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quantumcomputing/22108_db9c0f2f4b6f960d_2567.txt | Potential time trends in relative humidity (RH) were investigated for the Kamloops climate station in south-central British Columbia, Canada, between 1990 and 2012. Mean monthly 6 am and 3 pm RH at Kamloops achieve annual minima during the March to September period with substantially higher early morning RH compared to... |
quantumcomputing/14816_889bcb3d28cecf3a_159.txt | By employing displacement operations, single-photon subtractions, and weak cross-Kerr nonlinearity, we propose an alternative way of implementing several universal quantum logical gates for all-optical hybrid qubits encoded in both single-photon polarization state and coherent state. Since these schemes can be straight... |
quantumcomputing/44116_42627d408d9e484f_134.txt | environments have been identified in limit of an algae (the extinction the Gulf of Maine: rocky ledge, sandy depth) correspond to the lowest depth nearshore ramp, and basin. Rocky at which net photosynthesis can be ledges are swept clear of se... |
quantumcomputing/22087_db9c0f2f4b6f960d_2240.txt | The fluid equations, named after Claude-Louis Navier and George Gabriel Stokes, describe the motion of fluid substances. These equations arise from applying Newton's second law to fluid motion, together with the assumption that the stress in the fluid is the sum of a diffusing viscous term (proportional to the gradient... |
quantumcomputing/a575d92c_14614.txt | snapshots() can now be used with mcm_method="one-shot" and mcm_method="tree-traversal". (#8140) This improvement is particularly useful for extracting the state in finite-shot workflows: @qml.qnode(qml.device("default.qubit"), mcm_method="one-shot", shots=1) def circuit(): qml.RY(1.23, 0) m0 = qml.measure(0) qml.cond(m... |
quantumcomputing/32894_74845111e5423cd6_178.txt | The MPPT technique is most commonly used to maximize energy from solar panels charging a battery. It can also be applied to thermophotovoltaics, optical power transmission, wind turbines, and other sources of harvested energy. The efficiency of power transfer depends on the appropriate matching of the source's output v... |
quantumcomputing/1226_3fc4c296cc68989d_159.txt | MBE is more suited to grow 2–6 inch wafers rather than 30-inch ones.7 MBE graphene may find industrial applications in markets where highly specialised devices are required. Despite the conceptual simplicity, a great technological effort is required to produce systems that yield the desired quality in terms of material... |
quantumcomputing/4628_c2c01ebb412339b8_39.txt | This configuration is similar to the XOR gate, except that here the target qubit is always | 0⟩. The qubit to be copied, | a⟩, is the control qubit in register q[0]. The target qubit is clamped at | 0⟩. After the operation of the CNOT gate, the target qubit will also be | a⟩. To see that this arrangement works, let’s f... |
quantumcomputing/175_40094682244c3a83_355.txt | We introduce a framework that abstracts Reinforcement Learning (RL) as a sequence modeling problem. This allows us to draw upon the simplicity and scalability of the Transformer architecture, and associated advances in language modeling such as GPT-x and BERT. In particular, we present Decision Transformer, an architec... |
quantumcomputing/21985_b745cf4a986576b6_285.txt | Blood samples obtained from patients at a local hospital were intentionally spiked with known aliquots of *Escherichia coli, Staphylococcus aureus, Enterobacter cloacae*, and *Pseudomonas aeruginosa* to simulate blood infections. After deposition of these samples on inexpensive, disposable filter media, approximately 3... |
quantumcomputing/8337_9bb65989695b7ff4_235.txt | The experiment (fig 61) first prepares a pair of highly entangled photons with complementary polarization and then passes one into a double slit apparatus in which the photon to be measured is directed to one or other slit depending on its entangled twin's polarization. The measured photons are then passed through an a... |
quantumcomputing/17677_ecf384143be764f0_214.txt | calculated. Finally, security takes into account both rural and urban traffic rates because there are much fewer cars in rural places than there are in metropolitan ones. The simulation’s findings show that the suggested defensive mechanism achieves more security and dependability when compared to the VANET’s current d... |
