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Amendment to "Inhibition of efflorescence in mixed organic-inorganic particles at temperatures less than.. Bodsworth, A. 2011

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ADDITIONS & CORRECTIONS www.rsc.org/pccp | Physical Chemistry Chemical Physics Thermal reversion of spirooxazine in ionic liquids containing the [NTf2]  anion Simon Coleman, Robert Byrne, Stela Minkovska and Dermot Diamond Phys. Chem. Chem. Phys., 2009, 11, 5608–5614 (DOI: 10.1039/b901417a). Amendment published 30th November 2009. In the above paper, Table 1 inadvertently referenced the incorrect literature. The references should appear as shown in the table below (according to the numbering in the published paper). The literature value for a in ethanol is corrected to 0.86 from 0.83 and the literature value for b in ethanol is corrected to 0.75 from 0.77. 41 C. P. Fredlake, M. J. Muldoon, S. N. V. K. Aki, T. Welton, J. F. Brennecke, Phys. Chem. Chem. Phys., 2004, 6, 3280. 42 Y. Marcus, Chem. Soc. Rev., 1993, 22, 409. 43 M. J. Muldoon, C. M. Gordon, I. R. Dunkin, J. Chem. Soc., Perkin Trans. 2, 2001, 433. Analysis of isotope effects in NMR one-bond indirect nuclear spin–spin coupling constants in terms of localized molecular orbitals Patricio F. Provasi and Stephan P. A. Sauer Phys. Chem. Chem. Phys., 2009, 11, 3987–3995 (DOI: 10.1039/b819376b). Amendment published 7th December 2009. The numerical values given for the reduced coupling constants, KX–H (in 10 18 J1 T2), and for the changes in the reduced coupling constants, DKX–H (in 10 18 J1 T2), in Tables 2 to 7 and Figures 1 to 4 have to be multiplied by the constant factor p. These changes have no influence on the discussion or conclusions of the paper as all values are equally affected. Solvent Et(30)/kcal mol1 a b p* SO MC lmax k  102/s1 SD t/s Methanol 55.4 (55.4)8 1.06 (1.05)41 0.62 (0.61)41 0.71 (0.73)41 640 3.2 0.008 31.25 Ethanol 52.1 (51.9)8 0.90 (0.86)42 0.72 (0.75)42 0.63 (0.54)42 642 3.8 (2.0)20 0.009 26.32 Acetonitrile 46.4 (45.6)8 0.42 (0.35)41 0.37 (0.37)41 0.79 (0.79)41 642 5.0 (5.2)20 0.006 20 Acetone 42.5 (42.2)8 0.25 (0.20)41 0.57 (0.54)41 0.67 (0.70)41 642 5.1 (5.4)20 0.011 19.61 [bmIm][NTf2] 52.4 (51.5) 43 0.72 (0.69)41 0.24 (0.25)41 0.90 (0.97)41 642 2 0.005 50 [em2Im][NTf2] 50 0.42 0.1 1.02 640 2.3 0.011 43.48 [bmPy][NTf2] 49.6 (50.2) 14 0.57 (0.43)13 0.23 (0.25)13 0.87 (0.95)13 642 2.2 0.009 45.45 [P6,6,6,14][NTf2] 46.1 0.37 0.27 0.83 648 1.1 0.005 90.91 [N1,8,8,8][NTf2] 45.9 0.33 0.23 0.87 646 1.5 0.008 66.67 15132 | Phys. Chem. Chem. Phys., 2010, 12, 15132–15146 This journal is c the Owner Societies 2010 D ow nl oa de d on  1 8 A pr il 20 11 Pu bl ish ed  o n 10  N ov em be r 2 01 0 on  h ttp :// pu bs .rs c. or g | do i:1 0.1 039 /C0 CP 901 27J View Online Dependence of surface atomic arrangement of titanium dioxide on metallic nanowire nucleation by thermally assisted photoreduction Hsien-Tse Tung, Jenn-Ming Song, Shih-Wei Feng, Changshu Kuo and In-Gann Chen Phys. Chem. Chem. Phys., 2010, 12, 740–744 (DOI: 10.1039/b920150e). Amendment published 8th January 2010. The author affiliations should be as follows: aDepartment of Materials Science and Engineering, National Cheng Kung University, No.1, University Road, Tainan 70101, Taiwan. Fax: (+886)-6-238-1695; Tel: (+886)-6-276-3741; E-mail: