Direct write processing is one way to manufacture low-cost electronics. One process for fabricating structures used in circuits using direct write processing may involve the ejection of structure forming materials from a print head.
When performing direct write processing by ejecting material from a print head, the size of the drops ejected from the print head may affect the size of the resulting structures. Where the size of the drops ejected is large relative to the size of the features to be fabricated, formation of such structures can be difficult. Additionally, when performing direct write processing by ejecting material from a print head, the size of the drops ejected from the print head may affect the connectivity of the resulting structures or traces.
The accompanying drawings illustrate various embodiments of the present method and system and are a part of the specification. The illustrated embodiments are merely examples of the present system and method and do not limit the scope thereof.
Throughout the drawings, identical reference numbers designate similar, but possibly different, elements.
A number of exemplary methods and an apparatuses for using a dispenser, such as an inkjet material dispenser, to deposit material according to a deposition method are described herein. More specifically, the present method and apparatus is configured to fabricate lines or dots as small as 1 micron or smaller by initially creating droplets with an inkjet material dispenser, depositing the droplets into a mist containment structure, charging the droplets, accelerating the droplets through a venturi, and focusing the final droplets onto selected areas of a substrate. Additionally, the drop size may be filtered according to size prior to being focused onto the substrate. A detailed explanation of the components and functions of the present apparatus will be given hereafter.
As used in the present specification and the appended claims, the term “potential” is meant to be understood broadly as referring to a difference in an electrical charge, expressed in volts, between two points in a circuit.
In the following description, for purposes of explanation, numerous specific details are set forth in order to provide a thorough understanding of the present system and method for using an inkjet material dispenser to perform material dispensing. It will be apparent, however, to one skilled in the art that the present method may be practiced without these specific details. Reference in the specification to “one embodiment” or “an embodiment” means that a particular feature, structure, or characteristic described in connection with the embodiment is included in at least one embodiment. The appearance of the phrase “in one embodiment” in various places in the specification may be referring to different embodiments.
Exemplary Structure
According to the first exemplary embodiment illustrated in
Adjacent to the conductive screen (120) is a shutter (140). According to one exemplary embodiment, the shutter (140) acts as a filter to reduce the average size of the droplets allowed to pass. According to one exemplary embodiment, the shutter (140) includes a pair of electrodes producing a positive field in the trajectory path of the negatively charged droplets. Due to the negative charge imposed upon the droplets by the conductive screen (120), relatively small droplets are more likely to be allowed to pass the positive electric field produced by the shutter (140). The larger droplets will likely be attracted to the positive electric field and will not be allowed to continue towards the substrate (150). Additionally, the shutter (140) may be configured to focus the material droplet towards the material receiving substrate (150), as will be explained in further detail below with reference to
According to one exemplary embodiment, the inkjet material dispenser (210) is a thermal inkjet material dispenser similar to the one illustrated in
As discussed above, the thermal inkjet material dispenser (300) may be configured to function as a material deposition source by selectively dispensing a desired material. Accordingly, the thermal inkjet architecture, the drive waveform produced by the thermal inkjet, the pulse spacing of the thermal inkjet, and/or the material properties of the sample material may be adjusted to produce substantially uniform material droplets in the form of a mist. According to one exemplary embodiment, a fine drop mist may be formed with a thermal inkjet material dispenser (300) by reducing the size of the nozzle (310) employed. According to this exemplary embodiment, the drop sizes of the material emitted from the reduced nozzle (310) may be 2-3 orders of magnitude, or more, smaller than the nominal size of material droplets emitted. Additionally, even smaller droplet magnitudes are conceivable by further varying the thermal inkjet material dispenser (300).
In addition to producing uniform drop sizes, the use of an inkjet material dispenser allows for a desirable level of the material production frequency. According to one exemplary embodiment, the present printing system (200;
Returning again to
A conductive screen (230) electrically coupled to a power supply (235) is positioned adjacent to the exit (224) of the mist containment box (220). According to one exemplary embodiment, illustrated in
Immediately adjacent to the conductive screen (230) is a venturi (240). A venturi (240) is a tube with a smoothly varying constriction forming a throat in the middle thereof. Due to the varying constriction of the venturi (240), as a fluid or gas is passed therethrongh, it experiences changes in velocity and pressure, as described by Bernoulli's principle. According to one exemplary embodiment, as a gas (290) of suitabie velocity is passed through the venturi (240), the velocity will increase and the pressure in the venturi will be reduced below atmospheric pressure, thereby drawing in mist droplets from the mist containment box (220). As the mist droplets are drawn into the gas stream (290), they are accelerated with the gas until they exit the venturi (240).
