In their recent article [1], M. Couzi et al. develop a standard phenomenological model of coupled order parameters, which generates one single symmetry-breaking phase transition. They apply it to the phase transitions of n-nonadecane/urea and n-hexadecane/urea, while knowing that our measurements had demonstrated, via previously published diffraction experiments [2-6], that both materials undergo at least two symmetry-breaking events revealed by systematic absences of diffraction peaks.We have shown that in n-nonadecane-d40/urea-d4 and n-nonadecane-h40/urea-h4, there is a complex sequence of phases that follow crystallographic symmetry conditions. The first-phase transition at Tc1 is associated with the symmetry breaking from the hexagonal high-temperature phase to a second phase (phase II); a second transition to a different space group (phase III) occurs at a lower temperature Tc2. These results have been discussed extensively in the literature [3,4,6-9] and were obtained using excellent spatial resolution and temperature calibration, including measurements using cold neutron scattering on triple axis spectrometers [3,4], and on a synchrotron X-ray diffractometer [7]. For n-nonadecane-h40/urea-h4, Tc1 = (158.8 ± 0.1) K and Tc2 = (147.0 ± 0.1) K, according to adiabatic measurements [10].Instead of using these careful measurements, M. Couzi et al. used the results from their recently published article, which describes an X-ray diffraction study performed on n-nonadecane-h40/urea-h4 but with measurements reported at only two temperatures (147 K and 100 K) [11]. In a Comment concerning that article [2], which they did not contest, we demonstrated that their data have no relevance. There [2], we wrote: ‘As elaborated here, the data reported by Couzi et al. are not from phase II of n-nonadecane/urea and cannot be used to discuss the sequence of phases in this compound’.Inexplicably, Couzi et al. do not address this fundamental criticism of their data in the present article [1]. They have not presented any data on pure phase II on which to base their assertion that phase II is the same space group as phase III. Furthermore, M. Couzi et al. are fully aware of the extraordinarily high-quality X-ray data exhibiting the unique crystallographic signature of phase II shown in fig. 2(a) of [7], (ref. 32 in [1] and ref. 11 in [11]), which was acquired at 154.5 K, in the middle of phase II of n-nonadecane-h40/urea-h4. This figure, in fact, is the reconstructed image that they would have obtained if they had actually been measuring phase II instead of phase III. However, they have chosen to ignore these data in favour of their own, which were both measurements on phase III.In the same Comment [2], to which there was no reply, we asked Couzi et al. to explain how their measurements were actually made, since only one measurement was reported in the vicinity of phase II:It is for Couzi et al. to explain why they have failed to observe the absence/presence conditions that characterize phase II, in particular the common and host superstructure Bragg peaks, which are not in phase II and whose emergence with cooling signifies phase III.However, in their present article [1], Couzi et al. make the following surprising statement (where references [12,28,30] and [31] are references [5,3,4] and [11], respectively, in this Comment):Given that the (3 + 2)-dimensional superspace groups proposed previously [12,28,30] for n-nonadecane/urea and n-hexadecane/urea have been shown [31] to be incorrect,…We maintain that the data collected by Couzi et al. [11] were on the wrong phase, and as a consequence, their phenomenological description of the phase behaviour in n-nonadecane/urea [1] is contrary to reliable experimental measurements and does not apply to the isotopologues of n-nonadecane/urea. As already extensively argued in our previous Comment [2], we maintain also that two different symmetry-breaking events are indeed present in n-hexadecane/urea.
Authors: Bertrand Toudic; Pilar Garcia; Christophe Odin; Philippe Rabiller; Claude Ecolivet; Eric Collet; Philippe Bourges; Garry J McIntyre; Mark D Hollingsworth; Tomasz Breczewski Journal: Science Date: 2008-01-04 Impact factor: 47.728
Authors: S Zerdane; C Mariette; G J McIntyre; M-H Lemée-Cailleau; P Rabiller; L Guérin; J C Ameline; B Toudic Journal: Acta Crystallogr B Struct Sci Cryst Eng Mater Date: 2015-05-26
Authors: M Huard; B Toudic; P Rabiller; C Ecolivet; L Guérin; P Bourges; T Breczewski; Mark D Hollingsworth Journal: J Chem Phys Date: 2011-11-28 Impact factor: 3.488
Authors: A López-Echarri; I Ruiz-Larrea; A Fraile-Rodríguez; J Díaz-Hernández; T Breczewski; E H Bocanegra Journal: J Phys Condens Matter Date: 2007-04-11 Impact factor: 2.333
Authors: Laurent Guérin; Céline Mariette; Philippe Rabiller; Michael Huard; Sylvain Ravy; Pierre Fertey; Shane M Nichols; Bo Wang; Stefan C B Mannsfeld; Thomas Weber; Mark D Hollingsworth; Bertrand Toudic Journal: Phys Rev B Condens Matter Mater Phys Date: 2015-05-01
Authors: Kirsten Christensen; P Andrew Williams; Rhian Patterson; Benjamin A Palmer; Michel Couzi; François Guillaume; Kenneth D M Harris Journal: R Soc Open Sci Date: 2019-08-14 Impact factor: 2.963