<?xml version='1.0' encoding='UTF-8'?><?xml-stylesheet href="http://www.blogger.com/styles/atom.css" type="text/css"?><feed xmlns='http://www.w3.org/2005/Atom' xmlns:openSearch='http://a9.com/-/spec/opensearchrss/1.0/' xmlns:georss='http://www.georss.org/georss' xmlns:gd='http://schemas.google.com/g/2005' xmlns:thr='http://purl.org/syndication/thread/1.0'><id>tag:blogger.com,1999:blog-60030803362389929</id><updated>2012-02-16T13:29:09.513-05:00</updated><title type='text'>ITAMPblog</title><subtitle type='html'>Posts related to ITAMP, activities at ITAMP, and all things on ITAMP</subtitle><link rel='http://schemas.google.com/g/2005#feed' type='application/atom+xml' href='http://itamp.blogspot.com/feeds/posts/default'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default?max-results=100'/><link rel='alternate' type='text/html' href='http://itamp.blogspot.com/'/><link rel='hub' href='http://pubsubhubbub.appspot.com/'/><author><name>ITAMPbloger</name><uri>http://www.blogger.com/profile/12844502676999940232</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><generator version='7.00' uri='http://www.blogger.com'>Blogger</generator><openSearch:totalResults>16</openSearch:totalResults><openSearch:startIndex>1</openSearch:startIndex><openSearch:itemsPerPage>100</openSearch:itemsPerPage><entry><id>tag:blogger.com,1999:blog-60030803362389929.post-4762542417060075777</id><published>2012-02-16T11:53:00.035-05:00</published><updated>2012-02-16T13:29:09.524-05:00</updated><title type='text'>ITAMP Talks APS March March 2012</title><content type='html'>&lt;table&gt;&lt;tbody&gt;&lt;tr&gt;&lt;td valign="top"&gt;&lt;br /&gt;&lt;/td&gt;&lt;td valign="top"&gt;&lt;br /&gt;&lt;/td&gt;&lt;td valign="top"&gt;&lt;br /&gt;&lt;/td&gt;&lt;td valign="top"&gt;&lt;/td&gt;    &lt;td&gt;&lt;br /&gt;&lt;/td&gt;&lt;td&gt;&lt;br /&gt;&lt;/td&gt;&lt;td&gt;&lt;br /&gt;&lt;/td&gt;&lt;td&gt;&lt;br /&gt;&lt;/td&gt;&lt;td&gt;&lt;br /&gt;&lt;/td&gt;  &lt;/tr&gt;&lt;tr&gt;    &lt;td valign="top"&gt;&lt;br /&gt;&lt;/td&gt;    &lt;td&gt;&lt;div class="MsoNormal"&gt;&lt;b&gt;Aspuru-Guzik, Alan&lt;/b&gt;&lt;/div&gt;&lt;div class="MsoNormal"&gt;&lt;span style="font-family: Times; font-size: small;"&gt;V28.00004 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/165851"&gt;&lt;span style="color: blue;"&gt;Nonradiative lifetimes in intermediate band materials -- absence of lifetime recovery&lt;/span&gt;&lt;/a&gt;&lt;br /&gt;L35.00010 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/162980"&gt;&lt;span style="color: blue;"&gt;The  derivative discontinuity in density functional theory from an  electrostatic description of the exchange and correlation potential&lt;/span&gt;&lt;/a&gt;&lt;br /&gt;V48.00012 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/166069"&gt;&lt;span style="color: blue;"&gt;Accessing exciton transport in light-harvesting structures with plasmonic nanotip&lt;/span&gt;&lt;/a&gt;&lt;br /&gt;V34.00010 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/165927"&gt;&lt;span style="color: blue;"&gt;How much information do ultrafast spectra contain? The case for ultrafast quantum process tomography&lt;/span&gt;&lt;/a&gt;&lt;br /&gt;T30.00006 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/165266"&gt;&lt;span style="color: blue;"&gt;Algorithmic Quantum Cooling&lt;/span&gt;&lt;/a&gt;&lt;br /&gt;J34.00003 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/161989"&gt;&lt;span style="color: blue;"&gt;2-Dimensional  Fluorescence Spectroscopy: Determining the Temperature-Dependent  Conformations of Porphyrin Dimers and Nucleic Acids&lt;/span&gt;&lt;/a&gt;&lt;br /&gt;L36.00002 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/162983"&gt;&lt;span style="color: blue;"&gt;Study of excitonic energy transport in thin-film J-aggregates&lt;/span&gt;&lt;/a&gt;&lt;br /&gt;W41.00002 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/166613"&gt;&lt;span style="color: blue;"&gt;Absence of quantum oscillations in electronic excitation transfer in the Fenna-Matthews-Olson complex&lt;/span&gt;&lt;/a&gt;&lt;br /&gt;J30.00005 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/161945"&gt;&lt;span style="color: blue;"&gt;Quantum simulator of an open quantum system using superconducting qubits: exciton transport in photosynthetic complexes&lt;/span&gt;&lt;/a&gt;&lt;br /&gt;J34.00002 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/161988"&gt;&lt;span style="color: blue;"&gt;Conformation of self-assembled porphyrin dimers in liposome vesicles by phase-modulation 2D fluorescence spectroscopy&lt;/span&gt;&lt;/a&gt;&lt;br /&gt;X17.00004 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/166968"&gt;&lt;span style="color: blue;"&gt;Plasmonic nanotips for spectroscopy with nanometer-scale resolution&lt;/span&gt;&lt;/a&gt;&lt;br /&gt;W35.00009 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/162973"&gt;&lt;span style="color: blue;"&gt;Applying state-of-the-art signal processing to time-dependent density functional theory&lt;/span&gt;&lt;/a&gt;&lt;br /&gt;B7.00002 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/159413"&gt;&lt;span style="color: blue;"&gt;The  Harvard Clean Energy Project: High-throughput screening of organic  photovoltaic materials using cheminformatics, machine learning, and  pattern recognition&lt;/span&gt;&lt;/a&gt;&lt;br /&gt;B7.00001 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/159412"&gt;&lt;span style="color: blue;"&gt;The  Harvard Clean Energy Project: High-throughput screening of organic  photovoltaic materials using first-principles electronic structure  theory&lt;/span&gt;&lt;/a&gt;&lt;br /&gt;V35.00004 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/165933"&gt;&lt;span style="color: blue;"&gt;Time-dependent density functional theory for open quantum systems&lt;/span&gt;&lt;/a&gt;&lt;/span&gt;&lt;/div&gt;&lt;br /&gt;&lt;div class="MsoNormal"&gt;&lt;b&gt;Cappellaro, Paola&lt;/b&gt;&lt;/div&gt;&lt;div class="MsoNormal"&gt;K1.00260 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/162487"&gt;Composite-pulse magnetometry in the solid-state&lt;/a&gt;&lt;br /&gt;K1.00308 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/162536"&gt;Perfect mixed state quantum transport in correlated spin networks&lt;/a&gt;&lt;/div&gt;&lt;br /&gt;&lt;div class="MsoNormal"&gt;&lt;b&gt;Demler, Eugene&lt;br /&gt;&lt;/b&gt;J4.00001 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/161598"&gt;Non Equilibrium Quantum Criticality: an intuitive approach&lt;/a&gt;&lt;br /&gt;Z4.00003 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/167954"&gt;Collective mode of an impurity and a Tonks-Girardeau gas&lt;/a&gt;&lt;br /&gt;D4.00010 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/160357"&gt;Clustering of cold polar molecules in arrays of one-dimensional tubes&lt;/a&gt;&lt;br /&gt;V4.00001 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/165538"&gt;Doublon production rate by optical lattice modulation for strongly correlated Fermionic atoms&lt;/a&gt;&lt;br /&gt;D4.00007 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/160354"&gt;Tunable Superfluidity with Ultracold Polar Molecules on quasi-1D Optical Lattices&lt;/a&gt;&lt;br /&gt;J4.00003 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/161600"&gt;Stability of Counterflow Superfluidity&lt;/a&gt;&lt;br /&gt;A32.00015 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/159059"&gt;Photo-induced quantum Hall insulators without Landau levels&lt;/a&gt;&lt;br /&gt;D4.00006 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/160353"&gt;Quantum Magnetism with Polar Molecules: Tunable Generalized $t$-$J$ Model&lt;/a&gt;&lt;br /&gt;A8.00011 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/158737"&gt;Emergence and lifting of frustration for dipolar molecules&lt;/a&gt;&lt;/div&gt;&lt;div class="MsoNormal"&gt;&lt;br /&gt;&lt;b&gt;Feist, Johannes&lt;/b&gt;&amp;nbsp; &lt;br /&gt;D10.00005 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/160445"&gt;Accessing correlated electron motion on the attosecond timescale&lt;/a&gt;&lt;br /&gt;V48.00012 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/166069"&gt;Accessing exciton transport in light-harvesting structures with plasmonic  nanotip&lt;/a&gt;&lt;br /&gt;X17.00004 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/166968"&gt;Plasmonic nanotips for spectroscopy with nanometer-scale resolution&lt;/a&gt;&lt;br /&gt;V4.00013 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/165550"&gt;A Quantum Plasmonic Circuit for Cold Atoms&lt;/a&gt;&lt;br /&gt;A4.00003 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/158673"&gt;A nanoscale quantum interface for single atoms&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;/div&gt;&lt;b&gt;Laumann, Chris&amp;nbsp;&lt;/b&gt;&lt;br /&gt;K1.00283 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/162511"&gt;Topologically Protected Quantum State Transfer in a Chiral Spin Liquid&lt;/a&gt;&lt;br /&gt;D29.00009 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/160683"&gt;Long-range quantum gates using dipolar crystals&lt;/a&gt;&lt;b&gt;&amp;nbsp;&lt;/b&gt;&lt;br /&gt;T24.00005 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/165190"&gt;Microscopic Disorder-Based model for non-Abelian Quasi-Particles in $\nu=5/2$ FQH states&lt;/a&gt;&lt;/td&gt;&lt;/tr&gt;&lt;/tbody&gt;&lt;/table&gt;&lt;style&gt;@font-face {  font-family: "Cambria";}p.MsoNormal, li.MsoNormal, div.MsoNormal { margin: 0in 0in 0.0001pt; font-size: 12pt; font-family: "Times New Roman"; }a:link, span.MsoHyperlink { color: blue; text-decoration: underline; }a:visited, span.MsoHyperlinkFollowed { color: purple; text-decoration: underline; }div.Section1 { page: Section1; }&lt;/style&gt;     &lt;br /&gt;&lt;div class="MsoNormal"&gt;&lt;style&gt;@font-face {  font-family: "Cambria";}p.MsoNormal, li.MsoNormal, div.MsoNormal { margin: 0in 0in 0.0001pt; font-size: 12pt; font-family: "Times New Roman"; }a:link, span.MsoHyperlink { color: blue; text-decoration: underline; }a:visited, span.MsoHyperlinkFollowed { color: purple; text-decoration: underline; }div.Section1 { page: Section1; &lt;/style&gt;     &lt;/div&gt;&lt;div class="MsoNormal"&gt;&lt;br /&gt;&lt;/div&gt;&lt;div class="MsoNormal"&gt;&lt;b&gt;Lemeshko, Mikhail&lt;/b&gt;&lt;br /&gt;K1.00334 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/168987"&gt;Sensitive imaging of electromagnetic fields with cold polar molecules&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;b&gt;Lukin, Mikhail&amp;nbsp;&lt;/b&gt;&lt;br /&gt;D4.00007 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/160354"&gt;Tunable Superfluidity with Ultracold Polar Molecules on quasi-1D Optical Lattices&lt;/a&gt;&lt;br /&gt;A30.00010 