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quantumcomputing/32894_c65187f488c01dde_969.txt | 3D convolution neural networks (CNNs) have been the prevailing option for video recognition. To capture the temporal information, 3D convolutions are computed along the sequences, leading to cubically growing and expensive computations. To reduce the computational cost, previous methods resort to manually designed 3D/2... |
quantumcomputing/a4c56a91_114846.txt | - LangExtract Milvus: A Practical Guide to Building a Hybrid Document Processing and Search System - Hands-on RAG with Qwen3 Embedding and Reranking Models using Milvus - MinHash LSH in Milvus: The Secret Weapon for Fighting Duplicates in LLM Training Data - Generating More Creative and Curated Ghibli-Style Images wi... |
quantumcomputing/20489876_12558.txt | This paper studies the strongly-convex-strongly-concave minimax optimization with unbalanced dimensionality. Such problems contain several popular applications in data science such as few shot learning and fairness-aware machine learning task. The design of conventional iterative algorithm for minimax optimization typi... |
quantumcomputing/6b1fd01c_7574.txt | We thank National Research Foundation of Korea (Project Number RS-2024-00337004) for the financial support. |
quantumcomputing/a7b1fa7f_1141.txt | M. Grajcar, et al. We present the first experimental results on a device with more than two superconducting qubits. The circuit consists of four three-junction flux qubits, with simultaneous ferro- and antiferromagnetic coupling implemented using shared Josephson junctions. Its response, which is dominated by the groun... |
quantumcomputing/650d45a6_123778.txt | A single qubit's state can be visualized as a point on the Bloch sphere, and single-qubit gates correspond to rotations of this Bloch vector. These gates change the amplitudes and relative phase of the basis states 0 rangle and 1 rangle . In matrix form, a single-qubit gate is a 2 2 unitary matrix. Here are th... |
quantumcomputing/1629_62d962bdf1d2852a_105.txt | A state, understood as a catalogue of probabilities, can be measured by producing many identical copies of the system at hand and performing measurements on these copies. I describe the pertinent experimental procedure, which also works in the presence of knowledge constraints. I show how the state estimate changes, an... |
quantumcomputing/9c71cab5_4370.txt | Quantum computing is a beautiful fusion of quantum physics with computer science. It incorporates some of the most stunn 16,735 2,444 10MB Read more |
quantumcomputing/9772f8c1_14206.txt | Add this session to my calendar Date: Thursday, 17 March 2022Time: 16:40 CET - 17:20 CET Session chair:Andy Pimentel, University of Amsterdam, NL Session co-chair:Matthias Jung, Fraunhofer IESE, DE This session highlights the importance of system modeling for an efficient design. The first three papers showcase solutio... |
quantumcomputing/22108_db9c0f2f4b6f960d_1671.txt | In this paper it is proved the existence of a prime number in the interval between the square of any natural number greater than one, and the number resulting from adding or subtracting this natural number to its square (Oppermann’s Conjecture). As corollaries of this proof, they are proved three classical prime number... |
quantumcomputing/2132f85c_125501.txt | But while it would be marvelous, it is not possible. You can see the trouble if you think closely about the protocol. Remember, for Bob to recover the state ψ psi rangle ψ , Alice must send Bob two bits of classical information. The speed of that transmission is limited by the speed of light. Without that cla... |
quantumcomputing/20712_73a38e5351f0bd0f_42.txt | Already in 1948 Kety and Schmidt1 had demonstrated that hypoxemia increases CBF in healthy adults, and many more studies on this followed, mainly motivated by aviation medicine. It was not until 1991, however, that the effects of hypoxia was studied systematically in newborn infants.2 Unfortunately, the technique used ... |
quantumcomputing/17894_d2459b6037275255_20.txt | We next explore scaling to larger systems and circuit depths. To ensure high complexity of our logical circuits, we use nonlocal connections to entangle the logical triplets on up to 4D hypercube graphs (Extended Data Fig. 6 and Supplementary Video 3), which results in fast scrambling19."). Exploring entangled systems ... |
