<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Ivan Šupić | LIP6 - Équipe QI</title><link>https://qi.lip6.fr/fr/people/ivan-supic/</link><atom:link href="https://qi.lip6.fr/fr/people/ivan-supic/index.xml" rel="self" type="application/rss+xml"/><description>Ivan Šupić</description><generator>Hugo Blox Builder (https://hugoblox.com)</generator><language>fr</language><copyright>© 2022 LIP6 Quantum Information Team</copyright><lastBuildDate>Mon, 09 Mar 2026 00:00:00 +0000</lastBuildDate><image><url>https://qi.lip6.fr/media/icon_hudf2fdaa51677944daa4f50609104ef9a_13950_512x512_fill_lanczos_center_3.png</url><title>Ivan Šupić</title><link>https://qi.lip6.fr/fr/people/ivan-supic/</link></image><item><title>Composable simultaneous purification: when all communication scenarios reduce to spatial correlations</title><link>https://qi.lip6.fr/fr/publication/5543334-composable-simultaneous-purification-when-all-communication-scenarios-reduce-to-spatial-correlations/</link><pubDate>Mon, 09 Mar 2026 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/5543334-composable-simultaneous-purification-when-all-communication-scenarios-reduce-to-spatial-correlations/</guid><description>&lt;p>Bell non-locality is a powerful framework to distinguish classical, quantum and post-quantum resources, which relies on non-communicating players. Under which restriction can we have the same separations, if we allow for communication? Non-signalling state assemblages, and the fact that they can always be simultaneously purified, turned out to be the key element to restrict the simplest bipartite communication scenario, the prepare-and-measure, to the standard bipartite Bell scenario. Yet, many distinctive features of quantum theory are genuinely multipartite and cannot be reduced to two-party behaviour. In this work we are interested in extending this simultaneous purification inspired result to all multipartite communication schemes. As a first step, we unify and extend the simultaneous purification result from states to instruments and super-instruments, which are composable structures, and open up the possibility to explore more complex communication scenarios. Our main contribution is to establish that arbitrary compositions of non-signalling assemblages cannot escape the standard spatial quantum Bell correlations set. As a consequence, any interactive quantum realization of correlations outside of this set must involve at least one signalling assemblage of quantum operations, even when the resulting correlations are non-signalling.&lt;/p></description></item><item><title>Quantitative quantum soundness for all multipartite compiled nonlocal games</title><link>https://qi.lip6.fr/fr/publication/5543393-quantitative-quantum-soundness-for-all-multipartite-compiled-nonlocal-games/</link><pubDate>Mon, 09 Mar 2026 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/5543393-quantitative-quantum-soundness-for-all-multipartite-compiled-nonlocal-games/</guid><description>&lt;p>Compiled nonlocal games transfer the power of Bell-type multi-prover tests into a single-device setting by replacing spatial separation with cryptography. Concretely, the KLVY compiler (STOC'23) maps any multi-prover game to an interactive single-prover protocol, using quantum homomorphic encryption. A crucial security property of such compilers is quantum soundness, which ensures that a dishonest quantum prover cannot exceed the original game&amp;rsquo;s quantum value. For practical cryptographic implementations, this soundness must be quantitative, providing concrete bounds, rather than merely asymptotic. While quantitative quantum soundness has been established for the KLVY compiler in the bipartite case, it has only been shown asymptotically for multipartite games. This is a significant gap, as multipartite nonlocality exhibits phenomena with no bipartite analogue, and the difficulty of enforcing space-like separation makes single-device compilation especially compelling. This work closes this gap by showing the quantitative quantum soundness of the KLVY compiler for all multipartite nonlocal games. On the way, we introduce an NPA-like hierarchy for quantum instruments and prove its completeness, thereby characterizing correlations from operationally-non-signaling sequential strategies. We further develop novel geometric arguments for the decomposition of sequential strategies into their signaling and non-signaling parts, which might be of independent interest.