Updates to publications and links

2018-04-23 15:10:05 +02:00 · 2018-04-23 15:10:05 +02:00 · 7f83a351a8
commit 7f83a351a8
parent 4551e8cc05
11 changed files with 1477 additions and 1577 deletions
--- a/.DS_Store
+++ b/.DS_Store
--- a/analysis/detail1.html
+++ b/analysis/detail1.html
@ -56,12 +56,11 @@
                  absorption spectrum which has a pronounced collection of
                  strength in the region of the Mie plasmon. TDLDA driven with
                  small amplitude excitations allows to explore the optical
-                  response [<a href="../literatur.html#own1155">9</a>]. The
+                  response [<a href="../publications.html#Cal97">Cal97</a>]. The
                  figure beneath shows results for Na<sub>8</sub><sup>+</sup> as
-                  example (taken from [<a href="../literatur.html#own1315"><font
-                      color="red">???</font></a>])
+                  example (taken from [<a href="../publications.html#Leg06">Leg06</a>])
                  in comparison to experiment (upper panel) and CI calculations
-                  (<font color="red"><b>???</b></font>)(second from above). The
+                  (second from above). The
                  overall position of the peak strength is nicely reproduced by
                  all methods, even by the semiclassical approach. CI produces
                  the most detailed spectrum. The green bars show the discrete
@ -86,10 +85,10 @@
                  Laser induced direct photo-emission of electrons allows to
                  conclude on the clusters single-electron states by measuring
                  the photo-electron spectra (PES). TDLDA with appropriate
-                  self-interaction correction (SIC) [<a href="../literatur.html#own1252">277</a>]
-                  allows to simulate that process in detail [<a href="../literatur.html#own1227">251</a>]
+                  self-interaction correction (SIC) [<a href="../publications.html#Leg02">Leg02</a>]
+                  allows to simulate that process in detail [<a href="../publications.html#Poh00">Poh00</a>]
                  . The figure to the left shows two examples for two clusters
-                  which are nearly spherical (taken from [<a href="../literatur.html#own1285">304</a>]).
+                  which are nearly spherical (taken from [<a href="../publications.html#Poh03">Poh03</a>]).
                  The arrows indicate the level classification according to
                  principal quantum number and angular momentum. The PES depend,
                  of course, on the direction of emission (checked here are the
@ -112,7 +111,7 @@
                  allows an enormous manifold of P&amp;P scenarios. The figure
                  to the right sketches a simple and robust scenario for a
                  nearly spherical cluster, actually Na<sub>41</sub><sup>+</sup>
-                  [<a href="../literatur.html#own1246">290</a>]. The idea is to
+                  [<a href="../publications.html#And02">And02</a>]. The idea is to
                  map the radius vibrations of the cluster by an off-resonant
                  laser pulse. The pump pulse ionizes the Na<sub>41</sub><sup>+</sup>
                  within 50 fs by three more charge units, see second panel from
--- a/analysis/detail2.html
+++ b/analysis/detail2.html
@ -60,7 +60,7 @@
                  <img src="figs/MD_fig5.gif" width="300" align="right" /> The
                  figure to the right shows the result of a molecular dynamics
                  simulation of electronic and ionic dynamics of Na<sub>41</sub><sup>+</sup>
-                  under the influence of strong laser fields [<a href="../literatur.html#own1308">332</a>].
+                  under the influence of strong laser fields [<a href="../publications.html#Bel06">Bel06</a>].
 Ionization
                  is drawn as function of laser intensity. One sees a sharp kink
                  at a critical intensity of I = 10<sup>16</sup> W/cm<sup>2</sup>.
