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Salgado answered a few questions from LongHash prior to being elected as the President of the Bitcoin Foundation. The “pulling out of four other nominees” was Salgado’s primary concern when making the decision to sign up to be a candidate for the new position.

LongHash: Your company, BPC, is one of the founding members of the Bitcoin Foundation. Does your experience as an operator of Bitcoin businesses mean that you have a unique perspective on working within the foundation?

Ricardo Salgado: My experience as a founder of some of the first Bitcoin exchanges in Europe, which is also the country with the biggest Bitcoin market, including the first

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Thanks for browsing our website. The magnetic field energy density $w_B$ can also be expressed in terms of the Hubble parameter $H$ [@Hodzas:2015zaa]: \begin{aligned} w_B \approx (\textrm{e}^{ -2N}-1)H^2\,.\end{aligned} Inserting the numerical values we find \begin{aligned} \label{eq:DW2} w_B \approx \left(-7.99 \cdot 10^{ -4} -9.19\cdot 10^{ -5} + \frac{0.5384}{N} \right)H^2\,.\end{aligned} Clearly, the dark energy equation of state parameter given by equation may be driven to a negative value for certain values of $N$. However, when the gauge parameter is close to $\eta = 10$, the coupling becomes small and the effect of the extra dimensions is suppressed. For example, if we take the gauge parameter to be $\eta = 9$ and the extra dimensions $N$ to be $N = 1$, $N = 2$ and $N = 3$, we find the following numerical values for the dark energy equation of state parameter \begin{aligned} w_{B,1} = \frac{0.000023 – 0.000037}{H^2}\,,\, w_{B,2} = \frac{0.000043 – 0.000063}{H^2}\,,\, w_{B,3} = \frac{0.000074 – 0.000144}{H^2}\,.\end{aligned} In view of this, we note that the present model may provide us with a cosmologically viable setup if the extra dimensions are large. This is clear from the plots presented in figure \[