quantumcomputing/14816_a8fc7655fde86ec1_37.txt | Robert, I see no reason whatsoever why a QC should be considered as *a priori* implausible as a 747 being assembled in a scrap-heap. While your previous comments revealed nothing but contempt for complexity theory, this really is largely a complexity issue: if, for example, QCs would solve NP-complete problems or the h... |
quantumcomputing/5a308f94_8860.txt | The resources required for quantum teleportation are a communication channel capable of transmitting two classical bits, a means of generating an entangled Bell state of qubits and distributing to two different locations, performing a Bell measurement on one of the Bell state qubits, and manipulating the quantum state ... |
quantumcomputing/22087_cfa6e6481b8cd2bd_91.txt | Isotropic positive definite functions are used in approximation theory and are for example applied in geostatistics and physiology. They are also of importance in statistics where they occur as correlation functions of homogeneous random fields on spheres. We study a class of function applicable for interpolation of ar... |
quantumcomputing/e684d52a_3739.txt | Anyone you share the following link with will be able to read this content: Sorry, a shareable link is not currently available for this article. Provided by the Springer Nature SharedIt content-sharing initiative |
quantumcomputing/14994_cdd61dafb85483f2_225.txt | A 160-bit elliptic curve cryptographic key could be broken on a quantum computer using around 1000 logical qubits while factoring the security-wise equivalent 1024-bit RSA modulus would require 2000 logical qubits. And to implement Shor’s algorithm for factoring a 2048 bit number we need more than 4000 logical qubits a... |
quantumcomputing/bfc6c691_120610.txt | displaystyle begin aligned S _ x rightarrow U dagger S _ x U amp; e i theta S _ z S _ x e -i theta S _ z amp; S _ x (i theta ) left S _ z ,S _ x right left( frac 1 2! right)(i theta ) 2 left S _ z , left S _ z ,S _ x right right left( frac 1 3! right)(i theta ) 3 left S _ z , left S _... |
quantumcomputing/22087_69ca229ec5299de3_1981.txt | Whitney proved in 1931 that 4-connected planar triangulations are Hamiltonian. Hakimi, Schmeichel, and Thomassen conjectured in 1979 that if $G$ is a 4-connected planar triangulation with $n$ vertices, then $G$ contains at least $2(n-2)(n-4)$ Hamiltonian cycles, with equality if and only if $G$ is a double wheel. On th... |
quantumcomputing/22108_808db5389f8f8e1e_77.txt | 8.2 Changing Basis States ALICE: Before we get too far off in the QIS direction, let’s tackle the fundamental issue of representing quantum states using different sets of basis vectors. In fact, a superposition state in one basis set will be a single basis state in some other appropriately chosen basis set. More import... |
quantumcomputing/25808_c03c7c8e205e1c7f_29.txt | | Session 8B: Memory: Address Translation and Tiering (Location: Grande D/E) | | --- | | 10:00 PDT â 10:15 PDT **METAL: Caching Multi-level Indexes in Domain-Specific Architectures** Anagha Molakalmur Anil Kumar and Aditya Prasanna (Simon Fraser University);Jonathan Balkind (University of California Santa Barbara);A... |
quantumcomputing/17894_a8a638dc956ff973_159.txt | | | | | | --- | --- | --- | | image file: d2cs00203e-f26.tif | | | | | **Fig. 26** Decision tree using extracted rules and design guidelines. The decision tree is generated using the reactant-to-barrier (R2B) method estimated activation barriers to predict changes in barrier heights by starting at all reactions (f... |
quantumcomputing/b48508de_12659.txt | To ensure we keep this website safe, please can you confirm you are a human by ticking the box below. If you are unable to complete the above request please contact us using the below link, providing a screenshot of your experience. https://ioppublishing.org/contacts/ |
quantumcomputing/4628_98bc330e6ca89479_656.txt | Although the theoretical ideas behind the threshold theorem can be adapted in a variety of different ways, depending upon the noise prevalent in a specific implementation of quantum computation, a skeptic might still claim that all such noise models for which a threshold may be proved are overly restrictive, and will n... |
quantumcomputing/4625_578753610752009e_191.txt | 8.3 Distinguishing mixed states In Sections 4.1 and 4.2 we proved two fundamental results about how well we can distinguish between quantum states. These theorems were proven for pure states described by state vectors; now we need to adapt them to mixed states described by density operators. First, consider a situation... |
