Lithographic technique using laser scanning for fabrication of electronic components and the like

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60412-2080 LITHOGRAPHIC TECHNIQUE USING LASER SCANNING FOR FABRICATION OF ELECTRONIC COMPONENTS AND THE LIKE BACKGROUND OF THE INVENTION Field of the Invention The invention relates generally to the field of lithographic processing techniques and more specifically to techniques uslng lasers for abrieation of eleetronle deviees uslng llthogràphy. The inventive la~er teehniques are partleularly useful in fabrieating sueh components as thin-film magnetic read/write heads for magnetic storage devices for digital data processing systems.

Description of the Prior Art Microlithographic techniques have been advantageously used for a number of years in the fabrication of a number of types of electronic equipment. Such technlques are used, for example, in semieonductor processing, and more recently have been applied to the manufacture of read/write heads used in disk mass data storage units.

In microlithograph fabrication of electronic components, a workpiece, such as a substrate in the 2 83-367CIP-l case of semiconductor processing, is ~irst ~ormed Lithographic technigues are then used to ~oxm the various circult and other roatures in the workpiece In such technigues, various layer~ o~ mat-rial are depo~it~d and th- ~atur~ ~r- outllned thar~ln by means of a photoresi~tive material (~photor~ t~) that is applied and patt-rned in a well-known manner After tho photoresist is patterned, portions o~ the workpiece or selected layers under the region~ not covered by the mask~ ar- removed by chemical or ion beam etching This procedure i~ typically repeated a numb-r o~ times to form the final device A number of problems arise, however, in both chemical and ion beam etching In chemical etching, the chemical- that are used to per~orm th- etch not only r-mov- th- unprotected mat~rial ~rom tho unmasked areas, they also tend to undercut, at least slightly, the portion~ o~ the workpiece directly under the edges of th- masked areas This occurs because, as the etching chemicals remove the unmasked material, the sidewalls of the regionQ directly under the masks are exposed to the chemicals, which also are etched This undercutting limits the size of the ~eatures that can be formed in the device In particular, in designing a device, the designer must take into account the degree . '- . .. .. . 20~8~6~ 3 83-367CIP-l of undercutting that would be expected during device fabrication when he is determining how close ~eatures can b~ and the minimum widths of the ~eatures With ion beam etching, th- ion beam which per~orms S the etch is unldir-etlon~l Aeeordlngly, i~ th- ion b-am i~ directet p-rpendleular to the ~ur~ae- o~ thworkpiece, undereutting does not oecur However, current ion beam etching technigues us- a broad ion beam which is appli-d to the entire workpiece, rather than to a specifie portion of the workpiece As a result, the ion beam not only remov-s material that is not ma~ked, it also cuts into at least th- masking ~aterial itself Accordlngly, care must be taken to ensure that the masks are thick enough 80 that all of the unmasked material that is to b- r0moved is in tact removed be~or- the mask it~el~ ls eompletely tehed away Th- m~sk cannot be arbitrarily thin: it must be at l-a~t thiek enough so that it is not etched away berore the portions of the underlying layer to be etched have been etched to the reguired depth Furthermore, if the mask i5 too thick, it will linit the minimum ~eature size on the workpiece Another problem with ion beam etching techniques is that they use energetic particles, such as atoms or ions, which are applied to the entire workpiece~ When - `~ 203L8r~6~2 4 83-367CIP-l the entire workpiece is so exposed to the energetic particles, it experiences a temperature increase and heat build-up which is undesirable ~or such devices as the magnetic read/write heads Furthermore, with ion ~eam tchlng, o~ten som- small amount o~ th- mat-rial inltially re~oved ~ro~ the workplece ls redepo~lt-d elsewhere on the workplece, which can llmit the ~eature r-solutlon slze possible with the technigue, and can also lnter~ere with proper operation o~ the device in somo circumstances Heroto~ore, lasers have also beon used to etch certain di~icult to etch workpiec- materials such as ceramics and certain polymers, and al~o in tr$~ming such clrcult elements as thin fllm reslstors $n the existing las-r technigues, the laser beam is ~ocu~ed to a tlny ~pot, whloh 1J dlrected onto the surfa¢e o~ a worXplece The spot is moved over the surface o~ the workplece to remove the unwanted material This ellmlnates the need for masking, but it has at least several drawbacks For example, in laser etching the size o~ the spot i~ a lower bound on the size of the ~eatures that can be formed in the workpiece, and so ~or a very small or arbitrarily-shaped ~eature sophisticated optical elements would be needed 2S Furthermore, since in the convent$onal laser technique r - ;2~ r~6~ .. , .. " . . . . . . . ............... _ . .. ... .. .. . . . . . . . ... . . . ..

