2000
DOI: 10.1201/9781420041767
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Engineering Applications of Noncommutative Harmonic Analysis

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Cited by 205 publications
(275 citation statements)
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“…Examples of (5) will be demonstrated in subsequent sections in the context of gyroscopes, kinematic carts, and flexible needle steering. Focusing on the "r" case, when h and H are constant, we can write (6) where When considering stochastic differential equations and the corresponding Fokker-Planck equations, it is usually important to specify whether the Ito or Stratanovich form is used. Without getting into too much detail, it suffices to say that the Ito form has been assumed in the derivation of both of the above Fokker-Planck equations.…”
Section: Fokker-planck Equationsmentioning
confidence: 99%
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“…Examples of (5) will be demonstrated in subsequent sections in the context of gyroscopes, kinematic carts, and flexible needle steering. Focusing on the "r" case, when h and H are constant, we can write (6) where When considering stochastic differential equations and the corresponding Fokker-Planck equations, it is usually important to specify whether the Ito or Stratanovich form is used. Without getting into too much detail, it suffices to say that the Ito form has been assumed in the derivation of both of the above Fokker-Planck equations.…”
Section: Fokker-planck Equationsmentioning
confidence: 99%
“…In particular, given the scalar parameters x i ∈ IR, the linearity of the Lie algebra allows one to write and a famous theorem states that 7,14,6 :…”
Section: Thenmentioning
confidence: 99%
“…In our previous works 28, 51 , a methodology for solving equations such as (3) was developed using the technique of the Fourier transform for SE (3). The matrix elements of this transform are 51, 61 (4) where for each r ∈ Z and p ∈ ℜ + , U r (a,R;p) is the irreducible unitary representation matrix of SE (3), p is the frequency factor introduced by the transform, and dRda is the invariant integration measure for SE (3).…”
Section: Review Of the General Inextensible Semi-flexible Macromolecumentioning
confidence: 92%
“…4). Therefore, in general, denoting f(β h ) as the probability distribution of the bending angle β h at the hinge, the PDF of rigid-body motion on SE(3) at this hinge can be obtained as a convolution (15) where α ∈ [0,2π], β ∈ [0, π], and γ ∈ [0,2π], and Then the Fourier transform of f j (a,R) on SE(3) can be obtained as (18) where (19) (20) where δ i,j is the Kronecker delta function, and is the generalized Legendre function 51,62 .…”
Section: The Hinge Casementioning
confidence: 99%
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