16 research outputs found
DE SAINT-MARTIN (Monique), SCARFO GHELLAB (Grazia) et MELLAKH (Kamal) (dir.),Étudier à l’Est : expériences de diplômés africains, lu par Françoise Blum
No full textDE SAINT-MARTIN (Monique), SCARFO GHELLAB (Grazia) et MELLAKH (Kamal) (dir.), Étudier à l’Est : expériences de diplômés africains, Paris, Karthala-FMSH, coll. « Hommes et sociétés », 2015, 300 pages Compte-rendu paru dans « La revue des livres », Politique africaine N° 141 - 2016/ 01 On connaissait déjà la belle thèse de Constantin Katsakioris, Leçons soviétiques. La formation des étudiants africains et arabes en Union Soviétique pendant la guerre froide (Paris, EHESS, 2015). On en espère d’..
Predictors of outcome in 369 patients with heart failure with preserved ejection fraction
No full text
Is youth unemployment really the major worry? (AOM)
No full textYouth unemployment is neither the only nor the basic problem of the European labour market. The comparative analysis of unemployment data demonstrates that the unemployment of older people is even more serious. The article proves that the weight of young people in total unemployment has as a tendency been declining in the “inner periphery” of the EU, among them in Central and Eastern European member states (CEECs). The trend is just the opposite in the developed or “core” countries of the Union where youngsters took a higher share in total unemployment in 2012 than 10-12 years ago. In Europe there are millions of young people beyond the active unemployed who do not want to work or think they cannot find a job that fulfils their expectations and refuse to take part in any kind of education or training (NEETs-“Not in Employment, Education or Training”). By estimating the rate of NEETs in the adult population the article claims that the NEETs-phenomenon is not the differentia specifica of the youth. At the end the article details two suggestions for the mitigation of the problem. It concludes that the joblessness in Europe is an old and tendencially worsening problem that cannot be solved by particular policies
Temperature Dependence of Elastic and Ultrasonic Properties of Sodium Borohydride
No full textWe present the temperature dependent elastic and ultrasonic properties of sodium borohydride. The second and third order elastic constants of NaBH4 have been computed in the temperature range 0-300K using Coulomb and Born-Mayer potential. The sodium borohydride crystallizes into NaCl-type structure. The computed values of second order elastic constants have been applied to evaluate the temperature dependent mechanical properties such as bulk modulus, shear modulus, tetragonal modulus, Poisson’s ratio and Zener anisotropy factor and ultrasonic velocity to predict futuristic information about sodium borohydride. The fracture to toughness ratio (bulk modulus/shear modulus) in sodium borohydride varied from 1.91 to 1.62, which shows its behavioral change from ductile to brittle on increasing the temperature. Then, ultrasonic Grüneisen parameters have been computed with the use of elastic constants in the temperature regime 100-300K. The obtained results have been discussed in correlation with available experimental and theoretical results. [1] A. Amudhavalli, M. Manikandan, A. Jemmy Cinthia, R. Rajeswarapalanichamy and K. Iyakutti, Z. Naturforsch. A 72 (2017) 321. [2] D.Singh, P.K.Yadawa and S.K.Sahu, Cryogenics 50 (2010) 476. [3] V. Bhalla, D.Singh and S.K.Jain, Int. J. Comput. Mat. Sc. Eng. 5 (2016) 1650012. [4] S. Kaushik, D. Singh and G. Mishra, Asian J. Chem. 24 (2012) 5655. [5] D. Chernyshov, A. Bosak, V. Dmitriev, Y. Filmchuk and H. Hagemann, Phys. Rev. B 78 (2008)172104. [6] H. Hagemann, S. Gomes, G. Renaudin and K. Yvon, J. Alloys Compd. 363 (2004) 126. [7] Y. Filinchuk, D. Chernyshov and V. Dmitriev, Z. Kristallogr. 223 (2008) 649. [8] Z.Xiao Dong, J.Z. Yi, Z. Bo, H. Z. Feng and H.Y. Qing, Chin. Phys. Lett. 28(2011)076201. [9] T. Ghellab, Z. Charifi, H. Baaziz, Ş. Uğur, G. Uğur and F. Soyalp, Phys. Scr. 91 (2016) 045804. [10] S. Bae, S. Gim, H. Kim and K. Hanna, Appl. Catal. B: Environm. 