S 83-367CIP-l only one feature is for~ed at a time, more tim would bo reguired than if the laser could operate on the entir- sur~aca of th workpiece at one time With all thre- t-chnlgu-~, it i~ al~o dl~icult, onc- tching b-gln~, to stop th- tcb to en~ur- that rece~se~ ar- formed whlch hav- predet-rmined depths th~t ar- fairly pr-cisely defined $h- depth of an etched re¢es~ varies not only with the time the etch is applied, but also with the characteristics of the materials being etch-d, and as botween various productlon runs even of nominàlly the same materials, varlatlons in the ~aterlal~ wlll result in varlations ln th- depths of the recesses Summary or the InventiQn Th- lnv~ntion provldes a new ~nd improv-d laser lithographic technlgue for etching a workpiece ~n the new tochniquo, a mask of a materlal that is hlghly refl-ctive in the wavelength~ of the laser to be used is placed on the surface of the workpiece by conventional techniques The laser radiation is then applied to the masked surface o~ the workpiece to remove unmasked workpiece ~aterial Etching may be performed with the workpiece in a liquid bath transparent to the laser radiation For improved performance, the liquid layer can be methylene 201~262 6 60412-2080 chloride, potassium hydroxide, or dilute nitric acid with small amounts of potassium dichromate.

In one aspect a laser scanning protocol includes exposing the surface of the material through a reflective mask layer with a pattern of laser radiation such that material is removed from the workpiece to leave a pattern in the remaining material corresponding to the openings in the reflective mask layer, ~he laser radiation being applied in a plurali~y of overlàpping irradiations ~pulses) to complete a full scan across the lQ workpiece. Preferably each scan is performed about 20 times.

Ater this set oE scans, each next set of scans is applied to overlap with the prior set. Preferable overlap is about onethird of beam dimension. Each scan can be performed in a straight line excursion between the outer dimensions of the workpiece at the location being scanned. The laser can be pulsed, preferably at around 4-5 hertz, having about 5 joules per pulse, and fluence at about 5.5 j/cm , the workpiece being moved at about 0.6 cm/sec.

According to a broad aspect of the invention there is provided a process of etching à pattern in a workpiece by applying laser radiation through a mask having an opening that defines said pattern, the mask being made from a material that is reflective at the wavelengths of the laser to prevent the portions of the workpiece covered by said mask from being etched by the laser radiation, comprising the steps of: applying the laser radiation in a plurality of sets of scans, each one of said sets of scans including producing relative motion between said workpiece and said laser radiation to cause said laser radiation to repeatedly trace a path across an assigned area of said workpiece a selected A 201~262 6a 60412-2080 number of times before another area of said workpiece is scanned in another one of said sets of scans, and performing successive ones of said sets of scans so that said laser radiation applied in adjacent ones of said sets of scans overlaps.

According to another broad aspect of the invention there is provided a process ~or etching a workpiece, under a pulsed laser beam, comprising the steps of: (a) configuring the laser beam as a cylindrical beam ~b) scanning the workpiece in a number o sets of ~can~, each set being pero~méd bys ~i) pulsing the beam on the workpiece at a first location to form a first etch profile, tii) producing relative movement between the workpiece and said laser beam in a selected direction and pulsing the laser to form at a second location a second etch profile that overlaps with the first etch profile, (iii) repeating step (ii) a sufficient number of times to etch the breadth of the workpiece in a strip defined along the selected direction, and (iv) repeating steps (ii) and (iii) a selected number of times for said strip before performing another one of said sets of scans to produce another one of said strips~ and (c) performing successive ones o said sets o scans so adjacent ones of said strips ov~rlap in a second direction.

