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1 neracy (the latter is due to spin and valley degrees of freedom).
2 nal constraints (available sensory and motor degrees of freedom).
3  would allow versatile control of the valley degree of freedom.
4 tical phenomena, anharmonicity, and the spin degree of freedom.
5 uency and subsequently determined the proper degree of freedom.
6 ces mixtures of Mn(3+) and Mn(4+) and charge degree of freedom.
7 arity-dependent optically addressable valley degree of freedom.
8 ounded the cost of precisely moving a single degree of freedom.
9 ul due to issues such as the large number of degree of freedoms.
10 the number of connected pieces and the total degrees of freedom.
11 lators of quantum Hamiltonians with internal degrees of freedom.
12 unction of lipid identity and conformational degrees of freedom.
13 ecular vibrations to the electronic 'system' degrees of freedom.
14 pensate for the loss of head- and body-motor degrees of freedom.
15  information about its dynamics and internal degrees of freedom.
16 th as many as 100 sparsely connected quantum degrees of freedom.
17 algorithms that greatly reduce the number of degrees of freedom.
18 an unprecedented ability to control photonic degrees of freedom.
19 s a non-linear response to the environmental degrees of freedom.
20  of the pigments' electronic and vibrational degrees of freedom.
21 attice distortions coupled to the electronic degrees of freedom.
22 enable simultaneous monitoring of additional degrees of freedom.
23 s possibly between multiple internal quantum degrees of freedom.
24 ons between the translational and rotational degrees of freedom.
25 from the interplay between spin and motional degrees of freedom.
26 olving electromagnetic, mechanical, and spin degrees of freedom.
27 teraction between the lattice and electronic degrees of freedom.
28 ibution of energy into different vibrational degrees of freedom.
29 e photons are indistinguishable in all their degrees of freedom.
30 described according to only three structural degrees of freedom.
31 atoms as rigid bodies and rotatable bonds as degrees of freedom.
32 ntum phases that naturally entangle multiple degrees of freedom.
33  to the interplay between charge and lattice degrees of freedom.
34 trong coupling of electronic and vibrational degrees of freedom.
35 ably, these tests required movements along 3 degrees of freedom.
36 , strong spin-orbit coupling and spin-valley degrees of freedom.
37 nts, coupled to the membrane's compositional degrees of freedom.
38 ogenides possess coupling of spin and valley degrees of freedom.
39 ed polarisation and orbital angular momentum degrees of freedom.
40 ir equilibrium counterparts with identical 5 degrees of freedom.
41 ting of material properties through external degrees of freedom.
42 quantum frustration between spin and orbital degrees of freedom.
43 is low rank, i.e. has only a small number of degrees of freedom.
44 en atomic-structure, electronic and magnetic degrees of freedom.
45 plings between the electronic and structural degrees of freedom.
46 ductors for controlling both spin and charge degrees of freedom.
47 mediate environment and also constrain their degrees of freedom.
48 idea of simulating quantum systems with many degrees of freedom.
49 bid underflows that involve nearly 1 billion degrees of freedom.
50  coupling between electronic and vibrational degrees of freedom.
51  family of optical elements with exceptional degrees of freedom.
52 erplay between the spin, charge, and lattice degrees of freedom.
53 ormat, but neither eliminated all researcher degrees of freedom.
54 far only been studied for systems with a few degrees of freedom.
55 y follows a chi-square distribution with one degree of freedom (1-df).
56 hanical ventilation (Wald statistic = 20.08; degrees of freedom = 1; p < 0.001), higher daily Subarac
57  quantum dot quantum state onto a mechanical degree of freedom(1).
58 specific results were combined using joint 2 degree-of-freedom (2df) meta-analyses of SNP association
59             Opportunistic use of "researcher degrees of freedom" aimed at obtaining statistical signi
60  in-plane inversion asymmetry, an additional degree of freedom allowing spin manipulation can be indu
61  for the analysis of qualitative data is the degrees of freedom analysis (DoFA), published in 1975.
