TY - JOUR
T1 - Electromigration behaviors of Ge2Sb2Te5 chalcogenide thin films under DC bias
AU - Huang, Yin Hsien
AU - Hang, Chi Hang
AU - Huang, Yu Jen
AU - Hsien, Tsung-Eong
PY - 2013/1/1
Y1 - 2013/1/1
N2 - Electromigration (EM) behaviors of pristine Ge2Sb 2Te5 (GST), nitrogen-doped GST (N-GST) and ceriumdoped GST (Ce-GST) thin-film strips under DC bias are presented. The mean-time-to-failure (MTTF) analysis based on the Black equation found that the EM failure times at room temperature are 1.2 × 104, 40 and 9.2 × 10 2 years and the activation energies (Ea) of EM process are 1.07, 0.57 and 0.68 eV for GST, N-GST and Ce-GST, respectively. Moreover, the calibration of the current density exponent, n, of Black's equation found n values are close to 2 for all samples, implying the dominance of grain boundary diffusion during the mass transport of EM process. For doped GSTs, the inferior EM failure lifespans and smaller Ea values were ascribed to the grain refinement effect which increases the number of grain boundaries in such samples. It consequently promoted the short-circuit diffusion and accelerated the EM failure in doped GSTs. The Blech-type tests on GSTs found that the threshold product, i.e., the product of current density and sample length ((j.L)th), is 200 A/cm for GST, 50 A/cm for N-GST and 66.67 A/cm for Ce-GST. Moreover, the product of diffusivity and effective charge number (i.e., DZ*) for GST, N-GST and Ce-GST was 2.0 × 10-7, 4.5 × 10-6 and 3.8 × 10-6 cm2/sec, respectively. Analytical results illustrated that the electrostatic force effect dominates the EM failure in samples with short strip lengths while the electron-wind force effect dominates the EM failure in samples with long strip lengths. Doping might alleviate the mass segregation in GST; however, its effect was moderate.
AB - Electromigration (EM) behaviors of pristine Ge2Sb 2Te5 (GST), nitrogen-doped GST (N-GST) and ceriumdoped GST (Ce-GST) thin-film strips under DC bias are presented. The mean-time-to-failure (MTTF) analysis based on the Black equation found that the EM failure times at room temperature are 1.2 × 104, 40 and 9.2 × 10 2 years and the activation energies (Ea) of EM process are 1.07, 0.57 and 0.68 eV for GST, N-GST and Ce-GST, respectively. Moreover, the calibration of the current density exponent, n, of Black's equation found n values are close to 2 for all samples, implying the dominance of grain boundary diffusion during the mass transport of EM process. For doped GSTs, the inferior EM failure lifespans and smaller Ea values were ascribed to the grain refinement effect which increases the number of grain boundaries in such samples. It consequently promoted the short-circuit diffusion and accelerated the EM failure in doped GSTs. The Blech-type tests on GSTs found that the threshold product, i.e., the product of current density and sample length ((j.L)th), is 200 A/cm for GST, 50 A/cm for N-GST and 66.67 A/cm for Ce-GST. Moreover, the product of diffusivity and effective charge number (i.e., DZ*) for GST, N-GST and Ce-GST was 2.0 × 10-7, 4.5 × 10-6 and 3.8 × 10-6 cm2/sec, respectively. Analytical results illustrated that the electrostatic force effect dominates the EM failure in samples with short strip lengths while the electron-wind force effect dominates the EM failure in samples with long strip lengths. Doping might alleviate the mass segregation in GST; however, its effect was moderate.
KW - Black's theory
KW - Blech structure
KW - Chalcogenides
KW - Electromigration
KW - Phase-change random access memory
UR - http://www.scopus.com/inward/record.url?scp=84884278178&partnerID=8YFLogxK
U2 - 10.1016/j.jallcom.2013.06.129
DO - 10.1016/j.jallcom.2013.06.129
M3 - Article
AN - SCOPUS:84884278178
VL - 580
SP - 449
EP - 456
JO - Journal of Alloys and Compounds
JF - Journal of Alloys and Compounds
SN - 0925-8388
ER -