quantumcomputing/14816_6b5eb0c4e42e043c_88.txt | Now, how many inputs are there of length n? Right: 2". And for each input, only a 2~ n fraction of random strings cause us to err. By the union bound (the most useful fact in all of theoretical computer science), this implies that at most a 2 n ~" 1 fraction of random strings can ever cause us to err on inputs of lengt... |
quantumcomputing/3960_1525ece966560489_38.txt | Unfortunately, there are no hard and fast definitions of “new-to-the-world” and “leading edge.” Moreover, for many products, firms incorporate many existing products and innovations, but also add some components and functions that are new. As a rough rule, ITIF defines “leading-edge innovation” as something a firm does... |
quantumcomputing/ab1fd96f_7252.txt | Finally, we must post-process our results to create outputs in the expected format, like values or graphs. As you can see, ∣00⟩|00\rangle∣00⟩ and ∣11⟩|11\rangle∣11⟩ are the most frequently observed. There are a few results other than the expected data, and they are due to noise and qubit decoherence. We will learn more... |
quantumcomputing/92202c66_117891.txt | You can already find quaternions hiding in regular, complex QM in the words of Wikipedia, The real linear span of I, iσ, iσ, iσ for σ a the Pauli matrices is isomorphic to the real algebra of quaternions ℍ. |
quantumcomputing/14816_5f2deb247b7d4485_229.txt | Hall who performed an experiment to test whether moving charge in conductors was deflected by static magnetic fields—a phenomenon known today as the Hall effect. Many of Rowland’s students went on to populate the first chairs of physics in university departments across the states, which is why Rowland is often called t... |
quantumcomputing/27984_723fd0fbfe5d7a11_427.txt | This thesis consists of two parts. The first part is about how quantum theory can be recovered from first principles, while the second part is about the application of diagrammatic reasoning, specifically the ZX-calculus, to practical problems in quantum computing. The main results of the first part include a reconstru... |
quantumcomputing/22108_db9c0f2f4b6f960d_1322.txt | Important polytope sequences, like the associahedra and permutohedra, contain one object in each dimension. The more particles labelling the leaves of a tree, the higher the dimension required to compute physical amplitudes, where we speak of an abstract categorical dimension. Yet for most purposes, we care only about ... |
quantumcomputing/13334_747474a2b9a780fd_96.txt | Figure 7-3. Example QFT input state This is state C from our previous example. Notice that if we look along the register from left to right, the relative phases of the 24 = 16 values go through two full anticlockwise rotations. Thus, we can think of the relative phases in our register as repre‐ senting a signal that re... |
quantumcomputing/1629_3abeac199875c936_553.txt | discussed in Sect. 2.1.2. We can quantify path predictability by the absolute value of the difference between the probabilities for the photon to be reflected and transmitted, that is, (5.32) Pˆ = T2 − R2 , where the absolute value is justified by the fact that we do not know a priori which one of the probabiliti... |
quantumcomputing/22087_db9c0f2f4b6f960d_2935.txt | In this work the authors apply concepts of Neutrosophic Logic to the General Theory of Relativity to obtain a generalisation of Einstein's fourdimensional pseudo-Riemannian differentiable manifold in terms of Smarandache Geometry (Smarandache manifolds), by which new classes of relativistic particles and non-quantum te... |
quantumcomputing/20712_73a38e5351f0bd0f_264.txt | I assume that the construct of *birth asphyxia* includes a critical reduction in fetomaternal gas exchange during labor and delivery which may lead to death, morbidity in the fetus/neonate and impaired neurodevelopmental outcome in infancy and childhood. However, I do not assume that birth asphyxia is either a necessar... |
quantumcomputing/22108_db9c0f2f4b6f960d_1385.txt | Mass spectrometry measures atomic masses giving precision of 10^{-10}, but its accuracy has not been verified - precision and accuracy are two independent aspects. The Lorentz force law underlying mass spectrometry has not been verified. In the 1920's, the atomic masses of some elements measured through the early mass ... |
