• Chinese Optics Letters
  • Vol. 14, Issue 9, 091001 (2016)
Kejia Wang1、2, Ziliang Ping3、4, and Yunlong Sheng1、*
Author Affiliations
  • 1Center for Optics, Photonics and Lasers, Department of Physics, Physical Engineering and Optics, Laval University, Quebec G1V0A6, Canada
  • 2Inner Mongolia Electronic Information Vocational Technical College, Huhhot 010070, China
  • 3School of Electronic Engineering, Beijing University of Posts and Telecommunications, Beijing 100876, China
  • 4Inner Mongolia Normal University, Huhhot 010020, China
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    DOI: 10.3788/COL201614.091001 Cite this Article Set citation alerts
    Kejia Wang, Ziliang Ping, Yunlong Sheng. Development of image invariant moments—a short overview[J]. Chinese Optics Letters, 2016, 14(9): 091001 Copy Citation Text show less

    Abstract

    We give a brief overview on the more than 50 years of development of the moment-based image description, the moment invariants, and the orthogonal moments. Some basic ideas for significantly improving the performance of the image moment-based methods, such as the use of the low-order radial moments for reducing information suppression drawback and the separation of the radial basis from the circular harmonic basis for a free selection of the orthogonal radial polynomials, are presented. Performance measures for the orthogonal moments are discussed from the point of view of image analysis. A moment family list is proposed, which includes most of the representative moments in use and the discrete orthogonal moments.
    mp,q=xpyqf(x,y)dxdy,(1)

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    h1=μ20+μ02,h2=(μ20μ02)2+4μ112,h3=(μ303μ12)2+(3μ21μ03)2,h4=(μ30+μ12)2+(μ21+μ03)2,h5=(μ303μ12)(μ30+μ12)[(μ30+μ12)23(μ21+μ03)2]+(3μ21μ03)(μ21+μ03)[3(μ30+μ12)2(μ21+μ03)2],h6=(μ20μ02)[(μ30+μ12)2(μ21+μ03)2]+4μ11(μ30+μ12)(μ21+μ03),h7=(3μ21μ03)(μ30+μ12)[(μ30+μ12)23(μ21+μ03)2](μ303μ12)(μ21+μ03)[3(μ30+μ12)2(μ21+μ03)2],(2)

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    Mn,m=02π01f(r,θ)rn1ejmθrdrdθ,(3)

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    Mn,m=02π0f(r,θ)rn1ejmθrdrdθ=f(x,y)(x+jy)(nm)/2(xjy)(n+m)/2dxdy,(4)

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    Fa,b,m=02π01ψa,b(r)ejmθf(r,θ)rdrdθ,(5)

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    ψ(r)=4αn+12π(n+1)σcos(2πf0(2r1))exp((2r1)22σ2(n+1)),(6)

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    fm(r)=02πejmθf(r,θ)dθ,(7)

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    ψa,b(r)=1aψ(rba),(8)

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    Anm=n+1π02π01Rnm(r)exp(jmθ)f(r,θ)rdrdθ,(9)

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    Rnm(r)=s=0(n|m|)/2(1)s(ns)!s!((n+|m|)/2s)!((n|m|)/2s)!rn2s,(10)

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    Φnm=12πan02π01Qn(r)exp(jmθ)f(r,θ)rdrdθ,(11)

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    Qn(r)=s=0nαnsrs,withαns=(1)n+s(n+s+1)!(ns)!s!(s+1)!.(12)

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    ϕnm=12π02π01Rn(r)exp(jmθ)f(r,θ)rdrdθ,(13)

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    Rn(r)=8π[w(r)]1/2r1/2Un*(r),(14)

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    Un*(r)=k=0[n/2](1)k(nk)!k!(n2k)![2(2r1)]n2k,(15)

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    01Un*(r)Uk*(r)w(r)dr=π8δnk,(16)

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    Φnm=12π02π01Jn(p,q,r)exp(jmθ)f(r,θ)rdrdθ,(17)

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    w(p,q,r)=(1r)pqrq1,(18)

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    01Gn(p,q,r)Gk(p,q,r)w(p,q,r)dr=bn(p,q)δnk,(19)

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    Gn(p,q,r)=n!Γ(q)Γ(n+p)s=0n(1)nsΓ(n+p+s)(ns)!s!Γ(q+s)rs,(20)

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    Jn(p,q,r)=Gn(p,q,r)w(p,q,r)/bn(p,q,r).(21)

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    bn(p,q)=n!Γ(n+pq+1)[Γ(q)]2(2n+p)Γ(n+p)Γ(n+q).(22)

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    Bnm=12παn02π01Jv(λnr)exp(jmθ)f(r,θ)rdrdθ,(23)

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    01Jv(λnr)Jv(λkr)dr=αnδnk,(24)