Adjacent to the venturi (240) is a first (250) and a second (260) shutter. According to one exemplary embodiment, the first shutter (250) acts as a filter to further reduce the average size of the droplets allowed to pass. According to the exemplary embodiment illustrated in
Similarly, the second shutter (260) is configured to focus the final droplet size used for printing. According to this exemplary embodiment, the second shutter (260) includes a pair of electrodes configured to receive a variable positive charge from a voltage source, thereby focusing and positionally directing the material droplets onto the substrate (270). Accordingly, the second shutter may be made of any conductive material including, but in no way limited to, stainless steel.
The substrate (270) used in the present system and method, may be any surface configured to receive a printed material including, but in no way limited to, a circuit board, a touch screen, a backplane, or a radio frequency identification label. Moreover, as illustrated in
Exemplary Implementation and Operation
As illustrated in
According to one exemplary embodiment, the nozzle adjustment (510) that may be performed on the present inkjet material dispenser (210;
Additionally, as illustrated in
Additionally, as illustrated in
Once the mist droplets are generated and/or pre-processed, the mist droplets are deposited in a mist containment box (step 410;
In conjunction with the storage of the contained mist (610) within the mist containment box (220), a gas of suitable velocity is passed through the venturi (240) causing a low pressure in the venturi. As a result of the lower pressure in the venturi (240), a pressure differential between the atmospheric pressure of the mist containment box (220) and the lower pressure of the venturi exists. As a result, the contained mist (610) is drawn out of the mist containment box (220) toward the lower pressure of the venturi (240).
As the contained mist (610) exits the mist containment box (220), it is passed through the conductive screen (230) coupled to a power supply (235). As the mist is passed through the conductive screen (230), a negative electrostatic charge is applied to the mist, according to one exemplary embodiment. Alternatively, a positive charge may be applied to the mist droplets.
Regardless of the charge of the mist, it is subsequently caught up in the gas (620) that is flowing through the venturi (240). Consequently, the charged mist droplets also flow through the venturi (240) towards the first shutter (250). According to one exemplary embodiment, the carrier gas is an inert gas. Alternatively, the carrier gas may be reactive, such as an oxidizing (O2) carrier gas or a reducing (H2) agent configured to initiate a chemical reaction (540;
Additionally, the carrier gas and the charged mist droplets (630) may be accelerated through the venturi (240) by an electrical potential between the conductive screen (230) and an additional electrode. According to this exemplary embodiment, the additional electrode forming an accelerating potential may include, but is in no way limited to, one or more of the shutters (250, 260) or the material receiving substrate (270). The velocity and acceleration of the mist droplets may be controlled by varying the electrical potential. For fluids which benefit from mixing of the droplets, the electrical potential, and consequently the velocity can be reduced to promote contact/mixing of the droplets.
As the charged droplets (630) exit the venturi (240), they are directed towards a first shutter (250). As noted above, the first shutter is configured to reduce the size of the charged droplets that are allowed to pass. According to one exemplary embodiment, the first shutter includes a plurality of positively charged electrodes. According to this exemplary embodiment, the positive charge placed on the electrodes of the first shutter (250) controls the size of the negatively charged drop allowed to pass. Due to the negative charge imposed upon the droplets by the conductive screen (230), primarily relatively small droplets will be allowed to pass the positive electric field produced by the first shutter (250). The larger droplets will frequently be attracted to the positive electric field and will usually not be allowed to continue towards the substrate (270). Additionally, the positive field generated by the first shutter (250) may be varied to vary the average size of the negatively charged droplets allowed therethrough. The voltage applied by the first shutter (250) is inversely proportional to the desired drop diameter, and subsequently the negative charge that will be allowed through. It should be kept in mind, however, that the drop size which is initially generated by the present system and method may be very different from the drop size which is actually deposited. This is achieved by size selection (e.g. by means of filtration) and also by size reduction (e.g. solvent evaporation during in-flight processing of droplets.)