182 (2016) 541. [11] G. Renaudin, S. Gomes, H. Hagemann, L. Keller and K. Yvon, J Alloys Compd. 375 (2004) 98. [12] P. Vajeeston, P. Ravindran, A. Kjekshus and H. Fjellvåg, J Alloys Compd. 387 (2005) 97. [13] S. Orimo, Y. Nakamori, J.R. Eliseo, A. Zuttel and C. M. Jensen, Chem. Rev. 107 (2007) 4111. [14] A. Istek and E. Gonteki, J. Environ. Bio.7 (2009) 951. [15] R. S. Kumar and A.L. Cornelinus, Appl. Phys. Lett. 87 (2005) 261916. [16] E. Kim, R. Kumar, P. F. Weck, A. L. Cornelius, M. Nicol, S. C. Vogel, J. Zhang, M. Hartl, A.C. Stowe, L. Daemen and Y. Zhao, J. Phys. Chem. Lett. B 111 (2007) 13873. [17] K. Brugger, Phys. Rev. 133 (1964) A1611. [18] P.B. Ghate, Phy. Rev. 139 (1965) A1666 [19] S. Mori, Y. Hiki, J. Phys. Soc. Jpn. 45 (1975) 1449. [20] V. Bhalla, R. Kumar, C. Tripathy and D. Singh, Int. J. Mod. Phys. B 27 (2013) 1350116. [21] D. Singh, S. Kaushik, S. Tripathi, V. Bhalla and A. K. Gupta, Arab. J. Sci. Eng. 39 (2014) 485. [22] K. Brugger, Phys. Rev.137 (1965) 1826. [23] W. P. Mason, Physical Acoustics, vol. IIIB, Academic Press, New York, 1965. [24] M.P. Tosi, Solid State Physics, vol. 12, Academic Press, New York, 1965. [25] Y. Nakamori and S. Orimo, J. Alloy Compd.370(2004)271. [26] D. Singh, D.K. Pandey and P.K. Yadawa, Cent. Eur. J. Phys. 7 (2009) 198. [27] V. Bhalla, D. Singh, G. Mishra and M. Wan, J. Pure Appl. Ultrason. 38 (2016)23. [28] D. Singh, S. Kaushik, S.K. Pandey, G. Mishra and V. Bhalla, VNU J. Sc.: Math. Phys. 32(2016)43. [29] J.P.Watt and L. Peselnick, J.Appl. Phys. 51 (1980) 1525. [30] S.F.Pugh, Philos.Mag. 45 (1954) 823. [31] V. Bhalla, D. Singh and S.K. Jain, Int. J. Thermophys. 37(2016)33. [32] V. Bhalla, D. Singh, S.K. Jain and R. Kumar, Pramana- J. Phys. 86 (2016)135
On the Empirics of Minimum Wages and Employment: Stylized Facts for The Austrian Industry
No full textWe ask for the empirical evidence of the textbook theory of minimum wages for the Austrian Industry. The bargaining result of unions and firms is interpreted as a minimum wage, as the bargaining situation in Austria may be described best by a "right to manage-model". Based on the analysis of micro-founded "employment functions" in contrast to the predictions of the textbook analysis no significant negative effect of minimum wages on employment is found.Minimum Wages; Employment; Austrian Industry
Temperature Dependence of Elastic and Ultrasonic Properties of Sodium Borohydride
No full textWe present the temperature dependent elastic and ultrasonic properties of sodium borohydride. The second and third order elastic constants of NaBH4 have been computed in the temperature range 0-300K using Coulomb and Born-Mayer potential. The sodium borohydride crystallizes into NaCl-type structure. The computed values of second order elastic constants have been applied to evaluate the temperature dependent mechanical properties such as bulk modulus, shear modulus, tetragonal modulus, Poisson’s ratio and Zener anisotropy factor and ultrasonic velocity to predict futuristic information about sodium borohydride. The fracture to toughness ratio (bulk modulus/shear modulus) in sodium borohydride varied from 1.91 to 1.62, which shows its behavioral change from ductile to brittle on increasing the temperature. Then, ultrasonic Grüneisen parameters have been computed with the use of elastic constants in the temperature regime 100-300K. The obtained results have been discussed in correlation with available experimental and theoretical results. [1] A. Amudhavalli, M. Manikandan, A. Jemmy Cinthia, R. Rajeswarapalanichamy and K. Iyakutti, Z. Naturforsch. A 72 (2017) 321. [2] D.Singh, P.K.Yadawa and S.K.Sahu, Cryogenics 50 (2010) 476. [3] V. Bhalla, D.Singh and S.K.Jain, Int. J. Comput. Mat. Sc. Eng. 5 (2016) 1650012. [4] S. Kaushik, D. Singh and G. Mishra, Asian J. Chem. 24 (2012) 5655. [5] D. Chernyshov, A. Bosak, V. Dmitriev, Y. Filmchuk and H. Hagemann, Phys. Rev. B 78 (2008)172104. [6] H. Hagemann, S. Gomes, G. Renaudin and K. Yvon, J. Alloys Compd. 363 (2004) 126. [7] Y. Filinchuk, D. Chernyshov and V. Dmitriev, Z. Kristallogr. 