&lt;/p></description></item><item><title>Bounding the asymptotic quantum value of all multipartite compiled non-local games</title><link>https://qi.lip6.fr/fr/publication/5543388-bounding-the-asymptotic-quantum-value-of-all-multipartite-compiled-non-local-games/</link><pubDate>Sun, 11 Jan 2026 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/5543388-bounding-the-asymptotic-quantum-value-of-all-multipartite-compiled-non-local-games/</guid><description>&lt;p>Abstract Non-local games are a powerful tool to distinguish between correlations possible in classical and quantum worlds. Kalai et al. (STOC’23) proposed a compiler that converts multipartite non-local games into interactive protocols with a single prover, relying on cryptographic tools to remove the assumption of physical separation of the players. While quantum completeness and classical soundness of the construction have been established for all multipartite games, quantum soundness is known only in the special case of bipartite games. In this paper, we prove that the Kalai et al.’s compiler indeed achieves quantum soundness for all multipartite compiled non-local games, by showing that any correlations that can be generated in the asymptotic case correspond to quantum commuting strategies. Our proof uses techniques from the theory of operator algebras, and relies on a characterisation of sequential operationally no-signalling strategies as quantum commuting operator strategies in the multipartite case, thereby generalising several previous results. On the way, we construct universal C(^&lt;em>)-algebras of sequential PVMs and prove a new chain rule for Radon-Nikodym derivatives of completely positive maps on C(^&lt;/em>)-algebras which may be of independent interest.&lt;/p></description></item><item><title>Translating Bell Non-Locality to Prepare-and-Measure Scenarios under Dimensional Constraints</title><link>https://qi.lip6.fr/fr/publication/5407959-translating-bell-non-locality-to-prepare-and-measure-scenarios-under-dimensional-constraints/</link><pubDate>Tue, 09 Dec 2025 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/5407959-translating-bell-non-locality-to-prepare-and-measure-scenarios-under-dimensional-constraints/</guid><description>&lt;p>Understanding the connections between different quantum information protocols has been proven fruitful for both theoretical insights and experimental applications. In this work, we explore the relationship between non-local and prepare-and-measure scenarios, proposing a systematic way to translate bipartite Bell inequalities into dimensionally-bounded prepare-and-measure tasks. We identify sufficient conditions under which the translation preserves the quantum bound and self-testing properties, enabling a wide range of certification protocols originally developed for the non-local setting to be adapted to the sequential framework of prepare-and-measure with a dimensional bound. While the dimensionality bound is not device-independent, it still is a practical and experimentally reasonable assumption in many cases of interest. In some instances, we find new experimentally-friendly certification protocols. In others, we demonstrate equivalences with already known prepare-and-measure protocols, where self-testing results were previously established using alternative mathematical methods. Our results unify different quantum correlation frameworks, and contribute to the ongoing research effort of studying the interplay between parallel and sequential protocols.&lt;/p></description></item><item><title>Quantum bounds for compiled XOR games and $d$-outcome CHSH games</title><link>https://qi.lip6.fr/fr/publication/4803631-quantum-bounds-for-compiled-xor-games-and-d-outcome-chsh-games/</link><pubDate>Tue, 28 Oct 2025 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/4803631-quantum-bounds-for-compiled-xor-games-and-d-outcome-chsh-games/</guid><description>&lt;p>Nonlocal games play a crucial role in quantum information theory and have numerous applications in certification and cryptographic protocols. Kalai et al. (STOC 2023) introduced a procedure to compile a nonlocal game into a single-prover interactive proof, using a quantum homomorphic encryption scheme, and showed that their compilation method preserves the classical bound of the game. Natarajan and Zhang (FOCS 2023) then showed that the quantum bound is preserved for the specific case of the CHSH game. Extending the proof techniques of Natarajan and Zhang, we show that the compilation procedure of Kalai et al. preserves the quantum bound for two classes of games: XOR games and d-outcome CHSH games. We also establish that, for any pair of qubit measurements, there exists an XOR game such that its optimal winning probability serves as a self-test for that particular pair of measurements.&lt;/p></description></item><item><title>Robustly self-testing all maximally entangled states in every finite dimension</title><link>https://qi.lip6.fr/fr/publication/5263472-robustly-self-testing-all-maximally-entangled-states-in-every-finite-dimension/</link><pubDate>Tue, 16 Sep 2025 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/5263472-robustly-self-testing-all-maximally-entangled-states-in-every-finite-dimension/</guid><description>&lt;p>We establish a device-independent, noise-tolerant certification of maximally entangled states in every finite dimension $d$. The core ingredient is a $d$-input, $d$-outcome Bell experiment that generalizes the Clauser-Horne-Shimony-Holt test from qubits to qudits, where each setting is a non-diagonal Heisenberg-Weyl observable. For every odd prime $d \geq 3$, the associated Bell operator has an exact sum-of-positive-operators decomposition, yielding the Cirelson bound in closed form, from which we reconstruct the Heisenberg-Weyl commutation relations on the support of the state. We then extend the Mayers-Yao local isometry from qubits to prime-dimensional systems and show that any $ε$-near-optimal strategy below that bound is, up to local isometries, within trace distance $δ= \mathcal{O}(\sqrtε)$ of the ideal maximally entangled state; the implemented measurements are correspondingly close to the target observables. Via a tensor-factor argument, the prime-dimension result extends the self-testing protocol to every composite dimension $d$. The protocol uses standard Heisenberg-Weyl operations and non-Clifford phase gates that are diagonal in the computational basis, making it directly applicable to high-dimensional photonic and atomic platforms.