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    ϕnm=12π02π01Tn(r)exp(jmθ)f(r,θ)rdrdθ.(25)

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    x=0N1pm(x)pn(x)w(x)=ρ(n)δmn,(26)

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    Pmn=x=0M1y=0N1f(x,y)p˜m(x)p˜n(y),(27)

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    p˜n(x)=pn(x)w(x)/ρ(n).(28)

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    tn(x)=n!k=0n(1)nk(N1knk)(n+kn)(xk),(29)

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    ρ(n,N)=N(N21)(N222)(N2n2)2n+1=(2n)!(N+n2n+1),n=0,1,N1.(30)

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    t˜n(x)=tn(x)/β(n,N),(31)

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    ρ˜(n,N)=ρ(n,N)/β(n,N)2andβ(n,N)=Nn.(32)

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    w(x;p,N)=(Nx)px(1p)Nx,(33)

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    ρ(n;p,N)=(1)n(1pp)nn!(N)n.(34)

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    Kn(x;p,N)=k=0Nak,n,pxk=F12(n,x;N;1p),(35)

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    Frs(a1,,ar;b1,,bs;z)=k=0(a1)k(a2)k(ar)k(b1)k(b1)k(bs)kzkk!,(36)

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    (a)k=a(a+1)(a+k1)=Γ(a+k)Γ(a).(37)

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    hn(μ,ν)(x,N)=(N+ν1)n(N1)n×k=0n(1)k(n)k(x)k(2N+μ+νn1)k(N+ν1)k(N1)k1k!,(38)

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    x=0N1w(x)hm(μ,ν)(x,N)hn(μ,ν)(x,N)=dn2δmn,(39)

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    w(x)=1Γ(x+1)Γ(x+μ+1)Γ(N+νx)Γ(Nnx),(40)

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    dn2=Γ(2N+μ+νn)(2N+μ+ν2n1)Γ(N+μ+νn)×1Γ(N+μn)Γ(N+νn)Γ(n+1)Γ(Nn).(41)

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    hn(x;α,β,N)=F23(n,n+α+β+1,x;α+1,N;1),(42)

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    w(x;α,β,N)=(α+xx)(β+NxNx),(43)

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    d2(n;α,β,N)=(1)n(n+α+β+1)N+1(β+1)nn!(2n+α+β+1)(α+1)n(N)nN!.(44)

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    Wnm=s=ab1t=ab1w^n(c)(s,a,b)w^m(c)(t,a,b)f(s,t),(45)

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    wn(c)(s,a,b)=(ab+1)n(a+c+1)nn!×F23(n,as,a+s+1;ab+1,a+c+1;1),(46)

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    s=ab1ρ(s)wn(c)(s,a,b)wm(c)(s,a,b)[Δx(s12)]=dn2δnm.(47)

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    ρ(s)=Γ(a+s+1)Γ(c+s+1)Γ(sa+1)Γ(bs)Γ(b+s+1)Γ(sc+1),(48)

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    dn2=Γ(a+c+n+1)n!(ban1)!Γ(bcn).(49)

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    w^n(c)(s,a,b)=wn(c)(s,a,b)ρ(s)dn2[Δx(s12)].(50)

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    Unm=s=ab1t=ab1u^n(α,β)(s,a,b)u^m(α,β)(t,a,b)f(s,t),(51)

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    un(α,β)(s,a,b)=1n!(ab+1)n(β+1)n(a+b+α+1)n×F34(n,α+β+n+1,as,a+s+1;β+1,ab+1,a+b+α+1;1),(52)

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    s=ab1ρ(s)un(α,β)(s,a,b)um(α,β)(s,a,b)[Δx(s12)]=dn2δnm,(53)

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    ρ(s)=Γ(a+s+1)Γ(sa+β+1)Γ(b+αs)Γ(b+α+s+1)Γ(aβ+s+1)Γ(sa+1)Γ(bs)Γ(b+s+1),(54)

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    dn2=Γ(α+n+1)Γ(β+n+1)Γ(ba+α+β+n+1)(α+β+2n+1)n!(ban1)!Γ(α+β+n+1)×Γ(a+b+α+n+1)Γ(a+bβn).(55)

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    u^n(α,β)(s,a,b)=un(α,β)(s,a,b)ρ(s)dn2[Δx(s12)].(56)

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    Spq=1nρ(p,m)r=0m1k=0n1tp,m(r)ej2πqknf(r,θk),(57)

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    tp,m(r)=p!mpk=0p(1)pk(m1kpk)(p+kp)(rk),(58)

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    ρ(p,m)=m(11m2)(122m2)(1p2m2)2p+1,(59)

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    Kejia Wang, Ziliang Ping, Yunlong Sheng. Development of image invariant moments—a short overview[J]. Chinese Optics Letters, 2016, 14(9): 091001
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