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1 for scalable generation and distribution of entanglement.
2 tum mechanical effects such as tunneling and entanglement.
3 nd then separate them while preserving their entanglement.
4 ng and exploration of the physics of quantum entanglement.
5 em experiences a loss of coherence following entanglement.
6 ks for long-distance distribution of quantum entanglement.
7 els between thermodynamics and the theory of entanglement.
8 oth of which confirm a high level of on-chip entanglement.
9 th-entangled two-qubit state and analyse its entanglement.
10 irements for creating and preserving quantum entanglement.
11 lene chain, as part of a kinetically trapped entanglement.
12 rk forms the first example of a new class of entanglement.
13 ajectories through a global measure of their entanglement.
14 polarization mode dispersion (PMD) degrades entanglement.
15 prevent the distribution and distillation of entanglement.
16 hotons separately, as this could destroy the entanglement.
17 way to create high-dimensional spatial mode entanglement.
18 involves a critical destruction of the Kondo entanglement.
19 nce between ordered nanostructure and fibril entanglement.
20 e-to-optical photon converters that preserve entanglement.
21 test a remedy to recover the high degree of entanglement.
22 opological order and high degrees of spatial entanglement.
23 stomeric behavior is caused by polymer chain entanglements.
24 ttribute to the unraveling of polysaccharide entanglements.
25 kers becomes smaller than the length between entanglements.
30 Bessel basis, thus once again revealing the entanglement after propagation beyond the obstruction.
33 rds, have been extensively documented (e.g., entanglement and choking), very little is known about ef
36 upper bound based on the relative entropy of entanglement and devising a dimension-independent techni
38 lement in a scenario in between the standard entanglement and fully device-independent scenarios, and
39 antum information, efficient distribution of entanglement and generation of completely secure keys.
43 applications ranging from studies of quantum entanglement and quantum information science to imaging.
47 s a state of matter characterized by quantum entanglement and the absence of any broken symmetry.
48 tructural centrosome aberrations, chromosome entanglements and defective telomere clustering, suggest
49 and RNA substrates in resolving topological entanglements and for the analysis of TDRD3 functions.
50 have measured dynamics consistent with spin entanglement, and have detected entanglement with macros
51 novo Topoisomerase II (TopoII)-dependent re-entanglements, and complete failure in chromosome segreg
55 ntroduce two approaches: The first one is an entanglement-based scheme, and the second one studies th
56 ing mechanism that is distinct from existing entanglement-based theories of polymer deformation and f
57 oaches are ubiquitous in the distribution of entanglement because entangled photons are easy to gener
58 pically satisfy an "area law": The amount of entanglement between a subsystem and the rest of the sys
59 t formulation of a Bell test to characterize entanglement between an artificial atom and a cat state,
60 ondegenerate narrow-band continuous-variable entanglement between bright light beams by using only co
61 How to conveniently and efficiently produce entanglement between bright light beams presents a chall
63 scheme that enables the generation of robust entanglement between distant electron spins (estimated s
65 op a witness which allow them to demonstrate entanglement between millions of atoms in a solid-state
66 nstructing a second chip, which measures the entanglement between multiple distant pairs of simulated
67 , the same technique can be used to generate entanglement between oscillators in the quantum regime.C
68 the input, and we experimentally demonstrate entanglement between over two hundred ensembles, each co
70 ity to a time-evolving Bell state, revealing entanglement between photons emitted up to 5 ns apart, e
72 are both found implausible due to structural entanglement between the DNA and connector loops that ha
73 d control photons, and confirm deterministic entanglement between the signal and control modes by ext
74 ructive quantum interference through quantum entanglement between the signal and the idler input fiel
78 Tenerife, verifying the presence of quantum entanglement between two previously independent photons
81 ha (TOP2A) has been proposed to resolve such entanglements, but the mechanisms governing TOP2A recrui
86 decoherence and loss, photon statistics and entanglement can be preserved in single plasmonic system
88 shows that significant amount of mechanical entanglement can indeed be obtained by balancing the opp
91 l coupling between these paired MFs, quantum entanglement cannot be induced from an unentangled (i.e.
