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1 computing the 'normalization term' in Bayes' theorem).
2 e (derived using the fluctuation dissipation theorem).
3 ons and experimentally demonstrate the shift theorem.
4 o the problem, inspired by the Fourier shift theorem.
5 minimal dilation guaranteed by the Sz.-Nagy theorem.
6 ctions being appropriate according to Bayes' theorem.
7 rium it is forbidden by the Bohr-van Leeuwen theorem.
8 aces, a quantum analogue of the Gauss-Bonnet theorem.
9 uence of a corollary of the Perron-Frobenius theorem.
10 expected to be Gaussian by the central limit theorem.
11 oncepts based on the fluctuation dissipation theorem.
12 chanical unfolding using Crooks' fluctuation theorem.
13 pology that is employed in the proof of this theorem.
14 is analyzed using the potential distribution theorem.
15 accordance with the fluctuation-dissipation theorem.
16 confidence intervals according to Fieller's theorem.
17 e II error' cases were ascertained by Bayes' theorem.
18 then determined using the Crooks fluctuation theorem.
19 model based on the general kinetic momentum theorem.
20 ical simulations, in accord with our general theorem.
21 oses an alternative approach based on Bayes' theorem.
22 blem exists in the form of the Ramo-Shockley theorem.
23 Weyl branching rule and the Gel'fand-Tsetlin theorem.
24 is studied via the martingale central limit theorem.
25 iables beyond the prediction of Buckingham's theorem.
26 ussian fluctuations or use the central limit theorem.
27 ing sequence in L2 for the pointwise ergodic theorem.
28 thermodynamics, the fluctuation-dissipation theorem.
29 persymmetric extension of the standard basis theorem.
30 n the error limit and Shannon's noisy coding theorem.
31 ankov's result are both special cases of one theorem.
32 sterior class probabilities by use of Bayes' theorem.
33 ratios derived for predictors by using Bayes theorem.
34 r binocular fixations using Euler's rotation theorem.
35 ar machines conforming to Shannon's capacity theorem.
36 than the limits predicted by the Sagawa-Ueda theorem.
37 lly be impeded from LRO by the Mermin-Wagner theorem.
38 tability is guaranteed by Lyapunov stability theorem.
39 endent tests using generalized central limit theorem.
40 was observed in accordance with the Warburg theorem.
41 tween Shelankov's prediction and Zeilinger's theorem.
42 th heuristics derived from the Central Limit Theorem.
43 ity, power, and scan geometry by using Gauss theorem.
44 distribution predicted by the central limit theorem.
45 ear violation of the fluctuation dissipation theorem.
46 be enhanced by harnessing the central limit theorem.
47 probabilities were estimated using the Bayes theorem.
48 at finite temperatures by the Mermin-Wagner theorem.
49 er (P < .001) in accordance with the Warburg theorem.
50 any related variables and are based on Bayes theorem.
51 wing the prescription of the Nyquist-Shannon theorem.
52 -ergodic hypothesis, and then to the ergodic theorems.
53 This method is based on the BH theorems.
54 of the Gauss-Bonnet and Poincare-Hopf index theorems.
55 neracy originates from a version of Kramers' theorem(16,17) in which fermionic time-reversal invarian
56 d in the distance between the pairs given by Theorem 2, and the alignments to the incorrect strand.
57 jugation, parity reversal and time reversal) theorem, a cornerstone of the Standard Model, requires t
59 dance with the Kolmogorov-Arnold-Moser (KAM) theorem--a cornerstone of nonlinear dynamics that explai
60 ly expressed genes is established based on a theorem about the distribution of ranks of genes sorted
66 techniques, particularly those based on work theorems, also do not address spatial variations in the
67 this analytical framework, a Kerr-comb area theorem and a pump-detuning relation are developed, prov
68 ge Fermi surface consistent with Luttinger's theorem and a strongly enhanced quasiparticle effective
70 ributions are then analysed according to the theorem and allow us to determine the difference in fold
74 distribution from sequence data using Bayes' theorem and Markov chain Monte Carlo (MCMC) sampling, wh
75 e provides verification of the equipartition theorem and Maxwell-Boltzmann statistics for flexural mo
77 neralization of MacMahon's celebrated Master Theorem and relate it to a quantum generalization of the
78 ased on the Zipf analysis, we employ Bayes's theorem and relate the conditional probability that a ba
79 theoretical analysis shows that Zeilinger's theorem and Shelankov's result are both special cases of
80 shing a robustness result for the isothermal theorem and using large deviation estimates to understan
82 ased on the application of the Newton-Girard theorem and Viete's formulae to the polynomial coding of
84 s in mathematics and physics, with a body of theorems and algorithms that have been applied successfu
85 (the unattainability principle and the heat theorem), and place ultimate bounds on the speed at whic
86 be satisfied, namely the famous Gauss-Bonnet theorem, and an inequality stemming from the definition
87 is an approximation to the central limiting theorem, and it explicitly depends on the cumulative pro
88 optimal and equivalent to the marginal value theorem, and perform simulations to analyze deviations f
89 xcitations as a consequence of the Goldstone theorem, and readily results in the emergence of energy
90 n technology-multi-attribute utility, Bayes' theorem, and subjective expected utility maximization.
