42,023 research outputs found
God and the Argument from Consciousness: A Response to Lim
Recently, Daniel Lim has published a thoughtful critique of one form of my argument for the existence of God from consciousness (hereafter, AC).1 After stating his presentation of the relevant contours of my argument, I shall present the main components of his critique, followed by my response. Since one purpose of my publications of AC has been to foster discussion about a neglected argument for God’s existence, I am thankful to lim for his interesting article and the chance to further the discussion
Zombies, Epiphenomenalism and Personal Explanations: A Tension in Moreland's Argument from Consciousness
In his so-called argument from consciousness (AC), J. P. Moreland argues that the phenomenon of consciousness furnishes us with evidence for the existence of God. In defending AC, however, Moreland makes claims that generate an undesirable tension. This tension can be posed as a dilemma based on the contingency of the correlation between mental and physical states. The correlation of mental and physical states is either contingent or necessary. If the correlation is contingent then epiphenomenalism is true. If the correlation is necessary then a theistic explanation for the correlation is forfeit. Both are unwelcome results for A
MR1: an unconventional twist in the tail
MR1 is a conserved molecule that binds microbial vitamin B metabolites and presents them to unconventional T cells. Lim and colleagues (2022. J. Cell Biol.https://doi.org/10.1083/jcb.202110125) uncover the role of AP2 in ensuring MR1 surface presentation, which relies on an atypical motif within the MR1 cytoplasmic tail
On Jiang's asymptotic distribution of the largest entry of a sample correlation matrix
Let be a double array of nondegenerate
i.i.d. random variables and let be a sequence of
positive integers such that is bounded away from and .
This paper is devoted to the solution to an open problem posed in Li, Liu, and
Rosalsky (2010) on the asymptotic distribution of the largest entry of the
sample correlation matrix where denotes the
Pearson correlation coefficient between and . We show under the assumption
that the following three statements are equivalent: \begin{align*} & {\bf (1)}
\quad \lim_{n \to \infty} n^{2} \int_{(n \log n)^{1/4}}^{\infty} \left(
F^{n-1}(x) - F^{n-1}\left(\frac{\sqrt{n \log n}}{x} \right) \right) dF(x) = 0,
\\ & {\bf (2)} \quad \left ( \frac{n}{\log n} \right )^{1/2} L_{n}
\stackrel{\mathbb{P}}{\rightarrow} 2, \\ & {\bf (3)} \quad \lim_{n
\rightarrow \infty} \mathbb{P} \left (n L_{n}^{2} - a_{n} \leq t \right ) =
\exp \left \{ - \frac{1}{\sqrt{8 \pi}} e^{-t/2} \right \}, - \infty < t <
\infty \end{align*} where and , . To establish this result, we
present six interesting new lemmas which may be beneficial to the further study
of the sample correlation matrix.Comment: 16 page
A Quasi-Hopf algebra interpretation of quantum 3-j and 6-j symbols and difference equations
We consider the universal solution of the Gervais-Neveu-Felder equation in
the case. We show that it has a quasi-Hopf algebra
interpretation. We also recall its relation to quantum 3-j and 6-j symbols.
Finally, we use this solution to build a q-deformation of the trigonometric
Lam\'e equation.Comment: 9 pages, 4 figure
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