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<channel><title><![CDATA[Physics of Information and Quantum Technologies Group - Physics of Information Seminar]]></title><link><![CDATA[http://www.phys-info.org/physics-of-information-seminar]]></link><description><![CDATA[Physics of Information Seminar]]></description><pubDate>Mon, 04 Aug 2025 18:03:21 +0100</pubDate><generator>Weebly</generator><item><title><![CDATA[Seeing earthquakes and distributing entanglement on the international telecoms network]]></title><link><![CDATA[http://www.phys-info.org/physics-of-information-seminar/seeing-earthquakes-and-distributing-entanglement-on-the-international-telecoms-network]]></link><comments><![CDATA[http://www.phys-info.org/physics-of-information-seminar/seeing-earthquakes-and-distributing-entanglement-on-the-international-telecoms-network#comments]]></comments><pubDate>Tue, 03 Jul 2018 16:11:31 GMT</pubDate><category><![CDATA[Uncategorized]]></category><guid isPermaLink="false">http://www.phys-info.org/physics-of-information-seminar/seeing-earthquakes-and-distributing-entanglement-on-the-international-telecoms-network</guid><description><![CDATA[Andr&eacute; Xuereb&nbsp;(University of Malta)Abstract:Detecting ocean-floor seismic activity is crucial for our understanding of the interior structure and dynamic behaviour of the Earth. However, 70% of the planet&rsquo;s surface is covered by water and seismometers coverage is limited to a handful of permanent ocean bottom stations.In the first part of this talk I discuss our recent results [1], where we showed that existing telecommunication optical fibre cables can detect seismic events whe [...] ]]></description><content:encoded><![CDATA[<div class="paragraph"><a href="http://quantum.edu.mt/" target="_blank">Andr&eacute; Xuereb</a><span style="color:rgb(51, 51, 51)">&nbsp;(</span>University of Malta<span style="color:rgb(51, 51, 51)">)</span><br /><br /><em style="color:rgb(51, 51, 51)">Abstract:</em><br /><br />Detecting ocean-floor seismic activity is crucial for our understanding of the interior structure and dynamic behaviour of the Earth. However, 70% of the planet&rsquo;s surface is covered by water and seismometers coverage is limited to a handful of permanent ocean bottom stations.<br /><br />In the first part of this talk I discuss our recent results [1], where we showed that existing telecommunication optical fibre cables can detect seismic events when combined with state-of-the-art frequency metrology techniques by using the fibre itself as the sensing element. We detected earthquakes over terrestrial and submarine links with length ranging from 75 to 535 km and a geographical distance from the earthquake's epicentre ranging from 25 to 18,500 km. Implementing a global seismic network for real-time detection of underwater earthquakes requires applying the proposed technique to the existing extensive submarine optical fibre network.<br /><br />In the second part of the talk I will discuss briefly how we distributed entanglement between Malta and Sicily [2] over the telecommunications network using polarisation-entangled photon pairs.<br /><br /><span style="color:rgb(51, 51, 51)">[1]&nbsp;</span>http://science.sciencemag.org/content/early/2018/06/13/science.aat4458<br /><span style="color:rgb(51, 51, 51)">[2]&nbsp;</span>http://arxiv.org/abs/1803.00583<br /><br />&#8203;<br /><span style="color:rgb(51, 51, 51)">* * *&nbsp;* *</span><br /><br /><em style="color:rgb(51, 51, 51)">Date &amp; time:</em><span style="color:rgb(51, 51, 51)">&nbsp;17/07/2018 at 15:00</span><em style="color:rgb(51, 51, 51)">.</em><br /><br /><span style="color:rgb(51, 51, 51)"><em>Location</em><em>:</em>&nbsp;</span>Room P9, Mathematics Building,<span style="color:rgb(51, 51, 51)">&nbsp;</span><a href="http://www.ist.utl.pt/en/" target="_blank">Instituto Superior T&eacute;cnico</a><span style="color:rgb(51, 51, 51)">, Lisbon</span><em style="color:rgb(51, 51, 51)">.