--- a/publications.html
+++ b/publications.html
--- a/publications.html.bak
+++ b/publications.html.bak
--- a/publications_old.html
+++ b/publications_old.html
--- a/pubs.html.bak
+++ b/pubs.html.bak
--- a/research.html
+++ b/research.html
--- a/tddft-md/detailQMMM.html
+++ b/tddft-md/detailQMMM.html
@ -1,4 +1,4 @@
-<!DOCTYPE html PUBLIC "-//W3C//DTD XHTML 1.0 Transitional//EN" "http://www.w3.org/TR/xhtml1/DTD/xhtml1-transitional.dtd">
<html xmlns="http://www.w3.org/1999/xhtml">
  <head>
    <meta http-equiv="content-type" content="application/xhtml+xml; charset=iso-8859-1" />
    <title>Theory of Cluster Dynamics</title>
    <link href="../style.css" rel="stylesheet" type="text/css" />
  </head>
  <body>
    <div id="container">
      <div id="header">
        <div id="menu">
          <div id="navMenu">
            <ul>
              <li style="margin-top:1px;border-top:1px solid #B0C4DE; "><a href="../index.html">Home</a></li>
              <li><a href="../intro.html">Introductory Overview</a></li>
              <li><a href="../research.html">Scientific Information</a></li>
              <li><a href="../staff.html">Staff</a></li>
              <li><a href="../publications.html">Publications/Talks</a></li>
              <li><a href="../contact.html">Contact</a></li>
            </ul>
          </div>
        </div>
        <div id="image">
          <p><font size="6" color="white"><b>Theory of Cluster Dynamics</b></font><font
              size="5"><br />
            </font><font size="6"> </font><font size="5">The Toulouse -
              Erlangen Collaboration</font></p>
        </div>
        <a name="oben"> </a>
        <div id="content"><a name="oben"> </a>
          <div style="margin:15px;width:770px;border:1px solid gray;float:left;font-size:10px;"><a
              name="oben">
            </a>
            <div style="width:180px;float:left;text-align:center;font-size:10px"><a
                name="oben">
              </a><a href="formal.html">1. Theoretical developments </a> </div>
            <div style="width:200px;float:left;text-align:center;font-size:10px;">
              <a href="../analysis/detail1.html"> 2. Analysis of cluster
                dynamics </a> </div>
            <div style="width:200px;float:left;text-align:center;font-weight:900;font-size:10px;">
              <a href="../analysis/detail2.html"> 3. Clusters in strong external
                fields </a> </div>
            <div style="width:180px;float:left;text-align:center;font-weight:900;font-size:12px;">
              <a href="detailQMMM.html"> 4. Embedded clusters </a> </div>
          </div>
          <div id="WideContent">
            <div id="contentBoxWide">
              <div id="contentBoxHeader">
                <p> Clusters in contact with a polarizable environment</p>
              </div>
              <div id="contentBoxContent">
                <!-- START CONTENT HERE --> <br />
                <p><img src="figs/na8_nacl_SHG.gif" width="300" align="right" />
                  Many experiments are done for clusters in contact with a
                  substrate. The strong interface interaction modifies the
                  cluster and theoretical simulations become more involved.
                  However, some features can only be explored in connection with
                  a substrate. E.g., the symmetry breaking through a surface
                  gives access to second-harmonic generation (SHG). <br />
                  <br />
                  The figure beneath shows the results from a TDLDA simulation
                  of SHG for Na<sub>8</sub> attached to a NaCl surface [<a href="../literatur.html#own1224">248</a>].
+<!DOCTYPE html PUBLIC "-//W3C//DTD XHTML 1.0 Transitional//EN" "http://www.w3.org/TR/xhtml1/DTD/xhtml1-transitional.dtd">
<html xmlns="http://www.w3.org/1999/xhtml">
  <head>
    <meta http-equiv="content-type" content="application/xhtml+xml; charset=iso-8859-1" />
    <title>Theory of Cluster Dynamics</title>
    <link href="../style.css" rel="stylesheet" type="text/css" />
  </head>
  <body>
    <div id="container">
      <div id="header">
        <div id="menu">
          <div id="navMenu">
            <ul>
              <li style="margin-top:1px;border-top:1px solid #B0C4DE; "><a href="../index.html">Home</a></li>
              <li><a href="../intro.html">Introductory Overview</a></li>
              <li><a href="../research.html">Scientific Information</a></li>
              <li><a href="../staff.html">Staff</a></li>
              <li><a href="../publications.html">Publications/Talks</a></li>
              <li><a href="../contact.html">Contact</a></li>
            </ul>
          </div>
        </div>
        <div id="image">
          <p><font size="6" color="white"><b>Theory of Cluster Dynamics</b></font><font
              size="5"><br />
            </font><font size="6"> </font><font size="5">The Toulouse -
              Erlangen Collaboration</font></p>
        </div>
        <a name="oben"> </a>
        <div id="content"><a name="oben"> </a>
          <div style="margin:15px;width:770px;border:1px solid gray;float:left;font-size:10px;"><a
              name="oben">
            </a>
            <div style="width:180px;float:left;text-align:center;font-size:10px"><a
                name="oben">
              </a><a href="formal.html">1. Theoretical developments </a> </div>
            <div style="width:200px;float:left;text-align:center;font-size:10px;">
              <a href="../analysis/detail1.html"> 2. Analysis of cluster
                dynamics </a> </div>
            <div style="width:200px;float:left;text-align:center;font-weight:900;font-size:10px;">
              <a href="../analysis/detail2.html"> 3. Clusters in strong external
                fields </a> </div>
            <div style="width:180px;float:left;text-align:center;font-weight:900;font-size:12px;">
              <a href="detailQMMM.html"> 4. Embedded clusters </a> </div>
          </div>
          <div id="WideContent">
            <div id="contentBoxWide">
              <div id="contentBoxHeader">
                <p> Clusters in contact with a polarizable environment</p>
              </div>
              <div id="contentBoxContent">
                <!-- START CONTENT HERE --> <br />
                <p><img src="figs/na8_nacl_SHG.gif" width="300" align="right" />
                  Many experiments are done for clusters in contact with a
                  substrate. The strong interface interaction modifies the
                  cluster and theoretical simulations become more involved.
