eljose
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hello i would like to open this post to recommend the english journal "Journal of Physics:A General mathematics", they have published my article in spite of me being a non-english speaker,they accept paper in .doc (Microsoft Word) format, when i give me the web address for my article i will put it in the forum...in fct is about RH i find an operator
H=cD^{2}+V(x) so all its eigenvalues are the roots of \zeta(a+is) where the potential can be written to first order in the form:
V(x)=\int_{-\infty}^{\infty}dnR(n,x)\delta{E(n)}
with E_n the roots of \zeta(a+is) so the potential will depend also on a,for a different from 1/2 we have complex energies in the form E*_{n}+(2a-1)i so the potential is complex and a complex potential can not have real roots then necessarily all the roots of \zeta(a+is) have real part a=1/2
H=cD^{2}+V(x) so all its eigenvalues are the roots of \zeta(a+is) where the potential can be written to first order in the form:
V(x)=\int_{-\infty}^{\infty}dnR(n,x)\delta{E(n)}
with E_n the roots of \zeta(a+is) so the potential will depend also on a,for a different from 1/2 we have complex energies in the form E*_{n}+(2a-1)i so the potential is complex and a complex potential can not have real roots then necessarily all the roots of \zeta(a+is) have real part a=1/2
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