1. Field of the Invention
The present invention relates to modifying structures by a laser, and, more particularly, to removing material from photomasks and/or integrated circuits by the use of a pulsed laser.
2. Brief Description of Related Developments
During the manufacture of photomasks and/or integrated circuits, undesirable structures or parts of structures require removal or modification. Several techniques have been used to accomplish these objects in the past.
Almost all photomasks manufactured and especially, leading edge photomasks require the correction of defects that normally form as a result of excess chromium (Cr), for example, on the underlying substrate such as quartz (SiO2). The removal of such defects must not damage adjacent structures with the material removed by a laser, for example. This damage may be the result of splatter or haze created during the ablation of the material.
Several techniques have been used in the past. For example, a focused ion beam of gallium (Ga) with a halogen gas has been used. Spatial resolution of less than 25 nm has been achieved. Several disadvantages are Ga implanting as the undesired material is removed which significantly reduces the optical transmission of the underlying quartz surface. Also, the underlying quartz is almost always damaged by erosion and pitting. Another technique is the use of nanosecond pulsed laser beams to ablate the Cr, for example. The pulsed laser excites electrons whose energy is converted into phonons that subsequently heat the material. This heat may melt Cr that evaporates in a completely thermal process. As a result of thermal diffusion, the material may have balling or curling at the edges and splatters the material across the photomask surface near the ablation. The evaporated material produces a general haze, which reduces significantly the optical transmission of the quartz substrate. Also, the underlying quartz substrate is ablated and this creates an optical phase shift. Thus, thermal ablation from nanosecond pulses is not acceptable for repairing features having a size below 1 micron.
In order to avoid these problems in the past, the use of ultrashort (femtosecond) laser pulses have been used. This puts sufficient energy into the excited electrons to cause the material to turn into a plasma without the use of the thermal process. This non-thermal process does not degrade the resolution, no metal is splattered, no balling at the edges of the material, no damage to the substrate. A description of the femtosecond laser process and the photomask repair system is described in the article “MARS: Femtosecond laser photomask advanced repair system in manufacturing,” by Richard Haight, et al., published in Journal of Vacuum Science Technology, B 17(6), November/December 1999, pp. 3137 to 3143.
The present invention is directed to a method and an apparatus for minimizing the deposition of debris onto a sample being ablated. In one embodiment the method includes the steps of: 1) reducing a laser pulse energy to approximately a threshold level for ablation; and 2) ablating a region of the sample using a multitude of laser pulses, each pulse being sufficiently separated in time to reduce a concentration of ablation products in a gas phase. In another embodiment an apparatus is used to ablate a region of a sample with a laser beam. The apparatus comprises: 1) a source providing a pulsed laser beam of a certain energy, the source focusing the laser beam on the sample to ablate a region of the sample; and 2) a device for providing a flowing fluid over the region being ablated to remove the ablation products.
The foregoing aspects and other features of the present invention are explained in the following description, taken in connection with the accompanying drawings, wherein:
Referring to
As shown in
The refractive index matching fluid 36 has two uses. The first use of the refractive index matching fluid 36 is to reduce the diameter of the focused laser spot by using an immersion objective. In this case, the index of the fluid is chosen to match the index of the final element of the objective lens. This effectively increases the numerical aperture of the objective by the index of the fluid. Since the focused spot diameter is inversely proportional to the numerical aperture, this results in a smaller focused spot (yielding a spot, which is approximately 1/1.3 times smaller for typical immersion objectives). The second use of the refractive index matching fluid 36 is designed to allow a higher aspect ratio hole to be ablated by selecting a fluid 36 whose index matches the refractive index of the substrate material. For chip modification, typical substrate materials would include SiO2, SiN, polymers, SiLK (a low dielectric constant insulator for metallization).
Further as shown in
In greater detail,
In the normal ablation process of the present invention, it is preferred that the material ablated by the pulsed laser beam 14 be from a photomask or an integrated circuit (IC) device. On a photomask, for example, the material of concern is chromium and the chromium is deposited on a substrate of glass such as silicon dioxide to provide a circuit structure that is used in making chips. During the manufacturing of the photomask, chromium defects occur with regular frequency and require removal from the photomask to be useable in making devices of concern. If the chromium is ablated by a thermal process, the chromium may then condense in the region above the ablated spot and then falls as debris onto the glass or other adjacent areas. This material is detrimental to the photomask or the IC device since it affects the finished product. The removal of material from certain features may be limited due to optical diffraction effects when the feature has a high aspect ratio such as a hole, channel or the like. The removal of the ablated products is thus critical to producing a high quality product.