62                       This novel twist angle degree of freedom and control should be generalizable to
63 lenge, where the released helicity/vorticity degree of freedom and higher skyrmion density result in
64 here the atomic internal levels mimic a spin degree of freedom and interact through long-range intera
65 on of the phase of the wave as an additional degree of freedom and lower footprint area compared to c
66       We trained a planar model containing 9 degrees of freedom and 18 musculotendon actuators to wal
67 igns based on origami patterns to attain new degrees of freedom and achieve enhanced electromagnetic
68 rce allows for its generalization to various degrees of freedom and even for the implementation in in
69 ion depends on the nature of the interacting degrees of freedom and is higher than three for all mode
70                          The large number of degrees of freedom and lack of symmetry pose a challenge
71 -dependent energy distribution among various degrees of freedom and reveal the nature of and the impa
72  by means of a data-driven estimation of the degrees of freedom and scaling parameters for the partia
73 tic coupling between experimentally measured degrees of freedom and subunit rotation.
74  controlling molecular internal and external degrees of freedom and the resulting interaction process
75                                 It has seven degrees of freedom and therefore admits a large space of
76 l resolution would provide access to coupled degrees of freedom and ultrafast response functions on t
77 alizing topological states without spin-like degrees of freedom and with transverse phonon polarizati
78 ing sets of primers for this method has many degrees of freedom and would benefit from an automated p
79 ncluding low statistical power, researcher's degrees of freedom, and an emphasis on publishing surpri
80 rise in model selection, abuse of researcher degrees of freedom, and hypothesis testing for baseline
81 , such as controllable deformation, infinite degrees of freedom, and self-assembly, which make them p
82 rong Hund's rule alignment of local magnetic degrees of freedom, and to undergo distinctive changes i
83  jointly modulating the spatial and temporal degrees of freedom, arbitrary group velocities are unamb
84 erties are decoupled more thoroughly, or new degrees of freedom are added to the overall optimization
85                                      Lattice degrees of freedom are found to be crucially important i
86 optimization problems with a large number of degrees of freedom are intractable by classical computer
87 aterials, for which the important electronic degrees of freedom are local rather than itinerant and a
88 pecially in complex many-body systems, which degrees of freedom are the most informative about their
89                          Successful chi2 and degrees-of-freedom are computed, allowing null-hypothesi
90 rs', which correspond to the spin and valley degrees of freedom, are not filled equally.
91 rial system to explore the electron's valley degree of freedom as a quantum information carrier.
92 modes, spatial modes of light with entangled degrees of freedom, as a basis for encoding information.
93               To take advantage of the extra degree of freedom associated with tilting we have perfor
94                    The substantial kinematic degrees-of-freedom available in human movement lead to i
95  a new environment where they have (a) lower degrees of freedom because they are fixed into position
96 stricted the opportunistic use of researcher degrees of freedom better (Cliff's Delta = 0.49) than th
97 y in formate perovskites of novel structural degrees of freedom beyond the familiar dipolar terms res
98 ate the potential applications of this novel degree of freedom by dynamically addressing the modulati
99 egistration is a mechanism for reducing such degrees of freedom by specifying designs and analysis pl
100 -dimensional electron gases where the charge degree of freedom can be actively controlled by chemical
101                                   The valley degree of freedom can be directly accessed by means of o
102      In magnetic molecular devices, the spin degree-of-freedom can be used to this end since the magn
103 cts, and that a variety of reconfigurational degrees of freedom can be achieved through micro-archite
104 econd optical pulses, electronic and lattice degrees of freedom can be transiently decoupled, giving
105 vestigation of quantum phases, in which rich degrees of freedom can be used to encode information and
106 well as the quantum discord between distinct degrees of freedoms can be extracted from a small contro
107 onstrate that a body with significantly more degrees-of-freedom can be controlled by the human nervou
108           Our demonstration introduces a new degree of freedom, cavity deformation, to the microcomb
109 nto the control of spin, charge, and orbital degrees of freedom, central pillars of future solid stat
110 ermined by nontrivial interplay of different degrees of freedom: charge, spin, lattice, and also orbi
111 m computing(5), owing to their rich internal degrees of freedom compared to atoms, and to facilitate
112 this unified macroscopic picture of emergent degrees of freedom constraining mechanisms provides a st
113 operating principle, scalability, and single-degree-of-freedom contractile actuation motions.
