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1
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33745606358
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For a review on PMO materials, Angew. Chem. 2006, 118, 3290-3328
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For a review on PMO materials, see: F. Hoffmann, M. Cornelius, J. Morell, M. Fröba, Angew. Chem. Int. Ed. 2006, 45, 3216-3251. Angew. Chem. 2006, 118, 3290-3328.
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(2006)
Angew. Chem. Int. Ed.
, vol.45
, pp. 3216-3251
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Hoffmann, F.1
Cornelius, M.2
Morell, J.3
Fröba, M.4
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2
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0029733122
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The LPG is prepared by modifying a small length of a single-mode fiber-optic cable (SMF) so that the refractive index (RI) of its core is changed periodically, with a repeat distance on the order of hundreds of micrometers. See
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The LPG is prepared by modifying a small length of a single-mode fiber-optic cable (SMF) so that the refractive index (RI) of its core is changed periodically, with a repeat distance on the order of hundreds of micrometers. See: A. M. Vengsarkar, P. J. Lemaire, J. B. Judkins, V. Bhatia, T. Erdogan, J. E. Sipe, J. Lightwave Technol. 1996, 14, 58-65.
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(1996)
J. Lightwave Technol.
, vol.14
, pp. 58-65
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Vengsarkar, A.M.1
Lemaire, P.J.2
Judkins, J.B.3
Bhatia, V.4
Erdogan, T.5
Sipe, J.E.6
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4
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77953156704
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f). This results in a spectrum, exemplified in Figure 1, in which the resonant wavelengths appear as attenuation peaks. For more details, see References [2] and [3]
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f). This results in a spectrum, exemplified in Figure 1, in which the resonant wavelengths appear as attenuation peaks. For more details, see References [2] and [3].
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5
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77953172324
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As the RI of the external environment approaches that of the cladding (1.44), the LPG's sensitivity to RI changes is maximized due to increased extension of the evanescent wave past the cladding-ambient interface into the external medium. For example, changing the external medium from air (RI=1.000) to a solution of RI=1.372 (ΔRI=0.372 at 1550 nm) results in a resonant peak shift towards shorter wavelengths of 4.2 nm. However, a more pronounced shift of 24.6nm is observed for a much smaller change in RI from 1.372 to 1.417 (ΔRI=0.045) as the external index approaches the RI of the fiber cladding (see Figure 1)
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As the RI of the external environment approaches that of the cladding (1.44), the LPG's sensitivity to RI changes is maximized due to increased extension of the evanescent wave past the cladding-ambient interface into the external medium. For example, changing the external medium from air (RI=1.000) to a solution of RI=1.372 (Delta;RI=0.372 at 1550 nm) results in a resonant peak shift towards shorter wavelengths of 4.2 nm. However, a more pronounced shift of 24.6nm is observed for a much smaller change in RI from 1.372 to 1.417 (Delta;RI=0.045) as the external index approaches the RI of the fiber cladding (see Figure 1).
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6
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54249148007
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For example
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For example: a) J. Barnes, M. Dreher, K. Plett, R. S. Brown, C. M. Crudden, H.-P. Loock, Analyst 2008, 133, 1541-1549.
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(2008)
Analyst
, vol.133
, pp. 1541-1549
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Barnes, J.1
Dreher, M.2
Plett, K.3
Brown, R.S.4
Crudden, C.M.5
Loock, H.-P.6
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7
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57949092827
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J. Zhang, X. Tang, J. Dong, T. Wei, H. Xiao, Sens. Actuators B 2009, 135, 420-425.
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(2009)
Sens. Actuators B
, vol.135
, pp. 420-425
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Zhang, J.1
Tang, X.2
Dong, J.3
Wei, T.4
Xiao, H.5
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8
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54249137686
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C. Caucheteur, M. Debliquy, D. Lahem, P. Mégret, Opt. Express 2008, 16, 16854-16859.
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(2008)
Opt. Express
, vol.16
, pp. 16854-16859
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Caucheteur, C.1
Debliquy, M.2
Lahem, D.3
Mégret, P.4
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9
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0042281753
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P. S. Kumar, C. P. G. Vallabhan, V. P. N. Nampoori, P. Radhakrishnan, Proc. SPIE Int. Soc. Opt. Eng. 2003, 5116, 348-352.
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(2003)
Proc. SPIE Int. Soc. Opt. Eng.
, vol.5116
, pp. 348-352
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Kumar, P.S.1
Vallabhan, C.P.G.2
Nampoori, V.P.N.3
Radhakrishnan, P.4
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10
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0035871659
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R. Falciai, A. G. Mignani, A. Vannini, Sens. Actuators B 2001, 74, 74-77.
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(2001)
Sens. Actuators B
, vol.74
, pp. 74-77
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Falciai, R.1
Mignani, A.G.2
Vannini, A.3
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11
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0035478961
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K. Zhou, H. Liu, X. Hu, Opt. Commun. 2001, 197, 295-299.
