<?xml version="1.0" encoding="utf-8"?>
<rss version="2.0" xml:base="http://www.tibercad.org" xmlns:dc="http://purl.org/dc/elements/1.1/">
<channel>
 <title>tiberCAD - Article</title>
 <link>http://www.tibercad.org/taxonomy/term/21/0</link>
 <description>Tag for article that show/describe tool capabilities</description>
 <language>en</language>
<item>
 <title>Multiscale Simulation of MOSFETs based on high-k oxides</title>
 <link>http://www.tibercad.org/sample_application/article/multiscale_simulation_mosfets_based_high_k_oxides</link>
 <description>&lt;p align=&quot;justify&quot;&gt;
In the following we will show an advanced application of &lt;strong&gt;&lt;em&gt;tiber&lt;/em&gt;CAD&lt;/strong&gt; which involves atomistic calculations based on the &lt;strong&gt;Empirical Tight Binding (ETB)&lt;/strong&gt; approach.
&lt;/p&gt;
&lt;p align=&quot;justify&quot;&gt;
This feature is not yet implemented in the current version 2.0, but it will be available from the next &lt;strong&gt;&lt;em&gt;tiber&lt;/em&gt;CAD&lt;/strong&gt; release. 
&lt;/p&gt;
&lt;p align=&quot;justify&quot;&gt;
Here we  present a &lt;strong&gt;multiscale simulation&lt;/strong&gt; approach to simulation of MOSFET devices. This kind of simulation includes both macroscopic drift-diffusion current model and quantum tunneling model. The models are solved together in a self-consistent way. As an example, we study the subthreshold transfer characteristics of MOSFETs based on high-k oxides. We compare the high-k gates based on HfO&lt;sub&gt;2&lt;/sub&gt; and ZrO&lt;sub&gt;2&lt;/sub&gt; with a SiO&lt;sub&gt;2&lt;/sub&gt; gate of the same equivalent thickness and show the effect of the gate oxide tunneling current on transistor performance.
&lt;/p&gt;
&lt;p&gt;&lt;a href=&quot;http://www.tibercad.org/sample_application/article/multiscale_simulation_mosfets_based_high_k_oxides&quot;&gt;read more&lt;/a&gt;&lt;/p&gt;</description>
 <category domain="http://www.tibercad.org/sample_applications/article">Article</category>
 <pubDate>Mon, 24 Sep 2012 12:11:09 +0000</pubDate>
 <dc:creator>stefanob</dc:creator>
 <guid isPermaLink="false">117 at http://www.tibercad.org</guid>
</item>
<item>
 <title>Selfconsistent EFA-Drift-diffusion 3D calculation for a GaAs quantum well in a nanocolumn</title>
 <link>http://www.tibercad.org/applications/selfconsistent_efa_drift_diffusion_3d_gaas_quantum_well</link>
 <description>&lt;p&gt; &lt;a title=&quot;top&quot; name=&quot;top&quot;&gt;&lt;/a&gt; &lt;/p&gt;
&lt;p style=&quot;text-align: justify&quot;&gt; In this application,  we show the results of fully &lt;b&gt;Self-Consistent Schroedinger (EFA) - Drift-diffusion&lt;/b&gt; calculations for a &lt;b&gt;3D&lt;/b&gt;  nanostructure: an &lt;b&gt;AlGaAs &lt;/b&gt;rectangular nanocolumn p-i-n diode structure with  an embedded  &lt;b&gt; GaAs quantum  well. &lt;/b&gt; &lt;/p&gt;
&lt;p&gt; Here is an overview of  the approach  chosen for  &lt;b&gt;self-consistent &lt;/b&gt;calculation in &lt;b&gt;&lt;i&gt;tiberCAD&lt;/i&gt;&lt;/b&gt;. &lt;/p&gt;
&lt;p style=&quot;text-align: justify&quot;&gt; First, the solution of the eigenvalue problems resulting from the &lt;b&gt;quantum EFA&lt;/b&gt; model provides the energy spectrum and  the particle densities. The particle densities are calculated by populating the electron and hole states according to the expectation value of the corresponding electrochemical potential;  then  they are fed back to the Poisson/drift-diffusion model for self-consistent Schroedinger–Poisson/drift-diffusion calculations. These can be classified as &lt;b&gt;overlap&lt;/b&gt; type simulations, where the results of the nanoscale calculation acts as an input – e.g. in form of parameters – to the microscale simulation. &lt;/p&gt;
