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<h2>Pooya Ronagh</h2>
<h3>University of <br> Waterloo</h3>
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<h1 class="">Pooya Ronagh</h1>
<ul class="list-unstyled">
<li>Research Assistant Professor</li>
<li>University of Waterloo</li>
</ul>
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<h3 class="title">Bio</h3>
<p> As of September 2020, I am a Research Assistant Professor in the <a href="https://uwaterloo.ca/physics-astronomy/">Department of Physics & Astronomy</a> and the <a href= "https://uwaterloo.ca/institute-for-quantum-computing/">Institute for Quantum Computing (IQC)</a> at the <a href= " ">University of Waterloo</a>. I am also a Scientific Lead at the <a href= "https://www.perimeterinstitute.ca/research/research-initiatives/perimeter-institute-quantum-intelligence-lab-piquil" >Perimeter Institute Quantum Intelligence Lab (PIQuIL)</a>, and direct the Hardware Innovation Lab of <a href= "https://1qbit.com/">1QBit</a>.</p>
<p> I am interested in algorithmic aspects of quantum computation. My research is in design and analysis of quantum algorithms for learning, quantum and classical optimal control, and architectures for fault-tolerant quantum computation.</p>
<p> To prospective students: I am accepting graduate students (MSc and PhD) in Fall 2021. Reach out if you are interested in interdisciplinary research on quantum computation and machine learning and you think you are good!</p>
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<h3>Past Positions</h3>
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<ul class="ul-dates">
<li>
<div class="dates"><span>2020</span> <span>2017</span></div>
<div class="content">
<h4>Postdoctoral Fellow</h4>
<p><em>University of Waterloo</em></p>
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</li>
<li>
<div class="dates"><span>2020</span> <span>2019</span></div>
<div class="content">
<h4>Head of Hardware Innovation Lab</h4>
<p><em>1QB Information Technologies</em></p>
</div>
</li>
<li>
<div class="dates"><span>2018</span> <span>2018</span></div>
<div class="content">
<h4>Applied Mathematics Lead</h4>
<p><em>1QB Information Technologies</em></p>
</div>
</li>
<li>
<div class="dates"><span>2017</span> <span>2016</span></div>
<div class="content">
<h4>Postdoctoral Fellow</h4>
<p><em>University of British Columbia</em></p>
</div>
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<li>
<div class="dates"><span>2017</span> <span>2013</span></div>
<div class="content">
<h4>Fundamental Research Lead</h4>
<p><em>1QB Information Technologies</em></p>
</div>
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<h3>Education and Training</h3>
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<ul class="ul-card">
<li>
<div class="dy"><span class="degree">Ph.D.</span> <span class="year">2016</span></div>
<div class="description">
<p class="what">Ph.D. in Mathematics</p>
<p class="where">University of British Columbia</p>
</div>
</li>
<li>
<div class="dy"><span class="degree">M.Sc.</span><span class="year">2011</span></div>
<div class="description">
<p class="what">M.Sc. in Mathematics</p>
<p class="where">University of British Columbia</p>
<p class="where">University of Pennsylvania</p>
</div>
</li>
<li>
<div class="dy"><span class="degree">B.Sc.</span><span class="year">2009</span></div>
<div class="description">
<p class="what">B.Sc. in Computer Science</p>
<p class="what">B.Sc. in Mathematics</p>
<p class="where">Sharif University of Technology</p>
</div>
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<h3>Interests</h3>
</div>
<ul class="ul-boxed list-unstyled">
<li>Quantum Computation</li>
<li>Quantum Information Processing</li>
<li>Quantum Algorithms</li>
<li>Machine Learning</li>
<li>Computational Complexity</li>
<li>Quantum Control</li>
<li>Quantum Error Correction</li>
<li>Fault-tolerant Quantum Computation</li>
<li>Convex Optimization</li>
<li>Optimal Control</li>
<li>Reinforcement Learning</li>
<li>Combinatorial Optimization</li>
<li>Mathematical Physics</li>
<li>Algebraic Geometry</li>
<li>String Theory</li>
<li>Quantum Mechanics</li>
</ul>
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<h3>Quantum Algorithms for Learning</h3>
<p>Convex Optimization</p>
<p>Mathematical Programming</p>
<p>Computational Complexity</p>
<p>Probabilisitc Graphical Models</p>
<p>Energy-based Models</p>
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<div class="details">
<p>In this research program I investigate applicability of quantum information processing to classical data processing tasks wherein the state-of-the-art algorithms, e.g. machine learning, are either incapable of tackling the computational challenges, <a href="https://openai.com/blog/ai-and-compute/">reaching their performance limits</a>, are <a href="https://www.wired.com/story/ai-great-things-burn-planet/">costly to train</a>, or provide <a href="https://arxiv.org/pdf/1712.07107.pdf">vulnerable solutions</a>.</p>
<p>For instance, reinforcement learning (RL), is an area of machine learning and artificial intelligence wherein the existing methods suffer from significant sample inefficiency. That is, the number of rounds of trial-and-error the agent has to undergo in order to learn optimal decision-making policies in the environment is far beyond the real-world expectations. Consequently, the existing techniques are not useful for training real-world autonomous agents. As an example, the impressive control achieved by many robotic systems are not through RL but rather achieved via traditional optimal control theory.</p>
