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	<title>Warsaw Quantum Computing Group Meetings &#8211; CFT PAN &#8211; Centrum Fizyki Teoretycznej Polskiej Akademii Nauk</title>
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	<link>https://www.cft.edu.pl</link>
	<description>CFT PAN – Fizyka Teoretyczna, Astrofizyka i Kwanty. Badania Naukowe i Szkoła Doktorska Fizyki Teoretycznej w Warszawie.</description>
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	<title>Warsaw Quantum Computing Group Meetings &#8211; CFT PAN &#8211; Centrum Fizyki Teoretycznej Polskiej Akademii Nauk</title>
	<link>https://www.cft.edu.pl</link>
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		<title>Full nonlocality of non-maximally entangled states</title>
		<link>https://www.cft.edu.pl/nauka/seminaria/full-nonlocality-of-non-maximally-entangled-states/</link>
		
		<dc:creator><![CDATA[cft]]></dc:creator>
		<pubDate>Mon, 23 Feb 2026 11:04:35 +0000</pubDate>
				<guid isPermaLink="false">https://www.cft.edu.pl/?post_type=seminar&#038;p=60982</guid>

					<description><![CDATA[Abstract:It is a well-established fact that some quantum correlations arenonlocal, meaning they cannot be described by a local hidden variablemodel. Beyond this, certain quantum correlations are so strong thatthey cannot be reproduced even if one allows only a small fraction ofthe rounds to admit a local hidden variable description. Suchcorrelations are called fully nonlocal and [&#8230;]]]></description>
										<content:encoded><![CDATA[Abstract:<br>It is a well-established fact that some quantum correlations are<br>nonlocal, meaning they cannot be described by a local hidden variable<br>model. Beyond this, certain quantum correlations are so strong that<br>they cannot be reproduced even if one allows only a small fraction of<br>the rounds to admit a local hidden variable description. Such<br>correlations are called fully nonlocal and they give rise to Bell<br>inequalities in which the quantum bound saturates the non-signaling<br>bound. A famous example is the Peres–Mermin square, in which the<br>underlying state is a four-dimensional maximally entangled state.<br>Surprisingly, examples of full nonlocality are rare and typically<br>restricted to maximally entangled states. In this work, we show that<br>in every local Hilbert space dimension d≥4 there exist non-maximally<br>entangled pure states that are fully nonlocal. In fact, we derive<br>simple criteria ensuring full nonlocality that depend only on the<br>smallest and largest Schmidt coefficients. Furthermore, we show that<br>all pure entangled states can be activated to exhibit full nonlocality<br>in the many-copy scenario.<br><br>Remote guests are invited via Zoom:<br>Zoom link: <a href="https://us06web.zoom.us/j/84248911743?pwd=ZsiAOQbRgYCm5IFsArOnb18Fj5IsZh.1" target="_blank" rel="noopener noreferrer" data-saferedirecturl="https://www.google.com/url?q=https://us06web.zoom.us/j/84248911743?pwd%3DZsiAOQbRgYCm5IFsArOnb18Fj5IsZh.1&amp;source=gmail&amp;ust=1771930144918000&amp;usg=AOvVaw34I12fADg2NIj8_KjObpl0">https://us06web.zoom.us/j/8424<wbr>8911743?pwd=ZsiAOQbRgYCm5IFsAr<wbr>Onb18Fj5IsZh.1</a><br>Meeting ID: 842 4891 1743<br>Passcode: 394021]]></content:encoded>
					
		
		
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		<title>Random unitaries in extremely low depth</title>
		<link>https://www.cft.edu.pl/nauka/seminaria/random-unitaries-in-extremely-low-depth/</link>
		
		<dc:creator><![CDATA[cft]]></dc:creator>
		<pubDate>Mon, 19 Jan 2026 07:27:17 +0000</pubDate>
				<guid isPermaLink="false">https://www.cft.edu.pl/?post_type=seminar&#038;p=60310</guid>

