Open main menu
Home
Random
Recent changes
Special pages
Community portal
Preferences
About Wikipedia
Disclaimers
Incubator escapee wiki
Search
User menu
Talk
Dark mode
Contributions
Create account
Log in
Editing
Phase-change memory
(section)
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
==Challenges== The greatest challenge for phase-change memory has been the requirement of high programming [[current density]] (>10<sup>7</sup>[[Ampere| A]]/cm<sup>2</sup>, compared to 10<sup>5</sup>...10<sup>6</sup> A/cm<sup>2</sup> for a typical [[transistor]] or [[diode]]). {{citation needed|date=June 2012}} The contact between the hot phase-change region and the adjacent [[dielectric]] is another fundamental concern. The dielectric may begin to leak [[Electric current|current]] at higher temperature, or may lose [[adhesion]] when expanding at a different rate from the phase-change material. Phase-change memory is susceptible to a fundamental tradeoff of unintended vs. intended phase-change. This stems primarily from the fact that phase-change is a thermally driven process rather than an electronic process. Thermal conditions that allow for fast [[crystallization]] should not be too similar to standby conditions, e.g. room temperature, otherwise data retention cannot be sustained. With the proper [[activation energy]] for crystallization it is possible to have fast crystallization at programming conditions while having very slow crystallization at normal conditions. Probably the biggest challenge for phase-change memory is its long-term [[Electrical resistance and conductance|resistance]] and [[threshold voltage]] drift.<ref>{{cite journal |first1=I.V. |last1=Karpov |first2=M. |last2=Mitra |first3=D. |last3=Kau |first4=G. |last4=Spadini |first5=Y.A. |last5=Kryukov |first6=V.G. |last6=Karpov |title=Fundamental drift of parameters in chalcogenide phase change memory |journal=J. Appl. Phys. |volume=102 |issue= 12|pages=124503β124503β6 |year=2007 |doi=10.1063/1.2825650 |bibcode=2007JAP...102l4503K }}</ref> The resistance of the [[Amorphous solid|amorphous]] state slowly increases according to a [[power law]] (~t<sup>0.1</sup>). This severely limits the ability for multilevel operation, since a lower intermediate state would be confused with a higher intermediate state at a later time, and could also jeopardize standard two-state operation if the threshold voltage increases beyond the design value. In April 2010, [[Numonyx]] released its Omneo line of parallel and serial interface 128 Mb [[NOR flash replacement]] PRAM chips. Although the NOR flash chips they intended to replace operated in the β40-85 Β°C range, the PRAM chips operated in the 0-70 Β°C range, indicating a smaller operating window compared to NOR flash. This is likely due to the use of highly temperature-sensitive [[pβn junction]]s to provide the high currents needed for programming.
Edit summary
(Briefly describe your changes)
By publishing changes, you agree to the
Terms of Use
, and you irrevocably agree to release your contribution under the
CC BY-SA 4.0 License
and the
GFDL
. You agree that a hyperlink or URL is sufficient attribution under the Creative Commons license.
Cancel
Editing help
(opens in new window)