2021
DOI: 10.1103/physrevb.103.014428
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Freezing of molecular rotation in a paramagnetic crystal studied by P31 NMR

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Cited by 4 publications
(4 citation statements)
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“…As the temperature increases to 360 K, the full width at half-maximum (FWHM) of the 31 P NMR signals slightly decreases (Figure c), which indicates the acceleration of the rolling rate of the PF 6 anions in the LTP. However, FWHM drops sharply at around 380 K, suggesting that the pure Lorentzian line shape was altered by the fluctuating field from the electric dipolar moment of radicals due to the phase transition, according to the previous report . As a consequence, the rolling rate of PF 6 – anions in the HTP is much higher than that in the LTP.…”
Section: Resultssupporting
confidence: 57%
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“…As the temperature increases to 360 K, the full width at half-maximum (FWHM) of the 31 P NMR signals slightly decreases (Figure c), which indicates the acceleration of the rolling rate of the PF 6 anions in the LTP. However, FWHM drops sharply at around 380 K, suggesting that the pure Lorentzian line shape was altered by the fluctuating field from the electric dipolar moment of radicals due to the phase transition, according to the previous report . As a consequence, the rolling rate of PF 6 – anions in the HTP is much higher than that in the LTP.…”
Section: Resultssupporting
confidence: 57%
“…However, FWHM drops sharply at around 380 K, suggesting that the pure Lorentzian line shape was altered by the fluctuating field from the electric dipolar moment of radicals due to the phase transition, according to the previous report. 42 As a consequence, the rolling rate of PF 6 − anions in the HTP is much higher than that in the LTP. This result is also consistent with the disordered and ordered crystal structures in the HTP and LTP, respectively.…”
Section: Free Radical Compound [(Nh 3 -Tempo)(18-crown-6)][asf 6 ]mentioning
confidence: 99%
“…As previously reported, the 31 P 1=T 1 rate in CuPOF yields several broad maxima at high temperatures, which are associated with a freezing of the PF 6 molecular reorientation modes [39]. Below about 10 K, in the range of interest in the present study, these modes are frozen out and 1=T 1 becomes temperature independent, indicating predominantly paramagnetic fluctuations.…”
supporting
confidence: 81%
“…[ 34 ] Towards further cooling, it increases to reach a maximum and falls down again, forming a well‐defined peak at ≈20 K. This low‐temperature peak is naturally reminiscent of the glassy spin freezing behavior. [ 35,36 ] In the BPP description, the occurrence of a peak in 1/ T 1 T reflects a progressive slowing down of the spin fluctuations, and the peak temperature is defined as spin freezing temperature T sf on the timescale of NMR. [ 37 ] The enhancement of 1/ T 1 T from ≈50 K is therefore ascribed to the low‐energy spin fluctuations.…”
Section: Resultsmentioning
confidence: 99%