The following U.S. patents are herein fully incorporated by reference:
U.S. Pat. No. 4,126,854 by Sheridon entitled “Twisting Ball Panel Display,”
U.S. Pat. No. 4,143,103 by Sheridon entitled “Method Of Making A Twisting Ball Panel Display;”
U.S. Pat. No. 5,262,098 by Crowley el al entitled “Method And Apparatus For Fabricating Bichromal Balls For A Twisting Ball Display;”
U.S. Pat. No. 5,344,594, by Shendon entitled “Method For The Fabrication Of Multicolored Balls For A Twisting Ball Display;”
U.S. Pat. No. 5,389,945, by Shendon entitled “Writing System Including Paper-Like Digitally Addressed Media and Addressing Device Therefor;”
U.S. Pat. No. 5,604,027 by Sheridon entitled “Some Uses Of Microencapsulalion For Electric Paper;”
U.S. Pat. No. 5,717,514 by Shendon entitled “Polychromal Segmented Bails For A Twisting Ball Display;”
U.S. Pat. No. 5,767,826 by Shendon el al. entitled “Subtractive Color Twisting Ball Display;”
U.S. Pat. No. 5,777,782 by Sheridon entitled “Auxiliary Optics For A Twisting Ball Display;”
U.S. Pat. No. 5,894,367 by Sheridon entitled “Twisting Cylinder Display Using Multiple Chromatic Values;”
U.S. Pat. No. 6,055,091 by Sheridon et al, entitled “Twisting Cylinder Display;”
U.S. Pat. No. 6,097,531 by Sheridon entitled “Method Of Making Uniformly Magnetized Elements For A Gyncon Display;”
U.S. Pat. No. 6,110,538 by Sheridon entitled “A Method Of Making A Gyncon Display Using Magnetic Latching;”
U.S. patent application Ser. No. 08/960,865 by Sheridon et ai entitled “Twisting Cylinder Display;”
U.S. Pat. No. 6,222,513 by Howard et al. entitled “Charge Retention Islands for Electric Paper And Applications Thereof;”
U.S. patent application Ser. No. 09/199,544 by Sheridon entitled “Gyncon Displays Utilizing Rotating Elements And Magnetic Latching;”
U.S. patent application Ser. No. 09/200,553 by Shendon entitled “Gyricon Displays Utilizing Magnetic Elements And Magnetic Trapping;”
U.S. Pat. No. 6,174,153 by Sheridon entitled “An Apparatus For Making Uniformly Magnetized Elements For A Gyricon Display;”
U.S. Pat. No. 6,174,153 by Sheridon entitled “An Apparatus For Making Uniformly Magnetized Elements For A Gyricon Display;”
U.S. Pat. No. 6,251,329 by Sheridon entitled “A Method Of Making A Gyricon Display Using Magnetic Latching;”
U.S. Pat. No. 6,197,228 by Sheridon entitled “A Method Of Making A Gyricon Display Using Magnetic Latching;”
U.S. Pat. No. 6,211,998 by Sheridon entitled “Magnetic Unlatching And Addressing Of A Gyricon Display;”
U.S. patent application Ser. No. 09/465,801 by Biegelsen et al entitled “System and method for rotatable element assembly and laminate substrate assembly;”
U.S. patent application Ser. No. 09/563,504 by Knights entitled “Rotating element sheet material with microstructured substrate and method of use;”
U.S. patent application Ser. No. 09/549,518 by Sheridon entitled “Rotating element sheet material with generalized containment structure;”
U.S. patent application Ser. No. 09/517,522 by Silverman entitled “Rotating element sheet material with reversible highlighting;” and
U.S. patent application Ser. No. 09/643,670 by Kazmaier et al entitled “Electromagnetophoretic display system and method.”
The present invention relates to a system for addressable displays that decreases the fringing effect of an addressing vector field. More particularly, the present invention relates to the use of sheet electrodes incorporated into rotating element sheet material, addressed with a stylus, in order to produce a saturated aspect.
Rotating element sheet material has been disclosed in U.S. Pat. Nos. 4,126,854 and 4,143,103, both hereinabove incorporated by reference, and generally comprises a substrate, an enabling fluid, and a class of rotatable elements. As discussed more below, rotating element sheet material has found a use as “reusable electric paper.”
In
The use of rotating element sheet material as “reusable electric paper” is due to that fact that the rotatable elements are typically given a second broken symmetry, a multivalued aspect, correlated with the addressing polarity discussed above. That is, the above-mentioned coatings may be chosen so as to respond to incident electromagnetic energy in distinguishable ways, as indicated in
For example, as disclosed in U.S. Pat. No. 4,126,854, hereinabove incorporated by reference, rotatable element 10 may comprise a black polyethylene generally spherical body with titanium oxide sputtered on one hemisphere, where the titanium oxide provides a light-colored aspect in one orientation. Such a rotatable element in a transparent dielectric liquid will exhibit the desired addressing polarity as well as the desired aspect.