Brief Description of the Drawinas This invention is pointed out with particularity in the appended claims. The above and further advantages of this invention may be better understood A ~ .

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7 83-367CIP-l by referring to the ~ollowing description taken in con~unction with the accompanying drawings, in which Fig 1, comprising Figs lA through lC, depict the new la~er lithography technigue in accordance with the S invention and Fig 2 depict~ a ~cannlng pattern in accordancwith th- lnvontlon Detall~d D~scription o~ th- Preferxg~ and Illustrative Embodiments With re~erence to the Figures, Fig lA depicts a workpiece 10 which may be used in connection with the new laser lithographic technlque The workpieclnclude~ a ~ubstrate 11 on whlch prior proc--slng may have been p-r~ormed be~ore th- la~er procosslng technigue described herein has begun In the workpiece 10 tepicted on Fig 1, prior processing has been per~ormed to deposit ~ layor 12 on top o~ sub~trste 11 In addltion, ln previous procesJing, various ~eatures and lectronic circuit elements which are not speci~ically shown in Fig 1 may have been formed in substrate 11 and layer 12 by means of conventional processes which form no part of the invention.

In accordance with the invention, a layer 13 is initially deposited on the layer 12, a third layer 14 in which a recess is to be formed by means of Laser 2G18~6~ 8. 83-367CIP-l radiation (represented by downwardly-going arrows 16) is then deposited on layer 13, and a top layer 15 i8 thQn ~ormed over layer 14. ~ayer 15 is patterned to for~ openings 20 (Fig. lB) in the layer, which ser~os to xpoJe portions of underlying layer 14. The l~yer 15 can b- patternod by, ~or xampl-, oonvontional photolithographlc technique- using ch-mical or ion b-a~ etch procedure~. Th- opening~ 20 ar- provided to defln- the ~idewall boundaries of the recesses which ar- to be formed in underlying layer 14. Two such opQnings 20 are depicted in Fig. lB. Th- opsning~ may b< o~ any arbitrary shap-.

Th- laser which will b~ u~ed i~ solQcted 80 that the ~aterial~ which comprise layers 13 and lS are highly re~lective at the wavelength Or the laser radiation. The matorial which compri~e~ lay~r 14 is s~lect-d to hav~ low rèfloctivity, and also low trans~iJslvity, at the wavelength of the laser radiation. AS shown in Fig. lC, since layer 15 is highly reflective at the wavelengths of the incident laser radiation 16, layer 15 reflects laser radiation as represented by arrows 17 and thus is not effected by the radiation. However, layer 14 does not reflect the radiation, and thus the regions exposed by openings 20 absorb the radiation and are sffectively vaporized 20~L8r~2 9. 83-367CIP-l thereby and thus removed to form recQsses 21. The removal o~ the exposed portions of layer 14 continues until the underlying portions of re~lectlve layer 13 are expos~d. ~ayer 13, likQ layer lS, reflQcts the S l~ser radlation, as represented by arrows 18, and ls also una~ected thor-by.

Thus, the pattern o~ layer lS d-termines the shap~ ~as viewed ~rom a direction orthogonal to the exposed surface of layer 15) o~ the recess in layer 14, and layer 13 e~octively ~erves to determine the maximu~ dep~h o~ the recess in the workpiece by preventing las-r radiation ~rom impinging on layer 12.

Accordingly, it is apparent that the recess will not extend into layer 12 or substrate 11.

While the pattern Or layer 15 has been de wribed as being ~ormed in ~ltu, that is, while layer lS has been in place on the workpiece, it will be appreciated by those skilled in the art that layer lS may comprise a mask which ha~ been patterned prior to being placed on layer 14.

