... g
m
(ζ))
b
a+deg
z,∞
a
r
m
{b
a+deg
z,∞
a
r
m
1
m
2
qk−p(r)
m
ρ
m
}
m
1
m
2
qk−p(r)
M
r
[g
m
](ζ).
(3.11)
11
3. Proof of the results
Proof of Theorem 1.4 Suppose that the conclusion of theorem is not true, then
there exists an entire solution w(z) satisfies the equation [Q(w(z))]
n
= ... YL and WY participated dis-
cussion and corrected the main theorem. All authors read and...
... and delocalize
the negative charge of the triphosphate moiety of
ATP, which is in close proximity to the negatively
charged carboxylate group of the amino acid sub-
strate [21]. The binding of ... with
the cognate tRNA. Because of the similar size of the
motif 2 loop in methanogenic-type SerRS and ThrRS
and the involvement of zinc ions in the recognit...
... with the polarity of the material and that the inhomogeneous broadening in Г
inh
may be accounted for implicitly and partly by the presence of various site symmetries of
the Mn
2+
ion in the ... x. The change of the band-gap energy E
g
with temperature is usually
attributed to the effect of electrons or phonons. The electron-hole pair is believed to
sof...
... unknown.
The purpose of this article is to study and establish the ASCLT for self-normalized partial sums of random variables
in the domain of attraction of the normal law, we will show that the ASCLT ... the domain of attraction of the normal law. Therefore, the class of random
variables in Theorems 1.1 is of very broad range.
Remark 1.5. Essentially, the...