A multivalued aspect in its simplest form is a two-valued aspect. When the aspect is the chromatic response to visible light, a rotatable element with a two-valued aspect can be referred to as a bichromal rotatable element. Such a rotatable element may be fabricated by the union of two layers of material as described in U.S. Pat. Nos. 5,262,098 and 6,147,791, herein incorporated by reference.
One skilled in the art should appreciate that first aspect set 120 will maintain its aspect after applied vector field 100 is removed, in part due to the energy associated with the attraction between rotatable element 10 and the substrate structure, as, for example, cavity walls (not shown). This energy contributes, in part, to the switching characteristics and the memory capability of rotating element sheet material 50, as disclosed in U.S. Pat. No. 4,126,854, hereinabove incorporated by reference, and discussed in more detail below.
Further still, one skilled in the art should appreciate that no-field set and first aspect set discussed above in
For example, U.S. Pat. No. 4,126,854 entitled “Twisting Ball Panel Display” issued Nov. 21, 1978, and U.S. Pat. No. 4,143,103 entitled “Method Of Making A Twisting Ball Display,” issued Mar. 6, 1979, both by Sheridon, describe a rotating element sheet material that comprises bichromal rotatable elements contained in fluid-filled cavities and embedded in an elastomer medium. One segment of the bichromal rotatable elements has a larger electrical charge in contact with the fluid and in the presence of the electrical field than the other segment. Thus, for a given polarity of applied electrical field, one segment will rotate toward and be visible to an observer of the display. Applying the opposite polarity of electrical field will cause the rotatable element to rotate and present the other segment to be seen by the observer.
U.S. Pat. No. 4,143,103 describes the response of the bichromal rotatable element to the applied electrical field as a threshold response. That is, as the external field is increased, the bichromal rotatable element remains stationary in position until a threshold voltage is reached, at which time the rotatable element starts to rotate from its initial position. The amount of rotation increases with an increasing electrical field until a 180-degree rotation can be achieved. The value of the external field that causes a 180-degree rotation is called the full addressing voltage.
The response pattern of the bichromal rotatable element to an external electrical field determines the type of addressing that may be used to create images on the rotating element sheet material. There are known in the art three types of addressing schemes for displays. The first of these is active matrix addressing, which places the least demands on the properties of the display.
In active matrix addressing a separate addressing electrode is provided for each pixel of the display and each of these electrodes is continuously supplied with an addressing voltage. The complete set of voltages can be changed for each addressing frame. While this type of addressing places the least demands on the properties of the display medium, active matrix addressing is the most expensive, most complicated and least energy efficient type of addressing.
The second type of addressing scheme is passive matrix addressing. Passive matrix addressing makes use of two sets of electrodes, one on each side of the display medium. Typically, one of these consists of horizontal conductive lines and the other consists of vertical conductive lines. The conductive lines on the front surface or window of the display are necessarily aspect-transparent. To address the display medium a voltage is placed on a horizontal conductive line and a voltage is placed on a vertical conductive line. The segment of medium located at the intersection of these two lines experiences a voltage equal to the sum of these two voltages. If the voltages are equal, as they usually are, the sections of medium located adjacent to the each of the lines, but not at the intersection of the lines, experience ½ the voltage experienced by the section of medium at the line intersection. Passive addressing is less complicated and more energy efficient because the pixels of the display medium are addressed only for as long as is required to change their optical states. However, the requirements for a medium that can be addressed with a passive matrix display are significantly greater than for the active matrix case. The medium must respond fully to the full addressing voltage but it must not respond to ½ the full addressing voltage. This is called a threshold response behavior. The medium must also stay in whichever optical state it has been switched into by the addressing electrodes without the continuous application of voltage—that is, it should store the image without power. Passive addressing is the most widely used method of addressing displays and is the lowest cost.
The third type of addressing consists of a linear array of addressing electrodes in the form of a bar that can be moved over the surface of the sheet material. In this form of addressing, the sheet material is placed over or incorporates a grounding electrode and is protected from possible mechanical damage from the moving bar by placing a thin window between the bar and the rotating element sheet material. As the bar is moved over the sheet material, it applies voltages to specific pixels of the sheet material for short periods of time and generates a full image each time the bar is scanned over the surface. In one variation of this method, the addressing bar deposits image-wise charge on the surface of the window.
The requirements imposed on the sheet material by this form of addressing then depend on which type of addressing bar is used. If the addressing bar simply exposes the sheet material to voltages as it passes over the surface, then it is necessary for the rotating sheet material to exhibit threshold behavior. Thus the area of the sheet material directly under the addressing bar electrode must undergo a change in aspect when exposed to the full addressing voltage; but as the bar moves to the next row of pixels, this same area of sheet material must not respond to the diminished voltages experienced by the sheet material from the moving addressing bar. As in passive addressing, this requires that the sheet material have a sharp threshold response. This addressing bar also requires that the change in aspect occur completely during the time the addressing bar electrodes move over its vicinity, which usually limits the display frame addressing speed. U.S. patent application Ser. No. 09/037,767 by Howard et al. entitled “Charge Retention Islands For Electric Paper And Applications Thereof” and also assigned to the same assignee as this application, describes an arrangement of addressing electrodes that greatly reduces the switching speed requirements of the medium due to this effect.
