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Pendellosung effect in photonic crystals

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Pendell¨o sung effect in photonic crystals S.Savo 1,E.Di Gennaro 1,https://www.wendangku.net/doc/162866801.html,etto 1,A.Andreone 1,P.Dardano 2,L.Moretti 2,3,V .Mocella 21CNISM and Department of Physics,Universit `a di Napoli “Federico II”,Piazzale Tecchio 80,I-80125Naples,ITALY 2IMM -CNR,Sezione di Napoli,via P .Castellino 111,I-80131Naples,ITALY 3DIMET -University ”Mediterranea”of Reggio Calabria Localit Feo di Vito,I-89100Reggio Calabria (Italy)emiliano.digennaro@na.infn.it References and links 1.P.P.Ewald,“Zur Theorie der Interferenzen der R¨o ntgenstrahlen,”Physik Z.14,465(1913).2.P.P.Ewald,“Crystal optics for visible light and X rays,”Rev.Mod.Phys.37,46(1965).3. A.Authier,Dynamical Theory of X-ray Diffraction (Oxford University Press,Oxford,2001).4.N.Kato and https://www.wendangku.net/doc/162866801.html,ng,“The projection topograph:a new method in X-ray diffraction microradiography,”Acta Cryst.12,249(1959).5. D.Sippel,K.Kleinstu,and G.E.R.Schulze,“Pendell¨o sungs-interferenzen mit thermischen neutronen an Si-einkristallen,”Phys.Lett.14,174(1965).6. C.G.Shull,“Observation of Pendell¨o sung Fringe Structure in Neutron Diffraction,”Phys.Rev.Lett.21,1585(1968).7.V .Mocella,J.Hrtwig,J.Baruchel,and A.Mazuelas,“In?uence of the transverse and longitudinal coherence in dynamical theory of X-ray diffraction,”J.Phys.D:Appl.Phys.32,A88(1999).8.M.Born,Athomtheorie des festen Zustandes (Springer,Berlin,1923).9.V .Mocella,“Negative refraction in Photonic Crystals:thickness dependence and Pendell¨o sung phenomenon,”Opt.Express 13,1361(2005).

10. A.Balestreri,L.C.Andreani,and M.Agio,“Optical properties and diffraction effects in opal photonic crystals,”Phys.Rev.E 74,036,603(2006).

11.O.Francescangeli,S.Melone,and R.D.Leo,“Dynamical diffraction of microwaves by periodic dielectric me-dia,”Phys.Rev.A 40,4988(1989).

12.M.L.Calvo,P.Cheben,O.Martnez-Matos,F.del Monte,and J.A.Rodrigo,“Experimental Detection of the Optical Pendell¨o sung Effect,”Phys.Rev.Lett.97,084,801(2006).

13.V .Mocella,P.Dardano,L.Moretti,and I.Rendina,“A polarizing beam splitter using negative refraction of photonic crystals,”Opt.Express 13,7699(2005).

14.N.Kato,“The determination of structure factors by means of Pendell¨o sung fringes,”Acta Cryst.A25,119(1969)

1.Introduction

Since the original formulation of the diffraction theory from Ewald[1],the Pendell¨o sung effect was predicted as a periodic exchange of energy between interfering wave-?elds.The German term comes from the formal analogy between the mechanical system composed by coupled pendula and the optical problem,where many waves contribute to the optical?eld.In this formal analogy pendulum is the counterpart of wave whereas the temporal dependence of the mechanical problem corresponds to the spatial dependence in the considered optical problem [2].Pendell¨o sung is a relatively well known effect of Dynamical Diffraction Theory(DDT),a rigorous formalism accounting for multiple scattering effects that are especially important in X-ray,electron and neutron diffraction from perfect crystals[3].The requirement of high quality crystals explains why the?rst experimental observation of the Pendell¨o sung effect has been obtained in1959only in X-ray measurements[4],and some years later in neutron diffraction[5, 6].Recently,using the coherence of third generation synchrotron beams,Pendell¨o sung fringes produced by a plane wave exiting a Si crystal have been recorded[7].

Photonic crystals(PhCs)are arti?cial periodic structures reproducing natural crystals at dif-ferent length scale.PhCs can control and manipulate the?ow of light in many different ways, since they exhibit a variety of properties,spanning from full photonic band gap to anomalous dispersion phenomena,including superprism and negative refraction effects.The wide range of characteristics shown by PhCs gave rise in the last decade to a multitude of new ideas for opto-electronic integrated devices and systems.Novel concepts of mirrors,waveguides,resonators, and frequency converters based on photonic crystals,to mention a few examples,have been proposed.Indeed,the band theory of the electrons in solids,that is usually the main reference of the PhC theory,is strongly inspired by DDT(as extensively discussed in the pioneering Born’s solid state textbook[8]),that represents one of the?rst example of two-state theory-later became very popular in modern physics-such as up and down spins,electron and hole pairs,etc.

