2023
DOI: 10.1016/j.molliq.2023.121570
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Two mechanisms for the formation of the ferronematic phase studied by dielectric spectroscopy

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Cited by 13 publications
(18 citation statements)
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“…However, this phase, though identified as an ordinary nematic, has some unique dielectric properties such as exhibition of collective relaxation process. This was observed in the high-temperature nematic phase in both known ferronematic compounds DIO, 11,12 RM734 5 and its homologues. 7 The collective relaxation process is directly related to the polarity and it might thus be unique for ferronematic materials.…”
Section: Introductionmentioning
confidence: 76%
“…However, this phase, though identified as an ordinary nematic, has some unique dielectric properties such as exhibition of collective relaxation process. This was observed in the high-temperature nematic phase in both known ferronematic compounds DIO, 11,12 RM734 5 and its homologues. 7 The collective relaxation process is directly related to the polarity and it might thus be unique for ferronematic materials.…”
Section: Introductionmentioning
confidence: 76%
“…In some cases, the supercooling nature of the LC phase and the lower crystal melting temperatures are observed due to the fluorine-substituted molecules with weaker intermolecular forces . It is interesting to note that the N F phase as well as the SmAP F and Iso P phases are enantiotropic, giving a wide accessible temperature range while almost all N F phases reported are monotropic. …”
Section: Resultsmentioning
confidence: 99%
“…A low-frequency (LF) mode is observed at 10–100 Hz in the N F , SmAP F and Iso P phases. The huge dielectric constants and low relaxation frequencies ( f r ) reveal that the LF mode is attributed to the collective fluctuation of polarization, which is typically observed in the ferroelectric phases. ,,, , The dielectric spectra were analyzed by fitting with the following Cole–Cole equation ε * = ε i ε = ε + normalΔ ε 1 + false( i ω τ false) 1 α 0 < α < 1 where ω is the angular frequency, Δε (=ε s – ε ∞ ) is the dielectric strength, and ε s and ε ∞ are the “static-frequency” and “infinite-frequency” dielectric constants, respectively. τ = 1/(2π f r ) is the relaxation time (where f r is the relaxation frequency), and α is the distribution parameter of relaxation time.…”
Section: Resultsmentioning
confidence: 99%
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“…RM734 and DIO have large molecular dipole moments of about 10 D, and a spontaneous polarization up to | | ~ 5 µC/cm 2 . The apparent dielectric permittivity and its anisotropy were reported to be orders of magnitude higher than those of classical nematics, reaching ~ 10 4 or higher 7 , 11 , 13 18 implying an extremely large sensitivity of the materials to electric fields. Such a large dielectric constant suggests a giant dielectrowetting at unprecedentedly low voltages, since its threshold scales with the square root of the fluid’s permittivity 19 21 .…”
Section: Introductionmentioning
confidence: 98%