94 s a way to circumvent the quantum no-cloning theorem, approximate quantum cloning protocols have rece
96 ational methods and the application of Bayes theorem are used to form hypotheses about how informatio
101 ns on von Neumann algebras that displays the theorem as the basic result of noncommutative, metric, E
102 figurations that is based on a mountain pass theorem asserting that, if two solutions of the problem
103 e most general result so far, the isothermal theorem, assumes the propensity for change in each posit
105 d those calculated using the simple Koopmans theorem-based "neutral in-cation geometry" calculations
106 he more that outputs deviate from the coding theorem bound, the lower the complexity of their inputs.
107 Hurwitz class number generating series and a theorem by Serre, which allows us to rule out certain co
108 eory overcomes the lack of implicit function theorems, by formally establishing an often implicitly u
109 We show that the constraints of the scallop theorem can be escaped in frictional media if two asymme
110 Here we show that the Crooks fluctuation theorem can be used to determine folding free energies f
112 Von Neumann's celebrated double commutant theorem characterizes von Neumann algebras R as those fo
114 nd Law of Thermodynamics and its fluctuation theorem corollaries, irreversibility in nonequilibrium p
117 throughout in which all inline references to Theorems, Definitions and Lemmas given in the main Artic
119 Although the current mathematical structure theorems do not apply to the full NCR circuit, extensive
120 calculation or simulation, the Ramo-Shockley theorem eliminates a class of interpretations of experim
121 y John von Neumann and the pointwise ergodic theorem established by George Birkhoff, proofs of which
122 This perspective highlights the mean ergodic theorem established by John von Neumann and the pointwis
124 ace indicate the robustness of the Luttinger theorem even for materials with strong interactions.
126 nalysis based on the fluctuation-dissipation theorem (FDT) to characterize origins of activity fluctu
130 probabilities were calculated by using Bayes theorem for all elderly patients and for patients who un
131 was in good agreement with Wald's likelihood theorem for both metrics and all models that were tested
132 tructure formation-one employing the Kramers theorem for calculating radii of gyration, and the other
133 ntically distributed samples, and Girsanov's theorem for change of measures to examine rare behaviors
134 d from the same logical model as the Shannon theorem for channel capacity, arise from exactly the opp
135 e sensitivity and specificity values, Bayes' Theorem for conditional probability was applied to the h
136 ts shed light on the significance of a no-go theorem for exact ground-state cooling, as well as on th
138 it is derived as a special case of an index theorem for hypoelliptic operators on contact manifolds.
148 im of this paper is to announce a uniqueness theorem for these objects (within a fixed homotopy class
149 eory (QIT) allowed to formulate mathematical theorems for conditions that data-transmitting or data-p
150 ns with quite simple forms, we present limit theorems for partial sums, empirical processes, and kern
151 elop several criteria motivated by classical theorems for symmetric random walks, which lead to algor
154 t-output maps, arguments based on the coding theorem from algorithmic information theory (AIT) predic
155 to be frustration-free by lifting Shearer's theorem from classical probability theory to the quantum
162 mperature coming from the extensions of that theorem has been recently introduced to study glasses an
163 nsity fluctuations violate the central limit theorem, highlighting the role of nonequilibrium driving
164 fluctuations, according to the Mermin-Wagner theorem; however, these thermal fluctuations can be coun
165 l account of animal behavior (marginal value theorem), human participants of either sex decided when
166 ing sequence in L2 for the pointwise ergodic theorem if in any dynamical system (Omega, Sigma, m, T)
167 lization; (ii) sampling based on The Nyquist Theorem; (iii) internal correlation optimized shifting,
171 tested the predictions of the marginal value theorem in the context of hunter-gatherer residential mo
173 critical for refining neurocognitive memory theorem in the context of other endogenic processes and
174 ts such as the inverse and implicit function theorems in scale calculus-a generalization of multivari
176 tion-dissipation theorem, one of the central theorems in thermal dynamics, breaks down in out-of-equi
177 e defies expectations from the Mermin-Wagner theorem, in contrast to the much-reduced transition temp
180 l with the predictions of the marginal value theorem, indicating that communal perceptions of resourc
188 A direct operational consequence of Bell's theorem is the existence of statistical tests which can
189 coming the constraints of the Hobart-Derrick theorem, like in two-dimensional ferromagnetic solitons,
192 this inconsistency we employ the formulated theorem, modeling simulations and optimization along wit
193 In order to reach their full potential, the theorems must be extended to handle very hard problems.
195 d of analysis for testing the marginal value theorem (MVT) in natural settings that does not require
196 ic-connection fluctuation-dissipation (ACFD) theorem (namely the Rutgers-Chalmers vdW-DF, Vydrov-Van
199 Markov chain formalism, Conley's Fundamental Theorem of Dynamical Systems, and the core ingredients o
201 all quantum unipotent groups, extending the theorem of Geiss et al. for the case of symmetric Kac-Mo
203 ymmetric extension of the second fundamental theorem of invariant theory is obtained as a corollary.