92 High molecular weight, thus sufficient chain entanglement, combined with a small-amount dynamic CB[8]
95 upling between many degrees of freedom whose entanglement convolutes understanding of the instigating
98 ficiently than a generic quantum state whose entanglement could be proportional to the total system's
100 he impact of coupling factor of networks and entanglement degree in quantum games on the evolutionary
101 hallmark of non-classicality--and verify an entanglement depth (the minimum number of mutually entan
104 lop a novel nonlinear criterion which infers entanglement dimensionality of a global state by using o
105 f a quantum repeater, a device that performs entanglement distillation and quantum teleportation.
107 eater, which would work beyond the limits of entanglement distillation, hence possibly tolerating hig
111 This enables some very early approaches to entanglement distribution to be revisited, in particular
112 ty to govern DNA topology and resolve strand entanglements during fundamental molecular processes, th
113 ns, leads to a complete understanding of the entanglement dynamics in the space-time scaling limit.
116 We further show that cross-links dominate entanglement dynamics when the length between cross-link
117 ow that it is possible to distribute quantum entanglement encoded in OAM over a turbulent intracity l
118 y demonstrate a widely applicable method for entanglement-enhanced measurements without low-noise det
120 inding interference processes from which the entanglement entropy and Hubbard interactions are quanti
123 scaling of various quantities (concurrence, entanglement entropy, magnetic and fidelity susceptibili
124 ssions of area laws have been constrained to entanglement entropy, whereas a full understanding of a
129 at the standard quasiparticle picture of the entanglement evolution, complemented with integrability-
130 ults for low N and arbitrary d show that the entanglement fidelity asymptotically approaches N/d(2) f
131 ounds for various success measures, such as (entanglement) fidelity, are known, but some become trivi
133 ces with a potential for generating "useful" entanglement for the purpose of quantum computing and th
135 e formation and unraveling of conformational entanglements from newly incorporated monomers, whose ke
137 ate quantum nature of this router by showing entanglement generated between the initially unentangled
139 emonstrate the power of heralded methods for entanglement generation, and illustrate how the informat
142 reads to determine the shortest path via the entanglement gradient coefficient, which describes the f
150 f intense research with the observation that entanglement holds interesting information about quantum
153 te quantum steering, give a method to detect entanglement in a scenario in between the standard entan
154 and optimisation of the extensive growth of entanglement in a spin chain, and opens up the use of ph
155 , Zarkeshian et al. demonstrate multipartite entanglement in an atomic frequency comb storing a singl
156 Our results clarify the role of multipartite entanglement in ensemble-based quantum memories and demo
161 limited experimental control.The presence of entanglement in macroscopic systems is notoriously diffi
162 t highlights the counterintuitive concept of entanglement in macroscopically distinguishable systems.
166 is work, we study the preservation of photon entanglement in polarization, created by spontaneous par
170 method to certify all kinds of multipartite entanglement in this asymmetric scenario and experimenta
171 tic neutron scattering enables us to portray entanglement in weakly coupled molecular qubits and to q
173 nnections and structures, including physical entanglements in polymer networks, knots along polymer c
174 henomenon, named electromagnetically induced entanglement, in the conventional Lambda-type three-leve
175 he state is slightly below the threshold for entanglement-induced metrological gain, further technica
176 arge state space allows for complex types of entanglement, interesting both for quantum communication
177 Fabry-Perot resonators will allow multimode entanglement involving electromagnetic, mechanical, and
183 tangled photon pairs, however, the degree of entanglement is maintained when photon pairs are distrib
185 e contains further entanglement.Multipartite entanglement is of both fundamental and practical intere
188 the parties involved to be able to verify if entanglement is present before they carry out a given di
189 angled photon, we find that its polarization entanglement is preserved and non-locally correlated wit
195 meters, we show that our architecture allows entanglement lifetimes orders of magnitude longer than t
198 at each individual ensemble contains further entanglement.Multipartite entanglement is of both fundam
200 d photon pairs maintain their high degree of entanglement, no matter what type of spatial modes they
201 A molecules can be described in terms of an "entanglement number" and yield a nonmonotonic mobility a
203 ent on atomic chemical potentials due to the entanglement of atomic chemical potentials and Fermi ene
204 field splitting, implying quantum mechanical entanglement of charge-carrier spins over distances of 2
205 long-range qubit coupling and the long-range entanglement of electrons in semiconductor quantum dots.
