For the vibrational structure in Tetrachloro-carbon spectrum.

[1] BORN M, 1933, OPTIK, P537

[2] The vibrational levels of linear symmetrical triatomic molecules [J]. PHYSICAL REVIEW, 1932, 41 (03): : 304 - 312

[3] The Raman effect of carbon dioxide [J]. ZEITSCHRIFT FUR PHYSIK, 1931, 71 (3-4): : 250 - 259

[4] FERMI E, 1932, PHYS REV 2, V41, P304

[5] Fine structure of Raman bands [J]. ZEITSCHRIFT FUR PHYSIK, 1931, 72 (5-6): : 350 - 367

[6] Marvin H. H., 1912, PHYS REV, V34, P161

[7] MARVIN HH, 1912, PHYS REV, V34, P1616

[8] About the Raman effect [J]. ZEITSCHRIFT FUR PHYSIK, 1928, 50 (11-12): : 741 - 755

[9] Raman Effect and ultra-red Spectrum of CCl(4) and SiCl(4) [J]. ZEITSCHRIFT FUR PHYSIK, 1930, 60 (9-10): : 586 - 594

[1] BORN M, 1933, OPTIK, P537

[2] The vibrational levels of linear symmetrical triatomic molecules [J]. PHYSICAL REVIEW, 1932, 41 (03): : 304 - 312

[3] The Raman effect of carbon dioxide [J]. ZEITSCHRIFT FUR PHYSIK, 1931, 71 (3-4): : 250 - 259

[4] FERMI E, 1932, PHYS REV 2, V41, P304

[5] Fine structure of Raman bands [J]. ZEITSCHRIFT FUR PHYSIK, 1931, 72 (5-6): : 350 - 367

[6] Marvin H. H., 1912, PHYS REV, V34, P161

[7] MARVIN HH, 1912, PHYS REV, V34, P1616

[8] About the Raman effect [J]. ZEITSCHRIFT FUR PHYSIK, 1928, 50 (11-12): : 741 - 755

[9] Raman Effect and ultra-red Spectrum of CCl(4) and SiCl(4) [J]. ZEITSCHRIFT FUR PHYSIK, 1930, 60 (9-10): : 586 - 594