114 rodynamic system where internal and external degrees of freedom cooperate to maximize a selective exc
115 cy in the assignment of constraints, and the degrees of freedom depend on constraint density in a sca
116                           Charge and orbital degrees of freedom determine properties of many material
117   Interactions were evaluated using both a 1 degree of freedom (DF) interaction term and a 2DF joint
118                          These include the 1-degree-of-freedom (df) test of G x E interaction, the 2-
119 action (likelihood ratio test (LRT) = 73.58, degrees of freedom (df) = 1, P = 4.83 x 10(-18)), which
120  omalizumab levels in serum (chi(2) = 65.84; degrees of freedom [df] = 2; P < .0005).
121  focused on the control of the electron spin degree of freedom (DOF) in materials such as multiferroi
122  valley pseudospin as an information bearing degree of freedom (DOF).
123 eption of a self-generated torque during a 2-degree-of-freedom (DOF), multi-joint task is largely inf
124 interplay between the electronic and nuclear degrees of freedom (DoF) during the excitation energy tr
125           A typical hand muscle spans over 3 degrees of freedom (DOF), wrapping over complex geometri
126 igami structures significantly constrain the degrees of freedom (DOFs) in both deformation and actuat
127 emonstrated greater utilization of redundant degrees of freedom (DoFs) supported by the greater task-
128 ltaneous and independent control of multiple degrees of freedom (DOFs), including wrist and digit art
129 inement technique is applied to decrease the Degrees-of-Freedom (DoFs) and computational requirements
130 ons of the electronic, magnetic, and lattice degrees of freedom drive an array of novel physical prop
131  versatility originating from the additional degrees of freedom due to atomic composition and orderin
132  dimensionality in many systems with orbital degrees of freedom due to the directional character of o
133 nducing step, and controlling the structural degrees of freedom during assembly and in the final COF.
134 d because of scattering by phonons and other degrees of freedom during exciton thermalization.
135                             These additional degrees of freedom enable new strategies and yield bette
136 e energy function is a quadratic form of the degrees of freedom, entropy and all other derived inform
137 n liquid with defect-induced frozen magnetic degrees of freedom.Experimental studies of frustrated sp
138 how that such structures offer an additional degree of freedom for adjusting optical properties with
139                               We introduce a degree of freedom for each marker effect obtained from O
140 mbrane and bending behavior via displacement degrees of freedom for a triangular element.
141 ations and wavelengths, providing additional degrees of freedom for agile polarization conversion in
142 ves charge transport by providing additional degrees of freedom for electron transfer.
143 d flexibility of metal oxides offer numerous degrees of freedom for enhancing catalytic activity by t
144             The threads in COF-505 have many degrees of freedom for enormous deviations to take place
145 action of two high intensity beams opens new degrees of freedom for manipulating electromagnetic wave
146 base pairs, thus in principle providing many degrees of freedom for modelling complex objects of defi
147 ll ladder along the frequency and pseudospin degrees of freedom for photons propagating in the ring.
148 metal and metal oxide may provide additional degrees of freedom for post-fabrication control of prope
149 ital angular momentum of light are important degrees of freedom for processing and encoding informati
150 h to explore the interplay between molecular degrees of freedom, framework topology, and supramolecul
151 ification at least partially decoupled these degrees of freedom from the population dynamics associat
152 gs between charge, spin, lattice, or orbital degrees of freedom, giving rise to remarkable phenomena
153 e time to thoroughly mix information among N degrees of freedom grows at least logarithmically in N.