Alternatively, the first shutter may be any mechanism for reducing the droplet size allowed to pass there through. According to one alternative embodiment, the first shutter (250) includes, but is in no way limited to, a size reducing filter, an electric field, a size reducing membrane, and the like.
The second shutter (260) of the exemplary printing system focuses the final droplet size used for printing so that it may be selectively and accurately deposited on the substrate (270). According to one exemplary embodiment, both of the shutters (250, 260) control the droplet size by the amount of positive voltage applied. The larger the voltage, the smaller the average drop diameter will be allowed through. Additionally, the positive voltage applied to the second shutter (260) may be varied to direct the final deposition charged droplets (640) towards the substrate (270). According to one exemplary embodiment, the electrodes of the second shutter (260) are more closely spaced than the electrodes of one exemplary embodiment of the first shutter (250) to aid in the focusing of the final deposition charged droplets (640) and to increase the resolution of the resulting deposition.
Moreover, the selective deposition of the present final deposition charged droplets (640) may be facilitated by the servo mechanism (280) coupled to the present printing system (200). As illustrated in
In general, the larger the drop ejected, the more likely the solid content of the drop will collect along the edges of the drop, thereby decreasing the connectivity of adjacent drops. Using the illustrated system and methods, a resolution of 1 micrometer lines and or 1 micrometer dots may be produced. As illustrated in
Additionally, the incorporation of an inkjet material dispenser as a mist generator allows for the generation of the droplets (760) at a desired frequency. According to one exemplary embodiment, the droplets (760) may be generated at frequencies of up to 1 KHz.
Moreover, the present system and method allow for the mist droplets to be transported in either a carrier gas or an electric field. According to the present system and method, the carrier gas and/or the electric field strength can be modified to vary the reaction experienced by the mist droplets. In the case of reactive mist droplets, duration of in-flight processing can be tuned to allow reaction between droplets. Additionally, in the case of a reactive carrier gas, the mist droplets may be oxidized for oxides or reduced for metals.
Alternative Embodiments
According to one alternative embodiment, a focused laser beam or ultraviolet (UV) beam may be used to increase adhesion of the deposited/printed mist droplets. As noted above, with reference to
In conclusion, the present system and method allow for the printing of a desired deposition material by incorporating an inkjet material dispenser. More specifically, the present system and method is configured to fabricate features of 1 micron or smaller by initially creating material sample droplets with an inkjet material dispenser, depositing the mist droplets into a mist containment structure, charging the droplets, accelerating the droplets through a venturi, and focusing the final droplets onto selected areas of a substrate. Additionally, the drop size may be further filtered prior to being focused onto the substrate.
The preceding description has been presented only to illustrate and describe exemplary embodiments of the present system and method. It is not intended to be exhaustive or to limit the present system and method to any precise form disclosed. Many modifications and variations are possible in light of the above teaching. It is intended that the scope of the present system and method be defined by the following claims.
Number | Name | Date | Kind |
---|---|---|---|
4019188 | Hochbert et al. | Apr 1977 | A |
4281333 | Tsuzuki et al. | Jul 1981 | A |
4314258 | Donahue et al. | Feb 1982 | A |
5403617 | Haaland | Apr 1995 | A |
5725672 | Schmitt et al. | Mar 1998 | A |
6161911 | Minemoto et al. | Dec 2000 | A |
6251488 | Miller et al. | Jun 2001 | B1 |
6268584 | Keicher et al. | Jul 2001 | B1 |
6296901 | Boyd et al. | Oct 2001 | B1 |
6349668 | Sun et al. | Feb 2002 | B1 |
6523928 | Peeters et al. | Feb 2003 | B2 |
6636676 | Renn | Oct 2003 | B1 |
20030048314 | Renn | Mar 2003 | A1 |
20030175411 | Kodas et al. | Sep 2003 | A1 |
20030180451 | Kodas et al. | Sep 2003 | A1 |
20030189167 | Schultz et al. | Oct 2003 | A1 |
20030228124 | Renn et al. | Dec 2003 | A1 |
20040013573 | Huang | Jan 2004 | A1 |
20040029033 | Boyd et al. | Feb 2004 | A1 |
Number | Date | Country |
---|---|---|
0 705 699 | Apr 1996 | EP |
0 761 445 | Mar 1997 | EP |
61106261 | May 1986 | JP |
Number | Date | Country | |
---|---|---|---|
20060007273 A1 | Jan 2006 | US |