Open Access

Table A.1

IDL procedure for the calculation of disk-averaged scattering functions and normalized quadrant polarization parameters.

pro quadrants,ideg,g,fiavg,fphiavg,qpp
incl = ideg*!pi/180. ; inclination i in radians
; array of disk azimuth angles φd for disk ring: 3600 point with [0, 0.1, .., 359.9] degrees in radians
phi_d = findgen(3600)*!pi/1800.
x = -sin(phi_d) ; x-sky for inclined disk ring
y = cos(incl)*cos(phi_d) ; y-sky
z = -sin(incl)*cos(phi_d) ; z along line of sight
phi = atan(-x,y) ; sky azimuth angle ϕxy(φd, i) (Eq. 34)
theta = acos(z) ; scattering angle θ(φd, i) (Eq.30)
; scattering intensity using HG-phase function 4π fI(θ, g) (Eq. 19)
fi = (1.-g2)/(1.+g2-2.*g*cos(theta))1.5 ; 4π fI (φd, i) (Fig. 6)
; polarized intensity using Rayleigh scattering splitting with pmax = 1 (Eqs. 21,22)
fper = fi/(1.+(cos(theta))2) ; f or azimuthal intensity
fpar = fi*(cos(theta))2 / (1.+(cos(theta))2) ; f or radial intensity
fphi = fper-fpar ; 4π fϕ (φd, i): azimuthal polarization (Fig. 6)
fq = fphi*(-cos(2.*phi)) ; 4π fQ (φd, i) for Stokes Qd (Fig. 7)
fu = fphi*(-sin(2.*phi)) ; 4π fU (φd, i) for Stokes Ud (Fig. 7)
; disk averaged scattering functions ⟨f(i, g)⟩
fiavg = mean(fi) ; intensity ⟨fI(i, g)⟩ (Eq. 37)
fphiavg = mean(fphi) ; azimuthal polarization ⟨fϕ(i, g)⟩ (Eq. 38)
; normalized quadrant polarization parameters
qpp = fltarr(5) ; initialize quadrant values
; sum-up of relevant ϕxy(φd, i)-points for each quadrant (according to Tab. 2)
for j=0,3599 do begin
if (phi[j] gt -0.25*!pi and phi[j] lt 0.25*!pi)then qpp[0]=qpp[0]+fq[j]/3600. ; quadrant Q000
if (phi[j] gt 0. and phi[j] lt 0.50*!pi) then qpp[1]=qpp[1]+fu[j]/3600. ; quadrant U045
if (phi[j] gt 0.25*!pi and phi[j] lt 0.75*!pi) then qpp[2]=qpp[2]+fq[j]/3600. ; quadrant Q090
if (phi[j] gt 0.50*!pi and phi[j] lt 1.00*!pi) then qpp[3]=qpp[3]+fu[j]/3600. ; quadrant U135
if (phi[j] gt 0.75*!pi or phi[j] lt -0.75*!pi) then qpp[4]=qpp[4]+fq[j]/3600. ; quadrant Q180
endfor
return
end

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