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Search for the Rare Decays B-s(0) -> e(+) e(-) and B-0 -> e(+) e(-)

Iodination ofcyclo-E-5-Complexes (E=P, As)

Search for the semileptonic decay D0(+) -> b(1) (1235)(-(0))e(+)v(e)

Hurwitz generation in groups of types F-4, E-6, E-2(6), E-7 and E-8

a, b,1,**, c, 1, d, a, c, b, c, b, e, e,, c,, b, e, **

Subleading logarithmic QED initial state corrections to e plus e ? ? ? * /Z 0*to O(? 6 L 5 )

Subleading logarithmic QED initial state corrections to e plus e ? ? ? * /Z 0*to O(? 6 L 5 )

The key particle and quark energy equality E-W + E-Z 5 E-top

(E)-3-(2,5-Dimethoxyphenyl)-1-{[4-(2,5-dimethoxy-phenyl)-6-((E)-2,5-dimethoxystyryl)-2-thioxo-1,2,3,4-tetrahydropyrimidin-5-yl]}prop-2-en-1-one and (E)-3-(2,5-Dimethoxyphenyl)-1-{[4-(2,5-dimethoxyphenyl)-6-methyl-2-thioxo-1,2,3,4-tetrahydropyrimidin-5-yl]

Decays h -> e(a) e(b), e(b) -> e(a)gamma, and (g-2)(e,mu) model with inverse seesaw neutrinos

Characterization and enumeration of reflectable bases of types E-6,E- 7,E- 8

Dynkin types B-n, C-n, F-4, g(2), E-6, E-7, E-8

The VOAs generated by two Ising vectors e and f with < e, f >=1/2(8), vertical bar tau(e)tau(f)verticalbar=3 or < e, f >=3/2(9)

Uninorms continuous on [0, e[U-2]e, 1](2)

) 5 8 0-5 9 3

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