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/159025"&gt;Towards Probing Living Cell Function with NV Centers in Nanodiamonds&lt;/a&gt;&lt;br /&gt;D4.00003 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/160350"&gt;Altering Photon Statistics  using Strong Rydberg Interactions&lt;/a&gt;&lt;br /&gt;D4.00002 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/160349"&gt;Towards single-photon optical nonlinearities using cold Rydberg atoms&lt;/a&gt;&lt;br /&gt;D4.00006 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/160353"&gt;Quantum Magnetism with Polar Molecules: Tunable Generalized $t$-$J$ Model&lt;/a&gt;&lt;br /&gt;A30.00006 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/159021"&gt;Decoherence imaging of spin ensembles by a scannable single nitrogen-vacancy  center in diamond&lt;/a&gt;&lt;br /&gt;V48.00012 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/166069"&gt;Accessing exciton transport in light-harvesting structures with plasmonic  nanotip&lt;/a&gt;&lt;br /&gt;A4.00003 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/158673"&gt;A nanoscale quantum interface for single atoms&lt;/a&gt;&lt;br /&gt;A4.00001 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/158671"&gt;A Light-Matter Interface with NV Centers&lt;/a&gt;&lt;br /&gt;V4.00013 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/165550"&gt;A Quantum Plasmonic Circuit for Cold Atoms&lt;/a&gt;&lt;br /&gt;A4.00002 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/158672"&gt;Probing the motion of a mechanical resonator via coherent coupling to a single spin qubit&lt;/a&gt;&lt;br /&gt;D29.00007 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/160681"&gt;Room temperature solid-state quantum bit with second-long memory&lt;/a&gt;&lt;br /&gt;D29.00005 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/160679"&gt;Optimizing the resolution and the sensitivity of a scanning NV magnetometer&lt;/a&gt;&lt;br /&gt;D29.00003 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/160677"&gt;Quantum interference of single photons from two remote Nitrogen-Vacancy centers in diamond&lt;/a&gt;&lt;br /&gt;D29.00010 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/160684"&gt;Magnetic imaging of a single electron spin using a scanning NV magnetometer  under ambient conditions&lt;/a&gt;&lt;br /&gt;X17.00004 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/166968"&gt;Plasmonic nanotips for spectroscopy with nanometer-scale resolution&lt;/a&gt;&lt;br /&gt;W41.00003 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/166614"&gt;Progress Towards Room-Temperature Electron Spin Detection in Biological Systems&lt;/a&gt;&lt;br /&gt;D29.00013 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/160687"&gt;Spectroscopy of composite solid-state spin environments for improved  metrology with spin ensembles&lt;/a&gt;&lt;br /&gt;B4.00005 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/159368"&gt;Coupling a single spin in diamond to the quantum motion of a mechanical cantilever&lt;/a&gt;&lt;br /&gt;L10.00003 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/162659"&gt;Quantum optics with solid-state atom-like systems&lt;/a&gt;&lt;br /&gt;A30.00005 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/159020"&gt;Cooling Nuclear Spins in Diamond via Dark State Spectroscopy&lt;/a&gt;&lt;br /&gt;A30.00003 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/159018"&gt;Quantum Optics with Spins and Photons in Diamond&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;b&gt;Mathy, Charles&lt;/b&gt;&lt;br /&gt;Z4.00003 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/167954"&gt;Collective mode of an impurity and a Tonks-Girardeau gas&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;div class="MsoNormal"&gt;&lt;b&gt;Onofrio, Roberto&lt;br /&gt;&lt;/b&gt;B1.00002 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/159336"&gt;Four techniques to achieve deeper Fermi degeneracy in Fermi-Bose mixtures&lt;/a&gt;&lt;br /&gt;B1.00003 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/159337"&gt;Optimized sympathetic cooling of atomic mixtures via fast adiabatic strategies&lt;/a&gt;&lt;/div&gt;&lt;/div&gt;&lt;div class="MsoNormal"&gt;&lt;b&gt;Rittenhouse, Seth&lt;/b&gt;&lt;br /&gt;D4.00011 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/160358"&gt;A dielectric superfluid of polar molecules&lt;/a&gt;&lt;/div&gt;&lt;div class="MsoNormal"&gt;&lt;br /&gt;&lt;/div&gt;&lt;b&gt;Safavi-Naini&lt;/b&gt;&lt;br /&gt;A.             A4.00010 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/158680"&gt;An ab-initio microscopic theory of anomalous heating in planar ion traps&lt;/a&gt;&lt;br /&gt;D4.00013 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/160360"&gt;Paired Phases of Dipoles in a Bilayer System&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;b&gt;Sadeghpour, H.R.&amp;nbsp;&lt;/b&gt;&lt;br /&gt;A4.00010 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/158680"&gt;An ab-initio microscopic theory of anomalous heating in planar ion traps&lt;/a&gt;&lt;br /&gt;D4.00013 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/160360"&gt;Paired Phases of Dipoles in a Bilayer System&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;style&gt;@font-face {  font-family: "Cambria";}p.MsoNormal, li.MsoNormal, div.MsoNormal { margin: 0in 0in 0.0001pt; font-size: 12pt; font-family: "Times New Roman"; }a:link, span.MsoHyperlink { color: blue; text-decoration: underline; }a:visited, span.MsoHyperlinkFollowed { color: purple; text-decoration: underline; }div.Section1 { page: Section1; }&lt;/style&gt;     &lt;br /&gt;&lt;style&gt;@font-face {  font-family: "Cambria";}p.MsoNormal, li.MsoNormal, div.MsoNormal { margin: 0in 0in 0.0001pt; font-size: 12pt; font-family: "Times New Roman"; }a:link, span.MsoHyperlink { color: blue; text-decoration: underline; }a:visited, span.MsoHyperlinkFollowed { color: purple; text-decoration: underline; }div.Section1 { page: Section1; }&lt;/style&gt;     &lt;br /&gt;&lt;div class="MsoNormal"&gt;&lt;style&gt;@font-face {  font-family: "Times";}@font-face {  font-family: "Cambria";}p.MsoNormal, li.MsoNormal, div.MsoNormal { margin: 0in 0in 0.0001pt; font-size: 12pt; font-family: "Times New Roman"; }div.Section1 { page: Section1; }&lt;/style&gt;     &lt;/div&gt;&lt;b&gt;Weimer, Hendrik&lt;br /&gt;&lt;/b&gt;K1.00283 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/162511"&gt;Topologically Protected Quantum State Transfer in a Chiral Spin Liquid&lt;/a&gt;&lt;br /&gt;&lt;div class="MsoNormal"&gt;&lt;br /&gt;&lt;div class="MsoNormal"&gt;&lt;b&gt;Yelin, Susanne&lt;br /&gt;&lt;/b&gt;A30.00005 &lt;a href="http://meetings.aps.org/Meeting/MAR12/Event/159020"&gt;Cooling Nuclear Spins in Diamond via Dark State Spectroscopy&lt;/a&gt;&lt;/div&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/60030803362389929-4762542417060075777?l=itamp.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://itamp.blogspot.com/feeds/4762542417060075777/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://itamp.blogspot.com/2012/02/font-face-font-family-cambriap.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/4762542417060075777'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/4762542417060075777'/><link rel='alternate' type='text/html' href='http://itamp.blogspot.com/2012/02/font-face-font-family-cambriap.html' title='ITAMP Talks APS March March 2012'/><author><name>ITAMPbloger</name><uri>http://www.blogger.com/profile/12844502676999940232</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-60030803362389929.post-737771093634047132</id><published>2012-01-09T18:37:00.001-05:00</published><updated>2012-01-09T18:45:58.957-05:00</updated><title type='text'>ITAMP/B2 Winter Graduate School on AMO Physics, Jan 8-20, 2012</title><content type='html'>The 1st morning session of the school went quite well. There were talks by Jun Ye (JILA) on control of light; how ultrafast laser pulses could be used to produce ultrastable frequency combs, and how different frequency scales, from UVU could be referenced to IR, a preview for his 2nd lecture tomorrow on controlling atomic matter with light. The 2nd talk was given by Pierre Meystre (replacing Mette Gaarde who could not be here) on cooling of optomechanical systems. This emerging subject of inquiry in AMO sciences has mushroomed over the last few years b/c a number of groups have succeeded in bringing the center of mass motion of nearly macroscopic objects to the quantum ground level. Pierre described what could be investigated with ground state objects, ala beyond ground state cooling.&lt;br /&gt;&lt;br /&gt;The afternoon talks are now being given by Ivan Deutsch (UNM) and Han Pu (Rice). Han is giving a rigorous account of theory of laser cooling.&lt;br /&gt;&lt;br /&gt;The students appear enthusiastic and engage the faculty with questions. The settings are beautiful- the mornings are quite and a bit chilly, and warming day hours which follow. The accommodations are first rate and comfortable.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/60030803362389929-737771093634047132?l=itamp.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://itamp.blogspot.com/feeds/737771093634047132/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://itamp.blogspot.com/2012/01/itampb2-winter-graduate-school-on-amo.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/737771093634047132'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/737771093634047132'/><link rel='alternate' type='text/html' href='http://itamp.blogspot.com/2012/01/itampb2-winter-graduate-school-on-amo.html' title='ITAMP/B2 Winter Graduate School on AMO Physics, Jan 8-20, 2012'/><author><name>ITAMPbloger</name><uri>http://www.blogger.com/profile/12844502676999940232</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-60030803362389929.post-6001580188179199411</id><published>2011-11-25T11:01:00.007-05:00</published><updated>2011-11-26T13:19:40.318-05:00</updated><title type='text'>A homonuclear molecule with a permanent dipole moment</title><content type='html'>Traditional wisdom tells us that homonuclear molecules cannot have a permanent dipole moment.  However, when one of the atoms in a diatomic molecule is in a highly excited Rydberg state, the exchange symmetry between the two atoms is broken.  In a &lt;a href="http://www.sciencemag.org/content/334/6059/1110.abstract"&gt;new article&lt;/a&gt; published today in Science [1], ITAMP postdoc Seth Rittenhouse and scientist Hossein Sadeghpour in collaboration with groups from the Max-Planck-Institut für Physik komplexer Systeme and the University of Stuttgart, we describe the first direct measurement of a homonuclear, diatomic molecule with a permanent electric dipole moment.