It will be appreciated that in certain circumstances it may be undesirable for the etch-stop layer 13 to extend throughout the entire workpiece lo.

For example, i~ copper is selected as the layer 13, and i~ layer 13 extends throughout the workpiece, ~he Z~3L8r~ 83-367CIP-l copper would ac~ a~ an electrical conductor throughout the entire workpiece If the workpiece is to have electrical connections through the openings 21 in layer 14, it would clearly be undQsirable ~or layer 13 to extend to all o~ th- opening~ mus, it may bneces~ary to also pattern otch-stop l~y r 13 o that the lay-r e~ecti~ly complementg the oponing- in lay-r 15.

Thi~ vould ~ut~ice to el~minat~ ctrical conduction paths through layer 13 betwoen th- opening~ 21 The material~ ~elected ~or lay-rs 13, 14 ~nd lS depend upon th- la~-r to b~ used in tha process, or alternatively, tho laser ~olected for u~o in thpraces~ dependJ on the types Or ~at-rlals which may be required for tho workpiece In ono particular examplo, the substrato 11 may compri~e ~ high den~ity c-ramlc sub~trato having about seventy percent alumina ~A1203) and thirty percent titanium carbide, and layer 12 may comprise alumina, and it is desired to produce a recess in a layer 14 also comprised of alumina Continuing with the aforementioned example, a carbon dioxide (C02) laser may effectively be used since the absorption by alumina o~ the carbon dioxide laser radiation is very high; that i5, the alumina comprising layer 14 readily absorbs radiation in the 2~18,~6~ 11 83-367CIP-l wavelengths emitted by the carbon dioxide laser, and thus the exposed areas of layer 14 will effectively be evaporated by the la~-r Suitable material ~or layers 13 and 15 ln that example aro copper and gold, both of which re~l-ct on the order o~ nlnety-elght p-rc-nt o~ r~dlation ln the wavelength~ produced by carbon dioxlde lasers In one partlcular example, layer 13 may be gold and layer 15 may b- copper, with both materials being deposited on th- respective underlying layers by means of ~puttering, and with the copper layer 15 being easily patterned by means o~ ion beam or chemical etching technigues It will b- appreciated that this method provides a number of bene~lt~ over conventional etching methods In particular, th- laser etching typically r-mov-a unwanted mat~rial much ~ster than c~n be achleved by mean~ o~ chemical etching technigues and with none o~ the undercutting problems that are present The new laser techniqu- may cause some minor deformations due to thermal energy being conducted in the vicinity of the openings in the worXpiece outside of the region being removed, and further to resolidi~ication of some of the melted material, but these can be minimized as explained below - 2~8~6;~:

12 83-367CIP-l The new laser etching technique doe~ not rely on di~erential etch rates between the ma~king material and the material to be etched, a~ do ion beam tching technigues Accordingly, the minimum thickne~s or the mask used in th- laser technigu- is not r-lat-d to tho thiakness o~ th- rec-J~ to be etahed, a- i8 th- ¢a~- in connectlon with ion beam technigues Tho re~l-ctivlayers u~ed in th- laser etching technigu- must be o~ sur~icient thi¢kness to be rerlectiv- over the sur~ac of th- workpiec- ln the areas not to be etched Furthermore, the new laser etching technigue does not require ~ocusing or the las-r beam to a Dmall spot and moving it over the sur~ace o~ the workpiece to de~ine the reguired ~-atures, as is n-cessary in present laser etching tochnique~ Thus, the sophlsticated optlcal ~y-tem~ charaat-rlstla o~ present laser teahnl~u-s are not requir-d in the new technigue In addition, the minimum ~eature size is not related to the ~ize o~ the la~er spot, and the workpiece can be processed at one time since the new technique allows the entire sur~ace o~ the workpiece to be processed at one time, ~or a reasonably small workpiece As has been noted, recesses formed by the new laser lithographic technique may be slightly de~ormed due to heating o~ the workpiece outside the region ,~ 2018r~6~ 13. 83-367CIP-l being removed, and also due to resolidification Or material which was heated by the laser but not evaporated, which could limit the resolution of the work. In additlon, some metal and ceramic materials may defor~ and som- c-ramic material~ may crack under lntens- laser radiation. However, theso probl-~ can b- minimized by immer-ing th- workpiece in ~ liquid, or providing a layer of liquid over the irradiated surface of th- worXpiece, whil- the las-r i- irradiating the surfacQ. The llguid can act both to cool the workpi-ce and, depending on the nature Or the liguid, may also either dissolve, by chemical action, or flu~h away, by mechanical action, debri~ that iJ thrown up from the worXpiece while the la~er is entrained thereon.

