FIGURE 1. C–P–F triad.
From the following article:
Chemical compass model of avian magnetoreception
Kiminori Maeda, Kevin B. Henbest, Filippo Cintolesi, Ilya Kuprov, Christopher T. Rodgers, Paul A. Liddell, Devens Gust, Christiane R. Timmel & P. J. Hore
Nature 453, 387-390(15 May 2008)
doi:10.1038/nature06834

Structure (top) and reaction scheme (bottom) of the C–P–F triad used to demonstrate the principle of a chemical compass. The interconversion of the singlet (S) and triplet (T) states of the radical pair [
C
+–P–F
-]
is driven by magnetic hyperfine interactions and is modulated by the Zeeman interaction with an external magnetic field. [
C
+–P–F
-]
can recombine spin-selectively, with rate constants kS and kT. As the hyperfine interactions are anisotropic, and kS
kT, the lifetime of the radical pair reaction depends on its orientation with respect to the external magnetic field. The inset at top left is a representation of the anisotropic hyperfine interactions in C
+; 22 of the 46 protons in this radical have isotropic hyperfine couplings larger than 100
T. F
-, by contrast, is almost devoid of hyperfine couplings. h
: light excitation.
