I must lay it by in my mind, and think it over some time or other, it's so kind of strange and unregular.
"Adventures of Huckleberry Finn, Complete" by Mark Twain (Samuel Clemens)
I must lay it by in my mind, and think it over some time or other, it's so kind of strange and unregular.
"Adventures of Huckleberry Finn, Part 6" by Mark Twain (Samuel Clemens)
I must lay it by in my mind, and think it over some time or other, it's so kind of strange and unregular.
"The Adventures of Huckleberry Finn" by Mark Twain
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There is a way one can get rid of the cut-off corrections; one can simply split the charge contribution at q2 = 0, which should be one, and compute the difference using a unregularized quark loop.
Pion Structure at High and Low Energies in Chiral Quark Models
Actually, in the case of the pion such a model corresponds to a unregularized NJL calculation.
Pion Structure at High and Low Energies in Chiral Quark Models
This only reﬂects the fact that for the unregularized quark loop the separation between soft and hard processes involved in the Bjorken limit ⊥ ∼ Q2 .
Pion Structure at High and Low Energies in Chiral Quark Models
PDA calculation for the unregularized quark loop Since γ ∗ → π0 γ is an abnormal parity process, the standard procedure in the NJL model is not to regularize it because this is the only way to preserve the anomaly (See also Ref. [35, 75])).
Pion Structure at High and Low Energies in Chiral Quark Models
If we formally take the limit we get an expression looking like Eq. (97) with, ϕπ (x) = 1 but with the unregularized form of f 2 π ( see Eq. (49).
Pion Structure at High and Low Energies in Chiral Quark Models
Floer, The unregularized gradient ﬂow of the symplectic action, Comm.
The Arnold-Givental conjecture and moment Floer homology
Floer, The unregularized gradient ﬂow of the symplectic action, Comm.
Floer Homology for Symplectomorphism
It is instructive to do so ﬁrst for the original unregularized 1D interaction in the ﬁnite Poisson system of N particles randomly distributed in the interval [−L, L′ ].
Gravitational force in an infinite one-dimensional Poisson distribution
From this formula it is clear that, as for the onepoint properties of the unregularized force, this two-point quantity is ill deﬁned in the limit N , L, L′ → ∞ with N/(L′ + L) = n0 .
Gravitational force in an infinite one-dimensional Poisson distribution
CM] Cieliebak, K., Mohke, K., “Symplectic hypersurfaces and transversality in Gromov-Witten theory ”, Journal of Symplectic Geometry (2008) Floer, A., “The unregularized gradient ﬂow of symplectic action ”, Comm.
Moduli Spaces of $J$-holomorphic Curves with General Jet Constraints
Both “unregularized” and regularized estimators are easy to compute with the EM algorithm; and the speed of the algorithm is not so painfully slow as in other inverse problems, since this is still a problem where “root n” rate estimation is possible.
Product-limit estimators of the gap time distribution of a renewal process under different sampling patterns
Floer, The unregularized gradient ﬂow of the symplectic action.
Applications of Polyfold Theory I: The Polyfolds of Gromov-Witten Theory
Comparison with unregularized linear frequency estimator.
Using linear predictors to impute allele frequencies from summary or pooled genotype data
Comparison between BLIMP estimator and unregularized linear estimators.
Using linear predictors to impute allele frequencies from summary or pooled genotype data
In this formula the necessity of the regularization becomes evident because in the unregularized form the right hand side consists of a product of two distributions, which a-priori is not well-deﬁned.
Photoacoustic imaging in attenuating acoustic media based on strongly causal models
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