quantumcomputing/11871_f5b0288e0ea8c1ae_19.txt | This purify-and-teleport architecture is not the only known approach; quantum error correction (QEC) can replace purification. Managed properly, QEC protects the data more completely, reducing the need for multi-hop purification and its associated need for round-trip delays. These advantages come at the expense of substa... |
quantumcomputing/aff7cc78_114257.txt | The Poincaré axis of the light SOP is conserved after passing through the diattenuator. If the Poincaré vector of the diattenuator is antiparallel with that of the incident SOP ( |
quantumcomputing/16341_d2459b6037275255_3.txt | **a**, Schematic of the logical processor, split into three zones: storage, entangling and readout (see Extended Data Fig. 1 for detailed layout). Logical single-qubit and two-qubit operations are realized transversally with efficient, parallel operations. Transversal CNOTs are realized by interlacing two logical qubit... |
quantumcomputing/29980_368043e4f61caf5c_7.txt | Quantum computing’s unparalleled data processing capabilities could significantly enhance influence operations and information warfare, which are central to modern irregular warfare and gray zone conflict. Quantum computing can analyze vast amounts of social media and information network data, identifying patterns, tre... |
quantumcomputing/13334_db9c0f2f4b6f960d_33.txt | A continuation of the Born Reciprocal Relativity Theory (BRRT) program in phase space shows that a natural temperature-dependence of mass occurs after recurring to the Fulling-Davies-Unruh effect. The temperature dependence of the mass $ m ( T ) $ resemblances the energy-scale dependence of mass and other physical para... |
quantumcomputing/af1d30a7_1839.txt | New Orleans Saints Ticket Office: (504) 731-1700 Monday-Friday: 8 a.m.-6 p.m. Saturday: 8:30 a.m.-1 p.m. (Only open on Saturdays before home game on Sunday) |
quantumcomputing/888b2212_8667.txt | PhysicistDave2:28 AM, September 27, 2019Sabine,I don't disagree with your criticisms, but it does seem to me that you have more or less reiterated the probability-measure problem and, perhaps, the preferred-basis problem.In concrete terms, how does MWI lead to the Born rule?I think you have mentioned on some other occa... |
quantumcomputing/14994_cdd61dafb85483f2_107.txt | The class of problems that quantum computers can solve efficiently is called BQP and not NP-complete problem. Having said that, it is important to note that quantum computers may (and do) provide polynomial or constant speed-up in many problems outside BQP (for example, quadratic search speed-up), including such speed-... |
quantumcomputing/f57197a8_123749.txt | (The 0 k lt; 2 n 3 0 leq k lt;2 n-3 part is will be decided following to the decision of β n ; i beta _ n;i for i 3 2 n 2 , , 2 n i 3 cdot 2 n-2 , cdots,2 n .) |
quantumcomputing/dc4d94a4_123725.txt | The central idea is to reduce generalized controlled-gate synthesis to a one-shot search over ℂ ℂ ( U ) mathbb CC (U) SU(2) residual cleanup. The family ℂ ℂ ( U ) mathbb CC (U) forms a structured subgroup inside SU(4) (and more generally SU( 2 n 2 n )). Restricting the search to this subgroup provides (i) an ef... |
quantumcomputing/c419e07f_115354.txt | 1 Jarrod R McClean, Sergio Boixo, Vadim N Smelyanskiy, Ryan Babbush, and Hartmut Neven. Barren plateaus in quantum neural network training landscapes. Nature communications, 9(1):4812, 2018. https: doi.org 10.1038 s41467-018-07090-4. https: doi.org 10.1038 s41467-018-07090-4 |
quantumcomputing/2270_2ed2d1df17fe28a3_203.txt | So God moved on universes with more elaborate laws, laws just complex enough to allow the spontaneous and regular emergence of sentience. These laws turned out to be much like what you and I know as classical mechanics, or variations thereof. But the inhabitants of such universes quickly reached a point where they had ... |
quantumcomputing/22108_db9c0f2f4b6f960d_80.txt | Starting from first principles, we point out an apparent contradiction in the behavior of light in the metric space of a stationary frame in gravity. We show that the issue is resolved provided an independent moving ’dual space’ exists along side the metric space of general relativity (GR). In this dual space clocks ru... |
quantumcomputing/6245_808db5389f8f8e1e_24.txt | ALICE: Anticipating the terminology used in quantum computing, we might call these classical states Cbits (C for classical). Cbit is pronounced see-bit. The 0s and 1s are called classical bits, or just bits; most people use the latter term. CARDY: But what happens if there are more than two possible states? I would lov... |
