Institutionalizing the New System in North Korea, 1961-1971: Reformation of Elites, Resocialization of the Masses, and the Search for Legitimacy

Divided Korea ◽  
1975 ◽  
pp. 287-331
Keyword(s):  
Author(s):  
Son Daekwon

Abstract This article investigates the linkage between Kim Jong-un’s power consolidation and Pyongyang’s abrupt return to the denuclearization negotiation table in 2018. It argues that behind Pyongyang’s turnabout lie the three unstable pillars of the Kim family’s rule: a faithful winning coalition, the juche ideology, and Chinese patronage. Upon taking office in 2011, Kim had to debilitate his father’s winning coalition to consolidate his power. With the winning coalition enervated, Kim could not expect its willingness to suppress the masses were they to develop into an ejectorate, and therefore introduced market reforms to secure the people’s support. The reforms, in return, inevitably eroded the ideological appeal of the Kim family, thereby rendering his hold on power more vulnerable to economic pressure. Under such circumstances, Chinese patronage increasingly faltered. It is due to the instability of these three pillars that Kim Jong-un returned to the negotiating table.


Author(s):  
Charles W. Allen

With respect to structural consequences within a material, energetic electrons, above a threshold value of energy characteristic of a particular material, produce vacancy-interstial pairs (Frenkel pairs) by displacement of individual atoms, as illustrated for several materials in Table 1. Ion projectiles produce cascades of Frenkel pairs. Such displacement cascades result from high energy primary knock-on atoms which produce many secondary defects. These defects rearrange to form a variety of defect complexes on the time scale of tens of picoseconds following the primary displacement. A convenient measure of the extent of irradiation damage, both for electrons and ions, is the number of displacements per atom (dpa). 1 dpa means, on average, each atom in the irradiated region of material has been displaced once from its original lattice position. Displacement rate (dpa/s) is proportional to particle flux (cm-2s-1), the proportionality factor being the “displacement cross-section” σD (cm2). The cross-section σD depends mainly on the masses of target and projectile and on the kinetic energy of the projectile particle.


2011 ◽  
Vol 9 (7) ◽  
pp. 20-21
Author(s):  
BRUCE JANCIN
Keyword(s):  

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