It is not surprising therefore that the Pendell¨o sung effect has been predicted for photonic crystals too.In2D case,it has been thoroughly studied using both analytical and numerical methods as a function of the PhC contrast index,beam incident angle,and light polarization [9].Moreover,this study has been extended to opal3D photonic crystals,where the dependence of diffraction intensity as a function of the layers number has been investigated using a scatte-ring matrix approach[10].On the experimental side the properties of microwave diffraction in periodic structures have been reported in literature by measuring the pattern of backscattered waves in two dimensional arti?cial dielectric media[11].Recently,the Pendell¨o sung effect has been detected also in the optical regime in volume holographic gratings,observing the oscilla-tory behavior of the angular selectivity of the diffracted light[12].

In this work,we present an accurate theoretical study and precise measurements of the Pen-dell¨o sung effect in photonic crystals by illuminating with a plane waves beam in the microwave region2D square lattice PhCs having different number of rows(i.e.slabs with different thick-nesses)and detecting the electromagnetic?eld inside and outside each slab.We show that under particular conditions the intensity of the diffracted wave at the exit surface can be periodically modulated with the slab thickness,presenting a maximum in the”positive”(forward diffracted) or in the”negative”(diffracted)direction.Moreover,we observe that inside the crystal the en-ergy is periodically exchanged between direct and diffracted beams.

2.Theoretical analysis

The Pendell¨o sung effect in PhCs can be understood as a beating phenomenon due to the phase modulation between coexisting plane wave components,propagating in the same direction.The coexistence is possible because such wavevectors are associated to two adjacent bands that are

overlapped,for a given frequency,in correspondence of suitably chosen PhC parameters.

X F r e q u e n c y (ωa /2πc =a /λ)Fig.1.The band structure of the square-lattice PhC for the T E polarization.The red line

represents the normalized frequency ωn =0.722at which the Pendell¨o sung effect takes

place (colour online).

In our case the 2D PhC consists of dielectric cylinders in air (dielectric permittivity εr =8.6)arranged in a square geometry and having r /a =0.255,where r is the cylinder radius and a is the lattice constant.If T E polarization (electric ?eld parallel to the rods axis)is considered,an overlap occurs between the forth and the ?fth mode for a normalized frequency ωn =νa /c =a /λ=0.722,as shown in Fig.1.Moreover,the crystal orientation is ?xed such that the normal at its surface is along the XM direction.Hence all possible wavevectors excited into the PhC will have the same tangential component lying on XM .

The Pendell¨o sung phenomenon is analyzed in this context for an incident wavevector that satis?es the Bragg law [9,13].In Fig.2we show in the reciprocal space the ?rst Brillouin zone and the corresponding symmetry points for the square lattice PhC under study.Considering the reciprocal lattice vector that enforces the momentum conservation oriented along ΓX in the ?rst Brillouin zone,the Bragg law is ful?lled when the projection of the incident wavevector coincides with ΓX ,so that k h is the diffracted wavevector whereas k i is the incident https://www.wendangku.net/doc/162866801.html,ing the dispersion surfaces (or Equi-Frequency Surfaces,EFSs),that represent the loci of propagat-ing wavevectors for a ?xed frequency,we are then able to evaluate the relevant parameters of the beating effect.The wavevectors inside the PhC are determined by the intersection between each EFS and the XM direction.Amongst the different intersections,only wavevectors having group velocity oriented inside the crystal -in Fig.2in opposite direction respect to the external normal to the incident surface -will be effectively excited.

Consider for instance the contribution of the incident wave:there is an interference between two excited components,with the respective wavevectors pointing in two different directions.This produces a spatial periodic modulation along the wavevectors difference vector ?k .The modulation distance in the real space along the PhC normal direction is therefore Λ0=2π/?k .The same effect occurs also for the diffracted wave,giving rise to a spatial modulation with the same length but 180?out-of-phase in respect to the previous case.

Fig.2.The reciprocal space with the?rst Brillouin zone(dotted line)and symmetry points

for the square-lattice PhC.The contours for the normalized frequencyωn=0.722are plot-

ted.Arrows indicate the directions of group velocity v g,whereas?n shows the normal to the

incident surface(colour online).

As a consequence of the Pendell¨o sung effect,the intensity I at the exit surface is harmon-ically modulated as a function of the thickness t[9].When t is an even multiple of half the Pendell¨o sung distance,the beam at the exit surface is parallel to the incident beam,forming a positive angle respect to the PhC normal.On the other hand,when t is an odd multiple ofΛ0 the beam at the exit surface is completely directed along the Bragg diffracted direction,forming a negative angle respect to the PhC normal.Denoting by+and-the two possible directions at the exit surface,this is summarized by:

t=2m

2?max(I?)

