FIGURE 2. Isotropic magnetic field effects on C–P–F.

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

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Transient absorption data recorded for frozen solutions of C–P–F showing the magnetic field-dependence of the recombination of the radical pair state, [ C bullet+–P–F bullet-] . Apart from the upper part of a, all data are field-on minus field-off differences: A(B0) - A(0). a, Top: absorption with and without an 8-mT applied field at 133 K. Bottom: difference signals as a function of temperature. All signals rise with the instrumental time constant (approx50 ns). b, Changes in the transient absorption of [ C bullet+–P–F bullet-] at 119 K averaged over a 50-ns period centred at 100 ns and 400 ns after its formation. c, Changes in the transient absorption of [ C bullet+–P–F bullet-] at 113 K caused by 39-muT and 49-muT applied magnetic fields. Error bars, plusminus1 s.d.

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