Masking, Photobleaching, and Spreading Effects in Hadamard Transform Imaging and Spectroscopy Systems

2001 ◽  
Vol 55 (3) ◽  
pp. 318-330 ◽  
Author(s):  
Quentin S. Hanley

In analyzing the behavior of a Hadamard transform imaging spectroscopic system in an optical sectioning microscope, a previously undescribed masking effect was observed. During the process of characterizing this artifact, it was noted that while many masking errors have been reported previously in the literature, no attempt has been made to classify them or to systematically treat their effects in a variety of imaging and spectroscopy arrangements. Previous reports have documented echo artifacts in one-dimensional Hadamard mask systems based on sequences of length 2 n – 1, for which the echoes are well defined. Other valid cyclic S-sequences, such as those of prime length 4 m + 3 ≠ 2 n – 1, do not exhibit such behavior. Masking errors may be present with these sequences, but they do not appear as echoes. Recovered intensities are observed having both positive and negative magnitude distributed throughout the transform axis. These masking defects appear superficially to be “noise”, making associated errors more difficult to diagnose. Masking effects in two-dimensional systems have not been previously reported. In these, the relationship between the original image and resulting “echoes” can be quite complicated. This paper treats a variety of masking effects theoretically and presents simulations based on that treatment. Mask errors are divided into first- and second-order effects depending on whether the encoding passes through a mask once or twice. Symmetric, asymmetric, and static masking errors in one-dimensional Hadamard transform systems are treated in both first- and second-order arrangements. Where prior data exist, an attempt has been made to collect and categorize known mask-related artifacts and where appropriate provide additional documentation. Mask errors may be spatially varying or spatially invariant over the mask or within a given pixel. In systems which are spatially variant, proper sampling of the image or spectrum by the elements composing the mask is a prerequisite for successful correction of the data. Corrections applied to data from masks with spatially variant errors may cause artifacts to appear and, in some instances, complete correction may be impossible. The effects of photobleaching and mask spreading due to processes such as diffraction or aberrations in both one- and two-dimensional mask systems are investigated. Photobleaching is relatively easy to correct when an exponential decay model is applicable. In second-order systems, mask spreading gives rise to echoes or distortion even in perfectly implemented masks. Mask spreading can, in many cases, be corrected by analyzing the observed “echoes” and building a correction matrix or by using knowledge of the point, line, or other spreading function of the system. Finally, in masks of length 2 n – 1, a few simple rules greatly assist in diagnosing masking effects.

1986 ◽  
Vol 108 (14) ◽  
pp. 4242-4244 ◽  
Author(s):  
Lewis E. Kay ◽  
T. A. Holak ◽  
B. A. Johnson ◽  
I. M. Armitage ◽  
J. H. Prestegard

2007 ◽  
Vol 22 (01) ◽  
pp. 17-28 ◽  
Author(s):  
R. N. GHALATI ◽  
N. KIRIUSHCHEVA ◽  
S. V. KUZMIN

Using the Gitman–Lyakhovich–Tyutin generalization of the Ostrogradsky method for analyzing singular systems, we consider the Hamiltonian formulation of metric and tetrad gravities in two-dimensional Riemannian spacetime treating them as constrained higher-derivative theories. The algebraic structure of the Poisson brackets of the constraints and the corresponding gauge transformations are investigated in both cases.


1956 ◽  
Vol 7 (2) ◽  
pp. 85-105 ◽  
Author(s):  
B. S. Stratford

SummaryOne of the main problems associated with the “ Jet Flap ” concerns the discrepancy in thrust between idealised theory and the experimental results. This discrepancy is attributable to the mixing with the surrounding flow of the thin two-dimensional jet while still in close proximity to the aerofoil. The effect of the mixing may be calculated to a first approximation from a formula derivable from first principles, while certain second order effects, which can be significant, may be considered qualitatively.It is concluded that.(i) the full thrust should be experienced by a jet flapped aircraft at cruise,(ii) it should be possible to attain a low form drag at cruise in comparison with a conventional aircraft,(iii) at take-off, an aircraft using a shrouded jet flap would have better thrust recovery than one using a pure jet flap (which shows appreciable losses),(iv) the use of by-pass engines would further improve the thrust characteristics,(v) the practical gains from thrust augmentation, as obtained by controlling the mixing, seem likely to be small.


2016 ◽  
Vol 13 (04) ◽  
pp. 1650045 ◽  
Author(s):  
Takahiro Yajima ◽  
Kazuhito Yamasaki

Geometric structures of dynamical systems are investigated based on a differential geometric method (Jacobi stability of KCC-theory). This study focuses on differences of Jacobi stability of two-dimensional second-order differential equation from that of one-dimensional second-order differential equation. One of different properties from a one-dimensional case is the Jacobi unstable condition given by eigenvalues of deviation curvature with different signs. Then, this geometric theory is applied to an overhead crane system as a two-dimensional dynamical system. It is shown a relationship between the Hopf bifurcation of linearized overhead crane and the Jacobi stability. Especially, the Jacobi stable trajectory is found for stable and unstable spirals of the two-dimensional linearized system. In case of the linearized overhead crane system, the Jacobi stable spiral approaches to the equilibrium point faster than the Jacobi unstable spiral. This means that the Jacobi stability is related to the resilience of deviated trajectory in the transient state. Moreover, for the nonlinear overhead crane system, the Jacobi stability for limit cycle changes stable and unstable over time.


2016 ◽  
Vol 64 (6) ◽  
Author(s):  
Anton Friedrich Koch

AbstractB-time, i. e. the temporal scale of the B-series of events, is one and the same for all times, while A-times (the temporal scales of A-series) are as many as there are moments of time. This means that A-theorists will have to consider one-dimensional time two-dimensionally: as changing within itself at every moment. The two-dimensional view is here put to service for a meta-compatibilist theory of freedom, a theory, that is, which reconciles freedom, determinism and their first order incompatibility at the second order. Kant’s position is interpreted as meta-compatibilist as well, but as having the drawback of separating time and freedom. In order to appreciate the connection of time and freedom, one has to acknowledge that in free acts the future is determined further according to plan, while at the same time the past is (with nomological necessity) co-determined further in countless unclear and inscrutable ways. A free act thus consumes its own range of freedom by positing retroactively the sufficient causal antecedents for its taking place: It was free before it occurred and is part of nature after.


1966 ◽  
Vol 25 ◽  
pp. 46-48 ◽  
Author(s):  
M. Lecar

“Dynamical mixing”, i.e. relaxation of a stellar phase space distribution through interaction with the mean gravitational field, is numerically investigated for a one-dimensional self-gravitating stellar gas. Qualitative results are presented in the form of a motion picture of the flow of phase points (representing homogeneous slabs of stars) in two-dimensional phase space.


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