Experimental and theoretical evidence for the existence of photonic bandgaps and selective transmissions in serial loop structures

被引:61
作者
El Boudouti, EH [1 ]
Fettouhi, N
Akjouj, A
Djafari-Rouhani, B
Mir, A
Vasseur, JO
Dobrzynski, L
Zemmouri, J
机构
[1] Univ Mohamed I, Fac Sci, Dept Phys, Lab Dynam & Opt Mat, Oujda 60000, Morocco
[2] Univ Moulay Ismail, Fac Sci, Dept Phys, Meknes, Morocco
[3] Univ Lille 1, UFR Phys, CNRS,UMR 8024, EDI, F-59655 Villeneuve Dascq, France
[4] Univ Lille 1, UFR Phys, CNRS,UMR 8523, PHLAM, F-59655 Villeneuve Dascq, France
关键词
D O I
10.1063/1.1633983
中图分类号
O59 [应用物理学];
学科分类号
摘要
We have investigated the electromagnetic band structure, transmission, and phase time through a one-dimensional structure made of loops pasted together with segments of finite length. In this serial loop structure, the loops and segments are constituted of dielectric monomode materials. Analytic expressions are reported for the band structure for a large number N of loops and for transmission coefficients and phase times for any value of N. Experimental and numerical results show the existence of large gaps in these structures. These gaps originate both from the periodicity of the system and the loop resonant states that create zeroes of transmission. The gap widths depend on the lengths of the finite segment and the loop diameters. Defect modes may occur in these bandgaps by introducing defective segments in the structure. The localized states appear as very narrow peaks both in the transmission spectrum and in the transmission phase time of finite serial loop structures. The localized state behavior is analyzed as a function of the length and of the position of the defect segment. The transmission phase measurements enable us to derive the group velocity as well as the density of states in these structures. The experimental results are obtained using coaxial cables in the frequency range of few hundreds of MHz. (C) 2004 American Institute of Physics.
引用
收藏
页码:1102 / 1113
页数:12
相关论文
共 56 条
[1]   Surface and interface optical waves in superlattices: Transverse electric localized and resonant modes [J].
Bah, ML ;
Akjouj, A ;
ElBoudouti, EH ;
DjafariRouhani, B ;
Dobrzynski, L .
JOURNAL OF PHYSICS-CONDENSED MATTER, 1996, 8 (23) :4171-4188
[2]  
BAH ML, 1995, THESIS U LILLE 1
[3]   Heavy photons at coupled-cavity waveguide band edges in a three-dimensional photonic crystal [J].
Bayindir, M ;
Ozbay, E .
PHYSICAL REVIEW B, 2000, 62 (04) :R2247-R2250
[4]  
Brillouin L., 1960, WAVE PROPAGATION GRO
[5]   TRAVERSAL TIME FOR TUNNELING [J].
BUTTIKER, M ;
LANDAUER, R .
PHYSICAL REVIEW LETTERS, 1982, 49 (23) :1739-1742
[6]   LARMOR PRECESSION AND THE TRAVERSAL TIME FOR TUNNELING [J].
BUTTIKER, M .
PHYSICAL REVIEW B, 1983, 27 (10) :6178-6188
[7]   LINEAR PULSE-PROPAGATION IN AN ABSORBING MEDIUM [J].
CHU, S ;
WONG, S .
PHYSICAL REVIEW LETTERS, 1982, 48 (11) :738-741
[8]   Group velocity, energy velocity, and superluminal propagation in finite photonic band-gap structures [J].
D'Aguanno, G ;
Centini, M ;
Scalora, M ;
Sibilia, C ;
Bloemer, MJ ;
Bowden, CM ;
Haus, JW ;
Bertolotti, M .
PHYSICAL REVIEW E, 2001, 63 (03)
[9]   Superluminal group velocities and information transfer [J].
Diener, G .
PHYSICS LETTERS A, 1996, 223 (05) :327-331
[10]   INTERFACE RESPONSE THEORY OF CONTINUOUS COMPOSITE SYSTEMS [J].
DOBRZYNSKI, L .
SURFACE SCIENCE REPORTS, 1990, 11 (5-6) :139-178