Self-Reduction Rate of a Microtubule
Takashi Hiramatsu, Tetsuo Matsui, Kazuhiko Sakakibara
arXiv Preprint Archive February 17, 2006 via arXiv
Summary
AI-generated from the abstractA quantum field theory of microtubules—basic components of living cells—is formulated and studied, building on Hameroff and Penrose's quantum theory of consciousness. The system is allowed to reduce to a classical state without measurement (self-reduction) under certain conditions, and the self-reduction time τ_N (the mean interval between successive self-reductions) is calculated for clusters of more than N neighboring tubulins. For large electron hopping amplitudes, τ_N follows a power law τ_N ∼ N^b, explained by percolation theory; for small hopping amplitudes, it follows an exponential law τ_N ∼ exp(c' N). Using this law, the condition for τ_N to be at least 0.1 seconds requires N to be at least about 1000.
Study at a glance
| Characteristics | Theoretical or philosophical paper Peer reviewed |
|---|---|
| Keywords | Quant-ph Q-bio.nc Q-bio.sc |
| Key finding | The self-reduction time τ_N of a microtubule tubulin cluster follows a power law for large electron hopping amplitudes and an exponential law for small amplitudes, with realistic timescales (≥0.1 s) requiring clusters of at least about 1000 tubulins. |
Abstract
We formulate and study a quantum field theory of a microtubule, a basic element of living cells. Following the quantum theory of consciousness by Hameroff and Penrose, we let the system to reduce to one of the classical states without measurement if certain conditions are satisfied(self-reductions), and calculate the self-reduction time $τ_N$ (the mean interval between two successive self-reductions) of a cluster consisting of more than $N$ neighboring tubulins (basic units composing a microtubule). $τ_N$ is interpreted there as an instance of the stream of consciousness. We analyze the dependence of $τ_N$ upon $N$ and the initial conditions, etc. For relatively large electron hopping amplitude, $τ_N$ obeys a power law $τ_N \sim N^b$, which can be explained by the percolation theory. For sufficiently small values of the electron hopping amplitude, $τ_N$ obeys an exponential law, $τ_N \sim \exp(c' N)$. By using this law, we estimate the condition for $τ_N $ to take realistic values $τ_N$ \raisebox{-0.5ex}{$\stackrel{>}{\sim}$} $10^{-1}$ sec as $N$ \raisebox{-0.5ex} {$\stackrel{>}{\sim}$} 1000.