Raman study of molecular motions in relation to phase transitions in [Ni(NH3)6](NO3)2

1987 ◽  
Vol 18 (7) ◽  
pp. 493-495 ◽  
Author(s):  
J. M. Janik ◽  
J. A. Janik ◽  
R. M. Pick ◽  
M. Le Postollec
1977 ◽  
Vol 6 (3) ◽  
pp. 130-134 ◽  
Author(s):  
J. A. Janik ◽  
T. Sarga ◽  
J. M. Janik ◽  
G. Pytasz ◽  
J. Sokotowski

1998 ◽  
Vol 64 (4) ◽  
pp. 179-190 ◽  
Author(s):  
A. Maaej ◽  
M. Bahri ◽  
Y. Abid ◽  
N. Jaidane ◽  
Z. B. Lakhdar ◽  
...  

1987 ◽  
Vol 87 (6) ◽  
pp. 3587-3590 ◽  
Author(s):  
A. Jayaraman ◽  
G. A. Kourouklis ◽  
R. C. Haddon

1991 ◽  
Vol 46 (3) ◽  
pp. 240-246 ◽  
Author(s):  
Qiang Xu ◽  
Taro Eguchi ◽  
Hirokazu Nakayama ◽  
Nobuo Nakamura ◽  
Michihiko Kishita

AbstractThe temperature dependence of 35C1, 81Br, and 127I NQR frequencies and 1Hspin-lattice relaxation times (T1) for CH3NH3PbX3 (X = Cl, Br, I) was measured through the successive phase transitions in these solids. The isotropic reorientation of the CH3NH3 ions takes place in the higher-temperature phases (tetragonal [I4/mcm] and cubic) of the three salts (Ea= 11 kJ mol -1). T1's in the lowest-temperature phases (orthorhombic) indicate that the cations undergo correlated C3-reorientation in the chloride (Ea = 5.45 kJ mol -1)and in the iodide (Ea = 5.80 kJ mol -1, whereas correlated (Ea = 2.40 kJ mol-1) and uncorrected (Ea = 7.50 kJ mol-1) C3- reorientations are excited in the bromide. It is also revealed that the rotational tunneling of the cations governs T1 at lowtemperature region in the orthorhombic phases of these salts


2011 ◽  
Vol 84 (10) ◽  
Author(s):  
Pei-Nan Chen ◽  
Chang-Sheng Zha ◽  
Xiao-Jia Chen ◽  
Jinfu Shu ◽  
Russell J. Hemley ◽  
...  

2012 ◽  
Vol 68 (4) ◽  
pp. 412-423 ◽  
Author(s):  
Nikolay A. Tumanov ◽  
Elena V. Boldyreva

The effect of pressure on DL-alanine has been studied by X-ray powder diffraction (up to 8.3 GPa), single-crystal X-ray diffraction and Raman spectroscopy (up to ∼ 6 GPa). No structural phase transitions have been observed. At ∼ 1.5–2 GPa, cell parameters b and c become accidentally equal to each other, but the space-group symmetry does not change. There is no phase transition between 1.7 and 2.3 GPa, contrary to what has been reported earlier [Belo et al. (2010). Vibr. Spectrosc. 54, 107–111]. The presence of the second phase transition, which was claimed to appear within the pressure range from 6.0 to 7.3 GPa (Belo et al., 2010), is also argued. The changes in the Raman spectra have been shown to be continuous in all the pressure ranges studied.


1997 ◽  
Vol 435 (1) ◽  
pp. 1-10 ◽  
Author(s):  
G. Bator ◽  
R. Provoost ◽  
R.E. Silverans ◽  
Th. Zeegers-Huyskens

2019 ◽  
Vol 50 (8) ◽  
pp. 1205-1216
Author(s):  
Chao Fu ◽  
Bing Du ◽  
Chao Dai ◽  
Pan Li ◽  
Li Lei ◽  
...  

1969 ◽  
Vol 50 (8) ◽  
pp. 3462-3466 ◽  
Author(s):  
Z. M. El Saffar ◽  
R. G. Eades ◽  
J. P. Llewellyn

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