Brevia

Directionally Controlled Fluorescence Emission in Butterflies

See allHide authors and affiliations

Science  18 Nov 2005:
Vol. 310, Issue 5751, pp. 1151
DOI: 10.1126/science.1116612

Abstract

Recently developed, high-efficiency, light-emitting diodes use two-dimensional photonic crystals to enhance the extraction of otherwise internally trapped light and multilayer reflectors to control the direction of light emission. This work describes the characterization of a naturally evolved light-extraction system on the wing scales of a small group of Papilio butterflies. The efficient extraction of fluorescence from these scales is facilitated by a two-dimensional photonic crystal slab that uses a multilayer to help control emission direction. Its light-extraction function is analogous to that of the light-emitting diode.

In synthetic optical emitters such as lightemitting diodes (LEDs), the majority of generated light is trapped internally. Recently developed high-efficiency devices, however, use two-dimensional (2D) photonic-crystal geometries to enhance the extraction efficiency of light, and the devices also use distributed Bragg reflectors (DBRs) to control emission direction. Here we detail the elaborate optical emission system on the wing scales of a small group of butterflies. Their scales comprise a pigment-infused 2D photonic crystal that provides intense directed fluorescence, which is directionally enhanced by a DBR. This biological system shares many design features with high-emission LEDs.

Swallowtail (Papilio) butterflies in the Princeps nireus group, which are endemic to eastern and central Africa, have dark wings with bright blue or blue-green dorsal wing bands or patches (fig. S1). The wing scales from their colored regions make up a nanostructure that is characterized by a ∼2-μm-thick 2D photonic crystal slab (PCS) of hollow air cylinders in a medium of solid cuticle (Fig. 1, A and B). The cylinders have a mean diameter of ∼240 nm and a spacing of ∼340 nm. The PCS rests parallel to and ∼1.5 μm above a three-layer, cuticle-based DBR, which forms the base of the scale (fig. S2). Highly fluorescent pigment is infused exclusively throughout the PCS; its peak emission wavelength is ∼505 nm, depending on species, with peak excitation at ∼420 nm (fig. S3). The arrangement of air cylinders within the PCS is quasiperiodic, made up of domains of triangular symmetry over a range exceeding several lattice constants (fig. S4A). Two-dimensional Fourier transforms of this structure confirm such quasiperiodicity, revealing a single principal component of spatial variation in refractive index (fig. S4B). This demonstrates the inplane directional independence with which this PCS scatters light.

Fig. 1.

(A) Scanning electron microscope image of the PCS in the P. nireus colored scale showing fractured air cylinder edges. Scale bar, 1 μm. (B) Transmission electron microscope image of a section through a P. nireus colored scale, taken at a small angle to the plane of the PCS. Scale bar, 1 μm. (C) Band diagram of P. nireus intradomain PCS structure (the horizontal bar at 505 nm represents fluorescence emission full width at half maximum).

Because photonic band diagrams indicate all possible electromagnetic scattering interactions in periodic systems, we calculated the photonic band structure for the idealized intradomain triangular symmetry in this crystal. We found that the peak fluorescence emission lies across a frequency band in which the density of accessible optical states is significantly depleted, i.e., the pseudo-gap region (Fig. 1C). This finding indicates that the 2D photonic crystal inhibits emission in the crystal plane and thereby increases its out-of-plane emission. To verify this, fluorescence emission was measured both with and without specimen immersion in index-matching fluid (immersion effectively removes the nanostructure's photonic influence). Time-resolved analysis yielded the fluorescence decay rate and the explicit influence of the PCS. Because decay rate depends on the local density of optical states (LDOS) (described by Fermi's Golden Rule), the immersion of a fluorescent photonic crystal in matching fluid will change the LDOS and, subsequently, the fluorescence lifetimes [previously demonstrated in synthetic photonic crystals (1)]. We found that immersion in matching fluids considerably modified the decay lifetime of fluorescent emission from the butterfly wing scales, principally around the peak emission wavelength. The primary decay lifetime increased from 0.43 to 0.58 ns in the case of Papilio nireus (fig. S5).

As in ultra–high-efficiency LEDs (2), these butterflies' DBRs support a spectral stop band that matches the peak emission from the structure above it. The DBRs reflect upwardly the downward-emitted fluorescence concurrently with nonabsorbed longer wavelengths pass through the PCS. The spatial separation between the DBR and PCS minimizes losses via coupling to guided modes in the DBR.

Excitation for this fluorescent material appears to be optimized for the radiance from blue skylight, which peaks around 420 nm. Additionally, because the α-absorbance band of rhodopsin (3) dominates the green wavelength photosensitivity of Papilio vision, the spectral form of this absorption is ideally placed for stimulation by fluorescence from conspecific wings (fig. S3). As with some shrimps (4) and birds (5), this enhances signaling, because absorption of visually less-productive short wavelengths leads to the emission of longer wavelengths that trigger photoreception.

Supporting Online Material

www.sciencemag.org/cgi/content/full/310/5751/1151/DC1

Figs. S1 to S5

References

References

View Abstract

Navigate This Article