Artur Tamm's Publications: Difference between revisions
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Measurement of collisional quenching rate of nitrogen states <math> N_2^{} (C^3 \Pi_u , \nu = 0) </math> and <math>N_2^+ (B^2 \Sigma_g^+ , \nu = 0) </math> | Measurement of collisional quenching rate of nitrogen states <math> N_2^{} (C^3 \Pi_u , \nu = 0) </math> and <math>N_2^+ (B^2 \Sigma_g^+ , \nu = 0) </math> | ||
F Valk , M Aints , P Paris , T Plank , J Maksimov and A Tamm | F. Valk , M. Aints , P. Paris , T. Plank , J. Maksimov and A. Tamm | ||
D. Appl. Phys. 43, 385202 (2010 doi: [http://dx.doi.org/10.1088/0022-3727/43/38/385202 10.1088/0022-3727/43/38/385202] | |||
Revision as of 18:16, 23 April 2015
Minu nimega artiklid
2014
First-principles study of point defects at a semicoherent interface.
E. Metsanurk, A. Tamm, A. Caro, A. Aabloo and M. Klintenberg
Sci. Rep. 4, 7567 (2014) doi: 10.1038/srep07567
Measurement of collisional quenching rate of nitrogen states [math] N_2^{} (C^3 \Pi_u , \nu = 0) [/math] and [math]N_2^+ (B^2 \Sigma_g^+ , \nu = 0) [/math]
F Valk , M Aints , P Paris , T Plank , J Maksimov and A Tamm
2010 J. Phys. D: Appl. Phys. 43 385202 doi: 10.1088/0022-3727/43/38/385202
2010
Measurement of collisional quenching rate of nitrogen states [math] N_2^{} (C^3 \Pi_u , \nu = 0) [/math] and [math]N_2^+ (B^2 \Sigma_g^+ , \nu = 0) [/math]
F. Valk , M. Aints , P. Paris , T. Plank , J. Maksimov and A. Tamm
D. Appl. Phys. 43, 385202 (2010 doi: 10.1088/0022-3727/43/38/385202