The present disclosure relates to integrating microdevices into a system substrate.
According to one embodiment the present invention discloses a method to activate a microdevice with an electron beam, the method comprising, having the microdevice in a substrate, having an electron beam source, having at least one electrode of the microdevice biased by a second electrode or a probe, having at least one electrode a part of the biasing circuits in the substrate, and activating the microdevice passing the electron beam through a pad to the microdevice to at least one electrode.
The foregoing and other advantages of the disclosure will become apparent upon reading the following detailed description and upon reference to the drawings.
The present disclosure is susceptible to various modifications and alternative forms, specific embodiments or implementations have been shown by way of example in the drawings and will be described in detail herein. It should be understood, however, that the disclosure is not intended to be limited to the particular forms disclosed. Rather, the disclosure is to cover all modifications, equivalents, and alternatives falling within the spirit and scope of an invention as defined by the appended claims.
In this description, the term “device” and “microdevice” are used interchangeably. However, it is clear to one skilled in the art that the embodiments described here are independent of the device size.
To develop a system (display, sensors or other), microdevices are integrated into a system substrate.
Microdevices can be microLED or sensors or MEMS or OLEDs or etc. A system substrate consists of a substrate and backplane circuitry which control the microdevices by biasing the microdevices.
The microdevices can be in different forms such as vertical where at least one contact is at the top and one contact is at the bottom surface of the device.
One approach to develop a solid state system made out of an array of optoelectronic devices (or other types of solid state devices) is to integrate microdevices into the system substrate. Microdevices are solid state devices made out of active layers, ohmic, contact and or pads. The microdevices can be microLED, micro sensors, micro chiplet, and so on. The microdevices are formed on a substrate and then transferred (or formed on) to a donor substrate. The microdevices are then transferred from the donor substrate into the system substrate. The system substrate can have different circuitry including pixels, electrodes, and pads for coupling to microdevices. The transfer can be done by different means. The microdevice can couple to the system substrate through different approaches such as deposition of conductive electrode or conductive bonding (e.g., eutectic, metallic, thermal, etc.). The microdevices on the donor or the system substrate are tested to identify the defects and performance of the microdevice. In one case, the defective microdevice can be replaced by a working microdevice which is called a repair process.
Measuring microdevices before and after integration into a system substrate is a major hurdle for developing high yield microdevice systems such as microLED displays.
In donor substrate, microdevices have higher pitch (very close to each other). As a result, to measure each device without causing interference, one needs to be able to measure devices selectively. For example, if the donor substrate has a 10 micrometer microLED pitch, turning one microLED ON can impact the result of the adjacent devices. Selective measurement of devices in such packed environments is challenging and may not be reliable and/or expensive.
In another case, some devices (e.g., vertical or lateral) when transferred into system substrate are not fully functional as some of the electrodes are not connected to the device yet. At this point, measuring the devices to make sure the transfer process, the substrate and microdevice is functional is crucial. This is because after connecting the electrodes, it will be challenging to repair or fix the devices. As shown in
At least one connection 104 of the microdevice 102 is biased by a probe or an electrode. Another connection 106 is biased by the ebeam 124. An electron source 100 is used to direct at least part of the electron beam 124 to a microdevice contact 106. The electron beam 124 passes through one contact 106 of the device to the microdevice 102 and to the said electrode 104 biased by the probe or the electrode. The part of electrode 104 can be part of the biasing circuits 110 in the substrate 108. The biasing circuit can be simple electrode or pixel circuits with complex functions such as control of the duty cycle, signal strength and so on.
The electron source can scan more than one microdevice in the substrate. In one case, a magnetic/electric field is used to redirect the electron beam 124 to different microdevices. In this case, if the distance 120 of beam source is further away from the microdevice 102, the effective spot size 122 of the beam 124 becomes larger. As a result, the electron beam 124 will cover other areas different from the microdevice contact 106. As a result, the current value will change. Here, the electron beam 124 power can be modified to compensate for the change in the current density. In another case, the electron source is moved closer to the microdevice (here the electron source is aligned with the device). Therefore, the beam shape is the same for the microdevices. In another case, a combination of the two approaches is used. The magnetic or electric field is used to direct the beam to some distance till the current density stays within a threshold value. Then the electron source is moved to a new position.