quantumcomputing/32894_c244c61d974ad5a8_204.txt | Abstract- That is why NebulaCloud is the new state of the art within cloud computing performance, utility and new frontiers in AI- centric workflows. optimized for AI-enabled cloud services, and scalable, intelligent, and elastic for the cloud. As the world becomes more and more AI-driven, NebulaCloud is identifying as... |
quantumcomputing/10115_34b0ba78ddd01800_180.txt | These relations generalise the corresponding expressions in the context of the Born rule, Eqs. (3.45) and (3.48), respectively. If we write \(\hat {O}\_k = E\_{k}^\dagger E\_{k}\) then Eqs. (3.158) and (3.159) describe a generalised measurement, or POVM, as introduced in Eq. (3.51). As we noted already in Sect. 3.3.2.2... |
quantumcomputing/d40e414c_8225.txt | Fraunhofer Institut für Kurzzeitdynamik, Ernst-Mach-Institut, EMI, Ernst-Zermelo-Str. 4, 79104, Freiburg, GermanyChristoph Brockt-Haßauer, Aishvarya Kumar Jain, Corinna Köpke, Alexander Stolz & Mirjam Fehling-Kaschek Fraunhofer Institut für Kurzzeitdynamik, Ernst-Mach-Institut, EMI, Ernst-Zermelo-Str. 4, 79104, Freibur... |
quantumcomputing/9339_a38937c5090409ef_622.txt | ˜ be the We aim to bound p(c)q(d) = |c|ψψ|d|2 from above. To do this, let |ψ ˜ has norm λ less than projection of |ψ into the plane spanned by |c and |d, so |ψ or equal to one. If θ is the angle |d makes with |c in this plane, and ϕ is the angle 2 ˜ makes with |d, then we see p(c)q(d) = |c|ψ ˜ ψ|d| ˜ |ψ... |
quantumcomputing/44c1bd0c_0939.txt | As famously noted by Richard P. Feynman in his Lectures on Computation (Feynman, Hey, and Allen 1998), accurately modeling quantum systems on classical computers is a fundamentally expensive task because the number of states a quantum system can potentially occupy grows exponentially with the size of a system. While no... |
quantumcomputing/6436_723fd0fbfe5d7a11_379.txt | ``` @article{wang2021representing, author = {Wang, Quanlong}, title = {{Representing Matrices Using Algebraic ZX-calculus}}, year = {2021}, journal = {arXiv preprint arXiv:2110.06898}, urldate = {2021-10-13}, link = {http://arxiv.org/abs/2110.06898}, keywords = {Algebraic ZX, Normal-Form}, abstract = {Elementary matric... |
quantumcomputing/14994_ba709dfaf74feae6_145.txt | 166 References [83] Schneier B. Applied cryptography: protocols, algorithms, source code in the C language. Williams Publishing House, 2016– 816 p. [84] Ebbinhaus G.D. Turing machines and recursive functions/ G.D. Ebbinhaus. M.: Mir, 1972– 264 p. [85] Shor P. Algorithms for quantum computation: discrete logarithms and ... |
quantumcomputing/24212_8f631342375c1193_44.txt | Molecular dynamics simulations are used to investigate driven nano-scale flows of liquids along open "chemical channels": patterns of completely-wetting solid embedded in a planar substrate, and sandwiched between less wetting solid regions. Liquid placed atop a long straight wetting stripe evolves into connected "pear... |
quantumcomputing/8652_a8fc7655fde86ec1_35.txt | As others have suggested in their comments, the key is that noise acting collectively on many qubits simultaneously should be adequately suppressed. I consider a Hamiltonian coupling the system to the bath, which includes terms acting collectively on many system qubits. Loosely speaking, the sufficient condition is tha... |
quantumcomputing/1ba8185c_114137.txt | ψ ψ ( cos 2 ( θ 2 ) e i ϕ cos ( θ 2 ) sin ( θ 2 ) e i ϕ cos ( θ 2 ) sin ( θ 2 ) sin 2 ( θ 2 ) ) vert psi rangle langle psi vert |
quantumcomputing/ea31bc1f_0357.txt | Right from the very start, there have been skeptics that challenged the possibility of a quantum computer superseding the power of a classical Turing machine. Most of these arguments are founded on beliefs that such quantum computation devices would be exponentially hard and complex to control [20,21,22,23,24]. The eff... |
quantumcomputing/14816_a8fc7655fde86ec1_34.txt | 4) The fact that the systems are far from equilibrium does not help, the laws of thermodynamics must be obeyed, in particular entropy production must be positive . Probability of deviations from this principle decreases exponentially with the size of a system x time (“fluctuation theorems”) and hence also does not help... |
quantumcomputing/32894_fc39bbe803b856a5_815.txt | In the last years, we have seen an increase in the number of Artificial Intelligence (AI)-powered applications for information retrieval and data science. This fact led to an increasing reliance on distributed computing infrastructures, including Cloud, Edge, and IoT environments. These architectures enable powerful an... |