In U.S. patent application Ser. No. 09/037,767 the addressing bar deposits image-wise charge on or near the surface of the sheet material. The charge deposition addressing method relaxes the requirements on the sheet material. The addressing bar speed over the surface is limited only by the rate at which it can deposit image-wise charge, because the sheet material can respond to the voltage associated with the deposited charge pattern at its own speed. Threshold response behavior is not so important; however, the ability to store the image is because it can be expected that the image-wise charge deposited on the sheet material will leak off over a short period of time. However, addressing bars that can deposit image-wise charge on or near the sheet material tend to be bulky and more expensive than bars that simply impose image-wise voltages directly.
As described earlier, rotatable elements 10 in the path of stylus 200 will tend to orient themselves in response to the vector field introduced between stylus 200 and infralayer 260. In
One skilled in the art should appreciate that the work function necessary to change the orientation and position of rotatable elements from a fixed position and orientation is greater than the work function necessary to change the orientation and position of rotatable elements that are already in motion. Such an effect is the result of a variety of factors, including such processes as conventionally understood as producing the difference between static friction and kinetic friction, and also as a result of fluid dynamics associated with the motion of the enabling fluid (not shown) in response to the motion of rotatable element. Similarly, one skilled in the art should appreciate that conventional displays relying on electrophoretic effects will exhibit a similar effect. Accordingly, the response of rotatable elements to leading fringe field 275 is different from the response of rotatable elements to trailing fringe field 285. Specifically, while the rotatable elements immediately beneath stylus 200 in
Accordingly, and from a macroscopic perspective, rather than producing a line with a saturated aspect, stylus 200 used to address rotating element sheet material 50 will produce unsaturated line 290. Such a macroscopic perspective is depicted in FIG. 10. Although the effect disclosed herein relates to a saturated aspect when addressing rotating element sheet material, in general, displays relying on electrophoretic effects may also exhibit undersirable aspects as a result of fringe fields.
As discussed above, a useful property of rotating element sheet material is the ability to maintain a given aspect after applied vector field 100 for addressing is removed. This ability contributes, in part, to the switching characteristics and the memory capability of rotating element sheet material 50, as disclosed in U.S. Pat. No. 4,126,854, hereinabove incorporated by reference. This will be referred to as aspect stability. The mechanism for aspect stability in the above embodiments is generally the energy associated with the attraction between the rotatable elements and the containment structure, or “work function.” A host of factors influence the magnitude of the energy associated with the work function including, but not limited to: surface tension of enabling fluid in contact with rotatable elements; the relative specific gravity of the rotatable elements to the enabling fluid; magnitude of charge on rotatable elements in contact with containment structure; relative electronic permittivity of enabling fluid and containment structure; “stickiness” of containment structure; and other residual fields that may be present. The applied vector field for addressing must be strong enough to overcome the work function in order to cause an orientation change; furthermore, the work function must be strong enough to maintain this aspect in the absence of an applied vector field for addressing.
One method for fabricating rotating element sheet material that produces a saturated aspect when addressed with a stylus has been disclosed in U.S. Pat. No. 6,147,791 entitled “Gyricon displays utilizing rotating elements and magnetic latching,” herein incorporated by reference. A rotatable element consistent with the invention disclosed in U.S. Pat. No. 6,147,791 is depicted in FIG. 12. The rotatable element of
In order to produce a saturated aspect, however, the rotatable element of
One skilled in the art should also appreciate that the element latching components 170 and the sheet latching components 172 will contribute to the “work function” energy associated with the attraction between rotatable element 10 and the substrate structure, as, for example, cavity walls (not shown), and that contributed to aspect stability. Again, this energy will contribute, in part, to the switching characteristics and the memory capability of rotating element sheet material 50, as disclosed in U.S. Pat. No. 4,126,854, hereinabove incorporated by reference. Such a system will help to produce a saturated aspect exhibited to observer 60, but requires detailed manufacturing procedures.
Accordingly, it is desirable to fabricate rotating element sheet material that will exhibit a saturated aspect but will not require detailed manufacturing procedures, such as the introduction of rotatable latching components and sheet latching components. Furthermore, it is generally desirable to decrease the effect of fringe fields in addressable displays.