					<description><![CDATA[Abstract:We prove that random quantum circuits on any geometry, including a one-dimensional line, can form approximate unitary designs over n qubits with logarithmic depth in n. In a similar spirit, we construct pseudorandom unitaries in one-dimensional circuits with polylogarithmic depth, and in all-to-all connected circuits with polyloglogarithmic depth. In all three settings, the dependence on [&#8230;]]]></description>
										<content:encoded><![CDATA[Abstract:<br><p data-start="110" data-end="588">We prove that random quantum circuits on any geometry, including a one-dimensional line, can form approximate unitary designs over <em data-start="241" data-end="244">n</em> qubits with logarithmic depth in <em data-start="278" data-end="281">n</em>. In a similar spirit, we construct pseudorandom unitaries in one-dimensional circuits with polylogarithmic depth, and in all-to-all connected circuits with polyloglogarithmic depth. In all three settings, the dependence on <em data-start="505" data-end="508">n</em> is optimal and yields an exponential improvement over previously known results.</p><p data-start="590" data-end="952">These shallow quantum circuits have low complexity and generate only short-range entanglement, yet they are indistinguishable from unitaries of exponential complexity. Our construction proceeds by gluing together local random unitaries acting on patches of qubits of logarithmic or polylogarithmic size, thereby forming a global random unitary on all <em data-start="941" data-end="944">n</em> qubits.</p><p data-start="954" data-end="1228">In the case of approximate unitary designs, the local unitaries are drawn from existing constructions of approximate unitary <em data-start="1079" data-end="1082">k</em>-designs and therefore inherit optimal scaling in <em data-start="1132" data-end="1135">k</em>. For pseudorandom unitaries, the local components are drawn from existing PRU constructions.</p><p data-start="1230" data-end="1601">Applications of our results include showing that classical shadows generated by one-dimensional logarithmic-depth Clifford circuits are as powerful as those obtained from deep circuits, demonstrating a superpolynomial quantum advantage in learning low-complexity physical systems, and establishing quantum hardness for recognizing phases of matter with topological order.</p><br><br>Remote guests are invited via Zoom:<br>Zoom link: <a href="https://us06web.zoom.us/j/84248911743?pwd=ZsiAOQbRgYCm5IFsArOnb18Fj5IsZh.1" target="_blank" rel="noopener noreferrer" data-saferedirecturl="https://www.google.com/url?q=https://us06web.zoom.us/j/84248911743?pwd%3DZsiAOQbRgYCm5IFsArOnb18Fj5IsZh.1&amp;source=gmail&amp;ust=1768676997153000&amp;usg=AOvVaw2sN3yCydZN0rlpRx0E84BU">https://us06web.zoom.us/j/8424<wbr>8911743?pwd=ZsiAOQbRgYCm5IFsAr<wbr>Onb18Fj5IsZh.1</a><br>Meeting ID: 842 4891 1743<br>Passcode: 394021<br><br>CET, Room D<br>]]></content:encoded>
					
		
		
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		<title>Certifying Majorana Fermions with Elegant-Like Bell Inequalities and a New Self-Testing Equivalence</title>
		<link>https://www.cft.edu.pl/nauka/seminaria/certifying-majorana-fermions-with-elegant-like-bell-inequalities-and-a-new-self-testing-equivalence/</link>
		
		<dc:creator><![CDATA[cft]]></dc:creator>
		<pubDate>Tue, 13 Jan 2026 07:18:37 +0000</pubDate>
				<guid isPermaLink="false">https://www.cft.edu.pl/?post_type=seminar&#038;p=60277</guid>