quantumcomputing/4ecbb7f6_124397.txt | Let a b be a best approximation of the first kind of x a 0 ; a 1 , , a N . Then a b is a convergent or a semiconvergent of x. |
quantumcomputing/9684_67376b44df69bab4_131.txt | + `QueuingContext` is renamed to `QueuingManager`. + `QueuingManager` should now be the global communication point for putting queuable objects into the active queue. + `QueuingManager` is no longer an abstract base class. + `AnnotatedQueue` and its children no longer inherit from `QueuingManager`. + `QueuingManager` i... |
quantumcomputing/6436_184d3f0af3fe5585_93.txt | uantum computing is the result of the fusion of early and classical computing (Chapter 2) and quantum mechanics (Chapter 3), aided by the use of the technologies developed as part of Quantum Technology 1.0 (Chapter 4). All of us alive today are living in the time of Quantum Technology 2.0. In this continuing revolution... |
quantumcomputing/4625_0e6b2f1bdcb98045_9.txt | The above analysis relies on Gaussian heuristic which is not guaranteed to work beneficially on every instance. To verify the validity of the approach, numerical tests are carried out summarized in Figure 2. Each subfigure shows the success rate of the lattice reduction method for chosen modulus *q*from Kyber22.")and D... |
quantumcomputing/20712_189d5b93841f4e0f_36.txt | Valeria R. Mas, MSc, PhD, Joseph and Corinne Schwartz, Professor of Surgical Sciences Research in Transplantation, Professor of Microbiology and Immunology, Chief, Surgical Sciences Division, Department of Surgery at University of Maryland. Dr Valeria Mas is a cellular and molecular transplant immunologist with experti... |
quantumcomputing/175_40094682244c3a83_1727.txt | To promote better performance-bandwidth trade-off for multi-agent perception, we propose a novel distilled collaboration graph (DiscoGraph) to model trainable, pose-aware, and adaptive collaboration among agents. Our key novelties lie in two aspects. First, we propose a teacher-student framework to train DiscoGraph via... |
quantumcomputing/6245_3db5b12f9b04f652_16.txt | A successful Bell-state measurement (BSM) relies on the indistinguishability of the two photons, which are generated by independent sources and have been distributed through a 22-km-long fiber channel for each. To do that, the spatial indistinguishability is ensured by using single-mode optical fibers. The spectral ind... |
quantumcomputing/15325_f9f57e706a901d24_33.txt | Hyperplanes and parity. Finally, we devise a data generation procedure that fixes several hyperplanes in a k𝑘kitalic\_k-dimensional space and labels randomly sampled points consulting the parity of perceptron classifiers that have these hyperplanes as decision boundaries. In other words, a label tells us whether a poi... |
quantumcomputing/27984_6acf32c49a1bbe4c_75.txt | 1. Note that, if *A* is not Hermitian, the problem can be restated as \({\bar{A}}{\bar{\mathbf{x}}}={\bar{\mathbf{b}}}\) with a Hermitian matrix \({\bar{A}}:=\bigl ({\begin{matrix} 0&{}A\\ A^\dagger &{}0 \end{matrix}} \bigr )\), see Sect. 3. 2. The aspect of PLATO most ly aligned with the topic of this paper was the un... |
quantumcomputing/1dfcc7ef_8832.txt | A CNOT("controlled NOT" or CX) gate is a two-qubit gate, meaning its action involves two qubits at once: the control qubit and the target qubit. A CNOT flips the target qubit only when the control qubit is ∣1⟩|1\rangle∣1⟩. Let us first simulate the action of this two-qubit gate when q0 and q1 are both ∣0⟩|0\rangle∣0⟩, ... |
quantumcomputing/9789_9b2d0cdee3ab6fa0_4.txt | * In 2016 for the first time the lifetime of a quantum bit was prolonged by employing a QEC code.[35] + The error-correction demonstration was performed on Schrödinger-cat states encoded in a superconducting resonator, and employed a quantum controller") capable of performing real-time feedback operations including rea... |
quantumcomputing/9073_303b46c6a5f64744_338.txt | different life cycles of all the partner systems. Synchronized deployments are impossible; implementation and update frequencies are measured in months and years and not in weeks. Thus, appropriate API evolution was one challenge. The technical integration also was made more complex by a rather generic Land Register AP... |