ingann@mail.ncku.edu.tw bDepartment of Materials Science and Engineering, National Dong Hwa University, No.1, Sec.2, Da Hsueh Road, Hualien 97401, Taiwan. Tel: (+886)-3-863-4605 cDepartment of Applied Physics, National University of Kaohsiung, 700, Kaohsiung University Rd., Nanzih District, 811. Kaohsiung, Taiwan. Tel: (+886)-7-5919354; Fax: (+886)-7-5919357; E-mail: swfeng@nuk.edu.tw Ionicity in ionic liquids: correlation with ionic structure and physicochemical properties Kazuhide Ueno, Hiroyuki Tokuda and Masayoshi Watanabe Phys. Chem. Chem. Phys., 2010, 8, 1649–1658 (DOI: 10.1039/b921462n). Amendment published 15th January 2010. Fig. 2 (corrected) This journal is c the Owner Societies 2010 Phys. Chem. Chem. Phys., 2010, 12, 15132–15146 | 15133 D ow nl oa de d on  1 8 A pr il 20 11 Pu bl ish ed  o n 10  N ov em be r 2 01 0 on  h ttp :// pu bs .rs c. or g | do i:1 0.1 039 /C0 CP 901 27J View Online The correct reference 55 is: 55 (a) H. Luo, G. A. Baker, and S. Dai, J. Phys. Chem. B, 2008, 112, 10077. (b) J. M. S. S. Esperanca, J. N. C. Lopes, M. Tariq, L. M. N. B. F. Santos, J. W. Magee, and L. P. N. Rebelo, J. Chem. Eng. Data, 2010, 55, 3. Characterization of the ~X1A1 and ~A 1B2 electronic states of titanium dioxide, TiO2 Hailing Wang, Timothy C. Steimle, Cristina Apetrei and John P. Maier Phys. Chem. Chem. Phys., 2009, 11, 2649–2656 (DOI: 10.1039/b821849h). Amendment published 1st March 2010. An error in the program code used to model the optical Stark effect in the ~A1B2  ~X1A1 band at 18655 cm1 of TiO2 has been discovered. Specifically, the previously used code erroneously included levels that are not allowed by nuclear spin statistics. The corrected code fits the optical Stark spectra to give the permanent electric dipole moments, me, of 7.00  0.10D and 5.11  0.23D Fig. 4 (corrected) Fig. 6 (corrected) 15134 | Phys. Chem. Chem. Phys., 2010, 12, 15132–15146 This journal is c the Owner Societies 2010 D ow nl oa de d on  1 8 A pr il 20 11 Pu bl ish ed  o n 10  N ov em be r 2 01 0 on  h ttp :// pu bs .rs c. or g | do i:1 0.1 039 /C0 CP 901 27J View Online for the ~X1A1 and ~A 1B2 states, respectively. The correlation coefficient is 0.66. The corrected differences between the observed and calculated Stark shifts and the standard deviation of the fit of Table 2 are given below. Time-dependent density functional theory of high excitations: to infinity, and beyond Meta van Faassen and Kieron Burke Phys. Chem. Chem. Phys., 2009, 11, 4437–4450 (DOI: 10.1039/b901402k). Amendment published 2nd March 2010. In the above paper, an acknowledgement of funding was missing. The following line should have been included: KB thanks the DOE DE-FG02-08ER46496. First steps in combining modulation excitation spectroscopy with synchronous dispersive EXAFS/DRIFTS/mass spectrometry for in situ time resolved study of heterogeneous catalysts Davide Ferri, M. Santosh Kumar, Ronny Wirz, Arnim Eyssler, Oxana Korsak, Paul Hug, Anke Weidenkaff and Mark A. Newton Phys. Chem. Chem. Phys., 2010, 12, 5634–5646 (DOI: 10.1039/b926886c). Amendment published 27th May 2010. The name of the second author should be spelled M. Santhosh Kumar. Table 2 The observed and calculated Stark shifts for the R202 line of the à 1B2’ X̃ 1A1 (000-000) band of TiO2 Field (V/cm) M0N M 00 N Obs. (MHz) D a (MHz) Field (V/cm) M0N M 00 N Obs. (MHz) D a (MHz) 1109 2 2 180 