					<description><![CDATA[Abstract:Bell inequalities provide a fundamental tool for probing nonlocal correlations, yet their quantum bound is rarely accessible analytically. In my talk, I will present a general construction of Bell inequalities whose quantum bound can be computed exactly. This framework generalizes the Clauser–Horne–Shimony–Holt and Gisin’s elegant inequalities, and yields Bell expressions maximally violated by any number [&#8230;]]]></description>
										<content:encoded><![CDATA[Abstract:<br>Bell inequalities provide a fundamental tool for probing nonlocal correlations, yet their quantum bound is rarely accessible analytically. In my talk, I will present a general construction of Bell inequalities whose quantum bound can be computed exactly. This framework generalizes the Clauser–Horne–Shimony–Holt and Gisin’s elegant inequalities, and yields Bell expressions maximally violated by any number of pairwise anticommuting Clifford observables together with the corresponding maximally entangled state. Under suitable assumptions, these inequalities also enable device-independent certification of Majorana fermions, viewed as multiqubit realizations of Clifford algebra generators. Finally, I will highlight an additional equivalence (beyond local isometries and transposition) that must be included in self-testing: partial transposition applied to the shared state and measurements, which can leave all observable correlations invariant.<br><br>Remote guests are invited via Zoom:<br>Zoom link: <a href="https://us06web.zoom.us/j/84248911743?pwd=ZsiAOQbRgYCm5IFsArOnb18Fj5IsZh.1" target="_blank" rel="noopener noreferrer" data-saferedirecturl="https://www.google.com/url?q=https://us06web.zoom.us/j/84248911743?pwd%3DZsiAOQbRgYCm5IFsArOnb18Fj5IsZh.1&amp;source=gmail&amp;ust=1768315385305000&amp;usg=AOvVaw1Dsb_aBf05kKI25rcUjGhc">https://us06web.zoom.us/j/8424<wbr>8911743?pwd=ZsiAOQbRgYCm5IFsAr<wbr>Onb18Fj5IsZh.1</a><br>Meeting ID: 842 4891 1743<br>Passcode: 394021<br>]]></content:encoded>
					
		
		
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		<title>Self-Testing Tilted Strategies for Maximal Loophole-Free Nonlocality</title>
		<link>https://www.cft.edu.pl/nauka/seminaria/self-testing-tilted-strategies-for-maximal-loophole-free-nonlocality/</link>
		
		<dc:creator><![CDATA[cft]]></dc:creator>
		<pubDate>Thu, 11 Dec 2025 13:00:49 +0000</pubDate>
				<guid isPermaLink="false">https://www.cft.edu.pl/?post_type=seminar&#038;p=60109</guid>

					<description><![CDATA[Abstract:The degree of experimentally attainable nonlocality, as gauged by the loophole-free or effective violation of Bell inequalities, remains severely limited due to inefficient detectors. We address an experimentally motivated question: Which quantum strategies attain the maximal loophole-free nonlocality in the presence of inefficient detectors? For any Bell inequality and any specification of detection efficiencies, the [&#8230;]]]></description>
										<content:encoded><![CDATA[<p data-start="200" data-end="1338"><strong data-start="200" data-end="213">Abstract:</strong><br data-start="213" data-end="216">The degree of experimentally attainable nonlocality, as gauged by the loophole-free or effective violation of Bell inequalities, remains severely limited due to inefficient detectors. We address an experimentally motivated question: Which quantum strategies attain the maximal loophole-free nonlocality in the presence of inefficient detectors? For any Bell inequality and any specification of detection efficiencies, the optimal strategies are those that maximally violate a tilted version of the Bell inequality in ideal conditions. In the simplest scenario, we demonstrate that the quantum strategies that maximally violate the doubly-tilted versions of Clauser-Horne-Shimony-Holt inequality are unique up to local isometries. We utilize Jordan&#8217;s lemma and Grobner basis-based proof technique to analytically derive self-testing statements for the entire family of doubly-tilted CHSH inequalities and numerically demonstrate their robustness. These results enable us to reveal the insufficiency of even high levels of the Navascues-Pironio-Acin hierarchy to saturate the maximum quantum violation of these inequalities.<br><br></p><p data-start="1340" data-end="1510">Remote guests are invited via Zoom:<br data-start="1375" data-end="1378">Zoom link: <a class="decorated-link" href="https://us06web.zoom.us/j/84248911743?pwd=ZsiAOQbRgYCm5IFsArOnb18Fj5IsZh.1" target="_new" rel="noopener" data-start="1389" data-end="1463">https://us06web.zoom.us/j/84248911743?pwd=ZsiAOQbRgYCm5IFsArOnb18Fj5IsZh.1</a></p><br data-start="1463" data-end="1466">Meeting ID: 842 4891 1743<br data-start="1491" data-end="1494">Passcode: 394021]]></content:encoded>
					
		
		
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		<title>Quantum computing with single photons</title>
		<link>https://www.cft.edu.pl/nauka/seminaria/quantum-computing-with-single-photons/</link>
		
