The photoacoustic (PA) technique has been employed to measure the thermal diffusivity of Ge20BixSe80-x (x at.% = 2 to 11) and Ge20BixSe70-xTe10 (x at.% = 2.5 to 12) glasses. The PA cell developed for these studies is also described briefly. The thermal diffusivity measurements show an anomaly near the p to n transition. Possible explanations have been given in the light of percolation threshold and chemically ordered network model
Photoacoustic spectroscopy (PAS) and Photothermal beam deflection spectroscopy (PBS) was used to stu...
An open cell configuration has been employed for the photoacoustic measurement of the thermal diffus...
The optical bandgap and thermal diffusivity of Si10AsxTe90−x (10 ≤ x ≤ 50) and Si15AsxTe85−x (5 ≤ x ...
The photoacoustic (PA) technique has been employed to measure the thermal diffusivity of Ge20BixSe80...
The composition dependence of optical energy gap \u85Eg and thermal diffusivity \u85a in three set...
The composition dependence of optical energy gap (E<SUB>g</SUB>) and thermal diffusivity a in three ...
The composition dependence of optical energy gap $(E_g)$ and thermal diffusivity (\alpha) in three s...
The optical band gap $(E_0)$ and thermal diffusivity (α) of bulk $Ge_xSb_5Se_{95-x}$ and $Ge_xSb_{10...
The thermal diffusivity of two sets of $Ge_xSb_ySe_{l00-x-y}, Ge_xAs_yTe_{100-x-y}$ and $Si_xAs_yTe_...
Bulk $Pb_{x}Ge_{42-x}$ (x= 0, 2.5, 5, 7.5, 9, 10 & 15 at.%) and $Pb_{20}Ge_{y}Se_{80-y}$ (y = 17, 1...
The photoacoustic technique is used to determine the optical energy gap E0 of bulk SixTe100−x glass...
Photoacoustic (PA) technique is used to study glass transition and temperature dependence of thermal...
The optical band-gap $(E_0)$ and thermal diffusivity $(\alpha)$ of bulk $Ge_{7.5}As_xTe_{92.5-x} (x=...
The thermal diffusivity of two sets of GexSbySe100-x-y, GexAsyTe100-x-y and SixAsyTe100-x-y glasses ...
The photoacoustic technique is used to determine the optical energy gap E0 of bulk SixTe100-x glasse...
Photoacoustic spectroscopy (PAS) and Photothermal beam deflection spectroscopy (PBS) was used to stu...
An open cell configuration has been employed for the photoacoustic measurement of the thermal diffus...
The optical bandgap and thermal diffusivity of Si10AsxTe90−x (10 ≤ x ≤ 50) and Si15AsxTe85−x (5 ≤ x ...
The photoacoustic (PA) technique has been employed to measure the thermal diffusivity of Ge20BixSe80...
The composition dependence of optical energy gap \u85Eg and thermal diffusivity \u85a in three set...
The composition dependence of optical energy gap (E<SUB>g</SUB>) and thermal diffusivity a in three ...
The composition dependence of optical energy gap $(E_g)$ and thermal diffusivity (\alpha) in three s...
The optical band gap $(E_0)$ and thermal diffusivity (α) of bulk $Ge_xSb_5Se_{95-x}$ and $Ge_xSb_{10...
The thermal diffusivity of two sets of $Ge_xSb_ySe_{l00-x-y}, Ge_xAs_yTe_{100-x-y}$ and $Si_xAs_yTe_...
Bulk $Pb_{x}Ge_{42-x}$ (x= 0, 2.5, 5, 7.5, 9, 10 & 15 at.%) and $Pb_{20}Ge_{y}Se_{80-y}$ (y = 17, 1...
The photoacoustic technique is used to determine the optical energy gap E0 of bulk SixTe100−x glass...
Photoacoustic (PA) technique is used to study glass transition and temperature dependence of thermal...
The optical band-gap $(E_0)$ and thermal diffusivity $(\alpha)$ of bulk $Ge_{7.5}As_xTe_{92.5-x} (x=...
The thermal diffusivity of two sets of GexSbySe100-x-y, GexAsyTe100-x-y and SixAsyTe100-x-y glasses ...
The photoacoustic technique is used to determine the optical energy gap E0 of bulk SixTe100-x glasse...
Photoacoustic spectroscopy (PAS) and Photothermal beam deflection spectroscopy (PBS) was used to stu...
An open cell configuration has been employed for the photoacoustic measurement of the thermal diffus...
The optical bandgap and thermal diffusivity of Si10AsxTe90−x (10 ≤ x ≤ 50) and Si15AsxTe85−x (5 ≤ x ...