207 ntum information processing is the efficient entanglement of multiple stationary quantum memories via
210 y (TS) plots show the strong preservation of entanglement of photons propagating in brain tissue.
211 ismatch of the two types of amphiphiles, the entanglement of polymer chains, and the mobility of NPAM
217 density interaction determine the long-range entanglement of the model which possesses "restricted pa
219 whereby we recover information lost from the entanglement of the optical orbital angular momentum and
220 operate without complete destruction of the entanglement of the quantum-bits are difficult to engine
222 littings indicative of quantum superposition/entanglement of the two SMMs, and parallel studies on Me
224 ch a negative Wigner function and the mutual entanglement of virtually all atoms is unprecedented for
225 rs the irreversible formation of topological entanglements of the fibers resulting in an entangled wa
228 ntum devices must generate and control qubit entanglement on-chip, where quantum information is natur
231 quantum behavior, such as superpositions and entanglement, only when they are sufficiently decoupled
233 the frame of the molecule, directly probing entanglement or disentanglement of quantum pathways as a
234 s, thus dispensing with quantum nonlocality, entanglement, or even discord between the players' input
237 the distribution of orbital angular momentum entanglement over more than 100 km of free space is feas
240 hould enable future studies of transport and entanglement propagation in a many-body system with long
243 lready allow for efficient implementation of entanglement purification, we anticipate our research to
244 tions present a new challenge: to distribute entanglement, qubits must be transported, merged for int
245 sses "restricted patterns" of the long-range entanglement realized in corresponding string-net models
247 ate in two all-optical experiments that such entanglement restoration can even be achieved on-demand.
248 brush architecture prevents the formation of entanglements, resulting in elastomers with precisely co
249 arkable quantum phase transition whereby the entanglement scaling changes from area law into extensiv
252 trol, both schemes improve the efficiency of entanglement sharing in distributed quantum networks.
257 rks using quantum resources with tailor-made entanglement structures have been proposed for a variety
258 y studying Renyi entropies and understanding entanglement structures in strongly coupled systems and
259 nder certain magnetic conditions a series of entanglement sudden-deaths and revivals occur between th
260 bed for fundamental tests of quantum science.Entanglement swapping in high dimensions requires large
262 en different anti-symmetric states, and thus entanglement swapping occurs for several thousand pairs
265 e teleportation of an entangled state, i.e., entanglement swapping, representing the central resource
267 s which we can prove have exponentially more entanglement than suggested by the area law, and violate
269 light provide an avenue for high-dimensional entanglement, the ability to transport such quantum stat
272 riments for sympathetic cooling, creation of entanglement through dissipation, and quantum non-demoli
274 the combination of a reduction of interchain entanglements through homopolymeric polyQ and barriers t
275 re of such dynamics is the growth of quantum entanglement to an amount proportional to the system siz
276 ic qubits, allowing quantum correlations and entanglement to be established between distant nodes.
277 These experiments pave the way for using entanglement to characterize quantum phases and dynamics
279 ter as the quantum interface to transfer the entanglement to the orbital angular momentum degree of f
281 to perform the locality-constrained tasks of entanglement transformation and its classical analog of
282 rics are derived from the characteristics of entanglement transmission and relevant measures of entan
284 hesin, condensin, and topoisomerase-mediated entanglements until all sister chromosomes bi-orient alo
286 t coherent for 15 seconds, during which spin entanglement was generated, as verified by a negative me
287 ion of resources, like quantum coherence and entanglement, which allow quantum information and comput
288 experimental measure of continuous variable entanglement, which relies on the detection of only one
290 lagellum cross-linking, as well as flagellar entanglement with bacterial bodies, suggesting that moti
291 t for quantum repeaters, we demonstrate that entanglement with flying optical qubits can be stored in
292 ssibility to certain classes of multipartite entanglement with limited experimental control.The prese
293 nt with spin entanglement, and have detected entanglement with macroscopic observables; we are now ab
296 mer chain motion is typically constrained by entanglements with surrounding molecules, nanoparticles
297 ameter of the polymer chains, diluting their entanglements without markedly increasing stiffness.
300 We obtained an expectation value for the entanglement-witness operator, more than 6 SDs beyond th
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