The Second — Order Raman — Spectrum of the Crystal NaCl for Low Temperatures

Author(s):  
A. I. Stekhanov ◽  
A. P. Corolkov
1966 ◽  
Vol 20 (6) ◽  
pp. 610-612 ◽  
Author(s):  
P.G. Marlow ◽  
J.P. Russell ◽  
C.T. Sennett

2008 ◽  
Vol 23 (29) ◽  
pp. 4709-4719 ◽  
Author(s):  
SAMINA S. MASOOD ◽  
MAHNAZ HASEEB

We calculate the second-order corrections to vacuum polarization tensor of photons at low temperatures, i.e. T ≪ 1010 K (T ≪ me). The thermal contributions to the QED coupling constant are evaluated at temperatures below the electron mass that is T < me. Renormalization of QED at these temperatures has explicitly been checked. The electromagnetic properties of such a thermal medium are modified. Parameters like electric permittivity and magnetic permeability of such a medium are no more constant and become functions of temperature.


1998 ◽  
Vol 53 (6-7) ◽  
pp. 419-426 ◽  
Author(s):  
Tetsuo Asaji ◽  
Keizo Horiuchi ◽  
Takehiko Chiba ◽  
Takashige Shimizu ◽  
Ryuichi Ikeda

Abstract From the measurements of DTA • DSC and the temperature dependences of 35Cl NQR frequencies, phase transitions were detected at 150 K, 168 K, and 172 K for (pyH)2 [PtCl4], and at 241 K for (PyH)2 [PdCl4]. In order to elucidate the motional state of the constituent ions in the crystals in connection with the structural phase transitions, the 35Cl NQR and 1H NMR spin-lattice relaxation times and the second moment of the 1H NMR line were measured as functions of temperature. For both compounds, the potential wells for the cationic reorientation are suggested to be highly nonequivalent at low temperatures. Above 168 K, the pyridinium ions in (pyH)2[PtCl4] are expected to reorient between almost equivalent potential wells. As for (pyH)2[PdCl4], it is expected that the orientational order of the cation still remains even above the second order transition at 241 K. A change of the potential curve from two-unequal to three-unequal wells is proposed as a possible mechanism of the second order transition. The activation energies for the cationic motion in the respective model potential are derived for both compounds at high and low temperatures.


1971 ◽  
Vol 4 (4) ◽  
pp. 1395-1395 ◽  
Author(s):  
N. B. Manson ◽  
W. Von der Ohe ◽  
S. L. Chodos
Keyword(s):  

1968 ◽  
Vol 168 (3) ◽  
pp. 1054-1056 ◽  
Author(s):  
John R. Hardy ◽  
Arnold M. Karo

1990 ◽  
Vol 167 (1-2) ◽  
pp. 11-19 ◽  
Author(s):  
L.G. Mamsurova ◽  
K.S. Pigalskiy ◽  
V.P. Sakun ◽  
A.I. Shushin ◽  
L.G. Scherbakova

1954 ◽  
Vol 32 (10) ◽  
pp. 630-634 ◽  
Author(s):  
B. P. Stoicheff

The pure rotational spectrum and the Q branch of the 1–0 band of N2 were photographed in the second order of a 21 ft. grating. An analysis of the rotational spectrum yields the rotational constants[Formula: see text]The value of B0 together with the Bν values obtained from the electronic bands of N2 gives[Formula: see text]Revised values of the vibrational constants have also been calculated using the results of the present work and the published data on the electronic spectra.


1969 ◽  
Vol 179 (3) ◽  
pp. 837-845 ◽  
Author(s):  
J. R. HARDY ◽  
A. M. KARO ◽  
I. W. MORRSION ◽  
C. T. SENNETT ◽  
J. P. RUSSELL

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