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1978
Information and Control
White Gaussian channels with nonlinear feedback, mutual information in, 37, 178 Z~ codes over, revisited, 37, 100 Zero-memory replacement optimal, control-limit policies, 37, 90 equivalence of, proof of ...
languages
form interpretations, 38, 330
Extended 0L systems
" propagating chain-free normal forms for,
36, 309
Extended quaternary quadratic residue
codes
binary images of, 38, 148
Extended T0L ...
doi:10.1016/s0019-9958(78)90707-6
fatcat:3g6qa5hi2zc2lgyyvndbar65di
Energetics of three interacting mass-imbalanced bodies in a three-dimensional spherical harmonic trap
[article]
2022
arXiv
pre-print
Using two approaches, one using an infinite sum of basis states for the wavefunction and the other a closed form wavefunction, we calculate the allowable energy eigenstates of the system as a function ...
of the interaction strength, including the strongly and weakly interacting limits. ...
We have also revisited, for fermions with mass imbalance, and bosons, the Efimov states in such systems. ...
arXiv:2204.09205v1
fatcat:rv2slxrpyzfcphc2r3nu3pjcd4
Lattice φ4Theory of Finite-Size Effects Above the Upper Critical Dimension
1998
International Journal of Modern Physics C
scaling functions are derived. ...
MC data of larger systems would be desirable for testing the magnitude of the L^(4-d)/2 and L^4-d terms predicted by our theory. ...
function of r 0L L 2 . ...
doi:10.1142/s012918319800100x
fatcat:wxqasko33nhinhmzfbcnqsemuu
Completion of the universal I–Love–Q relations in compact stars including the mass
2017
Monthly Notices of the Royal Astronomical Society: Letters
We compute the corrected mass vs radius configurations of rotating quark stars, revisiting a classical paper on the subject. ...
We thus complete the set of universal relations for the tidal problem in binary systems, involving four perturbation parameters, namely I, Love, Q, and δ M. ...
the surface choosing an explicit coordinate system. ...
doi:10.1093/mnrasl/slx078
fatcat:wsxn73tdsrdtrdlvpuk7zaqhxq
Shot-noise suppression in multimode ballistic Fermi conductors
1999
Physical Review B (Condensed Matter)
͑ E t ͓͒1Ϫ f 0L ͑ E t ͔͒ ϩ͓Tr͑t ϩ t͒ϪTr͑t ϩ tt ϩ t͔͒ ϫ f 0L ͑ E t ͓͒1Ϫ f 0R ͑ E t ͔͖͒. ͑1͒ Here f 0L (E t ) and f 0R (E t ) are the electron distribution functions on the left and right hand sides of ...
We will revisit this assumption at the end of the paper.͒ ...
doi:10.1103/physrevb.60.r2169
fatcat:fqzpmpyzjfc63curpwurz4scei
A Full Non-Monotonic Transition System for Unrestricted Non-Projective Parsing
[article]
2017
arXiv
pre-print
In this paper, we propose a novel, fully non-monotonic transition system based on the non-projective Covington algorithm. ...
As a non-monotonic system requires exploration of erroneous actions during the training process, we develop several non-monotonic variants of the recently defined dynamic oracle for the Covington parser ...
Therefore, this ex-Unigrams L0w; L0p; L0wp; L0l; L 0h w; L 0h p; L 0h l; L 0l w; L 0l p; L 0l l; L 0r w; L 0r p; L 0r l; L 0h2 w; L 0h2 p; L 0h2 l; L 0l w; L 0l p; L 0l l; L0rw; L0rp; L0rl; L0wd; L0pd; ...
arXiv:1706.03367v1
fatcat:macf7emksza2jnwsc5bznfdefu
A Full Non-Monotonic Transition System for Unrestricted Non-Projective Parsing
2017
Proceedings of the 55th Annual Meeting of the Association for Computational Linguistics (Volume 1: Long Papers)
In this paper, we propose a novel, fully non-monotonic transition system based on the non-projective Covington algorithm. ...
As a non-monotonic system requires exploration of erroneous actions during the training process, we develop several non-monotonic variants of the recently defined dynamic oracle for the Covington parser ...
Therefore, this ex-Unigrams L0w; L0p; L0wp; L0l; L 0h w; L 0h p; L 0h l; L 0l w; L 0l p; L 0l l; L 0r w; L 0r p; L 0r l; L 0h2 w; L 0h2 p; L 0h2 l; L 0l w; L 0l p; L 0l l; L0rw; L0rp; L0rl; L0wd; L0pd; ...
doi:10.18653/v1/p17-1027
dblp:conf/acl/Fernandez-Gonzalez17
fatcat:n7zvxboperczbascd6ohzd3gvq
On the choice of time in the continuum limit of polymeric effective theories
[article]
2012
arXiv
pre-print
We show that it is only through the introduction of a particular λ-dependent internal time function that the limit λ→ 0 can be well defined. ...