quantumcomputing/13334_db9c0f2f4b6f960d_151.txt | This article proposes the modified KNN (K Nearest Neighbor) algorithm which considers the feature similarity and is applied to the keyword extraction. The texts which are given as features for encoding words into numerical vectors are semantic related entities, rather than independent ones, and the keyword extraction i... |
quantumcomputing/f17962c6_13389.txt | 19 - Gerardo Honorato (Universidad de Valparaíso, Chile) 19 - Karina Marín (Universidade Federal de Minas Gerais, Brasil) 19 - Pablo Carrasco (Universidade Federal de Minas Gerais, Brasil) 24 - Alvaro Castañeda (Universidad de Chile, Chile) 10 - Nicolas Arévalo Hurtado (PUC, Chile) 20 - Sebastián Donoso (Universidad de... |
quantumcomputing/14816_8f631342375c1193_379.txt | The dynamic bond can be defined as any class of bond that selectively undergoes reversible breaking and reformation, usually under equilibrium conditions. The incorporation of dynamic bonds (which can be either covalent or non-covalent) allows access to structurally dynamic polymers. Such polymers can exhibit macroscop... |
quantumcomputing/4625_578753610752009e_231.txt | Quantum states and wave functions We can take the continuous limit for quantum states in a similar way. For each N, we have a quantum system described by the Hilbert space HN of dimension dim HN = 2N + 1. There is an observable xN on this system with eigenstates |k and eigenvalues xk , where as before k ranges from −N... |
quantumcomputing/15280_ca3752daa9705eee_27.txt | The Gottesman-Knill theorem states that circuits built with only Clifford gates can be simulated efficiently on classical computers assuming the following conditions: state preparation in the computational basis measurements in the standard basis any classical control conditioned on the measurement outcomes The C... |
quantumcomputing/8e1d99f3_11159.txt | The toric code is defined on a two-dimensional lattice, usually chosen to be the square lattice, with a spin-½ degree of freedom located on each edge. They are chosen to be periodic. Stabilizer operators are defined on the spins around each vertex v {\displaystyle v} and plaquette[definition needed] (or face i.e. a ver... |
quantumcomputing/f2aea88b_121441.txt | The European IT Certification framework has been established in 2008 as a Europe based and vendor independent standard in widely accessible online certification of digital skills and competencies in many areas of professional digital specializations. The EITC framework is governed by the , a non-profit certification au... |
quantumcomputing/15280_ca3752daa9705eee_173.txt | Or we could iteratively apply the matrices to the vector j0i, first applying the matrix X 0 1 1 0 X j0i D D D j1i (11.125) 1 0 0 1 then applying the matrix Z to the resulting vector, like so 0 1 0 0 0 Z.X j0i/ D Z.j1i/ D Z D D 1 0 1 1 1 (11.126) Either way, we get the same result! Please not... |
quantumcomputing/2007f856_118711.txt | This circuit provides the required prolongation along the xx direction. For more than one spatial dimension, we simply apply the same process recursively for each spatial direction to the qubits obtained in the previous prolongation step. |
quantumcomputing/22087_cfa6e6481b8cd2bd_407.txt | It is a classical problem in the theory of shape optimization to find a shape with minimal (linear) elastic compliance (or, equivalently, maximal stiffness) for a given amount of mass and prescribed external forces. It is an intriguing question with a long history, going back to Michell's seminal 1904 work on trusses, ... |
quantumcomputing/32894_1a8f0330de3b41ea_79.txt | Single-cell RNA sequencing (scRNA-seq) reveals cell heterogeneity, with cell clustering playing a key role in identifying cell types and marker genes. Recent advances, especially graph neural networks (GNNs)-based methods, have significantly improved clustering performance. However, the analysis of scRNA-seq data remai... |
quantumcomputing/3960_0678c516274774e4_508.txt | I had said, “If you can explain evolution – and if you can do so while leaving God out – … But you can’t. You can’t account for time, change, dynamism of any sort.”, and you responded, “Uh, we can.” Again, I say, “people who think that these two [why and that] are the same …” You continued, “Like I said, God isn’t need... |