		<dc:creator><![CDATA[cft]]></dc:creator>
		<pubDate>Wed, 26 Nov 2025 12:36:18 +0000</pubDate>
				<guid isPermaLink="false">https://www.cft.edu.pl/?post_type=seminar&#038;p=60001</guid>

					<description><![CDATA[Abstract: Quandela is a start-up dedicated to building a photonicquantum computer based on quantum dot single photon sources. In thistalk, I will review Quandela’s technology and discuss paths forscaling to a fault-tolerant quantum computer. I will also presentrecent results on how to design and run quantum algorithms for near-and mid-term processors based on linear optics.Remote [&#8230;]]]></description>
										<content:encoded><![CDATA[Abstract: Quandela is a start-up dedicated to building a photonic<br>quantum computer based on quantum dot single photon sources. In this<br>talk, I will review Quandela’s technology and discuss paths for<br>scaling to a fault-tolerant quantum computer. I will also present<br>recent results on how to design and run quantum algorithms for near-<br>and mid-term processors based on linear optics.<br><br>Remote guests are invited via Zoom:<br>Zoom link: <a href="https://us06web.zoom.us/j/84248911743?pwd=ZsiAOQbRgYCm5IFsArOnb18Fj5IsZh.1" target="_blank" rel="noopener noreferrer" data-saferedirecturl="https://www.google.com/url?q=https://us06web.zoom.us/j/84248911743?pwd%3DZsiAOQbRgYCm5IFsArOnb18Fj5IsZh.1&amp;source=gmail&amp;ust=1764246792612000&amp;usg=AOvVaw2N14hw_sQ-dAM4t7qwnJ6q">https://us06web.zoom.us/j/8424<wbr>8911743?pwd=ZsiAOQbRgYCm5IFsAr<wbr>Onb18Fj5IsZh.1</a><br>Meeting ID: 842 4891 1743<br>Passcode: 394021]]></content:encoded>
					
		
		
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		<title>Discrete conformal field theories with dual-unitary circuits</title>
		<link>https://www.cft.edu.pl/nauka/seminaria/discrete-conformal-field-theories-with-dual-unitary-circuits/</link>
		
		<dc:creator><![CDATA[cft]]></dc:creator>
		<pubDate>Mon, 17 Nov 2025 12:06:27 +0000</pubDate>
				<guid isPermaLink="false">https://www.cft.edu.pl/?post_type=seminar&#038;p=59897</guid>

					<description><![CDATA[Dear Colleagues,We are pleased to announce the next seminar:Date: Nov 19, 2025 3;15 PM CET, ONLINE ONLYSpeaker: Lluis Masanes (UCL)Abstract:I will introduce discrete conformal field theories based on aconstruction with dual-unitary circuits. Using holography, we willinterpret these discrete CFTs as toy theories of quantum gravity,which transparently display the processes of black-hole formation andevaporation.Remote guests are [&#8230;]]]></description>
										<content:encoded><![CDATA[<strong><br>Dear Colleagues,<br>We are pleased to announce the next seminar:<br><br>Date: Nov 19, 2025 3;15 PM CET, ONLINE ONLY<br>Speaker: Lluis Masanes (UCL)<br><br>Abstract:<br>I will introduce discrete conformal field theories based on a<br>construction with dual-unitary circuits. Using holography, we will<br>interpret these discrete CFTs as toy theories of quantum gravity,<br>which transparently display the processes of black-hole formation and<br>evaporation.<br><br>Remote guests are invited via Zoom:<br>Zoom link: <a href="https://us06web.zoom.us/j/84248911743?pwd=ZsiAOQbRgYCm5IFsArOnb18Fj5IsZh.1" target="_blank" rel="noopener noreferrer" data-saferedirecturl="https://www.google.com/url?q=https://us06web.zoom.us/j/84248911743?pwd%3DZsiAOQbRgYCm5IFsArOnb18Fj5IsZh.1&amp;source=gmail&amp;ust=1763465113144000&amp;usg=AOvVaw1Gk3llXZpcwZu1s3Yy1C7x">https://us06web.zoom.us/j/8424<wbr>8911743?pwd=ZsiAOQbRgYCm5IFsAr<wbr>Onb18Fj5IsZh.1</a><br>Meeting ID: 842 4891 1743<br>Passcode: 394021<br><br></strong>]]></content:encoded>
					
