Abstract. We investigated photoluminescence (PL) from one-dimensional photonic band gap structures. The photonic crystals, a Fabry-Perot (FP) resonator and a coupledmicrocavity (CMC) structure, were fabricated by using alternating hydrogenated amorphous-silicon-nitride and hydrogenated amorphous-silicon-oxide layers. It was observed that these structures strongly modify the PL spectra from optically active amorphous-silicon-nitride thin films. Narrow-band and wide-band PL spectra were achieved in the FP microcavity and the CMC structure, respectively. The angle dependence of PL peak of the FP resonator was also investigated. We also observed that the spontaneous emission increased drastically at the coupled-cavity band edge of the CMC structure due to extremely low group velocity and long photon lifetime. The measurements agree well with the transfer-matrix method results and the prediction of the tight-binding approximation. 42.70.Qs; 42.60.Da;78.66.Jg Ability to control spontaneous emission is expected to have practical importance in certain commercial applications. Thus, in the past decade, photonic band gap materials were proposed for alteration (inhibition and enhancement) of the spontaneous emission from atoms [1][2][3][4][5][6][7][8][9][10][11][12][13][14].
PACS:Recently, we reported a new type of propagation mechanism in which photons move along the localized coupledcavity modes [15,16]. Moreover, it was observed that the group velocity tends to zero and photon lifetime increases drastically at the coupled-cavity band edges [17]. In this paper, we experimentally demonstrate the modification of spontaneous emission from the hydrogenated amorphous-siliconnitride active layers in a Fabry-Perot (FP) resonator and a coupled-microcavity (CMC) structure.Since the density of electromagnetic modes (ω) is modified by the surrounding environments, the spontaneous emission from atoms can be controlled by placing the atoms inside * Corresponding author. (Fax: +90-312/266-4579, E-mail: bayindir@fen.bilkent.edu.tr) cavities. The spontaneous emission rate is directly proportional to the photon density of modes via Fermi's golden rule:. Thus, it is expected that spontaneous emission from a CMC structure can be enhanced by a low group velocity.Our structures were composed of alternating hydrogenated amorphous-silicon-nitride (Si 3 N 4 ) and hydrogenated amorphous-silicon-oxide (SiO 2 ) multilayers [18]. The SiO 2 and Si 3 N 4 layers were deposited on glass and silicon substrates by plasma-enhanced chemical vapour deposition (PECVD) at 250• C. Nitrogen (N 2 ) balanced 2% silane (SiH 4 ), pure ammonia (NH 3 ) and nitrous oxide (N 2 O) were used as the silicon, nitride and oxide sources, respectively. The refractive indices and thicknesses of layers were n SiO 2 = 1.46, n