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        <identifier>oai:www.ideals.illinois.edu:2142/18640</identifier>
        <datestamp>2023-07-10</datestamp>
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          <dc:contributor>Adesida, Ilesanmi</dc:contributor>
          <dc:contributor>Adesida, Ilesanmi</dc:contributor>
          <dc:contributor>Jain, Kanti</dc:contributor>
          <dc:contributor>Kim, Kyekyoon</dc:contributor>
          <dc:contributor>Bishop, Stephen G.</dc:contributor>
          <dc:creator>Yeo, Eng Guan</dc:creator>
          <dc:date>2011-01-21T22:52:48Z</dc:date>
          <dc:date>2011-01-21T22:52:48Z</dc:date>
          <dc:date>2013-01-22T11:00:18Z</dc:date>
          <dc:date>2011-01-21T22:52:48Z</dc:date>
          <dc:date>2010-12</dc:date>
          <dc:description>Phase change random access memory (PCRAM) is a leading contender for next generation nonvolatile
memory. The phase change mechanism from high resistance amorphous phase to low
resistance crystalline phase in nano-timescale is the most important characteristic of these
materials. However, full understanding of the mechanism is still not achieved.
Two time parameters were identified from the transient waveform, namely the delay and current
recovery times. The link between crystallization kinetics and the transient phase change effect
was established by associating nucleation with delay time and growth with current recovery time.
Real-time crystallization characterization was achieved.
Parasitic capacitance had strong implications on the programming performance of PCRAM.
Larger parasitic capacitance results in a larger leakage current, and hence higher applied voltage
for RESET operation needs to be applied. The larger parasitic capacitance also results in an
increased quenching time due to a longer voltage fall time, which results in a partially
crystallized amorphous state.
Continuing work is studying the effect of filament formation on phase change. Filament
formation is linked to the actual operating performance of the PCRAM device. This link is
important in understanding how phase change occurs electrically and whether filament formation
has any effect on scaling of PCRAM devices.</dc:description>
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          <dc:description>Item released from any restrictions by Sarah Shreeves (sshreeve@illinois.edu) on 2013-01-22T11:00:18Z</dc:description>
          <dc:identifier>http://hdl.handle.net/2142/18640</dc:identifier>
          <dc:language>en</dc:language>
          <dc:rights>Copyright 2010 Eng Guan Yeo</dc:rights>
          <dc:subject>phase change memory</dc:subject>
          <dc:subject>Phase change random access memory (PCRAM)</dc:subject>
          <dc:subject>transient effect</dc:subject>
          <dc:subject>time-resolved</dc:subject>
          <dc:subject>filament</dc:subject>
          <dc:title>Transient phase change effect in phase change memory devices</dc:title>
          <degree>
            <department>Electrical &amp; Computer Eng</department>
            <departmentCode>1933</departmentCode>
            <discipline>Electrical &amp; Computer Engr</discipline>
            <disciplineCode>1200</disciplineCode>
            <grantor>University of Illinois at Urbana-Champaign</grantor>
            <level>Dissertation</level>
            <name>Ph.D.</name>
            <program>PHD:Electr &amp; Computer Eng-UIUC</program>
            <programCode>10KS1200PHD</programCode>
          </degree>
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