Emission of Electromagnetic Radiation and Control of the Properties of the Emitted Electromagnetic Radiation

Abstract

Provided is a device for emitting electromagnetic radiation. The device includes a first electrode, a second electrode, and an exciton recombination layer extending from the first electrode to the second electrode. The device is configured to relocate a recombination zone in the exciton recombination layer by changing an electric field between the first electrode and the second electrode, or to emit electromagnetic radiation through a transparent substrate.

Claims

1. A device for emitting electromagnetic radiation, comprising: a first electrode; a second electrode; and an exciton recombination layer extending from the first electrode to the second electrode; wherein the device is configured to relocate a recombination zone in the exciton recombination layer by changing an electric field between the first electrode and the second electrode.

2. The device of claim 1, wherein the device is configured to relocate the recombination zone by reversing a polarity of the first and second electrodes.

3. The device of claim 1, wherein the first electrode causes a first electromagnetic radiation spectrum if the relocated recombination zone couples to the first electrode and the second electrode causes a second electromagnetic radiation spectrum if the relocated recombination zone couples to the second electrode, wherein the first spectrum and the second spectrum differ.

4. The device of claim 3, where the first electrode is configured to serve as a first optical antenna if the relocated recombination zone couples to the first electrode and the second electrode is configured to serve as a second optical antenna if the relocated recombination zone couples to the second electrode, wherein the first optical antenna and the second optical antenna differ in shape and/or orientation.

5. The device of claim 4, wherein the first optical antenna and the second optical antenna differ in directivity and/or polarization.

6. The device of claim 4, wherein a size of the first optical antenna is below 1 μm and a size of the second optical antenna is below 1 μm.

7. The device of claim 1, wherein a material of the exciton recombination layer allows either for higher hole mobility than electron mobility or for higher electron mobility than hole mobility.

8. The device of claim 1, wherein a barrier between the electrodes and the exciton recombination layer allows either for higher hole injectability than electron injectability or for higher electron injectability than hole injectability.

9. The device of claim 1, wherein the device is configured to control a radial intensity distribution of the electromagnetic radiation based on a voltage difference between the first electrode and the second electrode.

10. The device of claim 1, further comprising: a third electrode; wherein the device is configured to relocate the recombination zone in the exciton recombination layer by changing the electric field between the first electrode, the second electrode, and the third electrode.

11. The device of claim 1, further comprising: a transparent substrate; wherein the first and second electrodes are formed on the transparent substrate.

12. The device of claim 11, wherein the device is a display or an optical communication device.

13. A device for emitting electromagnetic radiation, comprising: a transparent substrate; a first electrode formed on the transparent substrate; a second electrode formed above the first electrode; and an exciton recombination layer between the first electrode to the second electrode; wherein the device is configured to emit the electromagnetic radiation through the transparent substrate.

14. A method of controlling properties of electromagnetic radiation, comprising deactivating a first optical antenna, of two, three or more optical antennas, and activating a second optical antenna, of the two, three or more optical antennas, by reversing a polarity of the first and second optical antennas which causes an exciton recombination zone in an exciton recombination layer extending from the first optical antenna to the second optical antenna to decouple from the first optical antenna and couple to the second optical antenna, wherein the first optical antenna emits electromagnetic radiation in a first spectrum and the second optical antenna emits electromagnetic radiation in a second spectrum which differs from the first spectrum and/or the first optical antenna and the second optical antenna lead to differences in directivity and/or polarization of the emitted electromagnetic radiation.

15. The method of controlling a spectrum of electromagnetic radiation of claim 14, wherein the two, three or more optical antennas form a pixel of a display.

Description

BRIEF DESCRIPTION OF DRAWINGS

[0040] The foregoing aspects and many of the attendant advantages will become more readily appreciated as the same become better understood by reference to the following description of embodiments, when taken in conjunction with the accompanying drawings, wherein like reference numerals refer to like parts throughout the various views, unless otherwise specified.

[0041] FIG. 1a and FIG. 1b illustrate relocating the recombination zone in an exciton recombination layer;

[0042] FIG. 2a and FIG. 2b illustrate decoupling the recombination zone from a first antenna and coupling the recombination zone to a second antenna and the related spectral shift;

[0043] FIG. 3 shows a top view and a cross-sectional view of a first exemplary embodiment of a device according to the present invention;

[0044] FIG. 4 shows a top view and a cross-sectional view of a second exemplary embodiment of a device according to the present invention;

[0045] FIG. 5 shows a top view and a cross-sectional view of a third exemplary embodiment of a device according to the present invention;

[0046] FIG. 6 shows a top view of a fourth exemplary embodiment of a device according to the present invention;

[0047] FIG. 7 shows a top view of a fifth exemplary embodiment of a device according to the present invention;

[0048] FIG. 8 shows a top view of a sixth exemplary embodiment of a device according to the present invention;

[0049] FIG. 9 shows a top view of a seventh exemplary embodiment of a device according to the present invention;

[0050] FIG. 10 shows a top view of an eighth exemplary embodiment of a device according to the present invention;

[0051] FIG. 11 shows a top view of a ninth exemplary embodiment of a device according to the present invention; and

[0052] FIG. 12 shows steps of a process for controlling properties of the electromagnetic radiation.