205 genetic effects, extending the central-limit theorem of Lange to allow for both inbreeding and domina
206 tionary dynamics follow Fisher's Fundamental Theorem of Natural Selection and a corollary, permitting
208 adaptive evolution, known as the Fundamental Theorem of Natural Selection, is well appreciated by evo
209 The Price Equation and Fisher's fundamental theorem of natural selection, two of the most powerful c
211 the equation of genetic change, (2) Fisher's theorem of partial change, (3) a new uncertainty princip
219 er novel feature of our approach is that our theorems on exponential stability of steady states for h
220 the relevant concept of stability, we report theorems on some basic properties of strategies that are
221 onary Yang-Mills connections and compactness theorems on Yang-Mills connections with bounded L(2) nor
223 nature, gives alternative proofs of density theorems originally due to E. Szemeredi, H. Furstenberg,
224 , and majority-voting and the Condorcet Jury Theorem pervade thinking about collective decision-makin
226 be predicted by the prescient marginal value theorem (pMVT), which assumes they have perfect knowledg
228 cation, to our knowledge, of using automated theorem proving for automatically generating highly-accu
229 conical hexagonal lattices, which by Euler's theorem requires quantization of their cone angles.
230 strategies, contrary to a widely cited "folk theorem" result that suggests that punishment can allow
232 expressed by Marshall et al., with the no-go theorem shown by Armata et al., which provides boundarie
234 prove that it satisfies an 'almost unbiased' theorem similar to that of random-sampling cross-validat
235 n fitness and hence, by Fisher's fundamental theorem, slows the rate of increase in mean fitness.
239 mploy monotone systems theory to formulate a theorem stating necessary conditions for non-monotonic t
240 und to be deeply related with the four color theorem, stating that four colors are sufficient to iden
241 our new parameter in conjunction with Bayes' theorem, stereostructure assignments can be made with qu
242 m optimization devices, although a threshold theorem such as has been established in the circuit mode
247 hich follows a modified energy equipartition theorem that accounts for the kinetic energy of the flui
248 ution to obtain a version of the fluctuation theorem that articulates the relation between the entrop
250 onservation principle is developed here in a Theorem that precisely accounts for the statistical ener
252 e relies on an established Fourier transform theorem that relates time-domain sections to frequency-d
253 entury, Thomas Bayes developed his eponymous theorem that teaches us that pretest probabilities can b
255 Based on this result, we prove a second main theorem that the integral operators in the computation o
256 ation argument is used to prove a third main theorem that the integral operators in the computation o
258 Among the applications are central limit theorems that give convergence to a Gaussian distributio
259 As a direct consequence of the no-cloning theorem, the deterministic amplification as in classical
260 e from chemical reactions: the central-limit theorem then explains the central lognormal, and a numbe
263 fferent amounts of atomic detail, we use the theorem to calculate the gating charge produced by movem
264 which uses the naive Bayes classifier (NBC) theorem to combine eight state of the art contact method
265 sed force-field and the Dead-End Elimination theorem to compute sequences that are optimal for a give
267 d on non-singular transformation, we prove a theorem to determine rigorously the control efficacy of
268 ical computational method, which uses Bayes' theorem to generate a posterior distribution for a coupl
269 conditions are not necessary for the welfare theorem to hold but that in general, the market yields i
271 tional approach and the Dead-End Elimination theorem to search for the optimal sequence, we designed
273 ion of classical non-equilibrium fluctuation theorems to the quantum regime and a new thermodynamic r
275 mensional analysis and its corollary, the Pi-theorem, to the class of problems in which some of the q
276 give a short unified proof of the following theorem, valid in the context of both classical probabil
277 cer at 3 logical steps in the workup; Bayes' theorem was applied in a stepwise fashion to generate a
279 or algebra of a Peano space yielding Pappus' theorem was originally given by Doubilet, Rota, and Stei
283 ment of joints was assumed, and the binomial theorem was used to give the frequency distribution of i
285 conjunction with the Maxwell-Calladine index theorem we derive a relation between the number of linea
287 oise; exploiting the fluctuation-dissipation theorem, we determine the associated micromechanics.
291 Combining Hi-C data and novel mathematical theorems, we show that contact domains are also not cons
294 rarely observed manifestations of Onsager's theorem when time reversal symmetry is broken at zero ap
295 ee text] These results follow from a general theorem which models such polynomials by Hermite polynom
296 is subject to the constraints of the scallop theorem, which dictate that body kinematics identical un
297 deviation from the conventional soliton area theorem, which is crucial to understanding cavity solito
298 ely general nonlocal fluctuation-dissipation theorem with nonlocal response of surface plasmons in th
299 ys the additive method and the Central Limit Theorem within each individual experiment and also acros