154 e orbital angular momentum of light, as this degree of freedom has an unbounded set of orthogonal hel
155                                     This new degree of freedom has enabled reaching unprecedented CHF
156               The elimination of unnecessary degrees of freedom has opened up large-scale simulations
157 s widely recognized, and abuse of researcher degrees of freedom has received little attention in the
158                                     Magnetic degrees of freedom have been extensively investigated in
159 ing energies, oscillator strength and valley degree of freedom, have emerged as a very attractive pla
160 ensional honeycomb lattices possess a valley degree of freedom in addition to charge and spin.
161        In silicon, valley states represent a degree of freedom in addition to spin and charge.
162       Our results demonstrate the control of degree of freedom in bilayer with magnetic field, which
163 on (OER) in alkaline media offering a higher degree of freedom in cation arrangement.
164 ral molecules, which could introduce another degree of freedom in controlling the spin transport, rem
165                                   The valley degree of freedom in crystals offers great potential for
166                                     The spin degree of freedom in magnetic devices has been discussed
167 s of direct imaging of the valley pseudospin degree of freedom in monolayer transition metal dichalco
168 , our compact design makes use of the valley degree of freedom in photonic crystals(10,11), analogous
169 s a powerful tool for engineering the charge degree of freedom in strongly correlated materials, whic
170                This allows for a substantial degree of freedom in the engineering of transgenes capab
171 ards the purely electrical control of valley degree of freedom in topological valleytronics.
172 sents a promising way towards using the spin degree of freedom in very fast, low-power electronic dev
173 nteraction between electron spin and orbital degrees of freedom in 5d oxides can lead to exotic elect
174         The coupling between spin and charge degrees of freedom in a crystal gives rise to magneto-op
175    Here we propose a method that reduces the degrees of freedom in a stepwise manner and leads to a d
176 ynamic quantity indicative of the accessible degrees of freedom in a system.
177  computing based on manipulation of electron degrees of freedom in a well-characterized environment.
178       The manipulation of charge and lattice degrees of freedom in atomically precise, low-dimensiona
179 omic level information to reduce the immense degrees of freedom in compositional space without sacrif
180 tematically probe the impact of the internal degrees of freedom in each amino acid residue of VVD on
181 rticles can in turn interact with electronic degrees of freedom in graphene, including the collective
182 ns and its strong interaction with fermionic degrees of freedom in kagome-net materials.
183  boron nitride in the plane, leaving limited degrees of freedom in manipulating light at the nanoscal
184 erful tool for measuring difficult-to-access degrees of freedom in materials science.
185 theories, but the vibrational and rotational degrees of freedom in molecules pose a challenge for con
186     The use of biopolymers allows additional degrees of freedom in photonic bandgap design through di
187  complex coupling between charge and lattice degrees of freedom in superconducting cuprates.
188 ties formed using alpha-MoO(3) to extend the degrees of freedom in the design of IR photonic componen
189  principles that keeps all of the electronic degrees of freedom in the model explicit and simulates c
190 s that both the participation of the protein degrees of freedom in the reaction coordinate and the er
191 l folds in the quads decreases the number of degrees of freedom in the system, first linearly and the
192 fuller exploitation of entanglement in other degrees of freedom, in this work we demonstrate control
193 , which usually involves cooperation of many degrees of freedom including orbitals, fluctuating local
194 Entanglement, determined by spin and orbital degrees of freedom, increases with increasing valence bo
195  in molecular weight (MW) and conformational degrees of freedom into the dynamic covalent network.
196                    We find that the photonic degrees of freedom introduce extra electron-electron cor
197  a detailed depiction of the crucial nuclear degrees of freedom involved typically remains elusive.
198                          This nanomechanical degree of freedom is normally invisible and ignored in e
199 ethering pneumatic soft robots with multiple degrees of freedom is bulky and unpractical.
200 ong interplay between electronic and nuclear degrees of freedom is essential to achieve a full unders
201 y between charge, spin, orbital, and lattice degrees of freedom is the key to boosting device perform
202               Here, we show that "replicator degrees of freedom" make it far too easy to obtain and p
203 are characterized by valley and spin quantum degrees of freedom, making it possible to explore new ph
204 in an optical path length equation and a two-degree-of-freedom model, we can simultaneously extract t
205 ent and simultaneous control of the two comb degrees of freedom (modes spacing and frequency offset)
206 MoTe2 bilayers, as a result of an additional degree of freedom, namely the layer pseudospin, and spin
207 mula: see text], the availability of orbital degrees of freedom needed for the hidden order in [Formu
208 nsity of compact optical components from the degree of freedom of angle.