&lt;/p></description></item><item><title>Experimental Fiber-Based Quantum Triangle-Network Nonlocality with a Telecom Al Ga As Multiplexed Entangled-Photon Source</title><link>https://qi.lip6.fr/fr/publication/5346284-experimental-fiber-based-quantum-triangle-network-nonlocality-with-a-telecom-al-ga-as-multiplexed-entangled-photon-source/</link><pubDate>Mon, 21 Apr 2025 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/5346284-experimental-fiber-based-quantum-triangle-network-nonlocality-with-a-telecom-al-ga-as-multiplexed-entangled-photon-source/</guid><description>&lt;p>The exploration of the concept of nonlocality beyond standard Bell scenarios in quantum network architectures unveils fundamentally new forms of correlations that hold a strong potential for future applications of quantum communication networks. To materialize this potential, it is necessary to adapt theoretical advances to realistic configurations. Here, we consider a quantum triangle network, for which is has been shown in theory that, remarkably, quantum nonlocality without inputs can be demonstrated for sources with an arbitrarily small level of independence. We realize such correlated sources experimentally by carefully engineering the output state of a single Al Ga As multiplexed entangled-photon source, exploiting energy-matched channels cut in its broad spectrum. This simulated triangle network, based on standard fiber telecom components, is then used to violate experimentally a Bell-like inequality that we derive to capture the effect of noise in the correlations present in our system. We also rigorously validate our findings by analyzing the mutual information between the generated states. Our results allow us to deepen our understanding of network nonlocality while also pushing its practical relevance for quantum communication networks.&lt;/p></description></item><item><title>Experimental Fiber-Based Quantum Triangle-Network Nonlocality with a Telecom Al Ga As Multiplexed Entangled-Photon Source</title><link>https://qi.lip6.fr/fr/publication/5405468-experimental-fiber-based-quantum-triangle-network-nonlocality-with-a-telecom-al-ga-as-multiplexed-entangled-photon-source/</link><pubDate>Mon, 21 Apr 2025 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/5405468-experimental-fiber-based-quantum-triangle-network-nonlocality-with-a-telecom-al-ga-as-multiplexed-entangled-photon-source/</guid><description>&lt;p>The exploration of the concept of nonlocality beyond standard Bell scenarios in quantum network architectures unveils fundamentally new forms of correlations that hold a strong potential for future applications of quantum communication networks. To materialize this potential, it is necessary to adapt theoretical advances to realistic configurations. Here, we consider a quantum triangle network, for which is has been shown in theory that, remarkably, quantum nonlocality without inputs can be demonstrated for sources with an arbitrarily small level of independence. We realize such correlated sources experimentally by carefully engineering the output state of a single Al Ga As multiplexed entangled-photon source, exploiting energy-matched channels cut in its broad spectrum. This simulated triangle network, based on standard fiber telecom components, is then used to violate experimentally a Bell-like inequality that we derive to capture the effect of noise in the correlations present in our system. We also rigorously validate our findings by analyzing the mutual information between the generated states. Our results allow us to deepen our understanding of network nonlocality while also pushing its practical relevance for quantum communication networks.&lt;/p></description></item><item><title>Experimental Sample-Efficient and Device-Independent GHZ State Certification</title><link>https://qi.lip6.fr/fr/publication/4803638-experimental-sample-efficient-and-device-independent-ghz-state-certification/</link><pubDate>Mon, 25 Nov 2024 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/4803638-experimental-sample-efficient-and-device-independent-ghz-state-certification/</guid><description>&lt;p>The certification of quantum resources is a critical tool in the development of quantum information processing. In particular, quantum state verification is a fundamental building block for communication and computation applications, determining whether the involved parties can trust the resources at hand or whether the application should be aborted. Self-testing methods have been used to tackle such verification tasks in a device-independent (DI) setting. However, these approaches commonly consider the limit of large (asymptotic), identically and independently distributed (IID) samples, which weakens the DI claim and poses serious challenges to their experimental implementation. Here we overcome these challenges by adopting a theoretical protocol enabling the certification of quantum states in the few-copies and non-IID regime and by leveraging a high-fidelity multipartite entangled photon source. This allows us to show the efficient and device-independent certification of a single copy of a four-qubit GHZ state that can readily be used for the robust and reliable implementation of quantum information tasks.