In particular one might ask whether the limit exists and, in that case, what the limiting theory is. ...
We have available some partial answers, that we have revisited in this contribution. ...
arXiv:1209.2752v1
fatcat:7xtb7upefjcpnjpkajdkylxqnu
Accuracy in Depth Recovery and 3D Image Synthesis from Single Image using Multi-Color Filter Aperture and Shallow Depth of Field
2021
IEEE Access
l th layer as below: D 0l = d 0l M M − (M +1) d ls d 0l . (12) Alternatively, (12) can be expressed in the form below: D 0l = d 0l M 2 1 − (M +1) M d 0l d ls . (13) In the similar lines, we can obtain ...
instead of d 0l . ...
doi:10.1109/access.2021.3109865
fatcat:vmpisxdwrjbepcm7imyayhnkhy
Adaptive Laplace Mechanism: Differential Privacy Preservation in Deep Learning
[article]
2018
arXiv
pre-print
To achieve this, we figure out a way to perturb affine transformations of neurons, and loss functions used in deep neural networks. ...
Detection systems for email spam integrate learning methods for analyzing data more effectively [2] . ...
However, the pSDG can only be applied to train the model by using a limited number of epochs; specifically because the privacy budget is accumulated after every training step. ...
arXiv:1709.05750v2
fatcat:gunsztz7mrfjpcahfv2cv4h3du
Direct search implications for a custodially-embedded composite top
2016
Physical Review D
In this paper, we revisit the model in light of the Higgs boson discovery and other data from LHC Run I. ...
The Lagrangian features a left-handed SM-like EW doublet q 0L consisting of the SM top and bottom quarks (t 0L , b 0L ), and right-handed SM-like EW singlets t 0R and b 0R . ...
doi:10.1103/physrevd.94.014002
fatcat:pitau4hakvb4fe2ze27apyzcw4
The Concept of a Minimal State in Viscoelasticity: New Free Energies and Applications to PDEs
2006
Archive for Rational Mechanics and Analysis
The energetics of linear viscoelastic materials is revisited and new free energies, expressed in terms of the minimal state descriptor, are derived together with the related dissipations. ...
We show here the impact on the initial-boundary value problem, and on the evolution of viscoelastic systems of the use of a new definition of state based on the stress-response (see, e.g., [48, 16, 41] ...
Now we can consider for the system (9.7) the function v:=u t as unknown and w:=ϕ t as a test function. ...
doi:10.1007/s00205-005-0406-1
fatcat:6bxpbvwgqfdpbfoe43vg5mdfra
A Class of Active-Set Newton Methods for Mixed ComplementarityProblems
2005
SIAM Journal on Optimization
For the special case of optimality systems with primal-dual structure, we further consider the question of superlinear convergence of primal variables. ...
Since ψ S is a complementarity function, the right-hand side of the latter equality is zero if and only if ξ i ≥ 0, F i (x), ξ ≥ 0, ξ i F i (x), ξ = 0, i ∈ A 0l , ξ i ≤ 0, F i (x), ξ ≤ 0, ξ i F i (x), ...
KKT systems. ...
doi:10.1137/s105262340343590x
fatcat:uhr7iizjyfbaphoqqbv7xras5i
On the Integral Identities Consisting of Two Spherical Bessel Functions
2007
IEEE Transactions on Antennas and Propagation
Therefore, this paper revisits thoroughly the evaluation of the integral of ( ). ...
It is realized that there exists a limitation of 1 in (2) and (3a). ...
doi:10.1109/tap.2006.888467
fatcat:dsgljb7j45agdm4qqtczxbejua
Kalman Filtering Over Graphs: Theory and Applications
2009
IEEE Transactions on Automatic Control
It is easy to verify that B i k0ljk0l B i k j k0l ; 8i; k; and 0 l D 0 1: In other words, S i has more measurements of time k 0l at time k than at time k 0l. ...
Therefore, S i can obtain a better estimate of x k0l at time k than at time k 0l. ...
systems [4] , analysis of interconnected systems [6] , and design of neural networks [7] , among others. ...
doi:10.1109/tac.2009.2026851
fatcat:7vfukd455vb7ncpl3af3mvrfum
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