×The lasing threshold of a microcavity is mainly determined by the spontaneous emission factor β, which is
inversely proportional to the mode volume Vc. We demonstrate an experimental way to decrease the mode
volume via lateral structuring of the microcavity. This redistributes both number and density of the transversal
cavity modes, which increases the amplitude of the internal electromagnetic field. Our samples are microcavities
with an active layer of variable thickness (0.2 to 2 μm) made of tris-(8-hydroxyquinoline) aluminium (Alq3) doped
with 4-(dicyanomethylene)-2- methyl-6-(p-dimethylaminostyryl)-4H-pyran (DCM). With thermal coevaporation
through a shadow mask, this layer is structured into an array of photonic boxes square-shaped microcavities with
an area of 55 μm2. Using a microscope objective, we record the spatial distribution of the cavity transmission
spectra with submicron resolution. The modes of the photonic boxes show a clear discretization, which is due
to the multidimensional optical confinement. Under selective excitation of the DCM molecules via a focused
pulsed laser (532 nm, 1.5 ns, 2 kHz , &diameter; ≈ 3μm), we record the spatially and spectrally resolved emission of
single photonic boxes. The laser pulse energy is varied to obtain input-output curves of the cavity modes. At
an excitation energy of ~30 pJ, we observe superlinear growth as well as a spectral narrowing of the emission
from the lowest energy mode of a single photonic box. For this lasing transition, we determine a spontaneous
emission factor β of ≈0.01.
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