quantumcomputing/48cbd811_12610.txt | Dongkuan (DK) Xu · Subhabrata Mukherjee · Xiaodong Liu · Debadeepta Dey · Wenhui Wang · Xiang Zhang · Ahmed Awadallah · Jianfeng Gao Traditional knowledge distillation (KD) methods manually design student architectures to compress large models given pre-specified computational cost. This requires several trials to find... |
quantumcomputing/34011_a5801def072ec91c_2502.txt | For Spinoza, therefore, the will is not free and is the same as the intellect. He is aware that this is a strange teaching, explicitly pointing out that most people do not recognize its truth. The reason for this failure to recognize the doctrine that the will is not free can, however, be understood both as an epistemi... |
quantumcomputing/22087_8e0cf300de8195aa_45.txt | The negation of AOE is an instance of Restriction A: the prediction of the violation of a Local Friendliness inequality, as demonstrated in [7], proves that Restriction A applies to quantum theory, if supplemented by the assumptions of Locality 111Note that the Locality assumption of [7] is an assumption only about var... |
quantumcomputing/22087_db9c0f2f4b6f960d_233.txt | Superconductivity in most metals is due to the activity of longitudinal spin waves binding electrons into pairs in such a way that the Meissner effect is generated along with the angular momentum responses in static magnetic fields. The bulk of these spin waves appear to be sourced by nuclear spins on the lattice. Expe... |
quantumcomputing/4625_ebeb95a89c78f21f_95.txt | 10.6 Shor’s Algorithm This is perhaps the most important quantum algorithm we will study in this chapter. Some sources say it is also the most complicated. That is why some texts deal with it last. However, once you have become comfortable with the previous three algorithms, you should be able to move forward with Sho... |
quantumcomputing/20712_2ed2d1df17fe28a3_111.txt | Seriously, though, I told you we weren’t going to agree, but FWIW, I’m well-aware of the fact that the “beables” (my phone keeps recommending “Beatles”) are the only observable thing in BM. The trouble, as you know as well as I, is that *either* a beable value is tied up with something decohered, macroscopic, and class... |
quantumcomputing/6436_723fd0fbfe5d7a11_28.txt | To enable practically useful quantum computing, we require hundreds to thousands of logical qubits (collections of physical qubits with error correction). Current monolithic device architectures have scaling limits beyond few tens of logical qubits. To scale up, we require architectures that orchestrate several monolit... |
quantumcomputing/26329_cdd61dafb85483f2_284.txt | Central to all these applications is the ability of a quantum internet to transmit quantum bits (qubits) that are fundamentally different than classical bits. Whereas classical bits can take only two values, 0 or 1, qubits can be in a superposition of being 0 and 1 at the same time. Moreover, qubits can be entangled wi... |
quantumcomputing/26329_cdd61dafb85483f2_147.txt | When trying to predict the future progress of quantum computers, the qubit count is often used as the primary indicator. This is misleading as there are other parameters that can inhibit the progress of quantum computers, even when the qubit count continues to increase. One of the biggest challenges is the need to perf... |
quantumcomputing/1629_3abeac199875c936_844.txt | The Mechanical View It may be noted that, according to the traditional view stemming from CM, the situation should be quite the opposite. In the nineteenth century, even in the case of more developed organisms, it was believed that perception and broadcasting of the information to the animal’s brain were mechanically p... |
quantumcomputing/14994_bb89c4acbf2bb616_335.txt | monarch butterfly optimization,3 ant colony algorithm,4 and others.5 These algorithms can search for quasi-optimistic solutions by balancing the global goal of a group with internal perturbations. The second direction is the development of biological computing, in which computing is implemented by living biological and/... |
quantumcomputing/1629_3abeac199875c936_80.txt | Therefore, we can start with the highest eigenstate |l, l of Lˆ z and apply recursively the lowering operator lˆ− on it in order to obtain the other eigenstates |l, l − 1 , |l, l − 2 , . . . of Lˆ z , where the process has to stop after finite steps because lˆ− |l, −l = 0. Thus, it is possible to order the eigensta... |
