Dear Steven:
>    I am learning to use the programme , and I try an examples about photonic 
> crystal filled with liquid crystals in 
>the Reference( physical review B 67,073106 (2003)). But I find the result, the 
>dispersion relations of guided modes are so different compared with the 
>results in the Reference, which will be a error though their basic curves is 
>similar.
>    This is 2D triangular lattice photonic crystal with air holes in GaAs 
> substrate. The backgound dielectric index is 11.4. We calculalte the 
> dispersion relations of line defect waveguides filled with liquid crystal, 
> and the attached  file is about the supercell, and Dark and light shaded 
> regions indicate GaAs and liquid crystals, respectively. When the rotation 
> angle of the director of the liquid crystal is 90°, the components of the 
> dielectric tensor are ne*ne,no*no,and zero in xx ,yy, and xy 
> directions,respectively, where ne is 1.706 ,and no is 1.522 ( this direction 
> is in accord with that in the supercell).  I try some examples about liquid 
> crystals, and the problem is also present. Would you mind scanning my ctl 
> file? 
>(define-param supercell-y 10) ; the (odd) number of lateral supercell periods
>(set! geometry-lattice (make lattice 
>                        (basis1 (/ (sqrt 3) 2) 0.5)
>                        (basis2 (/ (sqrt 3) 2) -0.5)
>                        (size 1 supercell-y no-size)))
>(define-param eps 11.4) ; the dielectric constant of the bandground
>(define-param r 0.45) ; the hole radius in the bulk crystal
>
>(set! default-material (make dielectric (epsilon eps)))
>(set! geometry (list (make cylinder
>                      (center 0 0 0) (radius r) (height infinity)
>                      (material air))))
>(set! geometry 
>      (append
>       ; duplicate the bulk crystal holes over the supercell:
>       (geometric-objects-lattice-duplicates geometry)
>
>       ; add a rod of dielectric, to erase a row of holes and form a waveguide:
>       (list 
>       (make cylinder (center 0 0 0) (radius r) (height infinity)
>             (material (make dielectric (epsilon eps)))))
>       (list 
>       (make cylinder (center 0 0 0) (radius r) (height infinity)
>             (material (make dielectric-anisotropic (epsilon-diag 2.910436 
> 2.316484 2.316484)))))))
>(define Gamma (vector3 0 0 0))
>(define K' (lattice->reciprocal (vector3 0.5 0 0))) ; edge of Brillouin zone.
>(set! k-points (interpolate 100 (list Gamma K')))
>; the bigger the supercell, the more bands you need to compute to get
>; to the defect modes (the lowest band is "folded" supercell-y times):
>(define-param extra-bands 6) ; number of extra bands to compute above the gap
>(set! num-bands (+ supercell-y extra-bands))
>
>(set-param! resolution 32)
> (run-te 
> (output-at-kpoint (list-ref k-points (quotient(length k-points) 4))
>                  fix-hfield-phase output-hfield-z))
>
>    Thank you a lot. Look forward to your reply!
>Best regards   
>Hongliang Ren 
>
> 
>       
>
>        hlren
>[EMAIL PROTECTED]
>          2006-08-20

= = = = = = = = = = = = = = = = = = = =
                        

        致
礼!
 
                                 
        hlren
[EMAIL PROTECTED]
          2006-08-20

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