</em><br />&#8203;</div>]]></content:encoded></item><item><title><![CDATA[Taming Complexity: Controlling Networks]]></title><link><![CDATA[http://www.phys-info.org/physics-of-information-seminar/taming-complexity-controlling-networks]]></link><comments><![CDATA[http://www.phys-info.org/physics-of-information-seminar/taming-complexity-controlling-networks#comments]]></comments><pubDate>Wed, 11 Oct 2017 16:52:34 GMT</pubDate><category><![CDATA[Uncategorized]]></category><guid isPermaLink="false">http://www.phys-info.org/physics-of-information-seminar/taming-complexity-controlling-networks</guid><description><![CDATA[Albert-L&aacute;szl&oacute; Barab&aacute;si&nbsp;(Center of Complex Networks Research, Northeastern University &amp; Division of Network Medicine, Harvard University)Abstract:The ultimate proof of our understanding of biological or technological systems is reflected in our ability to control them. While control theory offers mathematical tools to steer engineered and natural systems towards a desired state, we lack a framework to control complex self-organized systems. Here I will explore the co [...] ]]></description><content:encoded><![CDATA[<div class="paragraph"><a href="http://barabasi.com/about/about" target="_blank">Albert-L&aacute;szl&oacute; Barab&aacute;si</a><span style="color:rgb(51, 51, 51)">&nbsp;</span><span style="color:rgb(51, 51, 51)">(Center of Complex Networks Research, Northeastern University &amp; Division of Network Medicine, Harvard University)</span><br /><br /><em style="color:rgb(51, 51, 51)">Abstract:<br /><br /></em><span style="color:rgb(51, 51, 51)">The ultimate proof of our understanding of biological or technological systems is reflected in our ability to control them. While control theory offers mathematical tools to steer engineered and natural systems towards a desired state, we lack a framework to control complex self-organized systems. Here I will explore the controllability of an arbitrary complex network, identifying the set of driver nodes whose time-dependent control can guide the system's entire dynamics. Virtually all technological and biological networks must be able to control their internal processes. Given that, issues related to control deeply shape the topology and the vulnerability of real systems. Consequently, unveiling the control principles of real networks, the goal of our research, forces us to address series of fundamental questions pertaining to our understanding of complex systems. Finally, I will discuss how control principles inform our ability to predict neurons involved in specific processes in the brain, offering an avenue to experimentally falsify and test the predictions of network control.<br /><br /><br />* * *&nbsp;* *</span><br /><br /><em style="color:rgb(51, 51, 51)">Date &amp; time:</em><span style="color:rgb(51, 51, 51)">&nbsp;16/10/2017 at 17:00</span><em style="color:rgb(51, 51, 51)">.</em><br /><br /><span style="color:rgb(51, 51, 51)"><em>Location</em><em>:</em>&nbsp;</span>Abreu Faro Amphitheatre<span style="color:rgb(51, 51, 51)">,&nbsp;</span><a target="_blank" href="http://www.ist.utl.pt/en/">Instituto Superior T&eacute;cnico</a><span style="color:rgb(51, 51, 51)">, Lisbon</span><em style="color:rgb(51, 51, 51)">.<br /><br />Note:</em><span style="color:rgb(51, 51, 51)">&nbsp;Joint session with the&nbsp;</span><a href="http://www.phys-info.org/symposium.html">Symposium on Complex Networks: from Classical to Quantum&#8203;.</a><span style="color:rgb(51, 51, 51)"></span><span style="color:rgb(51, 51, 51)"></span><br /></div>]]></content:encoded></item><item><title><![CDATA[Complexity of Covering Problems on Hypergraphs]]></title><link><![CDATA[http://www.phys-info.org/physics-of-information-seminar/complexity-of-covering-problems-on-hypergraphs]]></link><comments><![CDATA[http://www.phys-info.org/physics-of-information-seminar/complexity-of-covering-problems-on-hypergraphs#comments]]></comments><pubDate>Fri, 14 Oct 2016 14:45:38 GMT</pubDate><category><![CDATA[Uncategorized]]></category><guid isPermaLink="false">http://www.phys-info.org/physics-of-information-seminar/complexity-of-covering-problems-on-hypergraphs</guid><description><![CDATA[Bruno Coutinho (Instituto de Telecomunica&ccedil;&otilde;es)Abstract:A hypergraph is a natural generalization of a graph, where an edge (often called hyperedge) can simultaneously connect any number of vertices. The fact that hyperedges can connect more than two vertices facilitates a more faithful representation of many real-world