&_mathId=si1.gif&_user=111111111&_pii=S0022247X15011920&_rdoc=1&_issn=0022247X&md5=384f537b5983aa92ee1eac1dbae93640" title="Click to view the MathML source">H=λG+Hμ,λ acting on Bargmann space wherev class="formula" id="fm0010">v class="mathml">ve&_eid=1-s2.0-S0022247X15011920&_mathId=si2.gif&_user=111111111&_pii=S0022247X15011920&_rdoc=1&_issn=0022247X&md5=f380886b51c9eaa60c80fc6cf917c0b7">View the MathML sourcev>v> Here a   and ve&_eid=1-s2.0-S0022247X15011920&_mathId=si3.gif&_user=111111111&_pii=S0022247X15011920&_rdoc=1&_issn=0022247X&md5=c5256264648556ac692696b4b789653d" title="Click to view the MathML source">a are the standard Bose annihilation and creation operators and in Reggeon field theory, the real parameters ve&_eid=1-s2.0-S0022247X15011920&_mathId=si4.gif&_user=111111111&_pii=S0022247X15011920&_rdoc=1&_issn=0022247X&md5=1183e80886822c7793c8bd27adee64ea" title="Click to view the MathML source">λ is the magic coupling of Pomeron, μ is Pomeron intercept, λ   is the triple coupling of Pomeron and ve&_eid=1-s2.0-S0022247X15011920&_mathId=si5.gif&_user=111111111&_pii=S0022247X15011920&_rdoc=1&_issn=0022247X&md5=5c66b4b250bebab77b11c21e584a8d38" title="Click to view the MathML source">i2=−1. By applying some abstract results of Sadovnichii–Podol'skii (2002) [23], we give the number of corrections sufficient for the existence of finite formula of the trace of concrete magic Gribov's operator.

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