quantumcomputing/9073_a8a638dc956ff973_250.txt | Since machine learning tasks are data-intensive efficient protocols for loading entries from a high-dimensional classical vector onto a quantum state without smarter preprocessing for feature extraction continues to be a significant challenge. The early domain of QML algorithms included HHL178 for PCA and clustering, r... |
quantumcomputing/4319b7f9_124020.txt | II.1 CNOT-ladders Figure 1: CNOT ladders and their implementation using dynamic circuits (for the derivation see Appendix A.1). An efficient way to implement CNOT-ladders using dynamic circuits is illustrated in Fig. 1. Implementing a CNOT ladder consisting of n𝑛nitalic_n CNOT gates in constant depth requires n𝑛nital... |
quantumcomputing/9073_303b46c6a5f64744_48.txt | In reality, this agreement can be highly asymmetrical because many APIs (especially public APIs) are offered as-is by the API provider. API clients can use it under those conditions or not at all; no negotiation or formal agreement on a contract between the participants takes place in such cases. This might be differen... |
quantumcomputing/22108_808db5389f8f8e1e_229.txt | ALICE: Let’s first look at the traditional Fourier analysis (sometimes called the Fourier transform) method and how it allows us to find the period of a “signal.” We plot a pure cosine function and another more complex periodic function with a period different from the pure cosine (Figure 13.4). You can see that becaus... |
quantumcomputing/2565_a8a638dc956ff973_163.txt | | | | | | --- | --- | --- | | image file: d2cs00203e-f28.tif | | | | | **Fig. 28** Classification of the metallic and insulating states of VO2 based on the quantum clustering algorithm. (a) Demonstrates the original data used for classification. All training instances are 2-d vectors (pressure and temperature), wh... |
quantumcomputing/9904_7ae05d4adf606362_208.txt | ∂U = ∅. Since Λ is normal, there is an open neighborhood NV of supp(f∗ V ) such that NV ∩ ∂U = ∅. Unravelling the definitions one finds V ∈ B(f −1 (U ), L) ∩ B(f −1 (NV ), {idH }) ⊂ f∗−1 (B(U, L)) so that f∗−1 (B(U, L)) is a neighborhood of V . Thus f∗−1 (B(U, L)) is open. The additional properties that we required in t... |
quantumcomputing/11875_543aaf591dd6eb2d_337.txt | 2 Swift Double-Tail Dynamic (DTD) Comparator The application of comparator is most commonly found in real-time applications which require low voltage. Hence, the design of proposed comparator is done using double-tail module. The proposed comparator’s significant notion is to advance the limitation V fn/fp to advance ... |
quantumcomputing/20712_189d5b93841f4e0f_47.txt | Join us for a unique evening at Wolfson College as we delve into the fascinating world of neuroethics. This lecture brings together experts in neuroscience and ethics to explore the ethical implications of advances in brain research. Don't miss this opportunity to expand your understanding of the intersection between t... |
quantumcomputing/939c8e27_9494.txt | Existing classical ciphertext retrieval schemes are mainly developed according to the homomorphic encryption that is a cryptographic technique based on computational complexity theory of mathematical puzzles. In quantum computing, on the one hand, most of traditional asymmetric encryption can be quickly cracked as the ... |
quantumcomputing/175_2133873ef2897b08_32.txt | Parameters: : * **loss** (*callable*) – Loss as a function of variational parameters to be optimized. * **initial\_parameters** (*np.ndarray*) – Initial guess for the variational parameters. * **args** (*tuple*")) – optional arguments for the loss function. * **method** (*str*")) – Name of method supported by `scipy.... |
quantumcomputing/27984_889bcb3d28cecf3a_392.txt | The operation of a quantum computer is considered as a general quantum operation on a mixed state on many qubits followed by a measurement. The general quantum operation is further represented as a Feynman-Vernon double path integral over the histories of the qubits and of an environment, and afterward tracing out the ... |
quantumcomputing/21aa6608_115953.txt | The expression of the degree of polarization of the output SOP, p o , can be obtained either from Equation (17) or from Equation (34). The computational advantage of Equation (34) is striking. It is straightforward to calculate p o as the square root of the sum of the square of the components of p o n o along the two o... |