9 1450 1 0 185 6 8 1 1 35 9 > 2 1 113 8 0 0 116 23 0 1 21 3 1450 2 2 279 12 3 2 198 8 8 1 1 39 5 1 2 373 21 0 0 163 4 1692 1 0 248 5 1692 2 2 374 20 > 2 1 152 10 8 1 1 61 2 0 1 36 5 0 0 201 15 3 2 250 6 1934 0 0 263 18 1 2 479 2 8 1 1 55 20 1933 1 0 298 20 2 2 508 4 > 2 1 173 11 967 2 1 39 8 0 1 15 24 > 3 2 81 3 3 2 342 9 1208 2 1 70 2 1 2 642 22 > 3 2 134 9 1 2 240 5 Std. of fit = 12.1 MHz This journal is c the Owner Societies 2010 Phys. Chem. Chem. Phys., 2010, 12, 15132–15146 | 15135 D ow nl oa de d on  1 8 A pr il 20 11 Pu bl ish ed  o n 10  N ov em be r 2 01 0 on  h ttp :// pu bs .rs c. or g | do i:1 0.1 039 /C0 CP 901 27J View Online Molecular dynamics simulations of atomically flat and nanoporous electrodes with a molten salt electrolyte Jenel Vatamanu, Oleg Borodin and Grant D. Smith Phys. Chem. Chem. Phys., 2010, 12, 170–182 (DOI: 10.1039/b917592j). Amendment published 26th March 2010. In our original publication of this work1 the effective integral electric double layer (EDL) capacitance CEDL eff was used. In this addendum we augment the original analysis by exploring behavior of the integral capacitance Ci. It will be shown that that CEDL eff and Ci behave quite differently as a function of voltage and usage of the conventional definition of Ci is preferred. The effective integral EDL capacitance is given by eqn (13) in ref. 1 and repeated in eqn (1) here: C eff EDL ¼ Qelectrode DUEDLA ; ð1Þ where Qelectrode is the electrode charge, A is the electrode area and DUEDL is the electric double layer potential, which is given by the potential difference between the electrode potential and bulk potential: DUEDL = Uelectrode  Ubulk (2) The effective integral EDL capacitance CEDL eff has been used by the simulation community (e.g., Feng et al.,2 Reed et al.,3 and Kislenko et al.4). It is well known that the effective EDL capacitance CEDL eff [see eqn (1)] shows a discontinuity near the potential of zero charge (UPZC) and negative values as shown in Fig. 8 of the original paper, 1 Fig. A1a of this Addition (see below), and Fig. 5b of ref. 2. Discontinuity in CEDL eff is also apparent in Fig. 6 of ref. 3. Such behavior originates from the particular definition of CEDL eff employed,2 and from the fact that the potential drop within EDL could be zero for the charged electrode (Fig. 9 of our original work1). As the two individual electrodes can be considered two serial individual condensers (see the discussion from the page 084704 of ref. 3), infinite capacitance at one plate still leads to finite and positive capacitance for the entire capacitor which can be obtained by adding the electrode capacitances as given by eqn (1) in series. While the definition of CEDL eff given by eqn (1) has been used in simulation studies,2–4 we feel that it is highly beneficial to augment the results presented in the original paper1 with the integral electrode capacitance data calculated using the conventional definition from Bard and Faulkener,5 Ci ¼ QelectrodeðDUEDL UPZCÞA ð3Þ 15136 | Phys. Chem. Chem. Phys., 2010, 12, 15132–15146 This journal is c the Owner Societies 2010 D ow nl oa de d on  1 8 A pr il 20 11 Pu bl ish ed  o n 10  N ov em be r 2 01 0 on  h ttp :// pu bs .rs c. or g | do i:1 0.1 039 /C0 CP 901 27J View Online The integral capacitance Ci [eqn (3)] reflects the charge stored in an electrode with the unit area