&lt;/p></description></item><item><title>Network-Device-Independent Certification of Causal Nonseparability</title><link>https://qi.lip6.fr/fr/publication/4760947-network-device-independent-certification-of-causal-nonseparability/</link><pubDate>Wed, 30 Oct 2024 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/4760947-network-device-independent-certification-of-causal-nonseparability/</guid><description>&lt;p>Causal nonseparability is the property underlying quantum processes incompatible with a definite causal order. So far it has remained a central open question as to whether any process with a clear physical realisation can violate a causal inequality, so that its causal nonseparability can be certified in a device-independent way, as originally conceived. Here we present a method solely based on the observed correlations, which certifies the causal nonseparability of all the processes that can induce a causally nonseparable distributed measurement in a scenario with trusted quantum input states, as defined in [Dourdent et al., Phys. Rev. Lett. 129, 090402 (2022)]. This notably includes the celebrated quantum switch. This device-independent certification is achieved by introducing a network of untrusted operations, allowing one to self-test the quantum inputs on which the effective distributed measurement induced by the process is performed.&lt;/p></description></item><item><title>Bell Nonlocality from Wigner Negativity in Qudit Systems</title><link>https://qi.lip6.fr/fr/publication/4610059-bell-nonlocality-from-wigner-negativity-in-qudit-systems/</link><pubDate>Wed, 12 Jun 2024 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/4610059-bell-nonlocality-from-wigner-negativity-in-qudit-systems/</guid><description>&lt;p>Nonlocality is an essential concept that distinguishes quantum from classical models and has been extensively studied in systems of qubits. For higher-dimensional systems, certain results for their two-level counterpart, like Bell violations with stabilizer states and Clifford operators, do not generalize. On the other hand, similar to continuous variable systems, Wigner negativity is necessary for nonlocality in qudit systems. We propose a family of Bell inequalities that inquire correlations related to the Wigner negativity of stabilizer states under the adjoint action of a generalization of the qubit $\pi/8$ gate, which, in the bipartite case, is an abstraction of the CHSH inequality. The classical bound is simple to compute, and a specified stabilizer state maximally violates the inequality among all qudit states based on the Wigner negativity and an inequality between the 1-norm and the maximum norm. The Bell operator not only serves as a measure for the singlet fraction but also quantifies the volume of Wigner negativity. Furthermore, we give deterministic Bell violations, as well as violations with a constant number of measurements, for the Bell state relying on operators innate to higher-dimensional systems than the qudit at hand.&lt;/p></description></item><item><title>Self-Testing Graph States Permitting Bounded Classical Communication</title><link>https://qi.lip6.fr/fr/publication/4568664-self-testing-graph-states-permitting-bounded-classical-communication/</link><pubDate>Sun, 05 May 2024 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/4568664-self-testing-graph-states-permitting-bounded-classical-communication/</guid><description>&lt;p>Self-testing identifies quantum states and correlations that exhibit non-locality, distinguishing them, up to local transformations, from other quantum states. Due to their strong non-locality, all graph states can be self-tested with strictly local measurement devices. Moreover, graph states display non-local correlations even when bounded classical communication on the underlying graph is permitted, a feature that has found applications in proving a circuit-depth separation between classical and quantum computing. In the framework of bounded classical communication, we show that certain graph states with appropriate symmetry can be robustly self-tested, by providing an explicit self-test for the circular graph state and the honeycomb cluster state. Since communication generally obstructs self-testing of graph states, we further provide a procedure to robustly self-test any graph state from larger ones that exhibit non-local correlations in the communication scenario. Furthermore, in the standard setup without classical communication, we demonstrate that any graph state from an underlying connected graph with at least three vertices can be robustly self-tested using only Pauli measurements.