networks. For example, given a set of proteins and a set of protein complexes, the corresponding hypergraph naturally captures the information on proteins that intera [...] ]]></description><content:encoded><![CDATA[<div class="paragraph">Bruno Coutinho (Instituto de Telecomunica&ccedil;&otilde;es)<br /><br /><em style="color:rgb(51, 51, 51)">Abstract:</em><br /><br />A hypergraph is a natural generalization of a graph, where an edge (often called hyperedge) can simultaneously connect any number of vertices. The fact that hyperedges can connect more than two vertices facilitates a more faithful representation of many real-world networks. For example, given a set of proteins and a set of protein complexes, the corresponding hypergraph naturally captures the information on proteins that interact together within a protein complex. For a biochemical reaction system, the hypergraph representation indicates which biomolecules participate in a particular reaction. Collaboration networks can also be &nbsp;represented by a hypergraph, where vertices represent individuals and hyperedges connect individuals who were involved in a specific collaboration, e.g. a scientific paper, a patent, a consulting task, or an art performance.<br /><br />The core of a graph - defined as the remainder of the greedy leaf removal &nbsp;procedure where leaves (vertices of degree one) and their neighbors are removed iteratively from the graph - has been related to the conductor-insulator transition, structural controllability, and many combinatorial optimization problems. In fact, the size of the core is related to a fundamental combinatorial issue: the computational complexity of the minimum vertex cover (MVC) problem. The MVC aims to find the smallest set of vertices in a graph (or hypergraph) &nbsp;so that every edge (or hyperedge) is incident to at least one node in the set.<br /><br />I will talk about two generalizations of the core in graphs to hypergraphs, one associated with the edge-cover problem and another associated with the vertex-cover problem. We found that these two cores tend to be very small in real-world hypergraphs. This result indicates that the hyperedge and vertex cover problems in real-world hypergraphs can actually be solved in polynomial time.<br /><br /><span style="color:rgb(51, 51, 51)">* * *&nbsp;* *</span><br /><br /><em style="color:rgb(51, 51, 51)">Date &amp; time:</em><span style="color:rgb(51, 51, 51)">&nbsp;21/10/2016 at 16:00</span><em style="color:rgb(51, 51, 51)">.</em><br /><br /><span style="color:rgb(51, 51, 51)"><em>Location</em><em>:</em>&nbsp;Room P3.10, Mathematics Building,&nbsp;</span><a target="_blank" href="http://www.ist.utl.pt/en/">Instituto Superior T&eacute;cnico</a><span style="color:rgb(51, 51, 51)">, Lisbon</span><em style="color:rgb(51, 51, 51)">.</em><br /></div>]]></content:encoded></item><item><title><![CDATA[Excitation energy transfer processes in photosynthesis: single molecule studies﻿]]></title><link><![CDATA[http://www.phys-info.org/physics-of-information-seminar/excitation-energy-transfer-processes-in-photosynthesis-single-molecule-studies]]></link><comments><![CDATA[http://www.phys-info.org/physics-of-information-seminar/excitation-energy-transfer-processes-in-photosynthesis-single-molecule-studies#comments]]></comments><pubDate>Fri, 15 Apr 2016 13:26:20 GMT</pubDate><category><![CDATA[Uncategorized]]></category><guid isPermaLink="false">http://www.phys-info.org/physics-of-information-seminar/excitation-energy-transfer-processes-in-photosynthesis-single-molecule-studies</guid><description><![CDATA[Jana B. Nieder&nbsp;(International Iberian Nanotechnolgy Laboratory - INL)Abstract:Single molecule techniques have the potential to reveal information about excitation energy transfer processes in complex multi chromophoric systems.In this seminar talk I will present the application of low temperature, plasmonic and ultrafast femtosecond pulse shaping single molecule spectroscopy techniques, that are able to advance the understanding of energy transfer processes in photosynthetic pigment protein [...] ]]></description><content:encoded><![CDATA[<div class="paragraph" style="text-align:justify;"><a href="http://inl.int/members/118" target="_blank">Jana B. Nieder</a>&nbsp;(International Iberian Nanotechnolgy Laboratory - INL)<br /><br /><em>Abstract:</em><br /><br />Single molecule techniques have the potential to reveal information about excitation energy transfer processes in complex multi chromophoric systems.