209 rm for valleytronics-the study of the valley degree of freedom of charge carriers to store and contro
210                                   The valley degree of freedom of dark excitons is accessed through t
211                                   The valley degree of freedom of electrons in solids has been propos
212  Hence, the strong hydrogen bond reduces the degree of freedom of the substrate and acts as a structu
213 f making functional activity out of the many degrees of freedom of a body.
214 hey do not explicitly capture the electronic degrees of freedom of a molecule, which limits their app
215 rest in synthetic dimensions, where internal degrees of freedom of a particle are coupled to form hig
216 egrees of freedom spreads over the many-body degrees of freedom of a quantum system, becoming inacces
217 e conformational space, which represents all degrees of freedom of a specified segment of protein cha
218 echanics, photons interact with the motional degrees of freedom of an optical resonator, for example,
219  concurrently probe spin and orbital/lattice degrees of freedom of Ba2NaOsO6 provide such tests.
220              The electronic and nuclear spin degrees of freedom of donor impurities in silicon form u
221  channels, selection of spatial channels and degrees of freedom of entanglement should be carefully c
222                           Resolving momentum degrees of freedom of excitons, which are electron-hole
223 es may be a useful strategy for reducing the degrees of freedom of flexible chains, enabling them to
224     Encoding information in high-dimensional degrees of freedom of photons has led to new avenues in
225 educe the geometric complexity and number of degrees of freedom of proteins, while element specific p
226 ructures in real space, manifest in external degrees of freedom of quantum states.
227 tries remain hidden in the space of internal degrees of freedom of subatomic particles.
228 ating a helical flagellum and the rotational degrees of freedom of the cell body and flagellum, and w
229 rthermore illustrate how the charge and spin degrees of freedom of the minimal DQD may be used to obt
230 ever, the intricate mechanisms and the large degrees of freedom of the multielement systems impede an
231 een the electronic state and the vibrational degrees of freedom of the probe ion.
232 ighlight the critical role played by the two degrees of freedom of the sigma-conjugated bridge on the
233 f individual statistics, but also reduce the degrees of freedom of the test statistic.
234 e evolution of the electronic and structural degrees of freedom of these systems on the time scales o
235 dynamics architectures to study the internal degrees of freedom of this many-body phenomenon.
236 r equations of hydrodynamics with rotational degrees of freedom, once linearized around a non-equilib
237 materials-especially those in which multiple degrees of freedom or energy scales are delicately balan
238 erally challenging to identify the essential degrees of freedom or, equivalently, the proper order pa
239  By examining the behavior of the electronic degrees of freedom, parity-breaking quasiparticles are r
240 e coupling between spin, charge, and lattice degrees of freedom plays an important role in a wide ran
241 hile entanglement can reside in any photonic degree of freedom, polarization permits perhaps the most
242 idual control of the electronic and motional degrees of freedom, preparation of a fiducial initial st
243                              By changing the degrees of freedom, protonation further affects the ther
244 terplay of spin, charge, orbital and lattice degrees of freedom provides a plethora of exotic phases
245 s have been achieved using the electron spin degree of freedom, realizing a robust CNOT gate has been
246   Depending on the couplings of the internal degrees of freedom, relaxation can be ultrafast, convert
247 exemplified by manipulating a single quantum degree of freedom, remains to be verified.
248 sition metal dichalcogenides provide further degrees of freedom requisite for information processing
249 l microbalance (QCM) substrate to form a two-degree- of-freedom resonance system (QCM-P).
250 utated monkeys exposed to control a multiple-degree-of-freedom robot arm.
