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dc.contributor.authorBessonette, PWRen_US
dc.contributor.authorWhite, MAen_US
dc.date.accessioned2013-08-23T15:58:36Z
dc.date.available2013-08-23T15:58:36Z
dc.date.issued1999-02en_US
dc.identifier.citationReproduced from Bessonette, PWR, and MA White. 1999. "Why is there no low-temperature phase transition in NaOH?." Journal of Chemical Physics 110(8): 3919-3925, with the permission of AIP Publishing.en_US
dc.identifier.issn0021-9606en_US
dc.identifier.urihttp://dx.doi.org/10.1063/1.478246en_US
dc.identifier.urihttp://hdl.handle.net/10222/36101
dc.description.abstractAlthough NaOH and NaOD exhibit parallel polymorphism at high temperatures, NaOD exhibits a low-temperature phase transition to a hydrogen-bonded antiferroelectric phase and no comparable transition has been found in NaOH. Measurements of NaOH by dielectric relaxation and adiabatic calorimetry were undertaken to determine if proton disorder becomes frozen in NaOH at low temperatures. No evidence for relaxation in NaOH was found from calorimetry or dielectric measurements. A comparison of the low-temperature heat capacities of NaOH and NaOD showed that NaOH has excess heat capacity, likely due to the existence of tunneling levels, and this was satisfactorily fit to a two-level Schottky anomaly. Thus, hydrogen-atom ordering in NaOH appears to take place through a more gradual process at low temperatures, rather than a low-temperature phase transition as in NaOD. The difference in the behaviour of NaOH and NaOD likely is associated with oxygen-oxygen distances that are slightly longer in NaOH than in NaOD, owing to the different nature of higher-temperature dynamical disorder (classical-double-well potential for OD- and tunneling for OH-).en_US
dc.relation.ispartofJournal of Chemical Physicsen_US
dc.titleWhy is there no low-temperature phase transition in NaOH?en_US
dc.typearticleen_US
dc.identifier.volume110en_US
dc.identifier.issue8en_US
dc.identifier.startpage3919en_US
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