quantumcomputing/01b151e0_4771.txt | A new state-of-the-art state preparation technique based on QROM is now available with the qml.QROMStatePreparation template. (#6974) Using qml.QROMStatePreparation is analogous to using other state preparation techniques in PennyLane. state_vector = np.array([0.5, -0.5, 0.5, 0.5]) dev = qml.device("default.qubit") wir... |
quantumcomputing/c7c84af2_124731.txt | Valid encodings are n n n -qubit quantum state vectors for which the measurement outcomes, as eigenvalues, are all guaranteed to be 1. 1. 1. Any other syndrome, where at least one 1 -1 1 measurement outcome occurs, signals that an error has been detected. |
quantumcomputing/22087_69ca229ec5299de3_2661.txt | We discuss an approach to estimate aggregation and adaptive estimation based upon (nearly optimal) testing of convex hypotheses. The proposed adaptive routines generalize upon now-classical Goldenshluger-Lepski adaptation schemes, and, in the situation where the observations stem from simple observation schemes (i.e., ... |
quantumcomputing/383c8704_9971.txt | We’ve now seen a simple quantum circuit and quantum logic gate. But it’s not quite the simplest possible quantum circuit. The simplest possible quantum circuit does nothing at all. That is, it’s a single quantum wire: This circuit is just a single qubit being preserved in time. To be more explicit, if some arbitrary qu... |
quantumcomputing/6436_33aa2e4d3544ccd9_13.txt | Diagonalising a mutually commuting set of Pauli observables could require an arbitrary Clifford circuit in general. If we are considering the near-term regime where âevery gate countsâ, the diagonalisation of the observables could introduce more of the (relatively) expensive two-qubit gates, giving us the speedup a... |
quantumcomputing/14816_5f2deb247b7d4485_55.txt | bright and dark fringes of diffraction. He wrote up a simple letter, one of his first attempts at generating professional scientific work on his own, which contained broad speculations and general arguments rather than a concrete model, but it was a start. The next step was to find if his ideas had any merit. Fresnel’s... |
quantumcomputing/20712_189d5b93841f4e0f_80.txt | In an era characterized by complex mobility patterns, health crises, shifting geopolitical landscapes and personal and family’s views toward international education, it is imperative to recognize the concurrent (im)mobility challenges at a global scale. Despite a growing body of literature on international students, li... |
quantumcomputing/15280_ca3752daa9705eee_126.txt | Explicitly computing the inverse of A is generally the most costly method. In practice, most general-purpose numerical solvers use Gaussian elimination and back-substitution, which runs in O.N 3 / time. In this discussion we restrict ourselves to square matrices, i.e., M D N . Faster classical algorithms are possible: ... |
quantumcomputing/2258_ba4096302e7b1742_53.txt | Loop quantum gravity (LQG) attempts to unify general relativity with quantum physics to offer a complete of the universe by quantising spacetime geometry, but the numerical calculations we encounter are extraordinarily difficult. Progress has been made in the covariant formulation of LQG, but the tools do not carry ov... |
quantumcomputing/38735_fabe5077e891c005_319.txt | Armed with this understanding of individual adatoms, we now consider chains of adatoms. For an isolated impurity, the d-levels are typically far from the Fermi level of the substrate superconductor. In a chain of adatoms, there is direct hopping between neighbouring adatom orbitals, and the d-levels form one-dimensiona... |
quantumcomputing/22108_db9c0f2f4b6f960d_1878.txt | Curry's paradox is generally considered to be one of the hardest paradoxes to solve. It is shown here that the paradox can be arrived in fewer steps and also for a different term of the original biconditional. Further, using different approaches, it is also shown that the conclusion of the paradox must always be false ... |
quantumcomputing/025f9a2a_121855.txt | First, the case of normally distributed (Gaussian) errors. Consider a normally distributed variable y and some corresponding set of normally distributed model predictions y . The model error is, therefore, the difference between two normal distributions. If y and y are independent, the error distribution is guaran... |
quantumcomputing/5c95b40c_9518.txt | Let us consider two quantum states – one reconstructed from the data produced by unit tests and represented by the density matrix ρB\rho_{B}, and the other being the expected state defined by the density matrix σ\sigma. A quantitative measure of their deviation can be expressed using the Uhlmann–Jozsa fidelity (UHLMANN... |
