  Using the PDG 22 compilation of the $e^+e^-\to$ Hadrons $\oplus$ the recent
CMD3 data for the pion form factor and the value of gluon condensate $<\alpha_s
G^2>$ from heavy quarkonia, we extract the value of the four-quark condensate :
$\rho\alpha_s<\bar\psi\psi>^2= (5.98\pm 0.64)\times 10^{-4}$ GeV$^6$ and the
dimension eight condensate: $d_8= (4.3\pm 3.0)\times 10^{-2}$ GeV$^8$from the
ratio ${\cal R}_{10}$ of Laplace sum rules to order $\alpha_s^4$. We show the
inconsistency in using at the same time the standard SVZ value of the gluon and
the vacuum saturation of the four-quark condensates. Using the previous values
of the four-quark and $d_8$ condensates, we re-extract $<\alpha_s G^2>$ from
${\cal R}_{10}$ to be: $(6.12\pm 0.61)\times 10^{-2}$ GeV$^4$ in perfect
agreement with the one from heavy quarkonia. We also use the lowest $\tau$-like
decay moment ${\cal R}_\tau^{ee}$ to extract the value of the QCD coupling
$\alpha_s(M^2_\tau)$=0.3385(145)[resp. 0.3262(86)] (mean of fixed order (FO)
and Contour Improved (CI) PT series) to order $\alpha_s^4$ [resp. $\alpha_s^5$]
and the standard OPE. The corresponding value of the sum of the
non-perturbative contribution is: $\delta_{NP}(M_\tau)=(3.74\pm 0.40)\times
10^{-2}$. Reciprocally, using $\alpha_s(M_\tau)$, $<\alpha_s G^2>$ and $d_8$ as
inputs, we test the stability of the value of the four-quark condensate
obtained from the lowest $\tau$-like moment. We complete our analysis by
updating our previous determinations of the lowest order hadronic vacuum
polarization contributions to the lepton anomalies and to $\alpha(M^2_Z)$. We
obtain in Table 2 : $a_\mu\vert^{hvp}_{l.o}= (7036.5\pm 38.9)\times10^{-11},
a_\tau\vert^{hvp}_{l.o}= (3494.8\pm 24.7)\times10^{-9} $ and
$\alpha(M^2_Z)=(2766.3\pm 4.5)\times 10^{-5}$. This new value of $a_\mu$ leads
to: $\Delta a_\mu\equiv a_\mu^{exp}-a_\mu^{th} = (142\pm 42_{th}\pm
41_{exp})\times 10^{-11}$.

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