&lt;br /&gt;&lt;br /&gt;Giant Rydberg molecules, first predicted over a decade ago [2], can bond courtesy of frequent scattering of the Rydberg electron off of a ground state atom.  These molecules were later observed spectroscopically in s-wave dominated states [3].  However, because the electronic distribution was assumed to be isotropic, it was thought that this type of molecule would not have any polar behavior.&lt;br /&gt;&lt;br /&gt;In our new work, we show that in truth a very small amount of the so-called "trilobite" state is admixed to the molecular electronic state resulting in appreciable dipole moments (on the order od 1 Debye).  This prediction is born out by the observation of a linear Stark shift a small fields in high precision spectroscopic measurements of the Stark map of homonuclear rubidium Rydberg molecules.&lt;br /&gt;&lt;br /&gt;&lt;a href="http://4.bp.blogspot.com/-nk4zG5qt_nY/TtAqBojr3vI/AAAAAAAAABg/Vd5nKr7MGNw/s1600/WFs.png"&gt;&lt;img alt="" border="0" id="BLOGGER_PHOTO_ID_5679085337669525234" src="http://4.bp.blogspot.com/-nk4zG5qt_nY/TtAqBojr3vI/AAAAAAAAABg/Vd5nKr7MGNw/s320/WFs.png" style="cursor: pointer; float: left; height: 103px; margin: 0pt 10px 10px 0pt; width: 311px;" /&gt;&lt;/a&gt;&lt;span style="font-size: 85%;"&gt;(a) The electron density for a Giant homonuclear molecule is show in cylindrical coordinates. (b) The trilobite-like electron density is shown after the isotropic amplitude has been subtracted. In both figures the Rb Rydberg core is at z = ρ = 0, the while the ground state atom is located z = 1900 atomic units&lt;/span&gt; &lt;span style="font-size: x-small;"&gt;(figure from Ref. [1])&lt;/span&gt;.&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;References:&lt;br /&gt;[1] W. Li, T. Pohl, J. M. Rost, S. T. Rittenhouse, H. R. Sadeghpour, J. Nipper, B. Butscher, J. B. Balewski,  V. Bendkowsky, R. Low and T. Pfau, &lt;a href="http://www.sciencemag.org/content/334/6059/1110.abstract"&gt;&lt;span style="font-style: italic;"&gt;Science&lt;/span&gt; &lt;span style="font-weight: bold;"&gt;334&lt;/span&gt;, 1110 (2011)&lt;/a&gt;.&lt;br /&gt;&lt;br /&gt;[2] H. R. Sadeghpour, A. S. Dickinson and C. H. Greene, &lt;a href="http://prl.aps.org/abstract/PRL/v85/i12/p2458_1"&gt;&lt;span style="font-style: italic;"&gt;Phys. Rev Lett.&lt;/span&gt; &lt;span style="font-weight: bold;"&gt;85&lt;/span&gt;, 2458 (2000)&lt;/a&gt;.&lt;br /&gt;&lt;br /&gt;[3] V. Bendkowsky &lt;span style="font-style: italic;"&gt;et al.&lt;/span&gt;, &lt;a href="http://www.nature.com/nature/journal/v458/n7241/full/nature07945.html"&gt;&lt;span style="font-style: italic;"&gt;Nature&lt;/span&gt; &lt;span style="font-weight: bold;"&gt;458&lt;/span&gt;, 1005 (2009)&lt;/a&gt;.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/60030803362389929-6001580188179199411?l=itamp.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://itamp.blogspot.com/feeds/6001580188179199411/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://itamp.blogspot.com/2011/11/homonuclear-molecule-with-permanent.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/6001580188179199411'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/6001580188179199411'/><link rel='alternate' type='text/html' href='http://itamp.blogspot.com/2011/11/homonuclear-molecule-with-permanent.html' title='A homonuclear molecule with a permanent dipole moment'/><author><name>Seth Rittenhouse</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><media:thumbnail xmlns:media='http://search.yahoo.com/mrss/' url='http://4.bp.blogspot.com/-nk4zG5qt_nY/TtAqBojr3vI/AAAAAAAAABg/Vd5nKr7MGNw/s72-c/WFs.png' height='72' width='72'/><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-60030803362389929.post-3780679184167125989</id><published>2011-09-01T14:45:00.001-04:00</published><updated>2011-09-01T14:45:51.306-04:00</updated><title type='text'>Watching correlated electron motion with attosecond pulses</title><content type='html'>&lt;div style="text-align: justify;"&gt;In a &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.107.093005"&gt;recent paper published in Physical Review Letters&lt;/a&gt;, we propose a new approach to observe the correlated motion of two electrons on the attosecond timescale. In this pump-probe setup, two identical extreme-ultraviolet light pulses with a duration of just a few hundred attoseconds (1 as = 10&lt;sup&gt;-18&lt;/sup&gt; s) are sent onto a helium atom. We expect that with the continuing development of intense attosecond pulses, this kind of experiment could be performed in the next few years. Most current experiments use a strong few-femtosecond infrared field in combination with an extreme-ultraviolet attosecond pulse. These rely on highly nonlinear effects to attain subcycle time resolution within the infrared pulse. In contrast to such setups, the wave packet dynamics are not modified by the fields when using two extreme ultraviolet pulses. The proposed measurement would thus be one of the first experiments to directly observe field-free correlated electron dynamics in atoms on their natural attosecond timescale. &lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;In our proposed setup, the first (pump) pulse excites a coherent wave packet of &lt;i&gt;doubly excited states&lt;/i&gt;. These are prototypical examples of highly correlated states where the two electrons influence each other strongly. After letting this wave packet evolve for some time, the second (probe) pulse ejects both electrons. By repeating the sequence many times with different time delays between the two pulses, a "movie" of the doubly excited wave packet can be created frame by frame.&amp;nbsp;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;In the paper, we show that by measuring only &lt;i&gt;one&lt;/i&gt; of the two ejected electrons and counting only those electrons within a specific energy interval, it is possible to gain direct access to an observable related to the dynamics of &lt;i&gt;both&lt;/i&gt; electrons: the distance between them at the moment of ionization.&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;There is one further problem to overcome: Both steps in the pump-probe sequence only occur with small probabilities. Both in double excitation (pump) and in double ionization (probe), absorption of &lt;i&gt;one&lt;/i&gt; photon has to lead to a &lt;i&gt;two&lt;/i&gt;-electron transition. As a photon only "talks" to one electron directly, these two-electron transitions are quite unlikely. We show that one can exploit quantum interference to increase the magnitude of the signal: Since the pump and probe pulses are identical, absorption of two photons from just one of them leads to the same final states as absorption of one photon from each pulse. This "direct" pathway, where each photon ejects one electron, is orders of magnitude more likely than the more interesting pump-probe pathway. However, it does not represent an incoherent background that masks the signal of interest. Instead, it provides a coherent &lt;i&gt;reference pathway &lt;/i&gt;that&lt;i&gt; &lt;/i&gt;the pump-probe pathway through the doubly excited states interferes with. The amplitude of the interference term is about a hundred times larger than the magnitude of the pump-probe signal by itself, thus providing an experimentally more accessible signal.&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;Reference: J. Feist, S. Nagele, C. Ticknor, B. I. Schneider, L. A. Collins, and J. Burgdörfer, &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.107.093005"&gt;Phys. Rev. Lett. 107, 093005 (2011)&lt;/a&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/60030803362389929-3780679184167125989?l=itamp.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://itamp.blogspot.com/feeds/3780679184167125989/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://itamp.blogspot.com/2011/09/watching-correlated-electron-motion.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/3780679184167125989'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/3780679184167125989'/><link rel='alternate' type='text/html' href='http://itamp.blogspot.com/2011/09/watching-correlated-electron-motion.html' title='Watching correlated electron motion with attosecond pulses'/><author><name>Johannes Feist</name><uri>http://www.blogger.com/profile/07841078783827808091</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-60030803362389929.post-2269508995284625423</id><published>2011-08-30T14:38:00.002-04:00</published><updated>2011-08-30T14:42:30.161-04:00</updated><title type='text'></title><content type='html'>&lt;a href="http://physics.aps.org/files/image_uploads/5696/medium_e1.png" onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}"&gt;&lt;img style="float:left; margin:0 10px 10px 0;cursor:pointer; cursor:hand;width: 300px; height: 135px;" src="http://physics.aps.org/files/image_uploads/5696/medium_e1.png" border="0" alt="" /&gt;&lt;/a&gt;&lt;span class="Apple-style-span" style="font-family: arial, helvetica, sans-serif; font-size: 10px; line-height: 17px; "&gt;What is causing trapped ions to heat up? In an ion trap, electrodes (shown here in gold) produce electric fields that confine the ion (green sphere) to a small volume. Randomly fluctuating dipoles on the surface of these electrodes generate electric field noise. The dipoles form when single atoms adsorb on the metal surface. Vibrations (phonons) in the metal cause the dipoles (purple arrows) to fluctuate. Ions trapped in the vicinity of the metal surface sense these electric field changes and heat up.