quantumcomputing/3960_fea6c5621abd8595_20.txt | **Douglas Rushkoff,** media theorist and author, wrote, “2025 may be a whole lot more local in spirit and local in practice. As global supply chains falter and reveal their structural inadequacies, people will come to depend more on locally produced goods. This will also mean fewer ridiculous, meaningless, valueless cu... |
quantumcomputing/27984_a6019ccf7080d97d_408.txt | We applied a mean-field firing rate model to implement this idea. Our model considers an ensemble of CA1 place cells with identical place fields. We model the mean-membrane potentials in three compartments – soma, proximal dendrites and distal dendrites, the firing rate at soma and the mean synaptic output over the cel... |
quantumcomputing/8337_03d7507a27b4708c_40.txt | Although we only operate f(x) once by applying Uf, the output register contains evaluations of the function f(x) for all possible values of x. The challenge is how to extract this information. Measuring the qubits in the output register produces f(x) at a random value of x, which is not unique to quantum computing. Wha... |
quantumcomputing/14994_cdd61dafb85483f2_56.txt | Entanglement Particles (such as photons, electrons, or qubits) that have interacted at some point retain a type of connection and can be entangled with each other in pairs, in a process known as correlation. Knowing the spin state of one entangled particle – up or down – allows one to know that the spin of its mate is ... |
quantumcomputing/bcd52e3b_113959.txt | Statevector: textit w rangle frac sqrt 3 3 001 rangle frac sqrt 3 i 3 010 rangle- frac sqrt 3 3 100 rangle Probability Amplitudes: begin split begin bmatrix 0 frac sqrt 3 3 frac sqrt 3 i 3 0 - frac sqrt 3 3 0 0 0 end bmatrix end split Probabilities: ... |
quantumcomputing/20750_ad4744a1e1e1b7e8_163.txt | α 2 |0⟩|0⟩ + αβ |0⟩|1⟩ + β α |1⟩|0⟩ + β 2 |1⟩|1⟩ ̸= α |0⟩|0⟩ + β |1⟩|1⟩ If the cloning transformation gate G exists, then two terms that are not equal must be equal. This is a contradiction. The only logical conclusion is that G can’t exist. Therefore, it is impossible to clone a qubit of an arbitrary state. This is kn... |
quantumcomputing/175_40094682244c3a83_1153.txt | Graph Convolutional Networks (GCNs) are known to suffer from performance degradation as the number of layers increases, which is usually attributed to over-smoothing. Despite the apparent consensus, we observe that there exists a discrepancy between the theoretical understanding of over-smoothing and the practical capa... |
quantumcomputing/0424c2da_126414.txt | displaystyle mbox CNOT e i frac pi 4 (I _ 1 -Z _ 1 )(I _ 2 -X _ 2 ) e -i frac pi 4 (I _ 1 -Z _ 1 )(I _ 2 -X _ 2 ) . |
quantumcomputing/575eeb60_120271.txt | !-- image -- - Borel group , a maximal solvable subgroup , which is generated by the product of the lower triangular invertible Boolean matrices (CNOT circuits with controls on top qubits and targets on the bottom qubits) with diagonal subgroup elements (circuits with Phase and CZ gates). 8 This group is a subgrou... |
quantumcomputing/13334_db9c0f2f4b6f960d_525.txt | Physics lacks a confirmed of dark matter, has yet to develop an adequate understanding of dark energy, and includes unverified conjectures regarding new elementary particles. This essay features modeling that addresses those problems and explains otherwise unexplained data. Our modeling starts from five bases — multip... |
quantumcomputing/4628_578753610752009e_351.txt | What role does the Markov hypothesis play in Lindblad-type dynamics? In the quantum communication context, we introduce a “bystander” system R and suppose that RQ is initially in a pure state | (RQ) . The quantum Markov process is RQ → RQ → RQ (though R’s own dynamical evolution is trivial). Given the superoperato... |
quantumcomputing/13334_db9c0f2f4b6f960d_2975.txt | A novel Weyl-Heisenberg algebra in Clifford-spaces is constructed that is based on a matrix-valued HAB extension of Planck's constant. As a result of this modifiedWeyl-Heisenberg algebra one will no longer be able to measure, simultaneously, the pairs of variables (x, px); (x, py); (x, pz); (y, px), ... with absolute p... |
quantumcomputing/14994_2ed2d1df17fe28a3_120.txt | I design a deterministic cellular automaton, and agents in it. The agents can not observe their environment without altering it, which gives rise to some version of Uncertainty Principle, which in turn forces them accept a quantum theory of physics. I am NOT saying that the agents are wrong, and their world is “really”... |