&lt;p&gt;&lt;a href=&quot;http://www.tibercad.org/applications/selfconsistent_efa_drift_diffusion_3d_gaas_quantum_well&quot;&gt;read more&lt;/a&gt;&lt;/p&gt;</description>
 <category domain="http://www.tibercad.org/sample_applications/article">Article</category>
 <pubDate>Mon, 26 Oct 2009 12:08:37 +0000</pubDate>
 <dc:creator>sacconi</dc:creator>
 <guid isPermaLink="false">105 at http://www.tibercad.org</guid>
</item>
<item>
 <title>Calculation of the electronic and optical properties of an AlGaN/GaN LED diode</title>
 <link>http://www.tibercad.org/applications/electronic_optical_properties_algan_gan_led_diode</link>
 <description>&lt;p&gt;
&lt;a title=&quot;top&quot; name=&quot;top&quot;&gt;&lt;/a&gt;
&lt;/p&gt;
&lt;p style=&quot;text-align:justify;&quot;&gt;
In this application, we show a 1D calculation of quantum and optical properties of a &lt;b&gt;AlGaN/GaN LED diode&lt;/b&gt; with three GaN quantum wells. 
&lt;/p&gt;
&lt;p style=&quot;text-align:justify;&quot;&gt;
The simulated structure is the following:&lt;br /&gt;
After a buffer n-doped AlGaN layer, a Al&lt;sub&gt;0.78&lt;/sub&gt;InN barrier layer is present, then a series of three AlGaN/GaN quantum wells, each 2 nm-wide, followed by a p-doped AlGaN layer.
&lt;/p&gt;
&lt;p style=&quot;text-align:justify;&quot;&gt;
In this wurtzite nitride heterostructure, strain and strain induced piezoelectric polarization play a fundamental role in the description of the electronic properties. In fact, on one hand, effects of strain on the conduction and band profiles have to be taken in account through the appropriate &lt;i&gt;&lt;b&gt;k.p&lt;/b&gt;&lt;/i&gt; model and, on the other hand, the piezoelectric polarization term, together with the spontaneous polarization one, have  to be included in the Poisson-Drift-Diffusion calculations.
&lt;/p&gt;
&lt;p&gt;&lt;a href=&quot;http://www.tibercad.org/applications/electronic_optical_properties_algan_gan_led_diode&quot;&gt;read more&lt;/a&gt;&lt;/p&gt;</description>
 <category domain="http://www.tibercad.org/sample_applications/article">Article</category>
 <pubDate>Sat, 21 Feb 2009 12:42:16 +0000</pubDate>
 <dc:creator>sacconi</dc:creator>
 <guid isPermaLink="false">95 at http://www.tibercad.org</guid>
</item>
<item>
 <title>Strain and transport properties in AlGaN nanocolumns with a GaN Quantum Disk</title>
 <link>http://www.tibercad.org/sample_applications/strain_transport_heterostructure</link>
 <description>&lt;p&gt;
In the last couple of years a huge effort has been devoted to achieve and to control
the growth of III-nitride columnar-shaped nanostructures: nanorods,
nanocolumns, nanopillars. Results have shown, so far, an extremely high crystal
quality of the AlGaN nanocolumns, that are strain-free and have no dislocations
or other extended defects, thus, yielding an outstanding emission efficiency. The
achievement of nanocolumnar heterostructures including quantum disks (QDisks) and
nanocavities with QDisks and Bragg mirrors have  been reported.
&lt;/p&gt;
&lt;p&gt;&lt;a href=&quot;http://www.tibercad.org/sample_applications/strain_transport_heterostructure&quot;&gt;read more&lt;/a&gt;&lt;/p&gt;</description>
 <category domain="http://www.tibercad.org/sample_applications/article">Article</category>
 <pubDate>Tue, 13 Nov 2007 14:42:23 +0000</pubDate>
 <dc:creator>sacconi</dc:creator>
 <guid isPermaLink="false">36 at http://www.tibercad.org</guid>
</item>
</channel>
</rss>