In a first embodiment, a display kit of the present invention comprises: an addressable display medium configured to exhibit a first aspect under the influence of an addressing vector field in a first direction at an addressing magnitude; and an addressor; where the addressor is configured to provide the addressing vector field in the first direction at the addressing magnitude to a portion of the display medium; and a filter comprising: a first sheet electrode and a second sheet electrode configured to exhibit a first vector field in the first direction at a first magnitude to the portion of the display medium; where the first magnitude is less than the addressing magnitude; where the display medium is located between the first sheet electrode and the second sheet electrode; and where the first sheet electrode is between the addressor and the display medium.
In a first embodiment of a method for addressing a display medium, the method comprises the steps of: providing the display kit described above where the first sheet electrode has a restivity equal to R ohms per square and a capacitance per unit area equal to C; where the distal end of the stylus has a width w; and moving the stylus with a speed substantially equal to 1/(wRC) such that the first sheet electrode is between the stylus and the substrate.
The accompanying drawings, which are incorporated in and constitute a part of this specification, illustrate an implementation of the invention and, together with the description, serve to explain the advantages and principles of the invention. In the drawings,
Reference will now be made in detail to an implementation consistent with the present invention as illustrated in the accompanying drawings. Whenever possible, the same reference number will be used throughout the drawings and the following description to refer to the same or like parts.
As used herein, “aspect” refers to a common response to incident electromagnetic energy of interest. For example, if the incident electromagnetic energy of interest lies in the visible spectrum, then a first aspect may correspond to a black appearance, and a second aspect may correspond to a white appearance. If the incident electromagnetic energy of interest lies in the x-ray region, then a first aspect may correspond to the transmission of the x-ray energy, while a second aspect may correspond to the absorption of the x-ray energy. Furthermore, the “common response” may comprise any of the phenomena of absorption, reflection, polarization, transmission, fluorescence, or any combination thereof.
As used herein, “observer” refers to a human perceiver, or to a human perceiver in conjunction with an apparatus sensitive to the electromagnetic energy of interest. If the electromagnetic energy of interest lies in the visible spectrum, then observer may refer to a human perceiver. If the electromagnetic energy of interest lies outside of the visible spectrum, then observer refers to an apparatus sensitive to the electromagnetic energy and capable of resolving the aspects of interest into human perceivable form.
As used herein, “diameter” refers to an order of magnitude dimension corresponding to any of height, width, and depth of any microencapsulation structure or aspect elements. The use of “diameter” does not imply that circular, spherical, or cylindrical geometry only is under consideration.
As used herein, “vector field” refers to a field whose amplitude in space is capable of having a magnitude and a direction. Vector fields of interest in the present invention include electric fields, magnetic fields, or electromagnetic fields.
As used herein, “work function” refers to the amount of energy necessary to overcome the attraction between an aspect element and the microencapsulation structure so as to enable displacement. As mentioned above, a host of factors influence the magnitude of the energy associated with the work function including, but not limited to: surface tension of first aspect medium in contact with second aspect element; the relative specific gravity of first aspect medium to second aspect element; magnitude of charge on second aspect element; relative electronic permittivity of first aspect medium and microencapsulation structure; “stickiness” of microencapsulation structure; and other residual fields that may be present.
As used herein, the term “prism-shaped” refers to a polyhedron whose ends have substantially the same size and shape and are substantially parallel, and whose remaining sides are each substantially parallelograms.
As used herein, the term “display medium” refers to any material that exhibits at least two distinct aspects under the influence of an external vector field, where the aspect exhibited is a function of the magntiude and direction of the external vector field.
As used herein, the terms “addressor” and “grounding sheet” refer to an apparatus configured to provide a vector field with a magnitude and direction at a portion of a region next to the grounding sheet.
A display medium consistent with the present invention is depicted in
Furthermore, as before, stylus 200 moving in the direction of arrow 250 and proximal to rotating element sheet material 400 will have an associated leading fringe field 275 and trailing fringe field 285.
In a preferred embodiment, a filter consistent with the present invention comprises first sheet electrode 420 and second sheet electrode 430. First sheet electrode 420 and second sheet electrode 430 are configured to exhibit a first vector field between them. This is illustrated in
One skilled in the art should appreciate that a perfect conductor placed between stylus 200 and rotatable element 10, where rotatable element 10 is between stylus 200 and grounding sheet 265, will shield rotatable element 10 from the influence of the vector field produced between stylus 200 and grounding sheet 265. Accordingly, if first sheet electrode 420 were a perfect conductor, then stylus 200, at rest, would have no influence on the display medium, such as the rotating element sheet material of FIG. 14.
