APS March Meeting 2011
Volume 56, Number 1
Monday–Friday, March 21–25, 2011;
Dallas, Texas
Session Q28: Focus Session: Carbon Nanotubes and Related Materials: Devices II
11:15 AM–2:15 PM,
Wednesday, March 23, 2011
Room: C156
Sponsoring
Unit:
DMP
Chair: David Tomanek, Michigan State University
Abstract ID: BAPS.2011.MAR.Q28.7
Abstract: Q28.00007 : Carbon nanotubes for interconnects in integrated circuits
12:27 PM–1:03 PM
Preview Abstract
Abstract
Author:
Jean Dijon
(CEA/Liten)
Carbon nanotubes are one of the materials that may be used for advanced
interconnects beyond the 16nm node thanks to there extreme resistance to
electro migration and to bottom up approach which allow to grow them in tiny
holes with very high aspect ratio. The resistance of a via with area A and
height h filled with CNT is expressed by $R_{via} =\frac{rq+rsh+rc}{Ad_t }$
where rq, rs, rc are respectively the 6.5k$\Omega $ quantum resistance, the
scattering resistance and the contact resistances of one tube. To be
competitive with copper via resistance, a large density d$_{t}$ of carbon
walls have to be paralleled. Following ITRS needs a density of 2 or 3
10$^{13 }$cm$^{-2}$ conducting CNT walls have to be obtained. This optimum
wall density requests the growth of highly packed few nanometre diameter
CNTs. Such density has been the main bottleneck for the development of CNT
interconnects. Recently ultra high density integration scheme have been
demonstrated and for the first time wall density close to the requested one
have been integrated in devices. Such density comes from the development on
conductive substrates of a CNT growth mode normally used to obtain forests
of small tube diameter on insulating substrate like alumina. With this mode,
CNTs are grown with base growth mode which is the mode requested for SWCNT
or DWCNT thus by continuity it will be possible to increase the density
still further by increasing the density of catalyst particles. Our bottom
metal of choice is AlCu with iron as catalyst. With this system tube contact
resistance between 10$^{4}$ to 10$^{6}$ Ohm have been measured on blanket
AlCu substrates. This resistance must be decreased by one or two order of
magnitude while increasing further CNT density. In this paper we will
present our last integration developments and the role of plasma
pre-treatment of the iron aluminium interface in order to decrease the
contact resistance. We will show that the bottom profile of via has a major
impact on the quality of CNT growing in the holes and discuss future
evolutions of this technology.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2011.MAR.Q28.7