Artur Tamm's Publications: Difference between revisions

From Intelligent Materials and Systems Lab

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E. Metsanurk, A. Tamm, A. Caro, A. Aabloo and M. Klintenberg
E. Metsanurk, A. Tamm, A. Caro, A. Aabloo and M. Klintenberg


Sci. Rep. 4, 7567 (2014) doi: [http://dx.doi.org/10.1038/srep07567]
Sci. Rep. 4, 7567 (2014) doi: [http://dx.doi.org/10.1038/srep07567 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>
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>

Revision as of 18:15, 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

2010 J. Phys. D: Appl. Phys. 43 385202 doi: 10.1088/0022-3727/43/38/385202