		
		
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		<title>Quantum and Classical Simulations of Non-Equilibrium Quantum Many-Body Dynamics</title>
		<link>https://www.cft.edu.pl/nauka/seminaria/quantum-and-classical-simulations-of-non-equilibrium-quantum-many-body-dynamics/</link>
		
		<dc:creator><![CDATA[cft]]></dc:creator>
		<pubDate>Thu, 30 Oct 2025 07:48:19 +0000</pubDate>
				<guid isPermaLink="false">https://www.cft.edu.pl/?post_type=seminar&#038;p=59693</guid>

					<description><![CDATA[Speaker: Marek Rams (Instytut Fizyki Teoretycznej, Uniwersytet Jagielloński w Krakowie)Abstract:Simulating dynamical processes in quantum many-body systems poses significant challenges. Much hope for advancing our understanding of such phenomena lies in the development of dedicated quantum simulators and quantum computers. In this context, we are currently witnessing a race for supremacy between advanced numerical algorithms—based on neural and [&#8230;]]]></description>
										<content:encoded><![CDATA[<p>Speaker: <strong>Marek Rams</strong> (Instytut Fizyki Teoretycznej, Uniwersytet Jagielloński w Krakowie)<br></p><p>Abstract:</p><p>Simulating dynamical processes in quantum many-body systems poses significant challenges. Much hope for advancing our understanding of such phenomena lies in the development of dedicated quantum simulators and quantum computers. In this context, we are currently witnessing a race for supremacy between advanced numerical algorithms—based on neural and tensor networks—and the current generation of quantum computers. In this presentation, I will explore aspects of this race through the lens of one of the simplest many-body models: the quantum Ising model on a square lattice, driven out of equilibrium by a time-dependent transverse field.</p><p>&nbsp;</p><p>Time and Place: <strong>Nov 05, 2025, 02:00 PM Warsaw, IF PAN, room D</strong></p><p>&nbsp;</p><p>Remote guests are invited via Zoom:</p><p>Zoom link: <strong><a href="https://www.google.com/url?q=https://us06web.zoom.us/j/84248911743?pwd%3DZsiAOQbRgYCm5IFsArOnb18Fj5IsZh.1&amp;source=gmail-imap&amp;ust=1762354857000000&amp;usg=AOvVaw17czXBTpei-JUS0VzNbiXT" target="_blank" rel="noopener">https://us06web.zoom.us/j/84248911743?pwd=ZsiAOQbRgYCm5IFsArOnb18Fj5IsZh.1</a></strong><br>Meeting ID: <strong>842 4891 1743</strong><br>Passcode: <strong>394021</strong><br><br><br></p>]]></content:encoded>
					
		
		
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		<title>Self-testing Quantum States and Measurements in Quantum Networks</title>
		<link>https://www.cft.edu.pl/nauka/seminaria/self-testing-quantum-states-and-measurements-in-quantum-networks/</link>
		
		<dc:creator><![CDATA[cft]]></dc:creator>
		<pubDate>Tue, 21 Oct 2025 10:24:47 +0000</pubDate>
				<guid isPermaLink="false">https://www.cft.edu.pl/?post_type=seminar&#038;p=59549</guid>