&lt;/span&gt;&lt;br /&gt;&lt;h1 style="padding-top: 10px; padding-right: 0px; padding-bottom: 0.375em; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-family: arial, helvetica, sans-serif; font-weight: bold; font-size: 1.6em; line-height: 1.3em; color: rgb(39, 20, 92); clear: left; "&gt;&lt;br /&gt;&lt;/h1&gt;&lt;h1 style="padding-top: 10px; padding-right: 0px; padding-bottom: 0.375em; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-family: arial, helvetica, sans-serif; font-weight: bold; font-size: 1.6em; line-height: 1.3em; color: rgb(39, 20, 92); clear: left; "&gt;Viewpoint&lt;/h1&gt;&lt;p class="topics" style="padding-top: 0.2em; padding-right: 0px; padding-bottom: 0.2em; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0.8em; margin-left: 0px; font-family: arial, helvetica, sans-serif; font-weight: bold; font-size: 0.75em; color: rgb(0, 0, 0); line-height: 1.75em; border-bottom-width: 1px; border-bottom-style: solid; border-bottom-color: rgb(230, 230, 230); border-top-width: 1px; border-top-style: solid; border-top-color: rgb(230, 230, 230); "&gt;&lt;a class="topic" href="http://physics.aps.org/browse/subjectarea/atomicandmolecularphysics" style="padding-top: 0px; padding-right: 6px; padding-bottom: 0px; padding-left: 12px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; color: rgb(153, 0, 0); text-decoration: none; background-image: url(http://physics.aps.org/sites/physics.staging.ridge.aps.org/themes/PHYSICS/graphics/icon_bullet.gif); background-attachment: initial; background-origin: initial; background-clip: initial; background-color: initial; background-position: 0px 0.5em; background-repeat: no-repeat no-repeat; "&gt;Atomic and Molecular Physics&lt;/a&gt;&lt;/p&gt;&lt;p   style="padding-top: 0px; padding-right: 0px; padding-bottom: 0.8em; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px;  font-weight: normal;  color: rgb(0, 0, 0); line-height: 1.75em; font-family:arial, helvetica, sans-serif;font-size:0.75em;"&gt;&lt;span class="reference" style="padding-top: 0px; padding-right: 0px; padding-bottom: 0px; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-weight: bold; display: block; "&gt;Physics 4, 66 (2011)&lt;/span&gt;DOI: 10.1103/Physics.4.66&lt;/p&gt;&lt;span class="Apple-style-span"   style="  ;font-family:Times;font-size:medium;"&gt;&lt;span class="Z3988" title="ctx_ver=Z39.88-2004&amp;amp;rft_val_fmt=info%3Aofi%2Ffmt%3Akev%3Amtx%3Ajournal&amp;amp;rft.genre=article&amp;amp;rfr_id=info%3Asid%2Faps.org&amp;amp;rft.title=Physics&amp;amp;rft.stitle=Physics&amp;amp;rft.atitle=All+that+is+gold+does+not+glitter&amp;amp;rft.date=2011-08-22&amp;amp;rft.volume=4&amp;amp;rft.spage=66&amp;amp;rft.aufirst=Nikos&amp;amp;rft.aulast=Daniilidis&amp;amp;rft_id=info:doi/10.1103%2FPhysics.4.66" style="padding-top: 0px; padding-right: 0px; padding-bottom: 0px; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; "&gt;&lt;/span&gt;&lt;/span&gt;&lt;h1 class="title" style="padding-top: 0px; padding-right: 0px; padding-bottom: 0.375em; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-family: arial, helvetica, sans-serif; font-weight: bold; font-size: 1.6em; line-height: 1.3em; color: rgb(0, 0, 0); clear: left; "&gt;All that is gold does not glitter&lt;/h1&gt;&lt;p   style="padding-top: 0px; padding-right: 0px; padding-bottom: 0.8em; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px;  font-weight: normal;  color: rgb(0, 0, 0); line-height: 1.75em; font-family:arial, helvetica, sans-serif;font-size:0.75em;"&gt;&lt;span class="author" style="padding-top: 0px; padding-right: 0px; padding-bottom: 0px; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-weight: bold; display: block; "&gt;&lt;a href="http://physics.aps.org/authors/nikos_daniilidis" style="padding-top: 0px; padding-right: 0px; padding-bottom: 0px; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; color: rgb(153, 0, 0); text-decoration: none; "&gt;Nikos Daniilidis&lt;/a&gt; and &lt;a href="http://physics.aps.org/authors/hartmut_h%C3%A4ffner" style="padding-top: 0px; padding-right: 0px; padding-bottom: 0px; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; color: rgb(153, 0, 0); text-decoration: none; "&gt;Hartmut Häffner&lt;/a&gt;&lt;/span&gt;&lt;i style="padding-top: 0px; padding-right: 0px; padding-bottom: 0px; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; "&gt;Department of Physics, University of California, Berkeley, CA 94720-7300, USA&lt;/i&gt;&lt;/p&gt;&lt;p   style="padding-top: 0px; padding-right: 0px; padding-bottom: 0.8em; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px;  font-weight: normal;  color: rgb(0, 0, 0); line-height: 1.75em; font-family:arial, helvetica, sans-serif;font-size:0.75em;"&gt;&lt;span class="reference" style="padding-top: 0px; padding-right: 0px; padding-bottom: 0px; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-weight: bold; display: block; "&gt;Published August 22, 2011&lt;/span&gt;&lt;/p&gt;&lt;div class="abstract" style="padding-top: 0px; padding-right: 0px; padding-bottom: 0px; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-style: italic; font-family: Times; font-size: medium; "&gt;&lt;p style="padding-top: 0px; padding-right: 0px; padding-bottom: 0.8em; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-family: arial, helvetica, sans-serif; font-weight: normal; font-size: 0.75em; color: rgb(0, 0, 0); line-height: 1.75em; "&gt;A microscopic model offers new insight into a pernicious source of electric field noise in ion traps.&lt;/p&gt;&lt;p style="padding-top: 0px; padding-right: 0px; padding-bottom: 0.8em; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-family: arial, helvetica, sans-serif; font-weight: normal; font-size: 0.75em; color: rgb(0, 0, 0); line-height: 1.75em; "&gt;&lt;a href="http://physics.aps.org/articles/v4/66"&gt;More here .... &lt;/a&gt;&lt;/p&gt;&lt;/div&gt;&lt;div class="orig-article" style="padding-top: 1em; padding-right: 1em; padding-bottom: 0.5em; padding-left: 1em; margin-top: 1em; margin-right: 0em; margin-bottom: 1em; margin-left: 0em; background-color: rgb(239, 239, 239); font-family: Times; font-size: medium; "&gt;&lt;h3 style="padding-top: 0px; padding-right: 0px; padding-bottom: 0.7em; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-family: arial, helvetica, sans-serif; font-weight: bold; font-size: 0.85em; line-height: 1.3em; color: rgb(0, 0, 0); "&gt;A Viewpoint on:&lt;/h3&gt;&lt;p style="padding-top: 0px; padding-right: 0px; padding-bottom: 0.8em; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-family: arial, helvetica, sans-serif; font-weight: normal; font-size: 0.75em; color: rgb(0, 0, 0); line-height: 1em; "&gt;&lt;a href="http://link.aps.org/doi/10.1103/PhysRevA.84.023412" style="padding-top: 0px; padding-right: 0px; padding-bottom: 0px; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; color: rgb(153, 0, 0); text-decoration: none; "&gt;&lt;b style="padding-top: 0px; padding-right: 0px; padding-bottom: 0px; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; "&gt;Microscopic model of electric-field-noise heating in ion traps&lt;/b&gt;&lt;/a&gt;&lt;/p&gt;&lt;p style="padding-top: 0px; padding-right: 0px; padding-bottom: 0.8em; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-family: arial, helvetica, sans-serif; font-weight: normal; font-size: 0.75em; color: rgb(0, 0, 0); line-height: 1em; "&gt;A. Safavi-Naini, P. Rabl, P. F. Weck, and H. R. Sadeghpour&lt;/p&gt;&lt;p style="padding-top: 0px; padding-right: 0px; padding-bottom: 0.8em; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-family: arial, helvetica, sans-serif; font-weight: normal; font-size: 0.75em; color: rgb(0, 0, 0); line-height: 1em; "&gt;Phys. Rev. A &lt;b style="padding-top: 0px; padding-right: 0px; padding-bottom: 0px; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; "&gt;84&lt;/b&gt;, 023412 (2011) – Published August 22, 2011&lt;/p&gt;&lt;p style="padding-top: 0px; padding-right: 0px; padding-bottom: 0.8em; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-family: arial, helvetica, sans-serif; font-weight: normal; font-size: 0.75em; color: rgb(0, 0, 0); line-height: 1em; "&gt;&lt;a href="http://physics.aps.org/pdf/10.1103/PhysRevA.84.023412.pdf" style="padding-top: 0px; padding-right: 0px; padding-bottom: 0px; padding-left: 0px; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; color: rgb(153, 0, 0); text-decoration: none; "&gt;Download PDF&lt;/a&gt; (free)&lt;/p&gt;&lt;div&gt;&lt;br /&gt;&lt;/div&gt;&lt;div&gt;&lt;br /&gt;&lt;/div&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/60030803362389929-2269508995284625423?l=itamp.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://itamp.blogspot.com/feeds/2269508995284625423/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://itamp.blogspot.com/2011/08/viewpoint-atomic-and-molecular-physics.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/2269508995284625423'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/2269508995284625423'/><link rel='alternate' type='text/html' href='http://itamp.blogspot.com/2011/08/viewpoint-atomic-and-molecular-physics.html' title=''/><author><name>caspian</name><uri>http://www.blogger.com/profile/00811609813518037383</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='32' src='http://3.bp.blogspot.com/-H37rmnGwyjw/Tl0skFqrmdI/AAAAAAAAAG0/RYehOdfo5pY/s220/soccerball.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-60030803362389929.post-3846797525087565549</id><published>2011-08-26T13:10:00.002-04:00</published><updated>2011-08-26T13:15:33.108-04:00</updated><title type='text'>Artificial Atoms Can Do More Than Atoms</title><content type='html'>In a recently published work in Physical Review Letters, we have shown that artificial atoms made of a large number of single atoms can exhibit superior properties compared to their individual counterparts. Our results provide a way to novel applications in photonic devices used for quantum communication and quantum metrology.&lt;br /&gt;&lt;br /&gt;In our work, we investigate an ensemble of strongly interacting atoms as found in Rydberg atoms or semiconductor quantum dots. The interaction of these systems with light can be described by an artificial atom with only two energy levels.  However, when applying controlled noise to the system, this approximation breaks down and additional energy levels have to be taken into account. If a light beam is then sent through the system, these additional levels result in exactly one photon being removed from the beam. This single photon absorption process can be used in number resolving photon counters or for the creation of non-classical states of light.&lt;br /&gt;&lt;br /&gt;Reference: J. Honer, R. Löw, H. Weimer, T. Pfau, H. P. Büchler, &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.107.093601"&gt;Phys. Rev. Lett. 107, 093601 (2011)&lt;/a&gt;.&lt;br /&gt;See also: &lt;a href="http://physics.aps.org/synopsis-for/10.1103/PhysRevLett.107.093601"&gt;Synopsis in Physics&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/60030803362389929-3846797525087565549?l=itamp.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://itamp.blogspot.com/feeds/3846797525087565549/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://itamp.blogspot.com/2011/08/artificial-atoms-can-do-more-than-atoms.