<br />In this seminar talk I will present the application of low temperature, plasmonic and ultrafast femtosecond pulse shaping single molecule spectroscopy techniques, that are able to advance the understanding of energy transfer processes in photosynthetic pigment protein complexes.<br />The results point towards the importance of quantum biology in photosynthesis.<br /><br /><span>* * *&nbsp;* *</span><br /><br /><em>Date &amp; time:</em><span>&nbsp;22/04/2016 at 14:30</span><em>.</em><br /><br /><span><em>Location</em><em>:</em>&nbsp;Room P3.10, Mathematics Building,&nbsp;</span><a target="_blank" href="http://www.ist.utl.pt/en/">Instituto Superior T&eacute;cnico</a><span>, Lisbon</span><em>.</em><br /><br /></div>]]></content:encoded></item><item><title><![CDATA[﻿Breathers and metastable states in the Discrete Nonlinear Schroedinger Equation]]></title><link><![CDATA[http://www.phys-info.org/physics-of-information-seminar/breathers-and-metastable-states-in-the-discrete-nonlinear-schroedinger-equation]]></link><comments><![CDATA[http://www.phys-info.org/physics-of-information-seminar/breathers-and-metastable-states-in-the-discrete-nonlinear-schroedinger-equation#comments]]></comments><pubDate>Wed, 13 Apr 2016 09:43:47 GMT</pubDate><category><![CDATA[Uncategorized]]></category><guid isPermaLink="false">http://www.phys-info.org/physics-of-information-seminar/breathers-and-metastable-states-in-the-discrete-nonlinear-schroedinger-equation</guid><description><![CDATA[Stefano Iubini&nbsp;(CNRS Orl&eacute;ans&#8203;)Abstract:Sometimes it is more convenient to store excess energy in a small region of space rather than&nbsp;spreading it over all the available volume. This may happen when the evolution of a system is&nbsp;characterized by additional dynamic constraints that promote energy localization for entropic reasons.In this seminar I will discuss the role of peculiar nonlinear excitations (discrete breathers)&nbsp;for the localization process in networks of [...] ]]></description><content:encoded><![CDATA[<div class="paragraph" style="text-align:justify;">Stefano Iubini&nbsp;<span>(</span>CNRS Orl&eacute;ans&#8203;<span>)</span><br /><br /><em>Abstract:</em><br /><br />Sometimes it is more convenient to store excess energy in a small region of space rather than&nbsp;spreading it over all the available volume. This may happen when the evolution of a system is&nbsp;characterized by additional dynamic constraints that promote energy localization for entropic reasons.<br />In this seminar I will discuss the role of peculiar nonlinear excitations (discrete breathers)&nbsp;for the localization process in networks of coupled oscillators.<br />Particular attention will be devoted to the dynamics of a Discrete Nonlinear Schroedinger Equation&nbsp;which exhibits a metastable phase with a finite density of breathers and partial energy localization.<br />Such state persists over very long (astronomical) times as a consequence of the extremely low interaction of these excitations with the surrounding background.<br /><br /><span>* * *&nbsp;* *</span><br /><br /><em>Date &amp; time:</em><span>&nbsp;19/04/2016 at 11:30.</span><br /><br /><span><span><span><em>Location</em><em>:</em>&nbsp;</span></span></span><span><span>Room P3.10, Mathematics Building,&nbsp;<a target="_blank" href="http://www.ist.utl.pt/en/">Instituto Superior T&eacute;cnico</a>, Lisbon.</span></span></div>]]></content:encoded></item><item><title><![CDATA[Quantum Machine Learning]]></title><link><![CDATA[http://www.phys-info.org/physics-of-information-seminar/quantum-machine-intelligence]]></link><comments><![CDATA[http://www.phys-info.org/physics-of-information-seminar/quantum-machine-intelligence#comments]]></comments><pubDate>Wed, 08 Jul 2015 14:29:38 GMT</pubDate><category><![CDATA[Uncategorized]]></category><guid isPermaLink="false">http://www.phys-info.org/physics-of-information-seminar/quantum-machine-intelligence</guid><description><![CDATA[Masoud Mohseni&nbsp;(Google Quantum Artificial Intelligence Lab)Abstract:Over the past 30 years, two different computational paradigms have been developed based on the premise that the laws of quantum mechanics could provide radically new and more powerful methods of information processing.