[0053] Notably, the drawings are not drawn to scale and unless otherwise indicated, they are merely intended to conceptually illustrate the structures and procedures described herein.

DESCRIPTION OF EMBODIMENTS

[0054] FIG. 1a shows device 10 comprising electrodes 12 and 14 and exciton recombination layer 16 which connects electrode 12 to electrode 14. Exciton recombination layer 16 may be formed from a transition metal dichalcogenide (TMDC) monolayer or an organic semiconductor material such as self-assembled monolayers, Zinc phthalocyanine (ZnPc), etc. The organic semiconductor material may be deposited by thermal evaporation (generating a 20 nm to 40 nm thick weakly absorbing homogeneous layer) after electrode 12 and electrode 14 have been formed on a (transparent) substrate 10a.

[0055] When a voltage applied to electrode 12 and electrode 14 is above a threshold, electrons and holes may be injected into exciton recombination layer 16. The injected electrons and holes may recombine and decay within recombination zone 18, causing the emission of electromagnetic radiation 20. If electron mobility and hole mobility differ (substantially), recombination zone 18 may be closer to one of electrodes 12 and 14, and farther away from the other one of electrodes 12 and 14.

[0056] In FIG. 1a, the electron mobility may be lower than the hole mobility and electrode 12 may have a higher electric potential than electrode 14, or the electron mobility may be lower than the hole mobility and electrode 12 may have a lower electric potential than electrode 14. In FIG. 1b, the electron mobility may be lower than the hole mobility and electrode 12 may have a lower electric potential than electrode 14, or the electron mobility may be lower than the hole mobility and electrode 12 may have a higher electric potential than electrode 14.

[0057] As illustrated by FIG. 1a and FIG. 1b, the directivity of the emission may be influenced by features (i.e., electrodes 12 and 14) in the vicinity of recombination zone 18. Likewise, the polarization and/or the spectrum of the emission may be influenced by features in the vicinity of recombination zone 18. Thus, the directivity, the polarization and/or the spectrum of electromagnetic radiation 20 may be controlled (to some extent) by relocating recombination zone 18 within exciton recombination layer 16, e.g., by moving recombination zone 18 towards or away from one of electrodes 12 and 14.

[0058] As illustrated in FIGS. 2a and 2b, electrodes 12 and 14 may be laterally arranged and parallelly oriented (nontransparent) nanostructures (e.g., nanorods) which differ (primarily) in size and which serve as (plasmonic) antennas 24 and 26. Antennas 24 and 26 may also differ (primarily) in shape and may be oriented along non-parallel axes. Depending on the polarity of the voltage applied to antennas 24 and 26, recombination zone 18 may couple selectively to either one of antennas 24 and 26.

[0059] As antennas 24 and 26 differ in size, the spectral and spatial emission characteristics, determined by the coupling of recombination zone 18 to the respective nearest antenna 24 or 26, depend on the polarity of the applied voltage. For example, when recombination zone 18 decouples from larger antenna 26 and couples to smaller antenna 24, the spectrum of electromagnetic radiation 20 may shift from spectrum 28a to spectrum 28b, i.e., electromagnetic radiation 20 may shift to smaller wavelengths. Likewise, when recombination zone 18 decouples from smaller antenna 24 and couples to larger antenna 26, the spectrum of electromagnetic radiation 20 may shift from spectrum 28b back to spectrum 28a, i.e., electromagnetic radiation 20 may shift to larger wavelengths.

[0060] Thus, reversing the polarity of the applied voltage may cause a spectral shift of electromagnetic radiation 20 which may be used, for example, to change a color of a pixel of a screen or to encode data. Moreover, reversing the polarity of the applied voltage may also cause a change in the directivity and/or the polarization of the emitted electromagnetic radiation 20. A change in the directivity may be used to switch between more focused and less focused electromagnetic radiation 20 or between different emission angles. As a result, electromagnetic radiation 20 may travel along different (optical) paths, a pixel may be made (more clearly) visible from different angles, electromagnetic radiation 20 may be coupled into different waveguides, etc.

[0061] Antennas 24 and 26 may be single-crystal electrically connected antennas which are fabricated by focused ion beam milling from single-crystal gold platelets. For example, antenna 24 and antenna 26 may be two horizontal gold bars of different lengths with resonances that overlap with a photoluminescence spectrum of the excitonic material but are sufficiently apart from each other to provide two distinguishable spectral signatures. The distance between antenna 24 and antenna 26 may be such that both resonances show no sign of hybridization.

[0062] Antenna 24 and antenna 26 may be connected to (relatively) large (gold) contact pads by (relatively) thin (gold) lines 30 and 32. The thin lines 30 and 32 may extend along symmetry axes of antenna 24 and antenna 26, respectively, to avoid any disturbance of the plasmon modes.