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/3846797525087565549'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/3846797525087565549'/><link rel='alternate' type='text/html' href='http://itamp.blogspot.com/2011/08/artificial-atoms-can-do-more-than-atoms.html' title='Artificial Atoms Can Do More Than Atoms'/><author><name>Hendrik Weimer</name><uri>http://www.blogger.com/profile/11194181731955663675</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-60030803362389929.post-2274832764294234789</id><published>2011-06-06T11:46:00.011-04:00</published><updated>2011-06-07T10:17:54.848-04:00</updated><title type='text'>ITAMP 2011 DAMOP presentations (in Atlanta, GA)</title><content type='html'>&lt;h3 style="margin-bottom: 0px;"&gt;&lt;span style="font-size: small;"&gt;&amp;nbsp;&lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Babb&lt;/b&gt;&lt;/span&gt;&lt;/h3&gt;&lt;div style="margin-top: 0px;"&gt;10:30&amp;nbsp;AM–12:30&amp;nbsp;PM, Tuesday, June 14, 2011&lt;br /&gt;Room: A705&lt;br /&gt;Chair: Ed Eyler, University of Connecticut&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: B5.00007 : Partial derivatives of eigenvalues without finite differences&lt;/div&gt;11:42&amp;nbsp;AM–11:54&amp;nbsp;AM&lt;br /&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147020&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Babb&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Tuesday, June 14, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;br /&gt;Abstract: E1.00059 : Long-Range Three-Body Dispersion Interactions&lt;/div&gt;&lt;span style="font-size: small;"&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147137&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Capogrosso&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;8:00&amp;nbsp;AM–10:00&amp;nbsp;AM, Wednesday, June 15, 2011&lt;br /&gt;Room: A704&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Chair: Nathan Gemelke, Pennsylvania State University&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: H4.00003 : Pair-Supersolidity of Dipoles in a Bilayer System&lt;/div&gt;8:42&amp;nbsp;AM–8:54&amp;nbsp;AM&lt;br /&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147294&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Capogrosso&lt;/b&gt;&lt;/span&gt; &lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;10:30&amp;nbsp;AM–12:30&amp;nbsp;PM, Thursday, June 16, 2011&lt;br /&gt;Room: A602&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Chair: Markus Greiner, Harvard University&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: N2.00005 : Quantum magnetic phases in harmonically trapped two-component bosons&lt;/div&gt;11:18&amp;nbsp;AM–11:30&amp;nbsp;AM&lt;br /&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147674&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Demler&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;10:30&amp;nbsp;AM–12:30&amp;nbsp;PM, Tuesday, June 14, 2011&lt;br /&gt;Room: A704&lt;br /&gt;Chair: Benjamin Lev, University of Illinois at Urbana-Champaign&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: B4.00005 : Quantum Magnetism with Polar Alkali Dimers&lt;/div&gt;11:54&amp;nbsp;AM–12:06&amp;nbsp;PMhttp://meetings.aps.org/Meeting/DAMOP11/Event/147010&lt;br /&gt;&lt;br /&gt;&amp;nbsp;&lt;span style="font-size: small;"&gt;&lt;b&gt;Demler&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Tuesday, June 14, 2011&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;Room: Atrium Ballroom BC&lt;br /&gt;Abstract: E1.00012 : Emulating Quantum Magnetism and t--J Models in Systems of Ultracold Polar Molecules&lt;/div&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147090&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Demler&lt;/b&gt;&lt;/span&gt; &lt;br /&gt;0:30&amp;nbsp;AM–12:30&amp;nbsp;PM, Thursday, June 16, 2011&lt;br /&gt;Room: A705&lt;br /&gt;Chair: Josh Zirbel, University of Illinois at Urbana-Champaign&lt;br /&gt;Abstract: N5.00003 : Non-Equilibrium Dynamics of 1d Bose Gases Studied via Noise Distributions&lt;br /&gt;10:54&amp;nbsp;AM–11:06&amp;nbsp;AM&lt;br /&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147699&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Demler&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;8:00&amp;nbsp;AM–10:00&amp;nbsp;AM, Friday, June 17, 2011&lt;br /&gt;Room: A705&lt;br /&gt;Chair: Alex Kuzmich, Georgia Institute of Technology&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: T5.00006 : Robust optical delay lines via topological protection&lt;/div&gt;9:00&amp;nbsp;AM–9:12&amp;nbsp;AM&amp;nbsp;http://meetings.aps.org/Meeting/DAMOP11/Event/147977&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Demler&lt;/b&gt;&lt;/span&gt; &lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;&amp;nbsp;8:00&amp;nbsp;AM–10:00&amp;nbsp;AM, Friday, June 17, 2011&lt;br /&gt;Room: A706&lt;br /&gt;Chair: Georg Raithel, University of Michigan&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: T6.00007 : Majorana Fermions in Cold Atom Quantum Wires&lt;/div&gt;9:48&amp;nbsp;AM–10:00&amp;nbsp;AM http://meetings.aps.org/Meeting/DAMOP11/Event/147989&lt;br /&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Feist&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;2:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Wednesday, June 15, 2011&lt;br /&gt;Room: A705&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Chair: Arvinder Sandhu, University of ArizonaAbstract: K5.00003 : Attosecond pump-probe of doubly excited states in helium&lt;/div&gt;2:24&amp;nbsp;PM–2:36&amp;nbsp;PM&amp;nbsp;http://meetings.aps.org/Meeting/DAMOP11/Event/147406&lt;br /&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Feist&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;2:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Thursday, June 16, 2011&lt;br /&gt;Room: A602&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Chair: David Reis, SLAC and Standford University&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: P2.00003 : Time-resolved photoemission by attosecond streaking: extraction of time information&lt;/div&gt;2:42&amp;nbsp;PM–2:54&amp;nbsp;PM&lt;br /&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147726 &lt;br /&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Gacesa&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;8:00&amp;nbsp;AM–10:00&amp;nbsp;AM, Friday, June 17, 2011&lt;br /&gt;Room: A601&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Chair: Steven Manson, Georgia State University&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: T1.00006 : Energy transfer in collisions of atmospheric O and H$_2$&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;9:36&amp;nbsp;AM–9:48&amp;nbsp;AM&lt;/div&gt;&amp;nbsp;http://meetings.aps.org/Meeting/DAMOP11/Event/147948&lt;br /&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Kharchenko&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;8:00&amp;nbsp;AM–10:00&amp;nbsp;AM, Friday, June 17, 2011&lt;br /&gt;Room: A601&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Chair: Steven Manson, Georgia State University&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: T1.00006 : Energy transfer in collisions of atmospheric O and H$_2$&lt;/div&gt;9:36&amp;nbsp;AM–9:48&amp;nbsp;AM&lt;br /&gt;&amp;nbsp;http://meetings.aps.org/Meeting/DAMOP11/Event/147948&lt;br /&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Kuznetsova&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;8:00&amp;nbsp;AM–10:00&amp;nbsp;AM, Thursday, June 16, 2011&lt;br /&gt;Room: A705&lt;br /&gt;Chair: Emily Edwards, JQI and University of Maryland&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: M5.00007 : Cluster state generation using long-range interactions&lt;/div&gt;9:12&amp;nbsp;AM–9:24&amp;nbsp;AMhttp://meetings.aps.org/Meeting/DAMOP11/Event/147652&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Kuznetsova&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Thursday, June 16, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;br /&gt;Abstract: Q1.00147 : Rydberg molecules mediated interaction between polar molecules: a new tool to realize two-qubit gates&lt;/div&gt;&lt;span style="font-size: small;"&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147915&lt;/span&gt;&lt;br /&gt;&lt;h3 style="margin-bottom: 0px;"&gt;&lt;span style="font-size: small;"&gt;&amp;nbsp;&lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Loreau&lt;/b&gt;&lt;/span&gt;&lt;/h3&gt;&lt;div style="margin-top: 0px;"&gt;10:30&amp;nbsp;AM–12:30&amp;nbsp;PM, Wednesday, June 15, 2011&lt;br /&gt;Room: A703&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Chair: Francis Robicheaux, Auburn University&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: J3.00009 : Isotope effect on charge transfer in collisions of H with He$^+$ and He$^{2+}$&lt;/div&gt;12:06&amp;nbsp;PM–12:18&amp;nbsp;PM&lt;br /&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147340&lt;br /&gt;&lt;h3 style="margin-bottom: 0px;"&gt;&lt;span style="font-size: small;"&gt;&amp;nbsp;&lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Lukin&lt;/b&gt;&lt;/span&gt;&lt;/h3&gt;10:30&amp;nbsp;AM–12:30&amp;nbsp;PM, Tuesday, June 14, 2011&lt;br /&gt;Room: A703&lt;br /&gt;Chair: Gretchen Campbell, JQI and NIST&lt;br /&gt;Abstract: B3.00009 : Sub-wavelength optical trapping and manipulation using far-field optics&lt;br /&gt;12:06&amp;nbsp;PM–12:18&amp;nbsp;PM&amp;nbsp;http://meetings.aps.org/Meeting/DAMOP11/Event/147003&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;Lukin&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;10:30&amp;nbsp;AM–12:30&amp;nbsp;PM, Tuesday, June 14, 2011&lt;br /&gt;Room: A704&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Chair: Benjamin Lev, University of Illinois at Urbana-Champaign&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: B4.00005 : Quantum Magnetism with Polar Alkali Dimers&lt;/div&gt;11:54&amp;nbsp;AM–12:06&amp;nbsp;PM&lt;span style="font-size: small;"&gt;&amp;nbsp;http://meetings.aps.org/Meeting/DAMOP11/Event/147010&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Lukin&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Tuesday, June 14, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: E1.00012 : Emulating Quantum Magnetism and t--J Models in Systems of Ultracold Polar Molecules&lt;/div&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;&lt;/b&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147090&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Lukin&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Tuesday, June 14, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: E1.00096 : Towards room temperature magnetic sensing of a single electron spin in biological systems&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147174&lt;/div&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;Lukin&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;&lt;/b&gt;&lt;/span&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Tuesday, June 14, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: E1.00042 : A Nanoplasmonic Lattice for Quantum Simulation with Cold Atoms&lt;/div&gt;&lt;span style="font-size: small;"&gt;&amp;nbsp;http://meetings.aps.org/Meeting/DAMOP11/Event/147120&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;Lukin&lt;/b&gt;&lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;&lt;/b&gt;&lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;&lt;/b&gt;&lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Tuesday, June 14, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract:  E1.00097 : All optical  real-time measurement and preparation of  nuclear spin states around an  individual NV center in diamond&lt;/div&gt;&lt;span style="font-size: small;"&gt;&amp;nbsp;http://meetings.aps.org/Meeting/DAMOP11/Event/147175&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&amp;nbsp;&lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;Lukin&lt;/b&gt;&lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;&lt;/b&gt;&lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;&lt;/b&gt;&lt;/span&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Tuesday, June 14, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: E1.00098 : Measurement-Based Nuclear Spin Cooling in NV Centers&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;&amp;nbsp;http://meetings.aps.org/Meeting/DAMOP11/Event/147176&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;&lt;br /&gt;&lt;/div&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;Lukin&lt;/b&gt;&lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Tuesday, June 14, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: E1.00099 : Sensing thermal motion of a mechanical resonator using a single spin qubit  in diamond&lt;/div&gt;&lt;span style="font-size: small;"&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147177&lt;/span&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt; &lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Lukin&lt;/b&gt;&lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;&lt;/b&gt;&lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Tuesday, June 14, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: E1.00100 : Long-lived solid-state room-temperature quantum memory&lt;/div&gt;&lt;span style="font-size: small;"&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147178 &lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt; &lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Lukin&lt;/b&gt;&lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;&lt;/b&gt;&lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Tuesday, June 14, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: E1.00148 : Topologically Protected Quantum State Transfer&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147226 &lt;/div&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;Lukin&lt;/b&gt;&lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;4 &lt;/b&gt;&lt;/span&gt;:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Tuesday, June 14, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;br /&gt;Abstract: E1.00152 : Coupling of NV centers to microscopic cavities&lt;br /&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147230 &lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;Lukin&lt;/b&gt;&lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt; &lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;8:00&amp;nbsp;AM–10:00&amp;nbsp;AM, Wednesday, June 15, 2011&lt;br /&gt;Room: A602&lt;br /&gt;Chair: Tatjana Curcic, Air Force Office of Scientific Research&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: H2.00001 : Optics with Nitrogen Vacancy Centers  in Diamond&lt;/div&gt;8:00&amp;nbsp;AM–8:30&amp;nbsp;AM&lt;br /&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147273&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;Lukin&lt;/b&gt;&lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt; &lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;8:00&amp;nbsp;AM–10:00&amp;nbsp;AM, Wednesday, June 15, 2011&lt;br /&gt;Room: A602&lt;br /&gt;Chair: Tatjana Curcic, Air Force Office of Scientific Research&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: H2.00002 : Magnetic field imaging with NV ensembles&lt;/div&gt;8:30&amp;nbsp;AM–8:42&amp;nbsp;AM http://meetings.aps.org/Meeting/DAMOP11/Event/147274&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;Lukin&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Wednesday, June 15, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: L1.00108 : Hybrid Devices for Cavity QED in Solid State Systems&lt;/div&gt;&lt;span style="font-size: small;"&gt;&amp;nbsp;http://meetings.aps.org/Meeting/DAMOP11/Event/147538&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;Lukin&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;8:00&amp;nbsp;AM–10:00&amp;nbsp;AM, Thursday, June 16, 2011&lt;br /&gt;Room: A705&lt;br /&gt;Chair: Emily Edwards, JQI and University of Maryland&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: M5.00004 : Long-range quantum gates using external symmetry breaking&lt;/div&gt;8:36&amp;nbsp;AM–8:48&amp;nbsp;AM&lt;br /&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147649 &lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;Lukin&lt;/b&gt;&lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt; &lt;/b&gt;&lt;/span&gt; &lt;br /&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Thursday, June 16, 2011&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;Room: Atrium Ballroom BC&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: Q1.00121 : Nanowire Plasmon Resonators&lt;/div&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147888&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;Lukin&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Thursday, June 16, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;br /&gt;Abstract: Q1.00137 : A nanoscale quantum interface for single atoms&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147905 &lt;/div&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;Lukin&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;8:00&amp;nbsp;AM–10:00&amp;nbsp;AM, Friday, June 17, 2011&lt;br /&gt;Room: A703&lt;br /&gt;Chair: Steve Rolston, JQI and University of Maryland&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: T3.00010 : Dark-State Polaritons with Rydberg Interactions&lt;/div&gt;9:48&amp;nbsp;AM–10:00&amp;nbsp;AM&lt;span style="font-size: small;"&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147965&lt;/span&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt; &lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt; Lukin&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;8:00&amp;nbsp;AM–10:00&amp;nbsp;AM, Friday, June 17, 2011&lt;br /&gt;Room: A705&lt;br /&gt;Chair: Alex Kuzmich, Georgia Institute of Technology&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: T5.00006 : Robust optical delay lines via topological protection&lt;/div&gt;9:00&amp;nbsp;AM–9:12&amp;nbsp;AMhttp://meetings.aps.org/Meeting/DAMOP11/Event/147977&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;Lukin&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;8:00&amp;nbsp;AM–10:00&amp;nbsp;AM, Friday, June 17, 2011&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;Room: A706&lt;br /&gt;Chair: Georg Raithel, University of Michigan&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: T6.00007 : Majorana Fermions in Cold Atom Quantum Wires&lt;/div&gt;9:48&amp;nbsp;AM–10:00&amp;nbsp;AMhttp://meetings.aps.org/Meeting/DAMOP11/Event/147989&lt;br /&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Mathy&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;8:00&amp;nbsp;AM–10:00&amp;nbsp;AM, Wednesday, June 15, 2011&lt;br /&gt;Room: A601&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Chair: Ken O'Hara, Pennsylvania State University&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: H1.00003 : Universal features of strongly polarized mass imbalanced fermi gases&lt;/div&gt;8:24&amp;nbsp;AM–8:36&amp;nbsp;AM&lt;br /&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147264&lt;br /&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Rittenhouse&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Wednesday, June 15, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;br /&gt;Abstract: L1.00004 : A Dielectric Superfluid of Polar Molecules&lt;/div&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147434&lt;br /&gt;&amp;nbsp;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Rittenhouse&lt;/b&gt;&lt;/span&gt; &lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;2:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Thursday, June 16, 2011&lt;br /&gt;Room: A706&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Chair: Doerte Blume, Washington State UniversityAbstract: P6.00003 : Probing universal few-body dynamics&lt;/div&gt;3:00&amp;nbsp;PM–3:30&amp;nbsp;PM&lt;br /&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147764&lt;br /&gt;&lt;br /&gt;&amp;nbsp;&lt;span style="font-size: small;"&gt;&lt;b&gt;Rittenhouse&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Thursday, June 16, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;br /&gt;Abstract: Q1.00008 : Ultralong-range polyatomic Rydberg molecules formed by a polar perturber&lt;/div&gt;&lt;span style="font-size: small;"&gt;&amp;nbsp;http://meetings.aps.org/Meeting/DAMOP11/Event/147774&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&amp;nbsp;&lt;span style="font-size: small;"&gt;&lt;b&gt;Rittenhouse&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Thursday, June 16, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: Q1.00147 : Rydberg molecules mediated interaction between polar molecules: a new tool to realize two-qubit gates&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147915 &lt;/div&gt;&lt;h3 style="margin-bottom: 0px;"&gt;&lt;span style="font-size: small;"&gt;&amp;nbsp;&lt;/span&gt;&lt;/h3&gt;&lt;h3 style="margin-bottom: 0px;"&gt;&lt;span style="font-size: small;"&gt;Sadeghpour&lt;/span&gt;&lt;/h3&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Wednesday, June 15, 2011&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;Room: Atrium Ballroom BC&lt;br /&gt;Abstract: L1.00151 : Self-broadening of helium $^1D$ and $^3D$ lines&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147582&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;&lt;/div&gt;&lt;h3 style="margin-bottom: 0px;"&gt;&lt;span style="font-size: small;"&gt;&amp;nbsp;&lt;/span&gt;&lt;/h3&gt;&lt;h3 style="margin-bottom: 0px;"&gt;&lt;span style="font-size: small;"&gt;Sadeghpour&lt;/span&gt;&lt;/h3&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Thursday, June 16, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;br /&gt;Abstract: Q1.00008 : Ultralong-range polyatomic Rydberg molecules formed by a polar