upon potential change from UPZC to a given EDL potential. The integral capacitance Ci does not lead to discontinuities and large negative values near UPZC provided that the value of UPZC is known precisely. It also allows one to make a more transparent comparison than CEDL eff given by eqn (1) with differential EDL capacitance: C diff EDL ¼ 1 A dQelectrode dUEDL The purpose of this comment is to emphasize that the effective integral EDL capacitance [eqn (1)] reported in a number of MD simulations,1–4 yields (as expected) a different behavior near PZC from the integral electrode capacitance given by eqn (3). A comparative plot between the two capacitances is shown in Fig. A1a and b for molten LiCl at 900 K, under a non-fluctuant flat electrode charge setup.1 The integral electrode capacitance [eqn (3)] was evaluated by assuming a PZC potential of 0.124 V. As expected, the integral capacitance Ci defined by eqn (3) does not have any discontinuity for the precisely known PZC. However, due to numerical errors, one particular point from simulations closest to PZC is out of trend with other simulation results (Fig. A1b). Fig. A1 A comparison between (a) the ‘‘effective integral EDL capacitance’’ [eqn (1)] and (b) the ‘‘integral electrode capacitance’’ Ci [eqn (3)] from simulation data (symbols) and from the fitted behavior of the electrode charge versus charge EDL potential (solid lines). For comparison, the fitted differential EDL capacitance CD is shown in (b) as dotted lines. This journal is c the Owner Societies 2010 Phys. Chem. Chem. Phys., 2010, 12, 15132–15146 | 15137 D ow nl oa de d on  1 8 A pr il 20 11 Pu bl ish ed  o n 10  N ov em be r 2 01 0 on  h ttp :// pu bs .rs c. or g | do i:1 0.1 039 /C0 CP 901 27J View Online The integral capacitance [eqn (3)] shows a U-shaped (Fig. A1b) behavior for LiCl molten salt next to the flat electrodes, which is similar to the behavior of the differential capacitance reported in the original paper.1 Note that close to UPZC the differential and integral capacitances are asymptotically equal as expected. In the original paper we focused on the analysis of the differential capacitance instead of focusing on the integral capacitance because the former is more useful in evaluation of the energy stored by the capacitor and allows a straightforward interpretation of the charge storing ability in the EDL as a function of applied voltage. References used in this Addition: 1 J. Vatamanu, O. Borodin, G. D. Smith, Phys. Chem. Chem. Phys., 2010, 12, 170. 2 G. Feng, J. S. Zhang and R. Qiao, J. Phys. Chem. C, 2009, 113, 4549. 3 S. K. Reed, O. J. Lanning and P. A. Madden, J. Chem. Phys., 2007, 126, 084704. 4 S. A. Kislenko, I. S. Samoylov, R. H. Amirov, Phys. Chem. Chem. Phys., 2009, 11, 5584. 5 J. A., Bard, L. R., Faulkner, Electrochemical Methods: Fundamentals and Applications, Second Edition, John Wiley & Sons Inc, 2001, p. 541. Theory of the photodissociation of ozone in the Hartley continuum; effect of vibrational excitation and O(1D) atom velocity distribution Ezinvi Baloı̈tcha and Gabriel G. Balint-Kurti Phys. Chem. Chem. Phys., 2005, 7, 3829–3833 (DOI: 10.1039/b511640f). Amendment published 2nd June 2010. Careful re-examination of the computer codes used to calculate the photodissociation dynamics in the title paper has uncovered some errors. The principal error occurred