[0063] When applying a voltage (e.g., 10 V) to antenna 24 and antenna 26, the emission of electromagnetic radiation 20 may be observed in the form of a diffraction-limited spot localized at the position of the antenna pair. However, instead of a broadband emission generated by the resonances of both antennas 24 and 26, spectrum 28a and 28b of electromagnetic radiation 20 may depend (strongly) on the polarity of the applied voltage. For instance, spectrum 28a may have a peak at about 900 nm whereas spectrum 28b may have a peak at about 830 nm.

[0064] If the excitonic material is ZnPc, the polarity-dependent spectral shift may be due to the fact that ZnPc is a preferential hole conductor. This means that holes may propagate across the entire ZnPc layer without inducing radiative charge carrier recombination processes until they reach the vicinity of the antenna which injects electrons into exciton recombination layer 16. As the electrons may be injected (e.g., by tunneling or thermal activation) at a much lower efficiency across the Schottky barrier, excitons may be formed close to the antenna that serves as the cathode. In other words, the unequal electron and hole mobilities may lead to an asymmetric position of recombination zone 18 closer to the antenna which serves as the cathode.

[0065] Due to the proximity of a plasmonic antenna, the excitonic decay may be enhanced within the bandwidth of the respective antenna resonance which may lead to the excitation of antenna plasmons that efficiently decay into photons.

[0066] In addition to the changes of the spectrum caused by the polarity switching, there may also be changes in the emission pattern. The structure of antenna 24 and antenna 26 resembles that of a Yagi-Uda antenna with the additional feature that the active and the passive element can be interchanged by reversing the polarity. Thus, the directionality of electromagnetic radiation 20 may change as the polarity is switched. Without a reflector on top of antennas 24 and 26, the directivity may be beyond the critical angle of total internal reflection of transparent substrate 10a.

[0067] As illustrated in FIG. 3, antenna 24 and antenna 26 may be perpendicular to each other to allow for polarization switching. Moreover, as illustrated in FIG. 4, antenna 24 may be paired with counter electrode 14. Whenever recombination zone 18 couples to antenna 24, electromagnetic radiation 20 with a characteristic spectrum is being emitted. Whenever recombination zone 18 couples to electrode 14, electromagnetic radiation 20 with a different spectrum is being emitted.

[0068] As illustrated in FIG. 5, electrode 14 may be arranged above antenna 24 (with exciton recombination layer 16 being sandwiched by electrode 14 and antenna 24) and serve as a reflector. For example, electrode 14 may be a (gold) layer. The reflector may redirect the emitted electromagnetic radiation perpendicular to the layer. Notably, switching the directionality by reversing the polarity may be less pronounced if a reflector is used.

[0069] As illustrated in FIG. 6, device 10 may comprise more than two antennas 24, 26 and 34, which have different resonance lengths. For example, antennas 24, 26 and 34 may be used to realize a three-color single pixel (using an in-plane design as in FIG. 4). As shown in FIG. 7, electrode 36 may be arranged above antennas 24, 26 and 34 with exciton recombination layer 16 being sandwiched by electrode 36 and antennas 24, 26 and 34. The size S of electrode 36 may be about 3 μm to 4 μm. The widths W1, W2, and W3 of antennas 24, 26 and 34, respectively, may be between 100 nm and 400 nm.

[0070] As illustrated in FIG. 8, device 10 may comprise a column of antennas 24, 26, 34, and 38 that share electrode 36 which is arranged above the column and serves as a reflector (similar to the arrangement shown in FIG. 5). Exciton recombination layer 16 is arranged between electrode 36 and antennas 24, 26, 34, and 38. When a reflector is used, a substrate on which antennas 24, 26, 34 and 36 are deposited may be transparent. Instead of the stacked design shown in FIG. 8, an in-plane design may be used as illustrated in FIG. 9. In FIG. 10 and FIG. 11, multiple columns as those shown in FIG. 8 and FIG. 9, respectively, are placed side by side. The resulting matrices may be used to produce a display.

[0071] FIG. 12 shows a flow-chart of a process for controlling spectrum 28a and 28b of electromagnetic radiation 20. The process starts at step 40 emitting electromagnetic radiation 20 by antenna 26. At step 42, the process is continued with deactivating antenna 26 and activating antenna 24 by reversing the polarity of antennas 24 and 26 which causes recombination zone 18 in exciton recombination layer 16 to decouple from antenna 26 and couple to antenna 24, wherein optical antenna 26 emits electromagnetic radiation 20 with spectrum 28a and antenna 24 emits electromagnetic radiation 20 with spectrum 28b which differs from spectrum 28a. At step 44, the process concludes with emitting electromagnetic radiation 20 by antenna 24.

REFERENCE SIGNS LIST

[0072] 10 device

[0073] 10a substrate

[0074] 12 electrode

[0075] 14 electrode

[0076] 16 exciton recombination layer

[0077] 18 recombination zone

[0078] 20 electromagnetic radiation

[0079] 22 features

[0080] 24 antenna

[0081] 26 antenna

[0082] 28a spectrum

[0083] 28b spectrum

[0084] 30 line

[0085] 32 line

[0086] 34 antenna

[0087] 36 electrode

[0088] 38 antenna

[0089] 40 step

[0090] 42 step

[0091] 44 step