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(2001)
Opt. Commun.
, vol.197
, pp. 295-299
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Zhou, K.1
Liu, H.2
Hu, X.3
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12
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0032628671
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C. J. Brinker, Y. Lu, A. Sellinger, H. Fan, Adv. Mater. 1999, 11, 579-585.
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(1999)
Adv. Mater.
, vol.11
, pp. 579-585
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Brinker, C.J.1
Lu, Y.2
Sellinger, A.3
Fan, H.4
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16
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77953148218
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Thin-film coatings prepared from a sol of the same composition as used for preparing thick films did not induce any observable changes in the LPG's sensitivity to variations in the RI of the surrounding environment above what was measured for a bare, uncoated LPG
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Thin-film coatings prepared from a sol of the same composition as used for preparing thick films did not induce any observable changes in the LPG's sensitivity to variations in the RI of the surrounding environment above what was measured for a bare, uncoated LPG.
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18
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0032208977
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Sol-preparation procedure adapted from
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Sol-preparation procedure adapted from: D. Zhao, P. Yang, N. Melosh, J. Feng, B. F. Chmelka, G. D. Stucky, Adv. Mater. 1998, 10, 1380-1385.
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(1998)
Adv. Mater.
, vol.10
, pp. 1380-1385
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Zhao, D.1
Yang, P.2
Melosh, N.3
Feng, J.4
Chmelka, B.F.5
Stucky, G.D.6
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19
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0037245296
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L. Zhang, W. Zhang, J. Shi, Z. Hua, Y. Li, J. Yan, Chem. Commun. 2003, 210-211.
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(2003)
Chem. Commun.
, pp. 210-211
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Zhang, L.1
Zhang, W.2
Shi, J.3
Hua, Z.4
Li, Y.5
Yan, J.6
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20
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77953155202
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Although the coating primarily consists of silica, which has an RI similar to the cladding, the introduction of porosity results in an overall decrease of the RI of the coating. TTIP was added as a dopant in order raise the RI of the overlay, further minimizing the difference in RI between the PMO film and the fiber cladding. See Reference [5]
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Although the coating primarily consists of silica, which has an RI similar to the cladding, the introduction of porosity results in an overall decrease of the RI of the coating. TTIP was added as a dopant in order raise the RI of the overlay, further minimizing the difference in RI between the PMO film and the fiber cladding. See Reference [5].
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21
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40049111883
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For reviews
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For reviews, see: a) C. Sanchez, C. Boissière, D. Grosso, C. Laberty, L. Nicole, Chem. Mater. 2008, 20, 682-737.
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(2008)
Chem. Mater.
, vol.20
, pp. 682-737
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Sanchez, C.1
Boissière, C.2
Grosso, D.3
Laberty, C.4
Nicole, L.5
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23
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0030881278
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Y. Lu, R. Ganguli, C. A. Drewien, M. T. Anderson, C. J. Brinker, W. Gong, Y. Guo, H. Soyez, B. Dunn, M. H. Huang, J. I. Zink, Nature 1997, 389, 364-368.
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(1997)
Nature
, vol.389
, pp. 364-368
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Lu, Y.1
Ganguli, R.2
Drewien, C.A.3
Anderson, M.T.4
Brinker, C.J.5
Gong, W.6
Guo, Y.7
Soyez, H.8
Dunn, B.9
Huang, M.H.10
Zink, J.I.11
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24
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33750379878
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L. C. Huang, E. K. Richman, B. L. Kirsch, S. H. Tolbert, Microporous Mesoporous Mater. 2006, 96, 341-349.
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(2006)
Microporous Mesoporous Mater
, vol.96
, pp. 341-349
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Huang, L.C.1
Richman, E.K.2
Kirsch, B.L.3
Tolbert, S.H.4
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26
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0033821358
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D. Grosso, A. R. Balkenende, P. A. Albouy, M. Lavergne, L. Mazerolles, F. Babonneau, J. Mater. Chem. 2000, 10, 2085-2089.
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(2000)
J. Mater. Chem.
, vol.10
, pp. 2085-2089
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Grosso, D.1
Balkenende, A.R.2
Albouy, P.A.3
Lavergne, M.4
Mazerolles, L.5
Babonneau, F.6
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27
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42649084371
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T. Maruo, S. Tanaka, H. W. Hillhouse, N. Nishiyama, Y. Egashira, K. Ueyama, Thin Solid Films 2008, 516, 4771-4776.