in the interpolation of the transition dipole moment surface and has resulted in the fact that the published cross sections and product state distributions in the paper are incorrect. The code has now been corrected and new calculations have been performed. In keeping with the comment of Schinke and Grebenshchikov,1 the number of angular grid points used has been increased from 32 to 70. All other parameters, i.e. grid sizes, number of radial grid points and total time, are the same as reported in ref. 2. Fig. 1 shows the calculated absorption cross section starting from different initial vibrational states of ozone. The molecule is initially has zero rotational angular momentum. The figure replaces Fig. 3 of ref. 2. The calculated cross sections now agree well with those published by Schinke and Grebenshchikov.1 Fig. 1 Calculated photodissociation cross section for O3 starting in different vibrational states, all with initial J = 0. 15138 | Phys. Chem. Chem. Phys., 2010, 12, 15132–15146 This journal is c the Owner Societies 2010 D ow nl oa de d on  1 8 A pr il 20 11 Pu bl ish ed  o n 10  N ov em be r 2 01 0 on  h ttp :// pu bs .rs c. or g | do i:1 0.1 039 /C0 CP 901 27J View Online Fig. 2 shows the calculated velocity distribution of the O(1D) atoms resulting from the photodissociation of O3 initially in its ground rotation-vibration state. The velocity distributions have been normalized so that the integral of the distribution over velocity yields unity. The peak velocity for the whole band is 2154.9 m s1. Compared to experiment3 the peak of the calculated absorption spectrum is at too low energy by 0.206528  1019 J and the calculated O(1D) +O2(a1Dg) asymptote leads to too great an energy release by 0.097 eV (0.15541198  1019 J). The overall relative kinetic energy release should therefore be increased by 0.051117  1019 J, leading to an adjusted peak O atom velocity of 2214.42 m s1 and a kinetic energy of 39.2 kJ mol1. Fig. 2 is the corrected version of Fig. 5 of ref. 2. References 1 R. Schinke and S. Y. Grebenshchikov, Phys. Chem. Chem. Phys., 2007, 9, 4026. 2 E. Baloı̈tcha and G. G. Balint-Kurti, Phys. Chem. Chem. Phys., 2005, 7, 3829 3 D. Freeman, K. Yoshino, J. Esmond and W. Parkinson, Planet. Spasce Sci., 1984, 32, 239. Towards an understanding of the vibrational mode specificity for dissociative chemisorption of CH4 on Ni(111): a 15 dimensional study Krishnamohan G. Prasanna, Roar A. Olsen, Álvaro Valdés and Geert-Jan Kroes Phys. Chem. Chem. Phys., 2010, 12, 7654–7661 (DOI: 10.1039/b924669j). Amendment published 8th July 2010. The true submission date is 23rd November 2009 Fig. 2 Calculated O(1D) velocity distributions arising from the photodissociation of ozone in the Hartley continuum. Velocity distribution arising; (A) from entire Hartley band 200 nm to 340 nm; (B) from high frequency range of the band 200 nm to 245 nm; (C) from central frequency range of the band 245 nm to 277 nm; (D) from low frequency range of the band 277 nm to 340 nm. This journal is c the Owner Societies 2010 Phys. Chem. Chem. Phys., 2010, 12, 15132–15146 | 15139 D ow nl oa de d on  1 8 A pr il 20 11 Pu bl ish ed  o n 10  N ov em be r 2 01 0 on  h ttp :// pu bs .rs c. or g | do i:1 0.1 039 /C0 CP 901 27J View Online Damage to fuel cell membranes. Reaction of HO with an oligomer of poly(sodium styrene sulfonate) and subsequent