quantumcomputing/13334_db9c0f2f4b6f960d_2277.txt | We establish a lower bound of 2^n conditional jumps for deciding the satisfiability of the conjunction of any two Boolean formulas from a set called a full representation of Boolean functions of n variables - a set containing a Boolean formula to represent each Boolean function of n variables. The contradiction proof f... |
quantumcomputing/4628_b32a98b8319d41d8_10.txt | The details on the implementation and computation of the error probabilities can be found in 2. Figure 10 shows the behaviour of different functional QADS, giving the geometric QADS the best performance. On the other hand, the differences between the two versions of the algorithm can be seen in Figs. 11, 12 and 13. In ... |
quantumcomputing/29980_0d146684cff49b5c_19.txt | In multi-qubit algorithms, interference often happens in a multi-step dance. First, put the qubits in a superposition of many inputs (parallel computation). Next, apply some transformation or oracle that *marks* the good answers (often by flipping the phase of states corresponding to solutions). Finally, interfere all ... |
quantumcomputing/03a17cff_4813.txt | Quantum just-in-time (qjit) compilation is the compilation of hybrid quantum-classical programs during execution of a program, rather than before execution. PennyLane provides just-in-time compilation with its @qml.qjit decorator, powered by the Catalyst compiler. Several templates are now compatible with qjit: qml.Amp... |
quantumcomputing/3960_98c38b4b94bcbcbd_159.txt | * *Continuous nitrators;* * *Centrifugal testing apparatus or equipment, having any of the following:* + *1. Driven by a motor or motors having a total rated horsepower of more than 298 kW (400 hp);* + *2. Capable of carrying a payload of 113 kg or more; **or*** + *3. Capable of exerting a centrifugal acceleration of 8... |
quantumcomputing/e5ba3b4f_126667.txt | The treatment of identical particles is very different for bosons (particles with integer spin) versus fermions (particles with half-integer spin). The above N -particle function must either be symmetrized (in the bosonic case) or anti-symmetrized (in the fermionic case) with respect to the particle numbers. If not all... |
quantumcomputing/1629_ffec68556b99fa4a_147.txt | We study an XXX open spin chain with variable number of sites, where the variability is introduced only at the boundaries. This model arises naturally in the study of giant gravitons in the anti-de Sitter-space/conformal field-theory correspondence. We show how to quantize the spin chain by mapping its states to a boso... |
quantumcomputing/32894_72cabeb6d560b66c_365.txt | Multi-bit flip-flops (MBFFs) are often used to reduce the number of clock sinks, resulting in a low-power design. A traditional MBFF is composed of individual FFs of uniform driving strength. However, if some but not all of the bits of an MBFF violate timing constraints, the MBFF has to be sized up or decomposed into s... |
quantumcomputing/22108_db9c0f2f4b6f960d_2353.txt | This paper will show through several experiments that time dilation, or modification of space-time, occurs only when there is a consciousness field or link (CFL) involved, along with velocity and/or acceleration. It also shows that consciousness can be applied remotely at great distance, can be connected directly or indi... |
quantumcomputing/2565_01bbb6e319e5fd22_221.txt | Bases and Dimension Finally, we can define a basis of a vector space. This definition will unlock a matrix-centric view of linear algebra, as we’re about to see. You might be wondering why we bothered defining all of the previous terms. It turns out that the precise definition of a matrix that we desire depends (linear... |
quantumcomputing/1629_3abeac199875c936_521.txt | Entanglement as a Combination of Classical and Quantum Correlations Now, what is the difference between classical and quantum correlations? As mentioned, classical correlation is interdependency among variables or parameters pertaining to different systems or subsystems (for instance, among the rotation direction of th... |
quantumcomputing/32894_1a3242be6d6d31f8_264.txt | We introduce the first direct policy search algorithm which provably converges to the globally optimal dynamic filter for the classical problem of predicting the outputs of a linear dynamical system, given noisy, partial observations. Despite the ubiquity of partial observability in practice, theoretical guarantees for... |