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(2008)
Thin Solid Films
, vol.516
, pp. 4771-4776
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Maruo, T.1
Tanaka, S.2
Hillhouse, H.W.3
Nishiyama, N.4
Egashira, Y.5
Ueyama, K.6
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Ellipsometric porosimetry experiments were attempted on PMO films dip coated onto silicon substrates in order to further characterize the material's porous properties. Unfortunately, these thick films did not give satisfactory isotherms - likely due to the film nonuniformity exceeding the tolerance of this characterization technique. However, the nitrogen porosimetry data for the large batch of scraped films (presented in Figure S2) are expected to be a reasonable alternative to the ellipsometric porosimetry data
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Ellipsometric porosimetry experiments were attempted on PMO films dip coated onto silicon substrates in order to further characterize the material's porous properties. Unfortunately, these thick films did not give satisfactory isotherms - likely due to the film nonuniformity exceeding the tolerance of this characterization technique. However, the nitrogen porosimetry data for the large batch of scraped films (presented in Figure S2) are expected to be a reasonable alternative to the ellipsometric porosimetry data.
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Higher tetrasulfide loadings did not provide increased sensitivity
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Higher tetrasulfide loadings did not provide increased sensitivity.
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77953141453
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Although the ellipsometric porosimetry yielded unsatisfactory results for the thick films, the modeled RI of a thin film (average thickness of 500 nm) prepared using a sol of the same composition as the thick films was averaged over three experiments with different adsorbates to be 1.391 (at 633 nm)
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Although the ellipsometric porosimetry yielded unsatisfactory results for the thick films, the modeled RI of a thin film (average thickness of 500 nm) prepared using a sol of the same composition as the thick films was averaged over three experiments with different adsorbates to be 1.391 (at 633 nm).
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DMSO was chosen as the modifying solvent due to its high water miscibility and its relatively high RI, which allows for the evaluation and calibration of the sensor responsivity over a larger RI range
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DMSO was chosen as the modifying solvent due to its high water miscibility and its relatively high RI, which allows for the evaluation and calibration of the sensor responsivity over a larger RI range.
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This is due to the fact that the RI of the area surrounding the LPG is now a composite RI of both the condensed matrix of the coating and the solution medium. In contrast, the RI of the area surrounding an uncoated grating comprises only the solution RI, which is often lower than the RI of the skeleton of the film. Thus a higher RI solution is required to induce significant peak shifts in the attenuation spectra for the uncoated LPG
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This is due to the fact that the RI of the area surrounding the LPG is now a composite RI of both the condensed matrix of the coating and the solution medium. In contrast, the RI of the area surrounding an uncoated grating comprises only the solution RI, which is often lower than the RI of the skeleton of the film. Thus a higher RI solution is required to induce significant peak shifts in the attenuation spectra for the uncoated LPG.
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77953146897
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This particular set of Pb(II) uptake data was collected in aqueous DMSO solutions with RI 1/4 1.402 (at 1550 nm) (28 mol% DMSO)
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This particular set of Pb(II) uptake data was collected in aqueous DMSO solutions with RI 1/4 1.402 (at 1550 nm) (28 mol% DMSO).
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Although the sensor selectivity remains to be explored in greater detail, under identical conditions, no response was observed to a mixture of metals including 10 ppm each of Cd(II), Co(II), Ni(II), Fe(II), and Zn(II). Hg(II) could not be tested under the same conditions due to its limited solubility in the solution medium. However, under acidic conditions, the optical response to Hg(II) was less than 10% of that observed for Pb(II). The effects of pH, metal-ligand binding affinity, and metal polarizability are currently under investigation
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Although the sensor selectivity remains to be explored in greater detail, under identical conditions, no response was observed to a mixture of metals including 10 ppm each of Cd(II), Co(II), Ni(II), Fe(II), and Zn(II). Hg(II) could not be tested under the same conditions due to its limited solubility in the solution medium. However, under acidic conditions, the optical response to Hg(II) was less than 10% of that observed for Pb(II). The effects of pH, metal-ligand binding affinity, and metal polarizability are currently under investigation.
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In an ideal scenario, this Pb(II) detection could be carried out in a purely aqueous medium. However, a predilution of a test sample with the requisite amount of DMSO could easily be accomplished in the field with a simple pump, which we argue is easier than currently employed off-site measurement techniques such as inductively coupled plasma mass spectrometry (ICP-MS)
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In an ideal scenario, this Pb(II) detection could be carried out in a purely aqueous medium. However, a predilution of a test sample with the requisite amount of DMSO could easily be accomplished in the field with a simple pump, which we argue is easier than currently employed off-site measurement techniques such as inductively coupled plasma mass spectrometry (ICP-MS).
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Due to the inherently low degree of silica condensation in these amorphous silica sol-gel films (see Reference [20]), we anticipate that the material is unstable to acid over prolonged periods of time. It is also possible that the ligand may break down with repeated exposure to the acidic solution since a reduced capacity for metal binding by a siliceous powder incorporating this ligand after exposure to acid was previously reported (see Reference [15])
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Due to the inherently low degree of silica condensation in these amorphous silica sol-gel films (see Reference [20]), we anticipate that the material is unstable to acid over prolonged periods of time. It is also possible that the ligand may break down with repeated exposure to the acidic solution since a reduced capacity for metal binding by a siliceous powder incorporating this ligand after exposure to acid was previously reported (see Reference [15]).
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