quantumcomputing/27984_723fd0fbfe5d7a11_148.txt | ``` @article{nagayoshi2024zx, author = {Nagayoshi, Hironari and Asavanant, Warit and Ide, Ryuhoh and Fukui, Kosuke and Sakaguchi, Atsushi and Yoshikawa, Jun-ichi and C. Menicucci, Nicolas and Furusawa, Akira}, title = {{ZX graphical calculus for continuous-variable quantum processes}}, year = {2024}, journal = {Physica... |
quantumcomputing/16776_afb95353be58d856_40.txt | The use of qubits to perform frequency measurements of classical fields arises naturally in a variety of contexts, from operating atomic clocks to calibrating quantum processors. In this context, it has long been known that the generation of entanglement with ensembles of qubits can provide a metrological advantage ove... |
quantumcomputing/5ba90290_4834.txt | The process161,467 of applying supervised ML or QML to a typical classification problem with physico-chemical applications is demonstrated in Fig. 25. The first step is to collect the dataset from chemical experiments. Due to the very existence of errors in measurement and impurities in the reaction, in most cases the ... |
quantumcomputing/7531799d_12832.txt | The weather has a huge impact on our lives, affecting health, transport, agriculture (see also §3.8.10), energy use (see also §3.4), and leisure. Since Bjerknes (1904) introduced hydrodynamics and thermodynamics into meteorology, weather prediction has been based on merging physical principles and observational informa... |
quantumcomputing/16776_2ed71ddce2e7681a_114.txt | Google Scholar * Defferrard M, Bresson X, Vandergheynst P (2016) Convolutional neural networks on graphs with fast localized spectral filtering * Monti F, Bronstein MM, Bresson X (2017) Geometric matrix completion with recurrent multi-graph neural networks * Velikovi P, Cucurull G, Casanova A, Romero A, Lio P, Bengio Y... |
quantumcomputing/a2267180_7313.txt | Thank you very much to the authors allowing figures from their work to be reproduced in this post, acknowledged individually in figure captions. Thanks to Dan Browne for helpful feedback. |
quantumcomputing/22087_b59e8b731151dc36_17.txt | We have seen that no two properties analysed here are equivalent. However, at least for the Werner states and the Gisin states there are some implications between them. One may ask whether these implications are specific to these classes of states or they hold in general. It turns out that in some cases the answer is p... |
quantumcomputing/14816_16a55bc42dde3474_32.txt | @Scott — While we are on the topic, a separate but quite related question. Though it was under less fortunate circumstances, this time last year I had the chance to read (IMHO) Terry Rudolph’s excellent primer ‘Q is for Quantum’. As I am not \*formally\* a Quantum Computing student, I forget the \*exact\* principal cit... |
quantumcomputing/9339_98bc330e6ca89479_31.txt | The modern incarnation of computer science was announced by the great mathemati¬ cian Alan Turing in a remarkable 1936 paper. Turing developed in detail an abstract notion of what we would now call a programmable computer, a model for computation now known as the Turing machine , in his honor. Turing showed that there ... |
quantumcomputing/44702_66cde76edf9656bf_0.txt | * Physically feasible, but lacking gravitas * If "bad" can be "badly" in adverbial form, then why not "good" to "goodly"? * PSE Advent Calendar 2025 (Day 2): Decorating in the Midst of Purple Skies * "Save as webpage, HTML Only" Fail while offiline, Firefox * How do Buddhists interpret the Buddha’s explanation of earth... |
quantumcomputing/dad5dd8b_6297.txt | There is no constant stabiliser group when viewing the X3Z3 Floquet code as a subsystem code (in a subsystem code, the stabiliser group is defined as the centre of the gauge group, which, in our case, is generated by all edge operators)13,18. Surprisingly, despite this fact, at every time step, there do exist operators... |
quantumcomputing/22087_d3b3bff6b46e90f8_456.txt | 2. Natural compounds used in heavy metals removal 2.1 Biosurfactant-based removal of heavy metals Biosurfactants are bioactive compounds derived from certain plants and microorganisms. They lower interfacial and surface tension forming micellar structures that enhance the bioavailability and mobility of heavy metals in... |
quantumcomputing/6e49c260_2847.txt | Valeriy19Valeriy19 Jan 16, 2018#712018-01-16T20:02+00:00 Good Elf797Good Elf797 Jan 17, 2018#722018-01-17T00:43+00:00 Jan 17, 2018#732018-01-17T16:29+00:00 Jan 18, 2018#742018-01-18T04:39+00:00 Apr 22, 2018#752018-04-22T15:47+00:00 Aug 07, 2018#762018-08-07T06:21+00:00 Oct 02, 2018#772018-10-02T04:55+00:00 Seewhat1,961... |
