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Fig. 4.5 Readouts for the porphyrin-functionalised holographic metal ion sensor. a, b The
shrinkage of the pHEMA-co-TACPP matrix due to Donnan osmotic pressure (dominant) and the
chelation effect at 24 ° C in citric acid-Na 2 HPO 4 buffers. c Blue Bragg shifts due to metal cation
chelation. The sensor displays a higher blue Bragg shifts for Cu 2+ and Fe 2+ cations than
monovalent and other divalent cations at 1.0 M. d Blue Bragg shifts as a function of Cu 2+ and Fe 2+
cation concentrations. Reproduced from Ref. [ 1 ] with permission from The Royal Society of
Chemistry
s response to Cu 2+ and Fe 2+ ions with 200 mM increments was mea-
sured over three trials (Fig. 4.5 d). The stability constant of the cavity of TACPP
with cations depends on the chelate effect (entropy) [ 22 ], macrocyclic effect [ 23 ],
geometrical factors [ 24 ], classi
The sensor
'
cation of donor atoms [ 25 ] and ionic radius [ 26 ].
For example, Cu 2+ ions have a greater capacity to bind to the cavity of TACPP than
other cations [ 26 ]. In terms of response time, for example, a variation in Cu 2+ ion
concentration from 0 to 200 mM, followed by the rinsing step, required
30 s to
*
equilibrate (
±
sub nm). The sensor response was reversible without hysteresis.
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