Pseudo-Zernike polynomials

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In mathematics, pseudo-Zernike polynomials are well known and widely used in the analysis of optical systems. They are also widely used in image analysis as shape descriptors.

Definition

They are an orthogonal set of complex-valued polynomials defined as

Vnm(x,y)=Rnm(x,y)ejmarctan(yx),

where x2+y21,n0,|m|n and orthogonality on the unit disk is given as

02π01r[Vnl(rcosθ,rsinθ)]*×Vmk(rcosθ,rsinθ)drdθ=πn+1δmnδkl,

where the star means complex conjugation, and r2=x2+y2, x=rcosθ, y=rsinθ are the standard transformations between polar and Cartesian coordinates.

The radial polynomials Rnm are defined as[1]

Rnm(r)=s=0n|m|Dn,|m|,s rns

with integer coefficients

Dn,|m|,s=(1)s(2n+1s)!s!(n|m|s)!(n+|m|s+1)!.

Examples

Examples are:

R0,0=1

R1,0=2+3r

R1,1=r

R2,0=3+10r212r

R2,1=5r24r

R2,2=r2

R3,0=4+35r360r2+30r

R3,1=21r330r2+10r

R3,2=7r36r2

R3,3=r3

R4,0=5+126r4280r3+210r260r

R4,1=84r4168r3+105r220r

R4,2=36r456r3+21r2

R4,3=9r48r3

R4,4=r4

R5,0=6+462r51260r4+1260r3560r2+105r

R5,1=330r5840r4+756r3280r2+35r

R5,2=165r5360r4+252r356r2

R5,3=55r590r4+36r3

R5,4=11r510r4

R5,5=r5

Moments

The pseudo-Zernike Moments (PZM) of order n and repetition l are defined as

Anl=n+1π02π01[Vnl(rcosθ,rsinθ)]*f(rcosθ,rsinθ)rdrdθ,

where n=0,, and l takes on positive and negative integer values subject to |l|n.

The image function can be reconstructed by expansion of the pseudo-Zernike coefficients on the unit disk as

f(x,y)=n=0l=n+nAnlVnl(x,y).

Pseudo-Zernike moments are derived from conventional Zernike moments and shown to be more robust and less sensitive to image noise than the Zernike moments.[1]

See also

References

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