&lt;/p></description></item><item><title>Experimental Certification of Quantum Transmission via Bell's Theorem</title><link>https://qi.lip6.fr/fr/publication/4306760-experimental-certification-of-quantum-transmission-via-bell-s-theorem/</link><pubDate>Sat, 25 Nov 2023 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/4306760-experimental-certification-of-quantum-transmission-via-bell-s-theorem/</guid><description>&lt;p>Quantum transmission links are central elements in essentially all implementations of quantum information protocols. Emerging progress in quantum technologies involving such links needs to be accompanied by appropriate certification tools. In adversarial scenarios, a certification method can be vulnerable to attacks if too much trust is placed on the underlying system. Here, we propose a protocol in a device independent framework, which allows for the certification of practical quantum transmission links in scenarios where minimal assumptions are made about the functioning of the certification setup. In particular, we take unavoidable transmission losses into account by modeling the link as a completely-positive trace-decreasing map. We also, crucially, remove the assumption of independent and identically distributed samples, which is known to be incompatible with adversarial settings. Finally, in view of the use of the certified transmitted states for follow-up applications, our protocol moves beyond certification of the channel to allow us to estimate the quality of the transmitted state itself. To illustrate the practical relevance and the feasibility of our protocol with currently available technology we provide an experimental implementation based on a state-of-the-art polarization entangled photon pair source in a Sagnac configuration and analyze its robustness for realistic losses and errors.&lt;/p></description></item><item><title>Quantum nonlocality in presence of strong measurement dependence</title><link>https://qi.lip6.fr/fr/publication/3783004-quantum-nonlocality-in-presence-of-strong-measurement-dependence/</link><pubDate>Sun, 01 Oct 2023 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/3783004-quantum-nonlocality-in-presence-of-strong-measurement-dependence/</guid><description>&lt;p>It is well known that the effect of quantum nonlocality, as witnessed by violation of a Bell inequality, can be observed even when relaxing the assumption of measurement independence, i.e. allowing for the source to be partially correlated with the choices of measurement settings. But what is the minimal amount of measurement independence needed for observing quantum nonlocality? Here we explore this question and consider models with strong measurement-dependent locality, where measurement choices can be perfectly determined in almost all rounds of the Bell test. Yet, we show that quantum nonlocality can still be observed in this scenario, which we conjecture is minimal within the framework we use. We also discuss potential applications in randomness amplification.&lt;/p></description></item><item><title>Self-testing nonlocality without entanglement</title><link>https://qi.lip6.fr/fr/publication/3630792-self-testing-nonlocality-without-entanglement/</link><pubDate>Sun, 01 Jan 2023 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/3630792-self-testing-nonlocality-without-entanglement/</guid><description>&lt;p>Quantum theory allows for nonlocality without entanglement. Notably, there exist bipartite quantum measurements consisting of only product eigenstates, yet they cannot be implemented via local quantum operations and classical communication. In the present work, we show that a measurement exhibiting nonlocality without entanglement can be certified in a device-independent manner. Specifically, we consider a simple quantum network and construct a self-testing procedure. This result also demonstrates that genuine network quantum nonlocality can be obtained using only non-entangled measurements. From a more general perspective, our work establishes a connection between the effect of nonlocality without entanglement and the area of Bell nonlocality.&lt;/p></description></item><item><title>Semi-device-independent Certification of Causal Nonseparability with Trusted Quantum Inputs</title><link>https://qi.lip6.fr/fr/publication/3764899-semi-device-independent-certification-of-causal-nonseparability-with-trusted-quantum-inputs/</link><pubDate>Fri, 26 Aug 2022 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/3764899-semi-device-independent-certification-of-causal-nonseparability-with-trusted-quantum-inputs/</guid><description>&lt;p>While the standard formulation of quantum theory assumes a fixed background causal structure, one can relax this assumption within the so-called process matrix framework. Remarkably, some processes, termed causally nonseparable, are incompatible with a definite causal order. We explore a form of certification of causal nonseparability in a semi-device-independent scenario where the involved parties receive trusted quantum inputs, but whose operations are otherwise uncharacterised. Defining the notion of causally nonseparable distributed measurements, we show that certain causally nonseparable processes which cannot violate any causal inequality, such as the canonical example of the quantum switch, can generate noncausal correlations in such a scenario. Moreover, by further imposing some natural structure to the untrusted operations, we show that all bipartite causally nonseparable process matrices can be certified with trusted quantum inputs.