However, one skilled in the art should further appreciate that if first sheet electrode is not a perfect conductor, then it is possible for the vector field produced between stylus 200 and grounding sheet 265 to have an influence on the display medium. Specifically, if first sheet electrode has a resistivity equal to R ohms per square, a capacitance equal to C farads per unit area, and stylus 200 has width w (
Further still, one skilled in the art should appreciate that there will be a portion of the field that is shielded, due to the spread-out nature of the vector field between stylus 200 and grounding sheet 265. Specifically, trailing fringe field 285 will be shielded by first sheet electrode 420. Accordingly, the plurality of rotatable elements in the path of stylus 200 will experience a sharp cutoff in the vector field that is introduced as stylus 200 moves past. It is this sharp cutoff that will prevent the plurality of rotatable elements from continuing to orient themselves according to the fringe field of stylus 200. As a result, the rotatable elements, addressed in this manner, will produce a saturated aspect in the direction of observer 60. A macroscopic perspective of the saturated aspect 490 is depicted in FIG. 17.
One skilled in the art may also understand the result produced by rotating element sheet material 400 by understanding that the selection of the magnitude of first vector field between first sheet electrode 420 and second sheet electrode 430. As stated earlier, the magnitude of first vector field is selected such that the energy coupling between the first vector field and the addressing dipole of the rotatable element is less than the work function associated with changing the position and orientation of rotatable element. However, after stylus 200 has introduced energy sufficient to change the position and orientation of rotatable element 10 from a static position and orientation, the energy coupling between the first vector field and the addressing dipole of the rotatable element will be sufficient to influence the orientation of rotatable element 10 until rotatable element 10 comes to rest again. Accordingly, rotating element sheet material 400 will produce a saturated aspect when addressed by stylus 200.
Second sheet electrode 430 is preferably a good conductor. Accordingly, one skilled in the art will appreciate that grounding sheet 265 is not necessary, as second sheet electrode 430 would then shield grounding sheet 265 from any fields originating above second sheet electrode 265. Furthermore, second sheet electrode 430 may be a non-conductor if grounding sheet 265 is located adjacent to it. Accordingly, the presence of grounding sheet 265 represents the most general case. Further still, one skilled in the art should appreciate that the filter will still function if grounding sheet 265 is absent and second sheet electrode 430 has a resistivity approximately equal to that of first sheet electrode 420.
One skilled in the art should appreciate that the resistivity of first sheet electrode 420 will be of the order of 1013 ohms/square, where stylus 200 is approximately 1 mm wide with a speed of 10 cm/sec, and where the capacitance of the display medium is approximately 5 picofarads/(cm2) (exemplary capacitance of rotating element sheet material). Accordingly, first sheet electrode 420 preferably comprises Indium Tin Oxide sputtered on glass or plastic. Further still, there are a number of other choices for a high resistivity coating of conductive layers on glass and plastic. Preferably, such a coating comprises platinum, gold, or their alloys, since these materials have the property that they provide conductive coatings in all thicknesses of deposited material. In contrast, many other materials, such as aluminum, provide conductive layers only after a certain thickness is reached and after that the conductivity increases very rapidly with the deposition of further material, making it difficult to obtain uniform conductivity. In particular, even very thin layers of platinum, gold, or platinum-alloys and gold-alloys on glass or plastic are conductive and the conductivity increases uniformly with increased thickness of deposited material. Further still, such materials are also transparent at thicknesses of 100 Angstroms, which is a preferably thickness. However, one skilled in the art should appreciate that there may be a range of thicknesses consistent with the present invention, since the conductivity of a given sheet electrode will be highly dependent on the coating conditions.
As stated earlier, it should be obvious to one skilled in the art that the fringe field filtering effects described herein are not limited to rotating element sheet materials. Indeed, any electro-sensitive or electro-optical sheet materials addressed by a stylus or stylus array will experience the saturation aspect depicted in FIG. 17.
Methods and apparatus consistent with the present invention can be used to address a display medium in order to produce a saturated aspect. The foregoing description of an implementation of the invention with rotating element sheet material has been presented for purposes of illustration and description. It is not exhaustive and does not limit the invention to the precise form disclosed. Modifications and variations are possible in light of the above teachings or may be acquired from practicing the invention. For example, some of the examples used the spectrum associated with visible light as the electromagnetic energy of interest. However, the use of any electromagnetic energy, including infrared, ultraviolet and x-rays as the electromagnetic energy of interest is consistent with the present invention. Still further,
The following identified United States patent applications are relied upon and are fully incorporated herein by reference: U.S. patent application entitled “Rotating element sheet material with dual vector field addressing,” by Nicholas K. Sheridon, filed on Jan. 11, 2001, and accorded Ser. No. 09/757,539. U.S. patent application entitled “Rotating element sheet material with dual vector field addressing,” by Nicholas K. Sheridon, filed on Jan. 11, 2001, and accorded Ser. No. 09/757,531.