&nbsp; One of these approaches is to encode the solution of a computational problem into the ground state of a programmable many-body quantum Hamiltonian system. Although, there is empirical evidence for quant [...] ]]></description><content:encoded><![CDATA[<div class="paragraph" style="text-align:justify;"><a href="https://plus.google.com/+QuantumAILab/posts" target="_blank">Masoud Mohseni</a>&nbsp;(<em><span></span></em>Google Quantum Artificial Intelligence Lab)<br /><br /><em>Abstract:</em><br />Over the past 30 years, two different computational paradigms have been developed based on the premise that the laws of quantum mechanics could provide radically new and more powerful methods of information processing.&nbsp; One of these approaches is to encode the solution of a computational problem into the ground state of a programmable many-body quantum Hamiltonian system. Although, there is empirical evidence for quantum enhancement in certain problem instances, there is not a full theoretical understanding of the conditions for quantum speed up for problems of practical interest, especially hard combinatorial optimization and inference tasks in machine learning. In his talk, I will provide an overview of quantum computing paradigms and discuss the progress at the Google Quantum Artificial Intelligence Lab towards developing the general theory and overcoming practical limitations. Furthermore, I will briefly discuss two recent quantum machine learning primitives that we have&nbsp;developed&nbsp;known&nbsp;as Quantum Principal Component&nbsp;Analysis and Multiqubit&nbsp;Quantum Tunneling.&#8203;<br /><br />* * *&nbsp;* *<br /><br /><em>Date &amp; time:</em>&nbsp;09/10/2015 at 16:30.<br /><br /><span><span><em>Location</em><em>:</em>&nbsp;</span></span>Seminar Room (2.8.3), Physics Department,&nbsp;<a target="_blank" href="http://www.ist.utl.pt/en/">Instituto Superior T&eacute;cnico</a>, Lisbon<span>.</span><br /><br /><span><em><span>Note:</span></em><span>&nbsp;Joint session with the&nbsp;</span><span><span><a href="https://math.tecnico.ulisboa.pt/seminars/qci/?action=show&amp;id=4149" target="_blank">Quantum Computation and Information Seminar</a></span></span><span>.</span></span></div>]]></content:encoded></item><item><title><![CDATA[Open quantum systems: life beyond the Markov approximation]]></title><link><![CDATA[http://www.phys-info.org/physics-of-information-seminar/open-quantum-systems-life-beyond-the-markov-approximation]]></link><comments><![CDATA[http://www.phys-info.org/physics-of-information-seminar/open-quantum-systems-life-beyond-the-markov-approximation#comments]]></comments><pubDate>Mon, 22 Jun 2015 13:24:05 GMT</pubDate><category><![CDATA[Uncategorized]]></category><guid isPermaLink="false">http://www.phys-info.org/physics-of-information-seminar/open-quantum-systems-life-beyond-the-markov-approximation</guid><description><![CDATA[Ines de Vega&nbsp;(LMU Munich)Abstract:Open quantum systems (OQS) cannot always be described with the Markov approximation, which requires a large separation of system and environment time scales. In this talk I will give an overview of some recent advances to tackle the dynamics of an OQS beyond the Markov approximation, with special emphasis in hierarchy-based [1,2] and chain mapping-based [3] approaches. In the latter context, I will discuss the use of a thermofield transformation to describe [...] ]]></description><content:encoded><![CDATA[<div class="paragraph" style="text-align:justify;"><a href="http://www.theorie.physik.uni-muenchen.de/lsschollwoeck/members/sci_mem/devega/index.html" style="" title="" target="_blank">Ines de Vega</a>&nbsp;(LMU Munich)<br /><br /><em style="">Abstract:</em><br />Open quantum systems (OQS) cannot always be described with the Markov approximation, which requires a large separation of system and environment time scales. In this talk I will give an overview of some recent advances to tackle the dynamics of an OQS beyond the Markov approximation, with special emphasis in hierarchy-based [1,2] and chain mapping-based [3] approaches. In the latter context, I will discuss the use of a thermofield transformation to describe thermal environments [4].