quantumcomputing/b6f8d5e9_9338.txt | As we just saw, one consequence of complementarity is base-level randomness, even under maximal information about a system: If an agent is justified in ascribing to a system an eigenstate of \(\hat {S}_z\), her prediction for a measurement of \(\hat {S}_x\) must be completely random, and this is borne out experimentall... |
quantumcomputing/18150_723fd0fbfe5d7a11_97.txt | In this thesis, I introduce new ZX-calculus rewrite rules and prove that these rules preserve the existence of Pauli flow. These rules have a variety of applications across many areas of quantum computation which will also be explored - to start, I show that these rules give us a procedure for rewriting any measurement... |
quantumcomputing/20712_4cc5a9fe2cd4e37a_164.txt | I'm glad someone has a similar mode of thought. Growing up, I had trouble reading people's expressions, so I had to rely on their words and actions. In my life, it's been the dishonest people who acted assured of their own righteousness, while honest people were willing to put themselves at a disadvantage by telling ug... |
quantumcomputing/6436_184d3f0af3fe5585_241.txt | As we are finishing this book, Chinese researchers have demonstrated a network 1,000km (roughly 600 miles) long for unhackable quantum communications — the longest such network yet — using photons in fiber-optic cables. Because quantum particles, such as coherent photons, can’t be copied or amplified, suppressing nois... |
quantumcomputing/25808_d15b917791bf267d_52.txt | To co-optimize the directives and floorplan of HLS designs on multi-die FPGAs, we propose the FADO framework, which formulates the directive-floorplan co-search problem based on the multi-choice multi-dimensional bin-packing and solves it using an iterative optimization flow. For each step of directive optimization, a ... |
quantumcomputing/29980_623ed82e56f30ead_21.txt | | | | --- | | foliationLines ✕ ``` foliationLines[{lineDensityHorizontal_ : 1, lineDensityVertical_ : 1}, {tanHorizontal_ : 0.0, tanVertical_ : 0.0}, offset : {_, _} : {0, 0}, lineStyles : {_, _} : {Red, Red}, transform_ : (# &)] := {If[lineDensityHorizontal != 0, Style[Table[ Line... |
quantumcomputing/13334_db9c0f2f4b6f960d_2347.txt | The chiral potential is inverse square. The family of inverse square potentials includes the vector Lorentz potential of the quantum Hall and Aharonov-Bohm effects, and the centrifugal, Coriolis, and three body potentials. The associated impedances are scale invariant, quantum Hall being the most familiar. Modes associ... |
quantumcomputing/1226_4503ad1eb65e514b_87.txt | where \(F\_{\mu \nu }\) and \(X\_{\mu \nu }\) denote the QED and \(U(1)\_{X}\) field strength tensors, respectively. The mixing parameter \(\epsilon \_A\) is in principle a free parameter of the theory since the above mixing term is a gauge-invariant, renormalisable operator. In many hidden photon models, however, \(\e... |
quantumcomputing/22087_69ca229ec5299de3_1476.txt | The Gabor system of a function is the set of all of its integer translations and modulations. The Balian-Low Theorem states that the Gabor system of a function which is well localized in both time and frequency cannot form an Riesz basis for $L^2(\mathbb{R})$. An important tool in the proof is a characterization of the... |
quantumcomputing/32894_1a8f0330de3b41ea_401.txt | Gaussian splatting techniques have recently revolutionized outdoor scene decomposition and relighting through multi-view images. However, achieving high rendering quality still requires a fixed lighting condition among all input views, which is costly or even impractical to capture in outdoor scenes. In this paper, we ... |
quantumcomputing/27927_67376b44df69bab4_123.txt | ``` >>> qml.adjoint(qml.PauliX(0)) ``` * The `Operation.inverse` property has been removed completely. (#3725) * The target wires of `qml.ControlledQubitUnitary` are no longer available via `op.hyperparameters["u_wires"]`. Instead, they can be accesses via `op.base.wires` or `op.target_wires`. (#3450) * The tape constr... |
quantumcomputing/13bc6fa0_0556.txt | This work was supported by Institute for Information & Communications Technology Planning & Evaluation (IITP) grant funded by the Korea government(Ministry of Science and ICT(MSIT)) (\(\langle\)Q\(\vert\)Crypton\(\rangle\), No.2019-0-00033, Study on Quantum Security Evaluation of Cryptography based on Computational Qua... |
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