Number | Name | Date | Kind |
---|---|---|---|
2326634 | Gebhard et al. | Aug 1943 | A |
2354018 | Heltzer et al. | Jul 1944 | A |
2354048 | Palmquist | Jul 1944 | A |
2354049 | Palmquist | Jul 1944 | A |
2407680 | Palmquist et al. | Sep 1946 | A |
2600963 | Bland | Jun 1952 | A |
2684788 | Bland | Jul 1954 | A |
2794301 | Law et al. | Jun 1957 | A |
2950985 | d'Adrian | Aug 1960 | A |
2965921 | Bland | Dec 1960 | A |
2980547 | d'Adrian | Apr 1961 | A |
3034177 | Hooper | May 1962 | A |
3036388 | Tate | May 1962 | A |
3063388 | Magarian et al. | Nov 1962 | A |
RE25363 | Tate | Apr 1963 | E |
3150947 | Bland | Sep 1964 | A |
3222204 | Weber et al. | Dec 1965 | A |
3243273 | Bland | Mar 1966 | A |
3310391 | Law | Mar 1967 | A |
3406363 | Tate | Oct 1968 | A |
3594065 | Marks | Jul 1971 | A |
3615993 | French | Oct 1971 | A |
3617333 | Brown | Nov 1971 | A |
3648281 | Dahms et al. | Mar 1972 | A |
3670323 | Sobel et al. | Jun 1972 | A |
3795435 | Schwab | Mar 1974 | A |
3915771 | Gatzke et al. | Oct 1975 | A |
3982334 | Tate | Sep 1976 | A |
4001140 | Foris et al. | Jan 1977 | A |
4002022 | Lopez C. | Jan 1977 | A |
4082426 | Brown | Apr 1978 | A |
RE29742 | Tung | Aug 1978 | E |
4117192 | Jorgensen | Sep 1978 | A |
4117194 | Barbe et al. | Sep 1978 | A |
4126854 | Sheridon | Nov 1978 | A |
4143103 | Sheridon | Mar 1979 | A |
4143472 | Murata et al. | Mar 1979 | A |
4229732 | Hartstein et al. | Oct 1980 | A |
4232084 | Tate | Nov 1980 | A |
4253909 | Lee | Mar 1981 | A |
4256677 | Lee | Mar 1981 | A |
4261653 | Goodrich | Apr 1981 | A |
4267946 | Thatcher | May 1981 | A |
4268413 | Dabisch | May 1981 | A |
4273672 | Vassiliades | Jun 1981 | A |
4283438 | Lee | Aug 1981 | A |
4288788 | Rogers et al. | Sep 1981 | A |
4299880 | Arens | Nov 1981 | A |
4367920 | Tung et al. | Jan 1983 | A |
4368952 | Murata et al. | Jan 1983 | A |
4374889 | Arens | Feb 1983 | A |
4381616 | Saxer | May 1983 | A |
4402062 | Batchelder | Aug 1983 | A |
4411973 | Gilmour et al. | Oct 1983 | A |
4417543 | Lee | Nov 1983 | A |
4418098 | Maistrovich | Nov 1983 | A |
4418346 | Batchelder | Nov 1983 | A |
4419383 | Lee | Dec 1983 | A |
4438160 | Ishikawa et al. | Mar 1984 | A |
4441791 | Hornbeck | Apr 1984 | A |
4457723 | Tate | Jul 1984 | A |
4492435 | Banton et al. | Jan 1985 | A |
4500172 | Gagnon et al. | Feb 1985 | A |
4511210 | Tung et al. | Apr 1985 | A |
4532608 | Wu | Jul 1985 | A |
4569857 | Tung et al. | Feb 1986 | A |
4592628 | Altman et al. | Jun 1986 | A |
4627689 | Asher | Dec 1986 | A |
4632517 | Asher | Dec 1986 | A |
4657349 | Labes et al. | Apr 1987 | A |
4675476 | Kobayashi | Jun 1987 | A |
4678695 | Tung et al. | Jul 1987 | A |
4688900 | Doane et al. | Aug 1987 | A |
4695528 | Dabisch et al. | Sep 1987 | A |
4701024 | Kobayashi et al. | Oct 1987 | A |
4710732 | Hornbeck | Dec 1987 | A |
4713295 | Laroche | Dec 1987 | A |
4721649 | Belisle et al. | Jan 1988 | A |
4725494 | Belisle et al. | Feb 1988 | A |
4729687 | Arens | Mar 1988 | A |
4740266 | Wu | Apr 1988 | A |
4781789 | Wu | Nov 1988 | A |
4781790 | Wu | Nov 1988 | A |
4783236 | Wu | Nov 1988 | A |
4795243 | Suzuki | Jan 1989 | A |
4795528 | Wu | Jan 1989 | A |
4810431 | Leidner | Mar 1989 | A |
4837071 | Tagoku et al. | Jun 1989 | A |
4877253 | Arens | Oct 1989 | A |
4890902 | Doane et al. | Jan 1990 | A |
4919521 | Tada et al. | Apr 1990 | A |