<p>Consequently, the current applications of RL have been confined to problems wherein relatively faithful simulation of the real-world environments is possible. The well-known examples include computer and video games. But even in these cases, the computing power required to simulate the environment sufficiently long has appeared as a major bottleneck for progress in the field. The well-known Atari benchmarks for deep RL by <a href="https://arxiv.org/abs/1710.02298">Hessel et al. in 2017</a> used equivalent of 83 hours of simulations of Atari games. The AlphaStar benchmark by <a href="https://www.nature.com/articles/s41586-019-1724-z">Vinyals et al. in 2019</a> used 200 years of real-time play. And the Rubik’s cube solver of <a href="https://openai.com/blog/solving-rubiks-cube/">OpenAI</a> in the same year use 10,000 years of simulation. The energy consumed by datacentres to simulate Rubik’s cube was as much as 3 hours of the energy produced by a nuclear energy plant.</p>
<p>These examples reveal that the mechanisms of learning in existing machine learning algorithms are far from that of humans and animals. This observation has motivated the computer scientists to explore <a href="https://mitpress.mit.edu/books/probabilistic-graphical-models">alternative models</a> that perhaps have better resemblance to the neurocognitive systems of humans and animals. However, training such models require simulation of physical systems and certain properties of them (e.g., the partition function of many-body systems) which appear to be interactive for classical computing. This has motivated us to investigate whether quantum computation and its capabilities in simulating complex physical systems can be used to devise the next generation of intelligence systems.</p>
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<h3>Quantum Control</h3>
<p>Optimal Control</p>
<p>Quantum Gates</p>
<p>Unitary Evolutions</p>
<p>Quantum Simulation</p>
<p>Quantum Error Correction</p>
<p>Fault-tolerant Quantum Computation</p>
</div>
</div>
</div>
<div class="details">
<p>Quantum control is the holy grail of creating improved quantum processors. On one hand, the goal is to protect quantum information from unwanted interactions with the environment, and on the hand the processor is expected to be accurately programmable. The two goals work against each other and give rise to the existing challenges in building scalable applicable quantum computers.</p>
<p>A paradigm of machine learning and artificial intelligence known as <a href="http://incompleteideas.net/book/the-book.html">reinforcement learning</a> (RL) is considered a promising approach to controlling complex systems (e.g., robots and rockets). The recent applications of deep RL to achieving human-level dexterity in playing Atari games, the game of Go, and <a href="https://www.youtube.com/watch?v=kVmp0uGtShk&feature=emb_title">solving rubik's cube</a> are impressive achievements that encourage exploring applications of deep reinforcement learning in optimal control.</p>
<p>I am interested in exploring applications of deep reinforcement learning in controlling dynamics of classical and quantum systems. In this line of work, I investigate whether machine learning and AI techniques such as deep reinforcement learning can help us to improve the state of the art in quantum control. In a <a href="https://rdcu.be/b6SMM">first paper</a> in this direction I take some early step towards intelligent control of Monte-Carlo simulation of spin glass systems (in this first case, completely classically).</p>
<p>Even with very good qubits, processing quantum information for long periods of time require strategies for protecting the desired wavefunctions undergoing quantum instructions (unitary gates). These strategies are called <a href="https://arxiv.org/abs/quant-ph/9712048">quantum error correction and fault-tolerant quantum computation</a>. Error correction consists of classical subprocedures that themselves have to be executed very fast in order for it to keep up with the pace of the execution of quantum gates. This is an area of exploration <a href="http://doi.org/10.1088/2058-9565/aad1f7">I am interested in</a>.</p>
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<h3>Quantum Invariants and Quantum Algebra (inactive)</h3>
<p>Algebraic Stacks</p>
<p>Calabi-Yau Geometry</p>
<p>Inertia Stacks</p>
<p>Hall Algebra</p>
<p>Enumerative Geometry</p>
<p>Donaldson-Thomas Invariants</p>
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<p>I studied algebraic geometry in grad school. My intersest in this field steamed from applicability of it in high-energy physics. Developing consistent and predictive mathematics guided by the physicist's wish list for a theory of quantum gravity is extremely exciting. My research in this area was focused on studying the moduli stacks that arise naturally in string theory.</p>
<p>According to string theory the world we live in is not the 4-dimensional time-space we see but has a minuscule 6-dimensional curled shape attached to each point of it known as a Calabi-Yau threefold. What physicists would really like from a good theory, is the capability of extracting quantitative information, simply numbers, that can be checked through experiments. These numbers are expected to be independent of the minor changes that can happen to the Calabi-Yau 3-fold. It is also possible to check this fact mathematically, hence these numbers are called invariants assigned to a Calabi-Yau 3-fold in mathematics. [<a href="http://bookstore.ams.org/qft-1-2-s">Deligne, et. al</a>]</p>