(1)

where m=1,2,....

Forcing the Pendell¨o sung distanceΛ0be an even number of the lattice constant a,eq.(1)holds for any number n of PhC rows.In particular,Λ0=4a ensures that the intensity maxima of the exit waves changes periodically if n is even,and that the energy beam equally splits between positive and negative direction if n is odd.

From the EFSs analysis,assuming a TE polarization,we found that an angleθi=43.8?and a normalized frequencyωn=0.722for the incident wave satisfy both the Bragg law and the peculiar conditionΛ0=4a.

3.Experimental setup

The experimental results are obtained on2D PhCs having a different number of rows inserted in a waveguide.First,the electromagnetic wave transmitted by the periodic structure is measured at the exit of the PhC for different crystal thickness and its spatial distribution is shown.Then, the periodic modulation of the intensity of the diffracted waves with respect to n is reported.

Finally,a comparison along selected directions inside the photonic crystal between the elec-tric?eld distribution measured and simulated using a Finite Difference Time Domain(FDTD) method is presented.

Measurements are carried out by placing alumina rods with nominal permittivityεr=8.6, radius r=0.4cm and height h=1cm in a square geometry with r/a=0.255(a=1.57cm) sandwiched in an aluminum parallel-plate waveguide terminated with microwave absorbers. Since the loss tangent of alumina is extremely small at the frequency relevant for this work (tanδ<10?4),dielectric losses can be neglected.Due to the presence of metallic plates acting as mirrors,current lines that are perpendicular to the plates can be considered as in?nitely long, as stated by the well-known mirror theorem.For the same reason the electric?elds produced by these currents are constant along the same direction and thus the whole system acts as a2D structure.

The microwave photonic crystal is built in the shape of a38.5cm wide slab(25rod columns), with a thickness that can be varied adding or removing rows.A dipole antenna is used as source, oriented to produce an electric?eld parallel to the rods axis and operating at the frequency of 13.784GHz,in order to reproduce the same normalized frequency a/λof the theoretical model. Due to the waveguide characteristics,the TEM mode only can propagate up to15GHz.The maps of the real part of the electric?eld are collected by using a HP8720C Vector Network Analyzer and another dipole antenna as a detector,that moves along the waveguide plane using an x-y step motor.The thickness dependence has been investigated based on the observation of the beams at the exit of the crystal-air interface.We focused our analysis on structures with a number of rows n ranging from1to10.

Fig.3.Schematic layout of the experiment carried out on the square-lattice PhC slab hav-

ing25rods columns and a number of rows n varying from10to1.The dashed line box

represents the scanned area during the measurements(colour online).

Fig.3shows the scheme of the measurement.Particular attention has been paid to the source characteristics.The incident beam has to be as collimated and directive as possible,ideally consisting of a single wavevector only.To realize the experiment,we inserted in the parallel plate waveguide two parallel microwave absorber stripes,having the role to”guide”the elec-tromagnetic wave.The channel is50cm long and10cm wide,with tapered sidewalls in order

to ensure a good matching condition at the air-to-absorber interface.The?eld generated by the dipole source is centered into the absorbers channel.To limit the diffraction at the exit of the waveguide,a phenomenon that strongly reduces the beam directivity,the channel section closer to the PhC interface has been shaped into a triangular pro?le.All these solutions provide a beam source having transmission properties close to ideal ones.

The incoming beam is then oriented at43.8?respect to the normal to the PhC interface, whereas the two arrows exiting the surface in both the forward diffracted and diffracted direc-tions represent the signals transmitted through the wave guide and the crystal.Furthermore, the angle that describes the outcoming waves is the same as the source.In the image plane,a tiny dipole antenna(radius～0.6mm)scans an area20cm long and40cm wide contiguous to the crystal-air interface,in steps of4mm in both x and y direction.As said before,for a?xed frequency and source orientation the intensities I+and I?reach a maximum or a minimum value depending on the difference between the wavevectors inside the crystal and,in turn,on the crystal thickness.

4.Results and discussion

In Fig.4(a)-(e)the real part of the electric?eld experimentally detected in different crystal con?gurations is mapped in the image plane,using a normalized scale.In Fig.4(a)the spatial distribution is shown for the case n=10.The maps for the other cases of crystals with an even number of rows(n=8,6,4,2)are presented in Figs.4(b),(c),(d),(e),respectively.Starting

Fig.4.(a)-(e):mapping of the measured electric?eld(real part)in a normalized scale for

even n;(f)-(j):mapping of the measured electric?eld(real part)in a normalized scale for

odd n(colour online).

the data analysis from the crystal consisting of10rows,that is an odd multiple ofΛ0/2,in this case the beam,as expected,is fully transmitted in the diffracted direction.On the contrary, when the PhC consists of8rows,the beam exits its surface in the forward diffracted direction (Fig.4(b)).By reducing the thickness down to2rows for any even n,the transmitted beam alternatively bends from the negative to the positive direction,as shown in Figs.4(c)-(e).Other

beams related to higher order of diffraction are negligible.Measurements clearly show therefore that for an even number of rows the involved energy is almost entirely concentrated along one exit direction only.It is also clear from the images that the transmitted?eld propagates along regular and periodic equiphase planes,in agreement with numerical simulations.