4931019 | Park | Jun 1990 | A |
4948232 | Lange | Aug 1990 | A |
4956619 | Hornbeck | Sep 1990 | A |
4991941 | Kalmanash | Feb 1991 | A |
4994204 | Doane et al. | Feb 1991 | A |
5006422 | Sakurai et al. | Apr 1991 | A |
5039557 | White | Aug 1991 | A |
5066559 | Elmasry et al. | Nov 1991 | A |
5075186 | Sheridon | Dec 1991 | A |
5128203 | LaRoche | Jul 1992 | A |
5131736 | Alvarez | Jul 1992 | A |
5151032 | Igawa | Sep 1992 | A |
5155607 | Inoue et al. | Oct 1992 | A |
5157011 | Okabe et al. | Oct 1992 | A |
5189658 | Moses | Feb 1993 | A |
5219820 | Morohoshi et al. | Jun 1993 | A |
5223473 | Oliver et al. | Jun 1993 | A |
5226099 | Mignardi et al. | Jul 1993 | A |
5233459 | Bozler et al. | Aug 1993 | A |
5249000 | Okabe et al. | Sep 1993 | A |
5251048 | Doane et al. | Oct 1993 | A |
5262098 | Crowley et al. | Nov 1993 | A |
5262374 | Okabe et al. | Nov 1993 | A |
5270872 | Spry | Dec 1993 | A |
5274460 | Yamada et al. | Dec 1993 | A |
5290066 | Mody | Mar 1994 | A |
5315418 | Sprague et al. | May 1994 | A |
5315776 | Strawbridge et al. | May 1994 | A |
5331454 | Hornbeck | Jul 1994 | A |
5344594 | Sheridon | Sep 1994 | A |
5351995 | Booker | Oct 1994 | A |
5354598 | Arens | Oct 1994 | A |
5363222 | Ledebuhr | Nov 1994 | A |
5383008 | Sheridon | Jan 1995 | A |
5384067 | Doane et al. | Jan 1995 | A |
5389426 | Arens et al. | Feb 1995 | A |
5389945 | Sheridon | Feb 1995 | A |
5392151 | Nelson | Feb 1995 | A |
5397503 | Yuasa et al. | Mar 1995 | A |
5411398 | Nakanishi et al. | May 1995 | A |
5416996 | Clemens et al. | May 1995 | A |
5432526 | Hyatt | Jul 1995 | A |
5432534 | Maruyama et al. | Jul 1995 | A |
5459602 | Sampsell | Oct 1995 | A |
5469020 | Herrick | Nov 1995 | A |
5475401 | Verrier et al. | Dec 1995 | A |
5515075 | Nakagiri et al. | May 1996 | A |
5526016 | Nakagiri et al. | Jun 1996 | A |
5535047 | Hornbeck | Jul 1996 | A |
5582700 | Bryning et al. | Dec 1996 | A |
5604027 | Sheridon | Feb 1997 | A |
5627562 | Skodlar | May 1997 | A |
5659330 | Sheridon | Aug 1997 | A |
5667924 | Ziolo | Sep 1997 | A |
5703671 | Narita et al. | Dec 1997 | A |
5708525 | Sheridon | Jan 1998 | A |
5717283 | Biegelsen et al. | Feb 1998 | A |
5717514 | Sheridon | Feb 1998 | A |
5717515 | Sheridon | Feb 1998 | A |
5723204 | Stefik | Mar 1998 | A |
5724064 | Stefik et al. | Mar 1998 | A |
5731792 | Sheridon | Mar 1998 | A |
5737115 | Mackinlay et al. | Apr 1998 | A |
5739801 | Sheridon | Apr 1998 | A |
5739946 | Iwanaga et al. | Apr 1998 | A |
5751268 | Sheridon | May 1998 | A |
5754332 | Crowley | May 1998 | A |
5757345 | Sheridon | May 1998 | A |
5760761 | Sheridon | Jun 1998 | A |
5767826 | Sheridon et al. | Jun 1998 | A |
5777782 | Sheridon | Jul 1998 | A |
5784189 | Bozler et al. | Jul 1998 | A |
5808593 | Sheridon | Sep 1998 | A |
5808783 | Crowley | Sep 1998 | A |
5815306 | Sheridon et al. | Sep 1998 | A |
5821624 | Pasch | Oct 1998 | A |
5825529 | Crowley | Oct 1998 | A |
5828441 | Narita et al. | Oct 1998 | A |
5866284 | Vincent | Feb 1999 | A |
5869929 | Eida et al. | Feb 1999 | A |
5877844 | Matsumoto | Mar 1999 | A |
5891479 | Sheridon | Apr 1999 | A |
5892497 | Robertson | Apr 1999 | A |
5893206 | Furlani et al. | Apr 1999 | A |
5894367 | Sheridon | Apr 1999 | A |
5900192 | Richley | May 1999 | A |
5900858 | Richley | May 1999 | A |
5904790 | Sheridon | May 1999 | A |
5906743 | Cohen et al. | May 1999 | A |