223 (2008) 649. [8] Z.Xiao Dong, J.Z. Yi, Z. Bo, H. Z. Feng and H.Y. Qing, Chin. Phys. Lett. 28(2011)076201. [9] T. Ghellab, Z. Charifi, H. Baaziz, Ş. Uğur, G. Uğur and F. Soyalp, Phys. Scr. 91 (2016) 045804. [10] S. Bae, S. Gim, H. Kim and K. Hanna, Appl. Catal. B: Environm. 182 (2016) 541. [11] G. Renaudin, S. Gomes, H. Hagemann, L. Keller and K. Yvon, J Alloys Compd. 375 (2004) 98. [12] P. Vajeeston, P. Ravindran, A. Kjekshus and H. Fjellvåg, J Alloys Compd. 387 (2005) 97. [13] S. Orimo, Y. Nakamori, J.R. Eliseo, A. Zuttel and C. M. Jensen, Chem. Rev. 107 (2007) 4111. [14] A. Istek and E. Gonteki, J. Environ. Bio.7 (2009) 951. [15] R. S. Kumar and A.L. Cornelinus, Appl. Phys. Lett. 87 (2005) 261916. [16] E. Kim, R. Kumar, P. F. Weck, A. L. Cornelius, M. Nicol, S. C. Vogel, J. Zhang, M. Hartl, A.C. Stowe, L. Daemen and Y. Zhao, J. Phys. Chem. Lett. B 111 (2007) 13873. [17] K. Brugger, Phys. Rev. 133 (1964) A1611. [18] P.B. Ghate, Phy. Rev. 139 (1965) A1666 [19] S. Mori, Y. Hiki, J. Phys. Soc. Jpn. 45 (1975) 1449. [20] V. Bhalla, R. Kumar, C. Tripathy and D. Singh, Int. J. Mod. Phys. B 27 (2013) 1350116. [21] D. Singh, S. Kaushik, S. Tripathi, V. Bhalla and A. K. Gupta, Arab. J. Sci. Eng. 39 (2014) 485. [22] K. Brugger, Phys. Rev.137 (1965) 1826. [23] W. P. Mason, Physical Acoustics, vol. IIIB, Academic Press, New York, 1965. [24] M.P. Tosi, Solid State Physics, vol. 12, Academic Press, New York, 1965. [25] Y. Nakamori and S. Orimo, J. Alloy Compd.370(2004)271. [26] D. Singh, D.K. Pandey and P.K. Yadawa, Cent. Eur. J. Phys. 7 (2009) 198. [27] V. Bhalla, D. Singh, G. Mishra and M. Wan, J. Pure Appl. Ultrason. 38 (2016)23. [28] D. Singh, S. Kaushik, S.K. Pandey, G. Mishra and V. Bhalla, VNU J. Sc.: Math. Phys. 32(2016)43. [29] J.P.Watt and L. Peselnick, J.Appl. Phys. 51 (1980) 1525. [30] S.F.Pugh, Philos.Mag. 45 (1954) 823. [31] V. Bhalla, D. Singh and S.K. Jain, Int. J. Thermophys. 37(2016)33. [32] V. Bhalla, D. Singh, S.K. Jain and R. Kumar, Pramana- J. Phys. 86 (2016)135.</jats:p
Electronic structure, optical and thermodynamic properties of ternary hydrides MBeH3 (M = Li, Na, and K)
No full textWOS: 000383768200010Electronic band structure, optical and thermodynamic properties of ternary hydrides MBeH3 (M = Li, Na, and K) were studied using ab initio density functional theory (DFT). The effect of the adopted approximation to the exchange-correlation functional of the DFT is explicitly investigated by considering four different expressions of two different classes (local-density approximation and generalized-gradient approximation). The calculated magnitude of B classifies MBeH3 (M = Li, Na, and K) as easily compressible materials. The bonding interaction in these compounds is quite complicated. The interaction between M and BeH6 is ionic and that between Be and H comprises both ionic and covalent characters. The electronic structure of the complex hydride was investigated by calculating the partial and total densities of states, and electron charge density distribution. Large gaps in the density of states appear at the Fermi energy of LiBeH3, NaBeH3, and KBeH3 indicating that these classes of hydrides are insulators. Optical properties, including the dielectric function, reflectivity, and absorption coefficient, each as a function of photon energy, are calculated and show an optical anisotropy for LiBeH3 and KBeH3. Through the quasi-harmonic Debye model, in which the phononic effects are considered, temperature dependence of volume V(T), bulk modulus B(T), and thermal expansion coefficient alpha(T), constant-volume and constant-pressure specific heat (C-v and C-p) and Debye temperature Theta(D), the entropy S, and the Gruneisen parameter gamma were calculated at wide pressure and temperature ranges. The principal aspect of the obtained results is the close similarity of MBeH3 (M = Li, Na, and K) compounds.Algerian University research project (CNEPRU) [D05620140014]This work is supported by the Algerian University research project (CNEPRU) under grant No. D05620140014