					<description><![CDATA[Abstract:Bell nonlocality—the existence of correlations that cannot be reproduced by means of local hidden variable models—is one of the most distinctive features of quantum theory. Indeed, the pioneering experiments to verify the existence of this phenomenon were awarded a Nobel Prize in Physics in 2022. What is more, beyond its fundamental interest, Bell nonlocality has [&#8230;]]]></description>
										<content:encoded><![CDATA[<div dir="ltr">Abstract:</div><div dir="ltr"><p>Bell nonlocality—the existence of correlations that cannot be reproduced by means of local hidden variable models—is one of the most distinctive features of quantum theory. Indeed, the pioneering experiments to verify the existence of this phenomenon were awarded a Nobel Prize in Physics in 2022. What is more, beyond its fundamental interest, Bell nonlocality has been recognized as a valuable resource for various applications within device-independent quantum information processing, where observers process information without placing trust into the devices themselves. One of such applications that has recently gained substantial interest, driven by the recent rapid development of new quantum technologies, is the device-independent certification of entangled quantum states and the measurements performed on them, commonly referred to as self-testing. In this talk I will present our recent results [1,2] exploiting Bell nonlocality to design self-testing schemes for arbitrary quantum states and measurements. Our results are formulated within the framework of quantum networks in which many observers share correlations, possibly quantum, which are distributed by multiple sources. The key ingredient of our method is the construction of a family of Bell inequalities that enable the self-testing of a tomographically complete set of measurements performed by an arbitrary number of observers, as well as an arbitrary number of maximally entangled pair of particles shared among them.</p><p>References:</p><p>[1] S. Sarkar, C. Datta, S. Halder, R. Augusiak, <i>Self-testing composite measurements and bound entangled state in a single quantum network</i>, <a href="https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.134.190203" target="_blank" rel="noopener" data-saferedirecturl="https://www.google.com/url?q=https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.134.190203&amp;source=gmail&amp;ust=1761126913043000&amp;usg=AOvVaw319tq1o6ddXhSfztQASb7J">Phys. Rev. Lett. </a><a href="https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.134.190203" target="_blank" rel="noopener" data-saferedirecturl="https://www.google.com/url?q=https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.134.190203&amp;source=gmail&amp;ust=1761126913043000&amp;usg=AOvVaw319tq1o6ddXhSfztQASb7J"><b>134</b>, 190203 (2025)</a>.</p><p>[2] S. Sarkar, A. C. Orthey, Jr., R. Augusiak, <i>A universal scheme to self-test any quantum state and extremal measurement</i>, <a href="https://arxiv.org/abs/2312.04405" target="_blank" rel="noopener" data-saferedirecturl="https://www.google.com/url?q=https://arxiv.org/abs/2312.04405&amp;source=gmail&amp;ust=1761126913043000&amp;usg=AOvVaw2Eq3zpJiQW8bTxq9ZVz1Pe">arXiv:</a><a href="https://arxiv.org/abs/2312.04405" target="_blank" rel="noopener" data-saferedirecturl="https://www.google.com/url?q=https://arxiv.org/abs/2312.04405&amp;source=gmail&amp;ust=1761126913043000&amp;usg=AOvVaw2Eq3zpJiQW8bTxq9ZVz1Pe">2312.04405</a>.</p><div><br></div><div>Time and Place: <b>Oct 22, 2025, 02:00 PM Warsaw, room D</b></div><div><br></div><div>Remote guests are invited via Zoom:</div><div>Zoom link: <b><a href="https://us06web.zoom.us/j/84248911743?pwd=ZsiAOQbRgYCm5IFsArOnb18Fj5IsZh.1" target="_blank" rel="noopener" data-saferedirecturl="https://www.google.com/url?q=https://us06web.zoom.us/j/84248911743?pwd%3DZsiAOQbRgYCm5IFsArOnb18Fj5IsZh.1&amp;source=gmail&amp;ust=1761126913043000&amp;usg=AOvVaw0kzRpApNxCeOLN6dRJBHAj">https://us06web.zoom.us/<wbr>j/84248911743?pwd=<wbr>ZsiAOQbRgYCm5IFsArOnb18Fj5IsZh<wbr>.1</a></b></div></div>]]></content:encoded>
					
		
		
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		<title>Optimal sample complexities for learning functions on the unitary group, and more</title>
		<link>https://www.cft.edu.pl/nauka/seminaria/optimal-sample-complexities-for-learning-functions-on-the-unitary-group-and-more/</link>
		
		<dc:creator><![CDATA[cft]]></dc:creator>
		<pubDate>Mon, 06 Oct 2025 08:36:24 +0000</pubDate>
				<guid isPermaLink="false">https://www.cft.edu.pl/?post_type=seminar&#038;p=59347</guid>

