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Remarks on M-theory coupling constants and M-brane tension quantizations

In the absence of a complete M-theory, we gather certain quantum aspects of this theory, namely, M-2 and M-5 brane duality and their tension quantization rule $2κ^2 T_2 T_5 = 2 πn$, the M-2 brane tension quantization $T_2 =\bigg({(2π)^2/2κ^2 m}\bigg)^{1/3}$, supersymmetry, perturbative gauge and gravitational anomaly cancellations, and the half-integral quantization of [$G^W/2π$], and study the consistency among these quantum effects. We find: (1) The complete determination of Hourava-Witten's $η= λ^6 /κ^4$ for M-theory on $R^{10} \times S^1/ Z_2$ requires not only the cancellation of M-theory gauge anomaly but also that of the gravitational anomaly, the quantization of M-2 brane tension, and the recently recognized half-integral quantization of $[G^W / 2 π]$. (2) A well-defined quantum M-theory necessarily requires the presence of both M-2 and M-5 branes and allows only $n = 1$ and $m =1$ for the respectively quantized M-2 and M-5 brane tensions. Implications of the above along with other related issues are discussed.