<br /><br />[1] Y. Tanimura. PRA, 41, 6676&ndash;6687 (1990).<br />[2]&nbsp;I. de Vega, J. Phys. A: Math. Theor. 48, 145202 (2015).<br />[3] A. W. Chin, J. Prior, S. F. Huelga, and M. B. Plenio, Phys. Rev. Lett. 107, 160601 (2011).<br />[4] I. de Vega and M.C. Ba&ntilde;uls,<span style="color: rgb(134, 134, 134); line-height: 1.5; background-color: initial;">&nbsp;</span><a href="http://arxiv.org/abs/1504.07228" title="" target="_blank" style="line-height: 1.5; background-color: initial;">arXiv:1504.07228</a>.<span style="color: rgb(134, 134, 134); line-height: 1.5; background-color: initial;"><br /></span><br />* * *&nbsp;* *<br /><br /><em style="">Date &amp; time:</em>&nbsp;20/07/2015 at 10:00.<br /><br /><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style=""><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style=""><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style=""><em style="">Location</em><em style="">:</em>&nbsp;</span></span></span><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style=""><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style=""></span></span><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style=""><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style="">Room P3.10, Mathematics Building,&nbsp;<a title="" target="_blank" href="http://www.ist.utl.pt/en/" style="">Instituto Superior T&eacute;cnico</a>, Lisbon.</span></span><br /></div>]]></content:encoded></item><item><title><![CDATA[The physics of impossible machines]]></title><link><![CDATA[http://www.phys-info.org/physics-of-information-seminar/the-physics-of-impossible-machines]]></link><comments><![CDATA[http://www.phys-info.org/physics-of-information-seminar/the-physics-of-impossible-machines#comments]]></comments><pubDate>Wed, 06 May 2015 16:54:00 GMT</pubDate><category><![CDATA[Uncategorized]]></category><guid isPermaLink="false">http://www.phys-info.org/physics-of-information-seminar/the-physics-of-impossible-machines</guid><description><![CDATA[Vlatko Vedral (University of Oxford)Abstract:Maxwell&rsquo;s demon was born in 1867 and his sole function was to illustrate some potential problems with the Second Law of thermodynamics. He still thrives in modern physics and plays an important role in clarifying connections between thermodynamics and information theory. In my talk I will present a variety of different demons which, when restricted by the Second Law, will lead to interesting consequences in electromagnetism, optics, gravity,&nbs [...] ]]></description><content:encoded><![CDATA[<div class="paragraph" style="text-align:justify;"><a href="http://www.vlatkovedral.org/" target="_blank" title="">Vlatko Vedral</a> (University of Oxford)<br /><br /><em style="">Abstract:</em><br /><span style="">Maxwell&rsquo;s demon was born in 1867 and his sole function was to illustrate some potential problems with the Second Law of thermodynamics. He still thrives in modern physics and plays an important role in clarifying connections between thermodynamics and information theory. In my talk I will present a variety of different demons which, when restricted by the Second Law, will lead to interesting consequences in electromagnetism, optics, gravity,&nbsp;quantum mechanics&nbsp;as well as quantum information. Finally, I will speculate if the concept of information could in some sense be considered deeper than the entities typically though of as fundamental in physics and will mention various efforts to derive quantum physics from simpler information theoretic axioms.</span><br /><br /><span style="">* * *&nbsp;* *</span><br /><br /><em style="">Date &amp; time:</em><span style="">&nbsp;01/06/2015 at 10:00.</span><br /><br /><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style=""><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style=""><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style=""><em style="">Location</em><em style="">:</em>&nbsp;</span></span></span><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style=""><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style=""></span></span><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style=""><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style="">Room P12, Mathematics Building,&nbsp;<a title="" target="_blank" href="http://www.ist.utl.pt/en/" style="">Instituto Superior T&eacute;cnico</a>, Lisbon.