5914805 | Crowley | Jun 1999 | A |
5917646 | Sheridon | Jun 1999 | A |
5919409 | Sheridon | Jul 1999 | A |
5922268 | Sheridon | Jul 1999 | A |
5930026 | Jacobson et al. | Jul 1999 | A |
5940054 | Harris | Aug 1999 | A |
5956005 | Sheridon | Sep 1999 | A |
5961804 | Jacobson et al. | Oct 1999 | A |
5969472 | Kisner | Oct 1999 | A |
5972493 | Iwasaki et al. | Oct 1999 | A |
5974901 | Zborowski et al. | Nov 1999 | A |
5975680 | Wen et al. | Nov 1999 | A |
5976428 | Richley | Nov 1999 | A |
5982346 | Sheridon et al. | Nov 1999 | A |
5986629 | Smith et al. | Nov 1999 | A |
5989629 | Sacripante et al. | Nov 1999 | A |
6014116 | Haynes et al. | Jan 2000 | A |
6014247 | Winter et al. | Jan 2000 | A |
6017584 | Albert et al. | Jan 2000 | A |
6034807 | Little et al. | Mar 2000 | A |
6038059 | Silverman | Mar 2000 | A |
6054071 | Mikkelsen, Jr. | Apr 2000 | A |
6054809 | Haynes et al. | Apr 2000 | A |
6055091 | Sheridon et al. | Apr 2000 | A |
6067185 | Albert et al. | May 2000 | A |
6072621 | Kishi et al. | Jun 2000 | A |
6097531 | Sheridon | Aug 2000 | A |
6110538 | Sheridon | Aug 2000 | A |
6118419 | Smith et al. | Sep 2000 | A |
6120588 | Jacobson | Sep 2000 | A |
6120839 | Silverman | Sep 2000 | A |
6122094 | Comiskey et al. | Sep 2000 | A |
6128124 | Silverman | Oct 2000 | A |
6130773 | Jacobson et al. | Oct 2000 | A |
6137467 | Sheridon et al. | Oct 2000 | A |
6147791 | Sheridon | Nov 2000 | A |
6162321 | Silverman | Dec 2000 | A |
6174153 | Sheridon | Jan 2001 | B1 |
RE37085 | Sheridon | Mar 2001 | E |
6196848 | Yamazaki | Mar 2001 | B1 |
6197228 | Sheridon | Mar 2001 | B1 |
6211998 | Sheridon | Apr 2001 | B1 |
6222513 | Howard et al. | Apr 2001 | B1 |
6243058 | Mikkelsen et al. | Jun 2001 | B1 |
6251329 | Sheridon | Jun 2001 | B1 |
6383619 | Engler et al. | May 2002 | B1 |
6396621 | Sheridon | May 2002 | B1 |
6421035 | Sheridon et al. | Jul 2002 | B1 |
6428868 | Sheridon et al. | Aug 2002 | B1 |
6441946 | Sheridon | Aug 2002 | B1 |
6473072 | Comiskey et al. | Oct 2002 | B1 |
6480322 | Engler et al. | Nov 2002 | B2 |
6485280 | Richley | Nov 2002 | B1 |
6487002 | Biegelsen | Nov 2002 | B1 |
6518948 | Berstis | Feb 2003 | B1 |
6521145 | Engler et al. | Feb 2003 | B1 |
6524500 | Sheridon et al. | Feb 2003 | B2 |
6531997 | Gates et al. | Mar 2003 | B1 |
6549327 | Foucher et al. | Apr 2003 | B2 |
6556470 | Vincent et al. | Apr 2003 | B1 |
6559820 | Mikkelsen, Jr. et al. | May 2003 | B1 |
6570700 | Engler et al. | May 2003 | B2 |
6573880 | Simoni et al. | Jun 2003 | B1 |
6577432 | Engler et al. | Jun 2003 | B2 |
6588131 | O'Connell, Jr. | Jul 2003 | B2 |
20020084539 | Sheridon et al. | Jul 2002 | A1 |
20020089486 | Sheridon | Jul 2002 | A1 |
20020089490 | Sheridon | Jul 2002 | A1 |
20020130831 | Engler et al. | Sep 2002 | A1 |
20020131148 | Engler et al. | Sep 2002 | A1 |
20020131149 | Engler et al. | Sep 2002 | A1 |
20020131150 | Engler et al. | Sep 2002 | A1 |
20020131151 | Engler et al. | Sep 2002 | A1 |
20020186197 | Biegelsen | Dec 2002 | A1 |
20020186450 | Foucher et al. | Dec 2002 | A1 |
20020186452 | Biegelsen | Dec 2002 | A1 |
20030046838 | O'Connell, Jr. | Mar 2003 | A1 |
Number | Date | Country |
---|---|---|
1578460 | Nov 1980 | GB |
WO 9803896 | Jan 1998 | WO |
WO 99107967 | Jan 1998 | WO |
WO 9841899 | Sep 1998 | WO |
Number | Date | Country | |
---|---|---|---|
20020089475 A1 | Jul 2002 | US |