perturber&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;&amp;nbsp;http://meetings.aps.org/Meeting/DAMOP11/Event/147774&lt;/div&gt;&lt;h3 style="margin-bottom: 0px;"&gt;&lt;span style="font-size: small;"&gt;&amp;nbsp;&lt;/span&gt;&lt;/h3&gt;&lt;h3 style="margin-bottom: 0px;"&gt;&lt;span style="font-size: small;"&gt;Sadeghpour&lt;/span&gt;&lt;/h3&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Thursday, June 16, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;br /&gt;Abstract: Q1.00147 : Rydberg molecules mediated interaction between polar molecules: a new tool to realize two-qubit gates&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147915&lt;/div&gt;&lt;h3 style="margin-bottom: 0px;"&gt;&lt;span style="font-size: small;"&gt;&amp;nbsp;&lt;/span&gt;&lt;/h3&gt;&lt;h3 style="margin-bottom: 0px;"&gt;&lt;span style="font-size: small;"&gt;Sadeghpour&lt;/span&gt;&lt;/h3&gt;&lt;div style="margin-top: 0px;"&gt;&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;10:30&amp;nbsp;AM–12:30&amp;nbsp;PM, Wednesday, June 15, 2011&lt;br /&gt;Room: A601&lt;br /&gt;Chair: Jake Taylor, JQI and NISTAbstract: J1.00003 : An ab-initio model of anomalous heating in planar ion traps&lt;/div&gt;10:54&amp;nbsp;AM–11:06&amp;nbsp;AM&lt;br /&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147318&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Weimer &lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Tuesday, June 14, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;br /&gt;Abstract: E1.00148 : Topologically Protected Quantum State Transfer&lt;/div&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147226&lt;br /&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Weimer&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;8:00&amp;nbsp;AM–10:00&amp;nbsp;AM, Thursday, June 16, 2011&lt;br /&gt;Room: A705&lt;br /&gt;Chair: Emily Edwards, JQI and University of Maryland&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: M5.00004 : Long-range quantum gates using external symmetry breaking&lt;/div&gt;8:36&amp;nbsp;AM–8:48&amp;nbsp;AM&lt;br /&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147649 &lt;br /&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Yelin&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Tuesday, June 14, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract:  E1.00097 : All optical  real-time measurement and preparation of  nuclear spin states around an  individual NV center in diamond&lt;/div&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147175&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Yelin&lt;/b&gt;&lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Tuesday, June 14, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: E1.00098 : Measurement-Based Nuclear Spin Cooling in NV Centers&lt;/div&gt;&lt;span style="font-size: small;"&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147176&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Yelin&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;8:00&amp;nbsp;AM–10:00&amp;nbsp;AM, Wednesday, June 15, 2011&lt;br /&gt;Room: A703&lt;br /&gt;Chair: Ivan Deutsch, University of New Mexico&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: H3.00006 : Superradiance in spin-J atoms: Effects of multiple atomic levels&lt;/div&gt;9:00&amp;nbsp;AM–9:12&amp;nbsp;AM&lt;br /&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147286 &lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Yelin&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;8:00&amp;nbsp;AM–10:00&amp;nbsp;AM, Thursday, June 16, 2011&lt;br /&gt;Room: A705&lt;br /&gt;Chair: Emily Edwards, JQI and University of Maryland&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: M5.00007 : Cluster state generation using long-range interactions&lt;/div&gt;9:12&amp;nbsp;AM–9:24&amp;nbsp;AM&lt;br /&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147652 &lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Yelin&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Thursday, June 16, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: Q1.00136 : On nearest-neighbor interactions of cold polar molecules in two-color arrays&lt;/div&gt;&lt;span style="font-size: small;"&gt;&amp;nbsp;http://meetings.aps.org/Meeting/DAMOP11/Event/147904&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Yelin&lt;/b&gt;&lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt; &lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Thursday, June 16, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: Q1.00147 : Rydberg molecules mediated interaction between polar molecules: a new tool to realize two-qubit gates&lt;/div&gt;&amp;nbsp;http://meetings.aps.org/Meeting/DAMOP11/Event/147915&lt;br /&gt;&lt;br /&gt;&lt;span style="font-size: small;"&gt; &lt;/span&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Zhang&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;4:00&amp;nbsp;PM–4:00&amp;nbsp;PM, Wednesday, June 15, 2011&lt;br /&gt;Room: Atrium Ballroom BC&lt;br /&gt;Abstract: L1.00151 : Self-broadening of helium $^1D$ and $^3D$ lines&lt;/div&gt;http://meetings.aps.org/Meeting/DAMOP11/Event/147582&lt;br /&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;Zhang&amp;nbsp;&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;&lt;span style="font-size: small;"&gt;&lt;b&gt;&amp;nbsp;&lt;/b&gt;&lt;/span&gt;8:00&amp;nbsp;AM–10:00&amp;nbsp;AM, Friday, June 17, 2011&lt;br /&gt;Room: A601&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Chair: Steven Manson, Georgia State University&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;Abstract: T1.00006 : Energy transfer in collisions of atmospheric O and H$_2$&lt;/div&gt;9:36&amp;nbsp;AM–9:48&amp;nbsp;AM&lt;br /&gt;&amp;nbsp;http://meetings.aps.org/Meeting/DAMOP11/Event/147948&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;div style="margin-top: 0px;"&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="margin-top: 0px;"&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/60030803362389929-2274832764294234789?l=itamp.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://itamp.blogspot.com/feeds/2274832764294234789/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://itamp.blogspot.com/2011/06/itamp-damop-presentations.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/2274832764294234789'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/2274832764294234789'/><link rel='alternate' type='text/html' href='http://itamp.blogspot.com/2011/06/itamp-damop-presentations.html' title='ITAMP 2011 DAMOP presentations (in Atlanta, GA)'/><author><name>ITAMPbloger</name><uri>http://www.blogger.com/profile/12844502676999940232</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-60030803362389929.post-2677955544267069247</id><published>2011-02-09T10:16:00.000-05:00</published><updated>2011-02-09T10:16:24.981-05:00</updated><title type='text'>talk by Swati Singh</title><content type='html'>Swati is talking about hybrid approaches to quantum mechanical cooling, in this case to a BEC as the medium. Phase contrast imaging was used by Stamper-Kurn and&amp;nbsp;&lt;span class="Apple-style-span" style="-webkit-border-horizontal-spacing: 2px; -webkit-border-vertical-spacing: 2px; color: #333333;"&gt;&lt;span class="Apple-style-span" style="font-family: Times, 'Times New Roman', serif;"&gt;Mukund Vengalattore to major the local spin domains in BEC. She is studying the feasibility of measuring the backaction.&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="-webkit-border-horizontal-spacing: 2px; -webkit-border-vertical-spacing: 2px; color: #333333;"&gt;&lt;span class="Apple-style-span" style="font-family: Times, 'Times New Roman', serif;"&gt;&lt;/span&gt;&lt;/span&gt;Photon scattering losses when objects are levitated to minimize environmental losses, enter the picture. Dipole scattering is not the major issue, as the losses are mostly in the forward direction. Motional squeezing in cantilevers with dipole-dipole interaction, is being discussed. The non-linearity of dipolar interaction is used.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/60030803362389929-2677955544267069247?l=itamp.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://itamp.blogspot.com/feeds/2677955544267069247/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://itamp.blogspot.com/2011/02/talk-by-swati-singh.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/2677955544267069247'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/2677955544267069247'/><link rel='alternate' type='text/html' href='http://itamp.blogspot.com/2011/02/talk-by-swati-singh.html' title='talk by Swati Singh'/><author><name>ITAMPbloger</name><uri>http://www.blogger.com/profile/12844502676999940232</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-60030803362389929.post-7444338661491490915</id><published>2011-02-08T09:32:00.001-05:00</published><updated>2011-02-08T09:40:28.315-05:00</updated><title type='text'>talk by Dan Brooks</title><content type='html'>He is talking about a microchip trap coupled to a cavity with an optomechanical hamiltonian containing both linear and quadratic couplings of photon and atomic COM. The detuning is about 20 MHz from the cavity resonance, with coupling parameters of order unity (small mass and Young's modulus). In linear coupling regime, the OM power intensity shows a dip when the trap is filled, due to so-called ponderomotive squeezing. The oscillations in the COM motion include a lot of mode excitations and likely the bath mode has frequency dependence.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/60030803362389929-7444338661491490915?l=itamp.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://itamp.blogspot.com/feeds/7444338661491490915/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://itamp.blogspot.com/2011/02/talk-by-dan-brooks.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/7444338661491490915'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/7444338661491490915'/><link rel='alternate' type='text/html' href='http://itamp.blogspot.com/2011/02/talk-by-dan-brooks.html' title='talk by Dan Brooks'/><author><name>ITAMPbloger</name><uri>http://www.blogger.com/profile/12844502676999940232</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-60030803362389929.post-7682179907077956585</id><published>2011-02-07T12:11:00.000-05:00</published><updated>2011-02-07T12:11:25.386-05:00</updated><title type='text'>talk by Oriol Romero-Isart</title><content type='html'>Oriol is talking about matter wave interferometry with levitating microspheres- real Sch. cats. Two strategies exist for quantum superposition: use the inherent non-linearity or inject non-linearity (with light, for instance). The measurement is done in analogy with atomic physics through "time of flight". Can optomechanics help with interferometry? First cooling, then expansion by TOF, and measure by putting the bead at the node of the cavity. The, allow for more TOF, and measurement of the position. The coupling to the cavity can done thru. linear or quadratic coupling. Using larger matter waves can extend the coupling too. The most important limiting factor is pressure.