</span></span><br /><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style=""><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style=""><br /></span></span><em>Note:</em>&nbsp;<span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style=""><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style=""><span "font-size:11.0pt;font-family:="" &quot;calibri&quot;,&quot;sans-serif&quot;;mso-ascii-theme-font:minor-latin;mso-fareast-font-family:="" calibri;mso-fareast-theme-font:minor-latin;mso-hansi-theme-font:minor-latin;="" mso-bidi-font-family:&quot;times="" roman&quot;;mso-bidi-theme-font:minor-bidi;="" mso-ansi-language:pt;mso-fareast-language:en-us;mso-bidi-language:ar-sa"="" style="">Joint event with the DP-PMI Day.</span><br /></span></span></div>]]></content:encoded></item><item><title><![CDATA[On Landauer principle for non-equilibrium quantum systems]]></title><link><![CDATA[http://www.phys-info.org/physics-of-information-seminar/on-landauer-principle-for-non-equilibrium-quantum-systems]]></link><comments><![CDATA[http://www.phys-info.org/physics-of-information-seminar/on-landauer-principle-for-non-equilibrium-quantum-systems#comments]]></comments><pubDate>Wed, 15 Apr 2015 10:55:24 GMT</pubDate><category><![CDATA[Uncategorized]]></category><guid isPermaLink="false">http://www.phys-info.org/physics-of-information-seminar/on-landauer-principle-for-non-equilibrium-quantum-systems</guid><description><![CDATA[Mauro Paternostro&nbsp;(Queen's University Belfast)Abstract:Using the operational framework of completely positive, trace preserving operations and thermodynamic fluctuation relations, I will derive a lower bound for the heat exchange in a Landauer erasure process on a quantum system. The bound comes from a non-phenomenological derivation of the Landauer principle which holds for generic non-equilibrium dynamics. Furthermore the bound depends on the non-unitality of dynamics, giving it a physica [...] ]]></description><content:encoded><![CDATA[<div class="paragraph" style="text-align:justify;"><span style=""><a href="http://pure.qub.ac.uk/portal/en/persons/mauro-paternostro(d10f9f5f-ce96-49f6-bc57-242feb5400e5).html" target="_blank" title="">Mauro Paternostro</a></span><span style="">&nbsp;(</span><span style="">Queen's University Belfast)</span><br /><br /><em style="">Abstract:</em><br />Using the operational framework of completely positive, trace preserving operations and thermodynamic fluctuation relations, I will derive a lower bound for the heat exchange in a Landauer erasure process on a quantum system. The bound comes from a non-phenomenological derivation of the Landauer principle which holds for generic non-equilibrium dynamics. Furthermore the bound depends on the non-unitality of dynamics, giving it a physical significance that differs from other derivations. I will illustrate the framework to the model of a spin-1/2 system coupled to an interacting spin chain at finite temperature.<br /><span style=""></span><br /><span style=""></span>I will further investigate the link between information and thermodynamics embodied by Landauer principle in an open-system dynamics embodied by a collision-based mechanism involving a suitable multipartite system and a multi-particle spin reservoir at finite temperature. I will demonstrate that Landauer principle holds, in such an open configuration, in a form that involves the flow of heat dissipated into the environment and the rate of change of the entropy of the system, Quite remarkably, such a principle for heat and entropy power can be explicitly linked to the rate of creation of correlations among the elements of the multipartite system and, in turn, the non-Markovian nature of their reduced evolution. I will illustrate such principle using two paradigmatic cases.<br /><br />* * *&nbsp;* *<br /><br /><em style="">Date &amp; time:</em>&nbsp;21/04/2015 at 10:00.