&lt;/p></description></item><item><title>Genuine network quantum nonlocality and self-testing</title><link>https://qi.lip6.fr/fr/publication/3591199-genuine-network-quantum-nonlocality-and-self-testing/</link><pubDate>Sat, 01 Jan 2022 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/3591199-genuine-network-quantum-nonlocality-and-self-testing/</guid><description>&lt;p>The network structure offers in principle the possibility for novel forms of quantum nonlocal correlations, that are proper to networks and cannot be traced back to standard quantum Bell nonlocality. Here we define a notion of genuine network quantum nonlocality. Our approach is operational and views standard quantum nonlocality as a resource for producing correlations in networks. We show several examples of correlations that are genuine network nonlocal, considering the so-called bilocality network of entanglement swapping. In particular, we present an example of quantum self-testing which relies on the network structure; the considered correlations are non-bilocal, but are local according to the usual definition of Bell locality.&lt;/p></description></item><item><title>Sample-efficient device-independent quantum state verification and certification</title><link>https://qi.lip6.fr/fr/publication/3584440-sample-efficient-device-independent-quantum-state-verification-and-certification/</link><pubDate>Sat, 01 Jan 2022 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/3584440-sample-efficient-device-independent-quantum-state-verification-and-certification/</guid><description>&lt;p>Authentication of quantum sources is a crucial task in building reliable and efficient protocols for quantum-information processing. Steady progress vis-à-vis verification of quantum devices in the scenario with fully characterized measurement devices has been observed in recent years. When it comes to the scenario with uncharacterized measurements, the so-called black-box scenario, practical verification methods are still rather scarce. Development of self-testing methods is an important step forward, but these results so far have been used for reliable verification only by considering the asymptotic behavior of large, identically and independently distributed (IID) samples of a quantum resource. Such strong assumptions deprive the verification procedure of its truly device-independent character. In this paper, we develop a systematic approach to device-independent verification of quantum states free of IID assumptions in the finite copy regime. Remarkably, we show that device-independent verification can be performed with optimal sample efficiency. Finally, for the case of independent copies, we develop a device-independent protocol for quantum state certification: a protocol in which a fragment of the resource copies is measured to warrant the rest of the copies to be close to some target state.&lt;/p></description></item><item><title>Network Quantum Steering</title><link>https://qi.lip6.fr/fr/publication/3433051-network-quantum-steering/</link><pubDate>Fri, 22 Oct 2021 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/3433051-network-quantum-steering/</guid><description>&lt;p>The development of large-scale quantum networks promises to bring a multitude of technological applications as well as shed light on foundational topics, such as quantum nonlocality. It is particularly interesting to consider scenarios where sources within the network are statistically independent, which leads to so-called network nonlocality, even when parties perform fixed measurements. Here we promote certain parties to be trusted and introduce the notion of network steering and network local hidden state (NLHS) models within this paradigm of independent sources. In one direction, we show how results from Bell nonlocality and quantum steering can be used to demonstrate network steering. We further show that it is a genuinely novel effect, by exhibiting unsteerable states that nevertheless demonstrate network steering, based upon entanglement swapping, yielding a form of activation. On the other hand, we provide no-go results for network steering in a large class of scenarios, by explicitly constructing NLHS models.&lt;/p></description></item><item><title>Device-Independent Quantification of Quantum Resources</title><link>https://qi.lip6.fr/fr/publication/3588309-device-independent-quantification-of-quantum-resources/</link><pubDate>Tue, 07 Sep 2021 00:00:00 +0000</pubDate><guid>https://qi.lip6.fr/fr/publication/3588309-device-independent-quantification-of-quantum-resources/</guid><description/></item></channel></rss>