reaction with O2 Sindy M. Dockheer, Lorenz Gubler, Patricia L. Bounds, Anastasia S. Domazou, Günther G. Scherer, Alexander Wokaun and Willem H. Koppenol Phys. Chem. Chem. Phys., 2010, 12, 11609–11616 (DOI: 10.1039/c0cp00082e). Amendment published 16th August 2010. Fig. 2 should appear as follows, with the correct unit on the y-axis. Interaction between silica in the presence of adsorbed poly(ethyleneimine): correlation between colloidal probe adhesion measurements and yield stress Shannon M. Notley and Yee-Kwong Leong Phys. Chem. Chem. Phys., 2010, 12, 10594–10601 (DOI: 10.1039/c003973j). Amendment published 13th July 2010. The published Fig. 7 is incorrect; the correct Fig. 7 is: Fig. 2 Pseudo-first-order rate constants for the reaction of HO with PSSS-1100 as a function of [PSSS-1100] at 30–300 mM; N2O-saturated solutions, irradiated (dose 8 Gy) near neutral pH. Data points reflect the mean for 4–10 measurements, and error bars correspond to t  s/On for the t-distribution at a confidence level of 95%. 15140 | Phys. Chem. Chem. Phys., 2010, 12, 15132–15146 This journal is c the Owner Societies 2010 D ow nl oa de d on  1 8 A pr il 20 11 Pu bl ish ed  o n 10  N ov em be r 2 01 0 on  h ttp :// pu bs .rs c. or g | do i:1 0.1 039 /C0 CP 901 27J View Online The versatile colour gamut of coatings of plasmonic metal nanoparticles Catherine S. Kealley, Michael B. Cortie, Abbas I. Maaroof and Xiaoda Xu Phys. Chem. Chem. Phys., 2009, 11, 5897–5902 (DOI: 10.1039/b903318a). Amendment published 16th August 2010. We have discovered that some of the numerical simulations of optical properties in the above paper1 were inaccurate in the red part of the spectrum. This was due to instabilities in the routine used in the program to interpolate dielectric properties from a sparse table, in this case of the glass substrate used. The program uses a parabolic interpolation routine and at least three values of the dielectric constants as a function of wavelength are required for stable interpolation. This was not the case in our original work in which we set the refractive index of the glass to be 1.52, specified at only two wavelengths (295 nm and 1770 nm). The result was that the interpolation routine erroneously inflated the dielectric constants of the glass substrate in the red part of the spectrum, which in turn red-shifted some of the plasmon resonances of the precious metal nanoparticles. Corrected versions of Fig. 5, 6, 7 and 9 are presented here. The change to the original Fig. 8 is small and not important. The dielectric data for glass used here are listed in Table 1. Fig. 7 The yield stress-pH behaviour of 50 wt% silica suspensions under the influence of PEI of (a) Mw 600 and (b) Mw 70000. Reproduced with permission from ref. 28. This journal is c the Owner Societies 2010 Phys. Chem. Chem. Phys., 2010, 12, 15132–15146 | 15141 D ow nl oa de d on  1 8 A pr il 20 11 Pu bl ish ed  o n 10  N ov em be r 2 01 0 on  h ttp :// pu bs .rs c. or g | do i:1 0.1 039 /C0 CP 901 27J View Online Fig. 5 Scattering and resonance colours from an individual Au particle with a 30 nm diameter of curvature on a glass window, with decreasing aspect ratio (90% to 10%). Fig. 6 Scattering and resonance colours from an individual Ag particle with a 30 nm diameter of curvature on a glass window, with increasing aspect ratio (10% to 90%). Fig. 7 Scattering and resonance colours from two Au particles (30 nm diameter) with increasing separation, spheres touching and 3 nm apart shown. 