                  However, some features can only be explored in connection with
                  a substrate. E.g., the symmetry breaking through a surface
                  gives access to second-harmonic generation (SHG). <br />
                  <br />
                  The figure beneath shows the results from a TDLDA simulation
                  of SHG for Na<sub>8</sub> attached to a NaCl surface [<a href="../publications.html#Koh00">Koh00</a>].
                  The spectra resulting from irradiation with a 1.4 eV pulse
                  shows nicely the peaks at multiple frequencies. The SHG signal
                  can be enhanced by increasing the laser intensity. This,
                  however, breaks down at some point where the signals are
                  substantially broadened. This is caused by a large ionization
                  which spoils the otherwise clean dipole response of metal
                  clusters. </p>
                <br />
                <br />
                <p> <img src="figs/na6_ar384d_deposit.gif" width="300" align="left" />TDLDA
 coupled
-                  with molecular dynamics (MD) for ionic motion is a very
                  powerfull tool to describe cluster dynamics. One application
                  is cluster deposition which is illustrated in the figure on
                  the left. It shows Na<sub>6</sub> impinging on an Ar surface
                  (see [<a href="../literatur.html#own1303">328</a>] for further
                  details). The substrate consists of six layers of Ar taken
                  from an appropriate cut of the Ar fcc structure. The Na<sub>6</sub>
                  cluster consist in a ring of 5 ions topped by one ion on the
                  symmetry axix. The Na<sub>6</sub> approaches the surface with
                  the symmetry axis in <i>z</i> direction (=perpendicular) and
                  the top ion facing away from the surface. <br />
                  <br />
                  The upper panel shows the evolution of the <i>z</i>
                  coordinates, Na ions in red and Ar atoms in green. The cluster
                  is immediately stopped by the surface. A large fraction of
                  impact momentum is transferred at once to the substrate and
                  propagates with velocity of light through the layers. The
                  large dissipation through energy transfer and intrinsic
                  cluster excitation leads to catching of the cluster by the
                  subtrate. The kinetic energies in the lower panel confirm the
                  dramatic and very fast energy exchange at the moment of first
                  impact. Another fraction of energy, not shown in the figure,
                  is turned into the large shape changes. </p>
                <br />
                <br />
                <center>
                  <table width="70%">
                    <tbody>
                      <tr>
                        <td align="right"> <a href="#top">Back to top </a> </td>
                      </tr>
                    </tbody>
                  </table>
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          <p></p>
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  </body>
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+                  with molecular dynamics (MD) for ionic motion is a very
                  powerfull tool to describe cluster dynamics. One application
                  is cluster deposition which is illustrated in the figure on
                  the left. It shows Na<sub>6</sub> impinging on an Ar surface
                  (see [<a href="../publications.html#Feh06">Feh06</a>] for further
                  details). The substrate consists of six layers of Ar taken
                  from an appropriate cut of the Ar fcc structure. The Na<sub>6</sub>
                  cluster consist in a ring of 5 ions topped by one ion on the
                  symmetry axix. The Na<sub>6</sub> approaches the surface with
                  the symmetry axis in <i>z</i> direction (=perpendicular) and
                  the top ion facing away from the surface. <br />
                  <br />
                  The upper panel shows the evolution of the <i>z</i>
                  coordinates, Na ions in red and Ar atoms in green. The cluster
                  is immediately stopped by the surface. A large fraction of
                  impact momentum is transferred at once to the substrate and
                  propagates with velocity of light through the layers. The
                  large dissipation through energy transfer and intrinsic
                  cluster excitation leads to catching of the cluster by the
                  subtrate. The kinetic energies in the lower panel confirm the
                  dramatic and very fast energy exchange at the moment of first
                  impact. Another fraction of energy, not shown in the figure,
                  is turned into the large shape changes. </p>
                <br />
                <br />
                <center>
                  <table width="70%">
                    <tbody>
                      <tr>
                        <td align="right"> <a href="#top">Back to top </a> </td>
                      </tr>
                    </tbody>
                  </table>
                </center>
              </div>
            </div>
          </div>
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        <div id="footer">
          <p></p>
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--- a/tddft-md/formal.html
+++ b/tddft-md/formal.html
--- a/tddft-md/formal.html.bak
+++ b/tddft-md/formal.html.bak