251 lking direction and trunk orientation as the degrees of freedom shaping this behavior; and cocaine as
252  both the number of connected pieces and the degrees of freedom show percolation transitions as a fun
253 ndently controlling all of light's classical degrees of freedom simultaneously.
254  consisting of two balloons connected by a 3 degrees of freedom soft pneumatic actuator.
255 e vastly expanded by exploiting its multiple degrees of freedom: spatial, temporal, and polarization.
256  such as manipulation and control of quantum degrees of freedom (spin and pseudospin), confinement of
257 process by which information stored in local degrees of freedom spreads over the many-body degrees of
258  conductance, which generally involves other degrees of freedom such as spin.
259 ulation of single charges and their internal degrees of freedom, such as spin, may enable application
260 ition metal dichalcogenides possess a valley degree of freedom that allows for optoelectronic applica
261 , the many-body states possess a pseudo-spin degree of freedom that corresponds with the two direct-g
262 interacting quantum coherent spin and charge degrees of freedom that allow all-electrical initializat
263 r dynamics, but are limited by the number of degrees of freedom that can be followed at one time.
264 n-Popper perovskites with greater structural degrees of freedom that define the electronic structures
265 s a coupling among charge, spin, and lattice degrees of freedom that differs not only from the single
266 vity is, in terms of the number of modes (or degrees of freedom) that it can independently explore.
267                        With their additional degree of freedom, the vorticity, they have been widely
268 ally ordered material provides an additional degree of freedom through which the resulting exotic qua
269 ogy of van der Waals structures offers a new degree of freedom through which to tailor their electric
270 uivalent electron pockets, offering a valley degree of freedom to charge carriers.
271 engineered pore structures add an additional degree of freedom to create advanced membranes by provid
272 ion has been observed, suggesting a possible degree of freedom to dynamically control this in high di
273 a result, nanoscale curvature provides a new degree of freedom to manipulate 3D graphene electrical p
274                        Exploiting the valley degree of freedom to store and manipulate information pr
275 ile on the top-most layer adds an additional degree of freedom to the phase matching conditions for B
276 t fields in both space and time provides new degrees of freedom to manipulate light-matter interactio
277 epitaxial device structure offers additional degrees of freedom to select for optimal material proper
278 uantum simulation, we directly map fermionic degrees of freedom to spin ones, and then use neural-net
279  These phonons are coupled to the electronic degrees of freedom to varying extents.
280 ia hyperfine coupling to the electronic spin degrees of freedom, to probe the nature of superconducti
281              These include a large number of degrees of freedom, transannular interactions such as hy
282 ehaviour of the translational and rotational degrees of freedom under inversion.
283                              Recently, a new degree of freedom, valley, has been demonstrated in two-
284 is discussed, and it is demonstrated on an 8-degree-of-freedom walking robot where each limb comprise
285 unintuitive proportional control of multiple degrees-of-freedom, we propose a novel approach: proprio
286 ing a coupling of vibrational and electronic degrees of freedom-were observed in ultrafast time-resol
287         Such OAM is a completely independent degree of freedom which can be readily integrated with o
288  the number of components would increase the degree of freedom which can provide more flexibility in
289 emiconductors have led to addressable valley degree of freedom, which is the cornerstone for emerging
290 can be aggregated into systems with multiple degrees of freedom, which are able to produce controllab
291 -optical devices using the photon's internal degrees of freedom, which form photonic crystals in such
292  electronic property, the walls own internal degrees of freedom, which is potentially related to the
293 rane proteins can anneal lipid translational degrees of freedom while preserving internal order, it c
294 ystems(1) interface a macroscopic mechanical degree of freedom with a single two-level system such as
295 teractions of biomolecules involving bosonic degrees of freedom with a digital-analog approach.
296 strate the considerable impact of researcher degrees of freedom with respect to exclusion of particip
297 ing between electronic, magnetic and orbital degrees of freedom with the crystal structure across the
298                              Due to the many degrees of freedom within even short peptides, the desig
299  quantify such timing correlations among the degrees of freedom within proteins.
300 demands broader utilization of the available degrees of freedom within the optical field.

 
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