<br /><br /><em style="">Location</em><em style="">:</em>&nbsp;Room P3.10, Mathematics Building,&nbsp;<a title="" target="_blank" href="http://www.ist.utl.pt/en/" style="">Instituto Superior T&eacute;cnico</a>, Lisbon.<br /><br /><em style="">Note:</em>&nbsp;Joint session with the&nbsp;<a title="" target="_blank" href="https://math.tecnico.ulisboa.pt/seminars/qci/?action=show&amp;id=4050" style="">Quantum Computation and Information Seminar</a>.<br /></div>]]></content:encoded></item><item><title><![CDATA[Generalized Landauer Bound as Universal Thermodynamic Entropy in Continuous Phase Transitions]]></title><link><![CDATA[http://www.phys-info.org/physics-of-information-seminar/generalized-landauer-bound-as-universal-thermodynamic-entropy-in-continuous-phase-transitions]]></link><comments><![CDATA[http://www.phys-info.org/physics-of-information-seminar/generalized-landauer-bound-as-universal-thermodynamic-entropy-in-continuous-phase-transitions#comments]]></comments><pubDate>Mon, 02 Mar 2015 11:09:18 GMT</pubDate><category><![CDATA[Uncategorized]]></category><guid isPermaLink="false">http://www.phys-info.org/physics-of-information-seminar/generalized-landauer-bound-as-universal-thermodynamic-entropy-in-continuous-phase-transitions</guid><description><![CDATA[Cristina Diamantini (University of Perugia)Abstract:The classic Landauer bound can be lowered when erasure errors are permitted. Here we point out that continuous phase transitions characterized by an order parameter can also be viewed as information erasure by resetting a certain number of bits to a standard value. The information-theoretic expression for the generalized Landauer bound in terms of error probability implies thus a universal form for the thermodynamic entropy in the partially ord [...] ]]></description><content:encoded><![CDATA[<div class="paragraph" style="text-align:justify;"><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style="">Cristina Diamantini (</span><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style="">University of Perugia)</span><br /><em><br />Abstract:<br /></em><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style="">The classic Landauer bound can be lowered when erasure errors are permitted. Here we point out that continuous phase transitions characterized by an order parameter can also be viewed as information erasure by resetting a certain number of bits to a standard value. The information-theoretic expression for the generalized Landauer bound in terms of error probability implies thus a universal form for the thermodynamic entropy in the partially ordered phase. We explicitly show that the thermodynamic entropy as a function of interaction parameters and temperature is identical to the information-theoretic expression in terms of error probability alone in the specific example of the Hopfield neural network model of associative memory, a distributed information-processing system of many interacting stochastic bits. In this framework the Landauer bound sets a lower limit for the work associated with "remembering" rather than "forgetting".</span><br /><br /><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style=""><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style=""><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style="">* * *&nbsp;* *<br /><br /><em style="">Date &amp; time:</em>&nbsp;<span "font-size:12.0pt;font-family:&quot;times="" roman&quot;,&quot;serif&quot;;="" mso-fareast-font-family:&quot;times="" roman&quot;;mso-ansi-language:en-gb;mso-fareast-language:="" en-gb;mso-bidi-language:ar-sa"="" style="">24/03/2015 at 10:00</span>.<br /><br /><em style="">Location</em><em style="">:</em>&nbsp;</span></span></span><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style=""><span "font-size:12.0pt;font-family:&quot;helvetica&quot;,&quot;sans-serif&quot;;="" mso-fareast-font-family:calibri;mso-fareast-theme-font:minor-latin;color:#222222;="" mso-ansi-language:en-gb;mso-fareast-language:en-gb;mso-bidi-language:ar-sa"="" style="">Seminar Room (2.8.3), Physics Department,&nbsp;<a title="" target="_blank" href="http://www.ist.utl.pt/en/" style="">Instituto Superior T&eacute;cnico</a>, Lisbon.</span><br /></span></div>]]></content:encoded></item></channel></rss>