					<description><![CDATA[Abstract:Estimating properties of unknown unitary operations is a fundamental task in quantum information science. While full unitary tomography requires a number of samples to the unknown unitary scaling linearly with the dimension (implying exponentially with the number of qubits), estimating specific functions of a unitary can be significantly more eﬃcient. In this paper, we present [&#8230;]]]></description>
										<content:encoded><![CDATA[<div dir="ltr">Abstract:<br>Estimating properties of unknown unitary operations is a fundamental task in quantum information science. While full unitary tomography requires a number of samples to the unknown unitary scaling linearly with the dimension (implying exponentially with the number of qubits), estimating specific functions of a unitary can be significantly more eﬃcient. In this paper, we present a unified framework for the sample-eﬃcient estimation of arbitrary square integrable functions f : U(d) → C, using only access to the controlled-unitary operation. We first provide a tight characterization of the optimal sample complexity when the accuracy is measured by the averaged bias over the unitary U(d). We then construct a sample-eﬃcient estimation algorithm that becomes optimal under the Probably Approximately Correct (PAC) learning criterion for various classes of functions.</div><p>Based on: <a href="https://scirate.com/arxiv/2509.05710" target="_blank" rel="noopener" data-saferedirecturl="https://www.google.com/url?q=https://scirate.com/arxiv/2509.05710&amp;source=gmail&amp;ust=1759684189410000&amp;usg=AOvVaw2_RW2dsXd_LJkTLSjjJwh6">https://scirate.com/arxiv/<wbr>2509.05710</a></p><p>I will then explore some other topics related to my earlier works, provided time permits.</p><div><span style="color: #000000; font-family: Arial;"><br></span>Time and Place: <b>Oct 8, 2025, 02:00 PM Warsaw, room 203</b></div><div><br></div><div>Remote guests are invited via Zoom:</div><div>Zoom link: <b><a href="https://us06web.zoom.us/j/84248911743?pwd=ZsiAOQbRgYCm5IFsArOnb18Fj5IsZh.1" target="_blank" rel="noopener" data-saferedirecturl="https://www.google.com/url?q=https://us06web.zoom.us/j/84248911743?pwd%3DZsiAOQbRgYCm5IFsArOnb18Fj5IsZh.1&amp;source=gmail&amp;ust=1759684189410000&amp;usg=AOvVaw3ExCifcuCt6WLylPm9jDph">https://us06web.zoom.us/<wbr>j/84248911743?pwd=<wbr>ZsiAOQbRgYCm5IFsArOnb18Fj5IsZh<wbr>.1</a></b><br><br></div>]]></content:encoded>
					
		
		
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		<title>All classes of informationally complete symmetric measurements in finite dimensions</title>
		<link>https://www.cft.edu.pl/nauka/seminaria/all-classes-of-informationally-complete-symmetric-measurements-in-finite-dimensions/</link>
		
		<dc:creator><![CDATA[dev]]></dc:creator>
		<pubDate>Wed, 15 Jan 2025 06:53:10 +0000</pubDate>
				<guid isPermaLink="false">https://cft.edu.pl/?post_type=seminar&#038;p=9569</guid>

					<description><![CDATA[Abstract:A broad class of informationally complete symmetric measurements is introduced. It can be understood as a common generalization of symmetric, informationally complete (SIC) POVMs and mutually unbiased bases (MUBs). Additionally, it provides a natural way to define two new families of mutually unbiased symmetric measurement operators in any finite dimension. I show a general method [&#8230;]]]></description>
										<content:encoded><![CDATA[<p>Abstract:</p><p id="">A broad class of informationally complete symmetric measurements is introduced. It can be understood as a common generalization of symmetric, informationally complete (SIC) POVMs and mutually unbiased bases (MUBs). Additionally, it provides a natural way to define two new families of mutually unbiased symmetric measurement operators in any finite dimension. I show a general method of their construction, together with an example of an optimal measurement. Finally, I analyze the properties of symmetric measurements and provide applications in entropic relations and entanglement detection.</p><p id=""><br>Time: <strong id="">Jan 8, 2025 02:30 PM Warsaw</strong><br>Zoom link: <a href="https://us05web.zoom.us/j/83922907300?pwd=S2Y2RiCKa7sD55bf3Rp2i6aamQuSkN.1" target="_blank" id="" rel="noopener"><strong id="">https://us05web.zoom.us/j/83922907300?pwd=S2Y2RiCKa7sD55bf3Rp2i6aamQuSkN.1</strong></a><br>Meeting ID: <strong id="">839 2290 7300</strong><br>Passcode: <strong id="">41FiTq</strong><br><br>&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;&#8212;-</p><p>‍</p>]]></content:encoded>
					
		
		
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