Let us now analyze the experimental results for crystals having an odd number of rows.In this case,according to the periodical modulation predicted for the?eld intensity at the exit surface, the thickness is such that at the crystal-air interface the transmitted energy is equally divided in both positive and negative directions.This is shown in Fig.4(f)-(j):the electromagnetic beam in the image plane actually splits in two rays having approximately the same intensity, with equiphase planes clearly evident in both directions.It is worth noting that the case with n=1(Fig.4(j))reduces to the well known Bragg grating.The fundamental feature of the Pendell¨o sung effect is the spatial periodic modulation of the transmitted?eld amplitude with the crystal thickness.

Fig.5.The measured electric?eld intensity ratio I?/I+for all the crystal con?gurations

considered.The case of10rows corresponds to the maximum thickness t=(10a+2r)=

16.4cm.

We then compared the electric?eld maximum intensity measured along the two different (positive and negative)transmitted directions as a function of the photonic crystal row number n(thickness).As shown in the Fig.5using a semi-log scale,the intensity ratio I?/I+changes periodically,being approximately equal to1for any odd n,and exhibiting pronounced maxima and minima alternatively for any even n.

We also evaluated the electromagnetic?eld distribution inside the PhC slab.FDTD simu-lations are performed considering a plane monochromatic incident wave having a rectangular transverse pro?le.The propagation in the slab is of course well different from that in free-space since Bloch modes will be excited and therefore a strong modulation of the electromagnetic ?eld is expected.In particular,in the Pendell¨o sung phenomenon,the positively and negatively refracted components of the incident wave interfere each other inside the crystal and give rise to a periodic exchange of energy.This translates in a spatial modulation of the?eld intensity, as it can be clearly seen when the dielectric contrast is not very high[13].

In the case discussed here the strong Bloch modulation makes the visualization of the wave pattern quite dif?cult.Moreover,when the contrast is high,the intensity maxima inside the rods mask the distribution in the outside region.Therefore,for the sake of clarity,we have suppressed

the?eld inside the dielectrics.Results are shown in Fig.6(a).It is worth mentioning that the spatial modulation observed in the crystal does not affect the energy direction,which remains normal to the PhC interface.To compare the numerical simulations with experimental data we have then measured the internal?eld along selected directions normal to the PhC interface. Particular attention has been paid to ensure that the detector antenna moves perfectly parallel to the dielectric rods.

Fig.6.(a)FDTD simulation of the propagation pattern inside a crystal consisting of10

rows of the13.784GHz plane wave modulated by a rectangular pro?le and incident at an

angle of43.8?across the XM interface;(b)&(c):electric?eld intensity distribution(blue

dashed lines)along line1and2respectively compared with the experimental results(red

solid lines)(colour online).

Figures6(b)and6(c)shows the simulated longitudinal pro?le of the?eld intensity along two different lines,(1)and(2)respectively,and the corresponding experimental results properly rescaled.In spite of the strong?eld modulation,the presence of peaks and valleys centered in different positions along the PhC normal direction and corresponding to different minima and maxima in the wave energy on the two longitudinal lines is evident,as expected by the theory. Besides that,the decrease in the intensity as far as the electromagnetic wave propagates inside the crystal re?ects the energy radiated from the?nite-size PhC.This can be also observed in Fig.6(a).

5.Conclusion

We have designed and realized an experiment to measure the Pendell¨o sung effect in PhCs, where two beams are180?out of phase each other,giving rise to the effect of energy?ow swapping back and forth between two different directions into the crystal.Pendell¨o sung can be in principle exploited to design a new kind of photonic crystal based devices.In a previous paper,it has been suggested that this effect can be used to realize a passive polarising beam splitter[13].In the case presented here,we have shown that adding or removing rows in a?nite thickness2D PhC can dramatically change the direction and the features of the electromagnetic wave transmitted through the slab.Data are in a very good agreement with calculations based

on the classical approach of the Dynamical Diffraction Theory,showing that this rigorous for-malism can be successfully applied to predict some anomalous features exhibited by PhCs.In particular,we underline that the Pendell¨o sung effect has been extensively used for the accurate determination of the structure factors in real crystals[14].It can be extremely useful in photonic crystals too,allowing precise measurements of some peculiar properties such as the dielectric contrast.

Acknowledgement

This work has been partially funded by MIUR under the PRIN-2006grant on”Study and real-ization of metamaterials for electronics and TLC applications”.