<p>Inside a Calabi-Yau 3-fold physical objects called the BPS-branes live that encodes the states in which certain particles can exist. Physical interpretation suggests that there should be only a finite number of these BPS-states. These invariants translate mathematically to the <a href="https://arxiv.org/abs/math/9806111">Donaldson-Thomas (DT) invariants</a> associated to the space of the BPS-states called moduli. Consistent definition of DT-invariants and studying their properties is a crucial ingredient of string theory, and a beautiful mathematical endeavor. The challenges for a suitable definition of these invariants are as follows: (1) beyond some special cases, the moduli are complicated objects that are called <a href="https://www.math.uzh.ch/index.php?pr_vo_det&key1=1287&key2=580">stacks</a>. (2) The invariants one hopes to associated to these spaces are supposed to behave very much like <a href="http://arxiv.org/pdf/0910.0105v2.pdf">Euler</a> characteristics. An important feature of Euler characteristic of a geometric shape is that it remains unchanged if one deforms the shape as if it was made of rubber. (3) A potential definition of such invariants, depends on extra factors (called stability conditions) and therefore this dependence also has to be understood thoroughly. <a href="http://arxiv.org/abs/0811.2435">Kontsevich-Soibelman</a>, and <a href="http://arxiv.org/abs/0810.5645">Joyce-Song</a> have independently developed two approached to the definition of generalized Donaldson-Thomas invariants.</p>
<p>In my <a href="https://doi.org/10.1112/S0010437X18007881">Ph.D. thesis</a>, in collaboration with my supervisor Prof. K. Behrend we developed a simple and geometric approach to define the generalized Donaldson-Thomas invariant following ideas of <a href="https://arxiv.org/abs/1002.4374">T. Bridgeland</a>. We consider the Hall algebra of algebroids over the Calabi-Yau 3-fold. We view the inertia construction of algebroids as an operator on this ring. We show that the (semi-simple variant of the) inertia operator is diagonalizable on this space and the eigenvalue decomposition of it creates a graded structure on the space of stack functions. We use this decomposition to define a Lie sub-algebra of the Hall algebra, generated as a Q-vector space by those eigenvectors of the inertia that do not have eigenvalues dividing (q-1)^2. We then show that there exists a well-defined integration map that associates an invariant to each object in this smaller Lie algebra.</p>
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<h4 class="pubtitle">The inertia operator and Hall algebra of algebraic stacks</h4>
<div class="pubauthor">Pooya Ronagh</div>
<div class="pubcite"><span class="label label-success">Ph.D. Thesis</span>University of British Columbia</div>
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<h4>Abstract</h4>
<p>We view the inertia construction of algebraic stacks as an operator on the Grothendieck groups of various categories of algebraic stacks. We are interested in showing that the inertia operator is (locally finite and) diagonalizable over for instance the field of rational functions of the motivic class of the affine line q = [A¹]. This is proved for the Grothendieck group of Deligne-Mumford stacks and the category of quasi-split Artin stacks. Motivated by the quasi-splitness condition we then develop a theory of linear algebraic stacks and algebroids, and define a space of stack functions over a linear algebraic stack. We prove diagonalization of the semisimple inertia for the space of stack functions. A different family of operators is then defined that are closely related to the semisimple inertia. These operators are diagonalizable on the Grothendieck ring itself (i.e. without inverting polynomials in q) and their corresponding eigenvalue decompositions are used to define a graded structure on the Grothendieck ring. We then define the structure of a Hall algebra on the space of stack functions. The commutative and non-commutative products of the Hall algebra respect the graded structure defined above. Moreover, the two multiplications coincide on the associated graded algebra. This result provides a geometric way of defining a Lie subalgebra of virtually indecomposables. Finally, for any algebroid, an ε-element is defined and shown to be contained in the space of virtually indecomposables. This is a new approach to the theory of generalized Donaldson-Thomas invariants.</p>
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<h4 class="pubtitle">Ringel-Hall algebras and applications to moduli </h4>
<div class="pubauthor">Pooya Ronagh</div>
<div class="pubcite"><span class="label label-success">M.Sc. Essay</span>University of British Columbia</div>
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<h4>Abstract</h4>
<p>In this essay we will survey some of the results of Markus Reineke on geometry of the moduli spaces of stable quiver representations, and Tom Bridgeland on properties of Donaldson-Thomas invariants of Calabi-Yau threefolds. The underlying idea of these results is to assign a suitable Hall algebra to the abelian category of objects of interest in the moduli problem and translate categorical statements about this category into identities in the Hall algebra. An integration on the Hall algebra is defined such that integrating identities in the Hall algebra will then produce generating functions involving invariants that we want to study.</p>
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Quantum Invariants of Calabi-Yau threefolds
