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Micro/Nano Lithography

A biomolecular light-emitting diode

An LED fabricated with biomolecular materials may signal the start of biomolecular electronics.
31 November 2006, SPIE Newsroom. DOI: 10.1117/2.1200609.0316

Light-emitting diodes (LEDs) have become key components of numeric and alphanumeric display technology. The most common are p–n-junction diodes fabricated from inorganic semiconductors. In the past decades, nanotechnology advances gave rise to a new type of LED, the organic light-emitting diode (OLED), a prototype of which was first fabricated by Vincett et al.1 OLED displays with small screens are now commercially available.

In the basic OLED design, a thin film of highly phosphorescent or fluorescent material is sandwiched between various types of metal electrode. These light-emitting materials are also especially designed for efficient charge injection from the electrodes. In this context, questions come to mind with no textbook to provide answers. What kind of organic materials can be used to fabricate OLEDs? Can we make them using common bio-functional materials?

Our work has allowed to provide answers in that we have recently succeeded in fabricating the first biomolecular light-emitting diode (BIODE).2 We decided to use metalloporphyrins and related biomolecules—such as cytochrome c,2–4 myoglobin,3 hemin,5 and chlorophyll a.6—for this purpose. Cytochrome c and myoglobin are known as heme proteins because their active site consists of an iron-porphyrin, called a heme (shown in Figure 1). In living systems, cytochromes are electron carriers, while myoglobin transports and stores oxygen. Chlorophyll a is the well-known photosynthetic pigment and hemin is the ferric oxidation product of heme. Except for chlorophyll a, these molecules exhibit no photoluminescence. We were, accordingly, greatly surprised to observe current flow and electroluminescence in all BIODE devices fabricated using them.

Figure 1. Shown is the molecular structure of heme, a porphyrin macrocycle coordinated to iron and found in many heme proteins.

Figure 2 shows a schematic illustration of a BIODE. The device is a simple sandwich-type junction. We did not prepare carrier-transport layers, as done in most OLEDs, to balance the density of electrons and holes. This is because we wanted to exclude light emission from the transport layers to observe the intrinsic emission of our biomolecules. The observed electroluminescence spectra were broad but consistent with the absorption spectra. The quantum efficiencies of the fabricated devices were 4 × 10-7 at most (in the case of a hemin BIODE 6), thus significantly lower than those of commercially available devices. However, one of the reasons for their small quantum efficiencies was their lack of transport layers.

Figure 2. Shown is a schematic illustration of a biomolecular light-emitting diode. The image at the lower right bottom is the emission of a cytochrome c device measured using a CCD detector.

As for observing electroluminescence in compounds that did not exhibit photoluminescence, our interpretation was to attribute the phenomenon to different excitation states in the electroluminescence and photoluminescence processes. In the case of electroluminescence, carriers are injected directly into d-orbitals whose energy levels are close to those of electrodes. On the other hand, photoexcitation produces electron-hole pairs in the π and π* orbitals. Therefore, d electrons (or d holes) are hardly formed in photoluminescence, since the probability of d – π and d – π* transitions are quite small.4

Figure 3 shows the drastic changes observed in the electroluminescence spectrum of hemin under applied voltages.6 On the basis of magnetic susceptibility and Raman measurements, we concluded that these changes resulted from the high-spin to low-spin transition of the iron. Since the spin state of the heme iron is associated with various bio-functionalities, this phenomenon is of significant interest. Although the transition is irreversible, reversibility may be induced by chemical modification of hemin. Such a transition could be applied to the design of new biosensors.

Figure 3. Shown is a voltage-induced transition of hemin. The red and blue curves illustrate the electroluminescence spectra in the low- and high-voltage states, respectively.

Biomolecular compounds have a wide range of functionalities. If we can learn to use them in electric devices, we may decrease environmental pollution and realize more eco-friendly technologies for the future. Our BIODE studies are a first step towards such a dream.

Hiroyuki Tajima,  Masaki Matsuda, Shingo Ikeda
Institute for Solid State Physics, University of Tokyo
Kashiwa, Chiba, Japan

Professor Tajima is a physical chemist specializing in optical and electrical measurements. Currently, his research effort is focused on molecular devices.

Dr. Matsuda has been studying molecular materials based on metal complexes. He has been designing, synthesizing and exploring related new materials.

Dr. Ikeda acquired his PhD in organic photochemistry. He is currently involved in photolithography and impedance-spectroscopy measurements.