15142 | Phys. Chem. Chem. Phys., 2010, 12, 15132–15146 This journal is c the Owner Societies 2010 D ow nl oa de d on  1 8 A pr il 20 11 Pu bl ish ed  o n 10  N ov em be r 2 01 0 on  h ttp :// pu bs .rs c. or g | do i:1 0.1 039 /C0 CP 901 27J View Online The text of the paper remains correct and unchanged except as follows: Section 3.2.1 Aspect ratio of particles on glass Change ‘The range of colours available from Ag, Fig. 6, is even wider than that of the Au particles’ to ‘The range of colours available from Ag, Fig. 6, is broad and includes pink and yellow.’ References 1 C. S. Kealley, M. B. Cortie, A. I. Maaroof and X. Xu, Phys. Chem. Chem. Phys., 2009, 11, 5897–5902. 2 Specification PCE - TKT B 270 Superwite, 2nd May 2000, Schott Desag, http://www.naugatuckglass.com/downloads/B270.pdf Fig. 9 Scattering and resonance colours from Au particles, simulated with increasing nucleation rate, growth rate 0.07 nm s1, for 300 seconds. Table 1 Refractive index, n, of Schott ‘B270 Superwite’ glass, from website of Schott glass company2 Wavelength/mm (vacuum) n Wavelength/mm (vacuum) n 0.30 1.517 0.62 1.522 0.32 1.562 0.64 1.521 0.34 1.562 0.66 1.520 0.36 1.548 0.68 1.520 0.38 1.539 0.70 1.519 0.40 1.535 0.72 1.519 0.42 1.534 0.74 1.518 0.44 1.535 0.76 1.518 0.46 1.534 0.78 1.517 0.48 1.530 0.80 1.517 0.50 1.528 0.82 1.517 0.52 1.527 0.84 1.516 0.54 1.526 0.86 1.516 0.56 1.524 0.88 1.516 0.58 1.523 0.90 1.515 0.60 1.522 This journal is c the Owner Societies 2010 Phys. Chem. Chem. Phys., 2010, 12, 15132–15146 | 15143 D ow nl oa de d on  1 8 A pr il 20 11 Pu bl ish ed  o n 10  N ov em be r 2 01 0 on  h ttp :// pu bs .rs c. or g | do i:1 0.1 039 /C0 CP 901 27J View Online Live celloidosome structures based on the assembly of individual cells by colloid interactions Rawil F. Fakhrullin, Marie-Laure Brandy, Olivier J. Cayre, Orlin D. Velev and Vesselin N. Paunov Phys. Chem. Chem. Phys., 2010, 12, 11912–11922 (DOI: 10.1039/c0cp00131g). Amendment published 1st September 2010. In the above paper, the address of Dr Rawil Fakhrullin was incorrect. The correct address is as follows: Department of Biochemistry, Kazan (Idel-Ural) Federal University, Kreml urami 18, Kazan, Republic of Tatarstan, 420008 Inhibition of efflorescence in mixed organic–inorganic particles at temperatures less than 250K A. Bodsworth, B. Zobrist and A. K. Bertram Phys. Chem. Chem. Phys., 2010, 12, 12259–12266 (DOI: 10.1039/c0cp00572j). Amendment published 8th September 2010. The acknowledgements to this paper did not include a complete list of projects that funded the work. The correct Acknowledgements are included below: Acknowledgements This research was supported by the Canadian Foundation for Climate and Atmospheric Science (CFCAS), the National Sciences and Engineering Research Council of Canada (NSERC), the Canada Research Chair Program and the European Commission through the EC Integrated Projects SCOUT-O3 (505390-GOCE-CT-2004) and RECONCILE (226365-FP7-ENV-2008-1). The authors thank U.K. Krieger for helpful discussions regarding the project. Specific cellular water dynamics observed in vivo by neutron scattering and NMR Marion Jasnin, Andreas Stadler, Moeava Tehei and Giuseppe Zaccai Phys. Chem. Chem. Phys., 2010, 12, 10154–10160 (DOI: 10.1039/c0cp01048k). Amendment published 8th October 2010. The final two authors in reference 30 are listed incorrectly in the above Perspective. The correct details are: 30 E. Deplazes, W. van Bronswijk, F. Zhu, L. D. Barron, S. Ma, L. A. Nafie and K. J. Jalkanen, Theor. Chem. Acc., 2008, 119, 155–176. 