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/60030803362389929-7682179907077956585?l=itamp.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://itamp.blogspot.com/feeds/7682179907077956585/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://itamp.blogspot.com/2011/02/talk-by-oriol-romero-isart.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/7682179907077956585'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/7682179907077956585'/><link rel='alternate' type='text/html' href='http://itamp.blogspot.com/2011/02/talk-by-oriol-romero-isart.html' title='talk by Oriol Romero-Isart'/><author><name>ITAMPbloger</name><uri>http://www.blogger.com/profile/12844502676999940232</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-60030803362389929.post-4289486504355145569</id><published>2011-02-07T11:34:00.000-05:00</published><updated>2011-02-07T11:34:20.852-05:00</updated><title type='text'>talk by Mark Raizen</title><content type='html'>Mark is discussing how the Brownian motion of macroscopic objects can be controlled. Fabricated microsphere (~ 1 micron diameter) are launched in high voltage and shaken off in air. The largest force turns out to be van der Waals force. The beads scatter photons in the focus of the laser beam. The power spectra of a 3.01 micron bead were shown. The time scale for a 3 micron silica instantaneous motion (velocity) is about 1.2 micro-sec for water and 56 micro-sec for air, giving a resolution restriction of about 100 nano-sec and 4 pico-meter for H_2O and more forgiving for air. The test of equipartition theorem is confirmed.&lt;br /&gt;&lt;br /&gt;Now the challenge is to confirm the Brownian motion is water. Preliminary results appear to show ballistic motion- possible breakdown of the equipartition theorem? It shall be seen.&lt;br /&gt;&lt;br /&gt;Moving toward the quantum limit; mK cooling of microbeads has been achieved. In arXiv, accepted for publication. Applications: spraying charges and using as thermometer, or for sympathetic cooling of antihydrogen.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/60030803362389929-4289486504355145569?l=itamp.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://itamp.blogspot.com/feeds/4289486504355145569/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://itamp.blogspot.com/2011/02/talk-by-mark-raizen.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/4289486504355145569'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/4289486504355145569'/><link rel='alternate' type='text/html' href='http://itamp.blogspot.com/2011/02/talk-by-mark-raizen.html' title='talk by Mark Raizen'/><author><name>ITAMPbloger</name><uri>http://www.blogger.com/profile/12844502676999940232</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-60030803362389929.post-8173221575142390319</id><published>2011-02-07T10:07:00.001-05:00</published><updated>2011-02-07T10:31:53.717-05:00</updated><title type='text'>on talk by Markus Aspelmayer</title><content type='html'>Markus is reviewing hi-quality micromechanical systems with atmospheric pressure, 100 ng masses, and 10^-3 N/m spring constants. The mechanical motion is carried away by photon emission from the system.&lt;br /&gt;&lt;br /&gt;The non-Markovian nature of the mechanical motion was referred to, as well as single-photon strong coupling beyond the ground state.&lt;br /&gt;&lt;br /&gt;The foundational aspect, quantum processing, and quantum metrology are tied here.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/60030803362389929-8173221575142390319?l=itamp.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://itamp.blogspot.com/feeds/8173221575142390319/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://itamp.blogspot.com/2011/02/on-talk-by-markus-aspelmayer.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/8173221575142390319'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/8173221575142390319'/><link rel='alternate' type='text/html' href='http://itamp.blogspot.com/2011/02/on-talk-by-markus-aspelmayer.html' title='on talk by Markus Aspelmayer'/><author><name>ITAMPbloger</name><uri>http://www.blogger.com/profile/12844502676999940232</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-60030803362389929.post-3213834162509564643</id><published>2011-02-07T09:24:00.010-05:00</published><updated>2011-02-07T09:40:50.772-05:00</updated><title type='text'>talk by Peter Zoller</title><content type='html'>Peter is reviewing the different schemes for coupling of mechanical oscillators to optical fields and specifically on two topics:&lt;br /&gt;&lt;br /&gt;1 - optomechanical transducer for quantum communication, as a way to couple/interface atomic/solid state nodes- in which local computing is done- and transfer them to each other. The implementation of already stationary qubit transfer to other nodes (flying qubit) can be done with --- stay tuned, the webcast audio is being fixed! --- Cascading quantum systems transform to the interaction picture, where there's now a quantum noise term, describing collective decay (Linblad master equation for qubit). There's a unidirectional term in H which describes the emitted photon transfer to the other atom/node.&lt;br /&gt;&lt;br /&gt;more on Peter's talk ...&lt;br /&gt;&lt;br /&gt;2 - free-space interactions with atoms (in optical lattices). The idea of coupling a cryo-oscillator to an OL under UHV. The backaction of the quantum oscillation of the mirror on the motion of atoms in OL leads to jitter of the optical field and gets a quantum noise. More like the cascading quantum system- a quantum stochastic Schroedinger equation with time delay, which describes the unbalanced atomic motion in the laser field, coupled to the mirror which introduces a phase.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/60030803362389929-3213834162509564643?l=itamp.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://itamp.blogspot.com/feeds/3213834162509564643/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://itamp.blogspot.com/2011/02/talk-by-peter-zoller.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/3213834162509564643'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/3213834162509564643'/><link rel='alternate' type='text/html' href='http://itamp.blogspot.com/2011/02/talk-by-peter-zoller.html' title='talk by Peter Zoller'/><author><name>ITAMPbloger</name><uri>http://www.blogger.com/profile/12844502676999940232</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-60030803362389929.post-3890952343303662591</id><published>2011-02-07T04:29:00.000-05:00</published><updated>2011-02-07T04:29:18.273-05:00</updated><title type='text'>watch this space (today thru. Wed) for blogs on the ITAMP Optomechanics workshop</title><content type='html'>watch this space for blogs on the ITAMP Optomechanics workshop!&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/60030803362389929-3890952343303662591?l=itamp.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://itamp.blogspot.com/feeds/3890952343303662591/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://itamp.blogspot.com/2011/02/watch-this-space-today-thru-wed-for.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/3890952343303662591'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/3890952343303662591'/><link rel='alternate' type='text/html' href='http://itamp.blogspot.com/2011/02/watch-this-space-today-thru-wed-for.html' title='watch this space (today thru. Wed) for blogs on the ITAMP Optomechanics workshop'/><author><name>ITAMPbloger</name><uri>http://www.blogger.com/profile/12844502676999940232</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-60030803362389929.post-7923478480830090286</id><published>2010-12-30T12:50:00.002-05:00</published><updated>2010-12-30T13:02:17.174-05:00</updated><title type='text'>Fundamental limit to Spin Exchange Optical Pumping (SEOP)</title><content type='html'>In a detailed calculation, we have shown that anisotropic hyperfine interaction between the atomic electron and the rare-gas nucleus spins sets a fundamental limit to the maximum attainable polarization transfer of electron spin to nuclear spin. (submitted to PRL)&lt;br /&gt;&lt;br /&gt;Tscherbul, Zhang, Sadeghpour and Dalgarno ( &lt;a href="http://arxiv.org/abs/1012.0593" target="_blank"&gt;http://arxiv.org/abs/1012.&lt;wbr&gt;0593&lt;/a&gt;).&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/60030803362389929-7923478480830090286?l=itamp.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://itamp.blogspot.com/feeds/7923478480830090286/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://itamp.blogspot.com/2010/12/fundamental-limit-to-spin-exchange.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/7923478480830090286'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/7923478480830090286'/><link rel='alternate' type='text/html' href='http://itamp.blogspot.com/2010/12/fundamental-limit-to-spin-exchange.html' title='Fundamental limit to Spin Exchange Optical Pumping (SEOP)'/><author><name>caspian</name><uri>http://www.blogger.com/profile/00811609813518037383</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='32' src='http://3.bp.blogspot.com/-H37rmnGwyjw/Tl0skFqrmdI/AAAAAAAAAG0/RYehOdfo5pY/s220/soccerball.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-60030803362389929.post-6917473740624769715</id><published>2010-12-28T09:38:00.001-05:00</published><updated>2010-12-28T09:42:18.428-05:00</updated><title type='text'>ITAMP intitial blog</title><content type='html'>To initiate blogging on ITAMP&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/60030803362389929-6917473740624769715?l=itamp.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://itamp.blogspot.com/feeds/6917473740624769715/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://itamp.blogspot.com/2010/12/itamp-intitial-blog.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/6917473740624769715'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/60030803362389929/posts/default/6917473740624769715'/><link rel='alternate' type='text/html' href='http://itamp.blogspot.com/2010/12/itamp-intitial-blog.html' title='ITAMP intitial blog'/><author><name>ITAMPbloger</name><uri>http://www.blogger.com/profile/12844502676999940232</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry></feed>