It has been determined that debris formation is minimized by reducing the laser pulse energy to a value just above the threshold for ablation of the desired material as well as using a pulsed laser to control the delivery of the laser pulse energy. This has been found to reduce significantly the amount of material ablated in each laser pulse, which normally appears as a puff. There is clearly an optimum operating energy range: a high energy pulse will create a large puff and significant debris but a low energy pulse will minimize the puff but the amount of ablated material will be insignificant thus increasing the time for the removal of any structure. Factors to be considered when ablating material are the material to be removed, the laser wavelength, the energy per laser pulse, the number of pulses over a period of time, and the threshold of ablation for the material.
As noted above and in greater detail as shown in
Alternatively, the laser beam can be focused to a gaussian spot and scanned over the sample in the desired pattern.
In further detail of the source 28 of fluid,
In another embodiment of the source 28 of fluid,
In greater detail, system 10 of
The following examples of the quality of the laser ablation by the method of the present invention are only illustrative, and other gases, liquids, and materials may be ablated.
In summary, the laser ablation system 10 is used to remove a material such as chromium from the sample 24 such as a photomask by means of the laser 12 having an ultrashort pulsed laser beam 14. In order to minimize debris, the laser pulse energy is selected to be minimally above the threshold of ablation of the material. This optimizes the amount of material ablated and minimizes the amount of debris created. To aid in the removal of the ablated material, the source 28 of flowing fluid 36 such as a gas or a liquid is positioned over the region to be ablated to further remove the debris formed. Preferably, the source provides a flowing liquid and one which is refractive index matched to the objective lens and/or the material being removed so that high resolution, high aspect structures may be removed and/or altered.
It should be understood that he foregoing description is only illustrative of the invention. Various alternatives and modifications can be devised by those skilled in the art without departing from the invention. Accordingly, the present invention is intended to embrace all such alternatives and variances which fall within the scope of the appended claims.
This application is a divisional of, claims priority to and the benefit of U.S. application Ser. No. 10/041,328, filed on Jan. 7, 2002, which is incorporated by reference herein in its entirety.
Number | Name | Date | Kind |
---|---|---|---|
3991296 | Kojima et al. | Nov 1976 | A |
4027137 | Liedtke | May 1977 | A |
4064308 | Laurin | Dec 1977 | A |
4208101 | Trapp et al. | Jun 1980 | A |
4413020 | McKee et al. | Nov 1983 | A |
4749259 | Ledebuhr | Jun 1988 | A |
4766009 | Imura et al. | Aug 1988 | A |
4906812 | Nied et al. | Mar 1990 | A |
5043556 | Aono et al. | Aug 1991 | A |
5057184 | Gupta et al. | Oct 1991 | A |
5112328 | Taboada et al. | May 1992 | A |
5171995 | Gast et al. | Dec 1992 | A |
5656186 | Mourou et al. | Aug 1997 | A |
6090507 | Grenon et al. | Jul 2000 | A |
6156461 | Grenon et al. | Dec 2000 | A |
6190836 | Grenon et al. | Feb 2001 | B1 |
6262390 | Goland et al. | Jul 2001 | B1 |
6285002 | Ngoi et al. | Sep 2001 | B1 |
6423921 | Beyer et al. | Jul 2002 | B2 |
6496257 | Taniguchi et al. | Dec 2002 | B1 |
6621045 | Liu et al. | Sep 2003 | B1 |
6627355 | Levinson et al. | Sep 2003 | B2 |
7007512 | Kamada et al. | Mar 2006 | B2 |
20010009250 | Herman et al. | Jul 2001 | A1 |
20030121897 | Patton et al. | Jul 2003 | A1 |
Number | Date | Country |
---|---|---|
H09127894 | May 1997 | JP |
Entry |
---|
MARS, Femtosecond laser mask advanced repair system in manufacturing, J. Vac. Soc. Technol. B 17(6), Nov./Dec. 1999, pp. 3137-3143. |
Number | Date | Country | |
---|---|---|---|
20090107964 A1 | Apr 2009 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 10041328 | Jan 2002 | US |
Child | 12241274 | US |