15144 | Phys. Chem. Chem. Phys., 2010, 12, 15132–15146 This journal is c the Owner Societies 2010 D ow nl oa de d on  1 8 A pr il 20 11 Pu bl ish ed  o n 10  N ov em be r 2 01 0 on  h ttp :// pu bs .rs c. or g | do i:1 0.1 039 /C0 CP 901 27J View Online Complete representation of isothermal mass and charge transport properties of mixed ionic–electronic conductor La2NiO4+d Hong-Seok Kim and Han-Ill Yoo Phys. Chem. Chem. Phys., 2010, 12, 12951–12955 (DOI: 10.1039/c0cp00722f). Amendment published 15th October 2010. The equations from pages 2–4 should be labelled consecutively. That is to say, on page 2, the second equation labelled as (I) should be (6), and those labelled as (6)–(8) should be (7)–(9). On page 3, the equation labelled as (9) should be (11) and on page 4, the equation labelled as (11) should be (12). The version of Fig. 2 published in the article contained errors and is replaced by the following figure: In addition, the signs of eqn (6) and (9) were incorrect; the correct versions are as follows: Eqn (6): UðtÞ ¼  ‘Ia  i 2As0e  LIte As0e 1 a  i 2   4 p2 X1 n¼1 2 ð2n 1Þ2 sin ð2n 1Þp 2    sin ð2n 1Þp 2 ‘ L   exp  p 2ð2n 1Þ2 ~Dt L2  ! Eqn (9): UðtÞ ¼LIte As0e 1 a  i 2   4 p2 X1 n¼1 2 ð2n 1Þ2 sin ð2n 1Þp 2    sin ð2n 1Þp 2 ‘ L   exp  p 2ð2n 1Þ2 ~Dt L2 " # Fig. 2 Typical behaviors of U(t) and V(t) vs. time during galvanostatic polarization and depolarization in ion-blocking electrode condition. The solid line through U is the best fitted results by eqn (6) and (9). This journal is c the Owner Societies 2010 Phys. Chem. Chem. Phys., 2010, 12, 15132–15146 | 15145 D ow nl oa de d on  1 8 A pr il 20 11 Pu bl ish ed  o n 10  N ov em be r 2 01 0 on  h ttp :// pu bs .rs c. or g | do i:1 0.1 039 /C0 CP 901 27J View Online Defect-chemical analysis of the nonstoichiometry, conductivity and thermopower of La2NiO4+d Hong-Seok Kim and Han-Ill Yoo Phys. Chem. Chem. Phys., 2010, 12, 4704–4713 (DOI: 10.1039/b918329a). Amendment published 15th October 2010 (this replaces the amendment published 7th July 2010). In Table 4, the value at 1173 K should be 0.18, not 0.08. The correct Table 4 is: In addition, eqn (22) contained errors. The version in the text: 2 1ffiffiffi 8 p s sV þ 3 16  ffiffiffi 3 p 9  ! s sV  2" # þ ln s 2eouh  s   s sV  2 ¼ lnKOx þ 1 2 ln aO2 is replaced by the following equation: 2 1ffiffiffi 8 p s sV þ 3 16  ffiffiffi 3 p 9  ! s sV  2" # þ ln s 4beouh  s   s sV  2 ¼ lnKOx þ 1 2 ln aO2 The Royal Society of Chemistry apologises for these errors and any consequent inconvenience to authors and readers. Additions and corrections can be viewed online by accessing the original article to which they apply. T/K Soh=kþ qh =kT 1073 0.20  0.01 1173 0.18  0.02 1273 0.21  0.02 15146 | Phys. Chem. Chem. Phys., 2010, 12, 15132–15146 This journal is c the Owner Societies 2010 D ow nl oa de d on  1 8 A pr il 20 11 Pu bl ish ed  o n 10  N ov em be r 2 01 0 on  h ttp :// pu bs .rs c. or g | do i:1 0.1 039 /C0 CP 901 27J View Online

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