quantumcomputing/2270_2ed2d1df17fe28a3_330.txt | As someone who simultaneously believes (1) and (2), I don’t think these are opposing extremes. I think these are different ways of expressing a typical physicist objection to this kind of question. The goal of physics is to explain the world we are in. Therefore, empirical facts are necessary. Counterfactuals about hyp... |
quantumcomputing/175_40094682244c3a83_615.txt | Reward function specification, which requires considerable human effort and iteration, remains a major impediment for learning behaviors through deep reinforcement learning. In contrast, providing visual demonstrations of desired behaviors presents an easier and more natural way to teach agents. We consider a setting w... |
quantumcomputing/8981723d_3336.txt | Below we present a method and experiment for the proposed work. We ran the experiment using the Qiskit library, IBM open-source software for working with quantum computers (refer for details). Our experimental results are divided into two parts; a) Simulation Results. b) Quantum Computer Results. While simulator exper... |
quantumcomputing/32894_1a8f0330de3b41ea_471.txt | In order to boost the performance of a convolutional neural network (CNN), several approaches have shown the benefit of enhancing the spatial encoding of feature maps. However, few works paid attention to the positional properties of convolutional kernels. In this paper, we demonstrate that different kernel positions a... |
quantumcomputing/0aff034b_4118.txt | Bioinspired Technologies Emerging Technologies Laser Technology Technological Discourse Technological Innovation Innovation and Technology Management |
quantumcomputing/4628_578753610752009e_394.txt | projection measurements, and only for those. (See also Problem D.5.) For a specific example, let us once again recall the discussion of the projection rule in Section 4.3. There, we considered a two-beam interferometer which had either one or zero photons in it. The Hilbert space for the system had basis states |0 (no ... |
quantumcomputing/22087_69ca229ec5299de3_1166.txt | Although the genetic information in each cell within an organism is identical, gene expression varies widely between different cell types. The quest to understand this phenomenon has led to many interesting mathematics problems. First, I will present a new method for learning gene regulatory networks. It overcomes the ... |
quantumcomputing/9904_7ae05d4adf606362_15.txt | see, that the career of Hermann Weyl provides us with a perspective and some key insights. • I’m fascinated with Bott’s struggle to reconcile old and new world sensibilities. I saw this encoded in my interactions with him and in the convocation address. I use the word “encoded” in reference to the address, because his ... |
quantumcomputing/22087_dc81a22ac6ea9da6_42.txt | When we represent the PD as a strategic-form game, we implicitly assume that the prisoners can’t attempt collusive agreement since they choose their actions simultaneously. In this case, agreement before the fact can’t help. If Player I is convinced that his partner will stick to the bargain then he can seize the oppor... |
quantumcomputing/44116_58b87e4807ca5e69_222.txt | People have pronounced and speculated about what is and isn’t true about infinity since they began thinking abstractly. Aristotle’s views on the subject in particular had a great influence. A discovery made by the Italian mathematician Torricelli in 1641 provides a very revealing example.9 He found that the volume of a... |
quantumcomputing/22087_723fd0fbfe5d7a11_374.txt | ``` @article{10.1145/3579367, author = {Cuomo, Daniele and Caleffi, Marcello and Krsulich, Kevin and Tramonto, Filippo and Agliardi, Gabriele and Prati, Enrico and Cacciapuoti, Angela Sara}, title = {Optimized Compiler for Distributed Quantum Computing}, year = {2023}, journal = {ACM Transactions on Quantum Computing},... |
quantumcomputing/22087_69ca229ec5299de3_1029.txt | We are going to discuss a generalization of the classical relation between Jacobi matrices and orthogonal polynomials to the case of difference operators on lattices. More precisely, the difference operators in question reflect the interaction of nearest neighbors on the lattice Z^2. It should be stressed that the gene... |
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