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<div class="pubauthor">Lecture notes by Pooya Ronagh</div>
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<span class="label label-warning">Lecture notes</span> University of British Columbia, Topics in Algebraic Geometry, Spring 2014 </div>
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<h4>Source</h4>
<p>These notes are live-TeXed and compiled in the format of a book based on a course Prof. Jim Bryan offered in 2014 on the enumerative geometry of Calabi-Yau threefolds.</p>
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<span class="label label-warning">Lecture notes</span> University of British Columbia, Lie Theory, Fall 2011 </div>
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<h4>Source</h4><p>These notes are live-TeXed and compiled in the present format based on a course offered by Prof. Julia Gordon.</p>
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<span class="label label-warning">Lecture notes</span> University of British Columbia, Lie Theory, Spring 2011 </div>
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<h4>Source</h4><p>These notes are live-TeXed and compiled in the present format based on a course offered by Prof. Kalle Karu.</p>
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<span class="label label-warning">Lecture notes</span> University of British Columbia, Lie Theory, Fall 2011 </div>
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<h4>Source</h4><p>These notes are live-TeXed and compiled in the present format based on a course offered by Prof. Sujatha Ramdora.</p>
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<div class="pubauthor">Lecture notes by Pooya Ronagh</div>
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<span class="label label-warning">Lecture notes</span> University of British Columbia, Lie Theory, Spring 2011 </div>
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<h4>Source</h4><p>These notes are live-TeXed and compiled in the present format based on a course offered by Prof. Donald Stanley.</p>
<h4>Disclaimer</h4><p>Any mistakes, typos, messy type-setting you may find are due to this fact and does not reflect upon the content of the lectures. I would appreciate it if you point them out to me.</p>
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<div class="pubauthor">Lecture notes by Pooya Ronagh</div>
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<span class="label label-warning">Lecture notes</span> University of British Columbia, Lie Theory, Fall 2011 </div>
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<h4>Source</h4><p>These notes are live-TeXed and compiled in the present format based on a course offered by Prof. Zinovy Reichstein.</p>
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<span class="label label-warning">Lecture notes</span> University of British Columbia, Lie Theory, Spring 2011 </div>
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<h4>Source</h4><p>These notes are live-TeXed and compiled in the present format based on a seminar course organized by Prof. Julia Gordon.</p>
<h4>Disclaimer</h4><p>Any mistakes, typos, messy type-setting you may find are due to this fact and does not reflect upon the content of the lectures. I would appreciate it if you point them out to me.</p>
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<span class="label label-warning">Lecture notes</span> University of British Columbia, Topics in Algebraic Geometry, 2007 </div>
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<h4>Source</h4><p>These notes are based on a course offered by Prof. Kai Behrend.</p>
<h4>Disclaimer</h4><p>Any mistakes, typos, messy type-setting you may find are due to this fact and does not reflect upon the content of the lectures. I would appreciate it if you point them out to me.</p>
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<h4>Source</h4><p>These notes are based on a short-course offered by Prof. Kai Behrend.</p>
<h4>Disclaimer</h4><p>Any mistakes, typos, messy type-setting you may find are due to this fact and does not reflect upon the content of the lectures. I would appreciate it if you point them out to me.</p>
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<div class="pubauthor">Lecture notes by Pooya Ronagh</div>
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<span class="label label-warning">Lecture notes</span> Isaac Newton Institute for Mathematical Sciences, School on Moduli Spaces, 2011 </div>
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<h4>Source</h4><p>These notes are based on a short-course offered by Prof. Brent Doran.</p>
<h4>Disclaimer</h4><p>Any mistakes, typos, messy type-setting you may find are due to this fact and does not reflect upon the content of the lectures. I would appreciate it if you point them out to me.</p>
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<div class="pubauthor">Lecture notes by Pooya Ronagh</div>
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<span class="label label-warning">Lecture notes</span> Isaac Newton Institute for Mathematical Sciences, School on Moduli Spaces, 2011 </div>
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<h4>Source</h4><p>These notes are based on a short-course offered by Prof. Markus Reineke.</p>
<h4>Disclaimer</h4><p>Any mistakes, typos, messy type-setting you may find are due to this fact and does not reflect upon the content of the lectures. I would appreciate it if you point them out to me.</p>
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