The electron beam can affect the microdevice surface other than the contact area 106 or the surfaces on the substrate 108 not coupled to the contact 106. As a result, the beam can directly damage those areas or the charge can accumulate on those areas damaging the area through a discharge.
In another case, as demonstrated in
To protect the other surface and the microdevice from unwanted electron beams,
In one aspect of the invention, a method is disclosed to activate a microdevice with an electron beam, the method comprising, having the microdevice in a substrate, having an electron beam source, having at least one electrode of the microdevice biased by a second electrode or a probe, having the at least one electrode a part of biasing circuits in the substrate and activating the microdevice passing the electron beam through a pad to the microdevice to the at least one electrode. Here the biasing circuits can be simple electrode or pixel circuits with complex functions such as control of the duty cycle and signal strength. Also, a magnetic or an electric field is used to redirect the electron beam to different microdevices, wherein a distance of the electron beam source can be further away making a spot size of the electron beam larger.
The method can further comprise steps wherein the magnetic or the electric field can be used to direct the beam to a distance such that the current density stays within a threshold value followed by movement of the electron beam source to a new position. Also, a protective layer can cover surfaces on the substrate, part of the pads and microdevice surface. Here the protective layer can be a dielectric or a conductive layer redirecting the excess charge.
The method can further comprise the electron beam source having a structure with substrate with a circuit layer. Here the circuit layer may control a voltage or a current going through a tip. Here, the tip can be made of nano-materials including nanowire and carbon nanotube or other materials comprising tungsten, metal, or a conductive material. Also, a gate layer may surround the tip and a dielectric may form a hollow chamber for the tip where the gate layer is formed on top of dielectric pillars. Here the gate layer may be biased through a circuit layer in the electron beam source structure.
The method can further comprise wherein the electron beam source structure may be aligned to the microdevice and a distance between microdevices is set so that the spot size does not affect adjacent microdevices or other components. Here, the tip may be biased and microdevice contact within the electron beam source structure is also biased to allow the electron to stream from the tip towards the microdevice such that a current is controlled by the gate layer or the biasing of the tip or the microdevices. Here, the electron beam source substrate may have tips only for a lesser number of microdevices on the system substrate resulting in a lesser number of microdevices being on and reducing an interference. In addition, the electron beam source substrate may have more than one tip. Here, the tips that are in an alignment range of the microdevice may provide electrons to the microdevice and activate the microdevice and wherein each tip in a set of tips provides a smaller amount of current that is smaller than a test current to the microdevice. Further, a lifetime of the tips may be extended with few smaller tips per microdevice due to lower current stress and redundancy effect.
The method may further comprise, wherein a protection electrode may cover critical areas of the substrate and is biased to collect excess electron beams. In addition, an electrode coupling the biasing circuit to the microdevice may be extended outside the microdevice to protect a part of substrate and the circuitry.
The method may further comprise, wherein another electrode is formed to cover a sidewall and a top surface of the microdevice while it is coupled to the pad.
The method may further comprise, wherein the pad and the electrode covering the sidewall the same and a dielectric separates the sidewall from the electrode.
The method may further comprise, wherein there is at least one tip associated with each microdevice on the substrate.
The method may further comprise, wherein the gate or tip or microdevice bias is controlled so that the spot size is small and only a few microdevices turns on at the time, reducing the interference.
Further aspects of the method may include aspects of functionalities and related structure described in FIGURE descriptions.
While particular embodiments and applications of the present invention have been illustrated and described, it is to be understood that the invention is not limited to the precise construction and compositions disclosed herein and that various modifications, changes, and variations can be apparent from the foregoing descriptions without departing from the spirit and scope of the invention as defined in the appended claims. Further, a power of the electron beam can be modified to compensate a change in a current density.
Filing Document | Filing Date | Country | Kind |
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PCT/CA2022/050118 | 1/28/2022 | WO |
Number | Date | Country | |
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63143220 | Jan 2021 | US |