AJ will be appreciated by one JXilled in the ~rt, the selection of a Juitabl- liquid wlll depend on a number of factor~. In particular, a suitable liquid shoula be fairly transparent to the laser radiation and should not react with the masking material (that is, layers 13 and lS in Fig. 1). It is also preferable that, if the liguid reacts with the material being etched (that is, layer 14 in Fig. 1) at all, it should react only very slowly at room temperature, so that the workpiece itself not be etched by the liquid outside of the area on which the laser beam is impinging. .

2018r~ 14. 83-367C~P-l If the liquid reacts with the material to be etched at olevated temperatures, which would be present at the areas illuminated by the laser radiation, it may assist the tch op-ration, e~ectively perforning a chemical etch on th- mater~al ln the area b-ing struck by the laser. Sinc- the temperature o~ the portion~ of the matQrial that do not directly receiv- laser radiation will not be increased as much a~ the portions that do, they will not be etched as much by the liquid.

The resulting etch by the liguid, which is offectiv-ly a chemical etch, would be more anisotropic than is a conventional chemical etch.

EXAMPLES Ex~mRlç No. 1 Etching of Alumina by C0~ ~aser An ~lu~ina layer w~s ~ormsd on a substrate, and a 200 Angstro~ layer of chromium was deposited by sputtering. The chromium layer was provided to act as an adhesion layer for the next layer, which ~as gold (alternatively, copper could have been used). The gold layer, which served as layer 13 (Fig. 1) was one-half micron thick. A sheet of alumina approximately thirty to forty microns thick was then deposited by sputtering to form layer 14, and a three-tenths to five-tenths 2~3~8~6~:

83-367CIP-l micron thick layer of copper (alternatively gold could have been used) was sputtered as layer 15 The copper layer (15) wa~ then patterned by conventional photolithographic technigue~ In on S cas-, a lay r ot photoresi~t was depo~it-d on top of the copper lay-r and patterned in ~ conv-ntlonal manner expo~lng a p~tt~rn o~ the coppor lay~r und-rn-ath The xposed copper was tched by an ion beau etch and any photoresist was disi~olved in a developer This leave~ the op-nings t20, Fig 1) exposing alumina in layer 14 In another cas-, th- copper layer 15 wa~ patterned using a conventlonal li~t-o~ techniqu- In that technique, the photoresist layer was depo~ited be~ore the copp-r lay-r ~the photoresist lay r i8 not shown in Pig 1) and a pattern in the photoresist was exposed in a convontional photolithography step A thin copper layer wao th-n ~putter deposit~d on top o~ th~ workplec- lncludlng the photoresist, and then the pattern~d photorQsist was dissolved in a developQr The disisolving photoresist took with it the copper directly on top o~ it, leaving the copper in the desired pattern After the copper layer 15 was patterned, the workpiece was covered by a thin film of methylene - 25 chloride liquid and irradiated using a pulsed carbon . , ~ . ,~j,.

- 2~L8r~6~2 16. 83-367CIP-l dioxide laser to etch the exposed alumina. ~hQ energy supplied by the laser was about four ~oule~ per laser pulse at four to ten pulses per second over an area of approximately one-~ourth sguare inch.

E~m~le No. 2 Etchinq U~lng A Re~ovabl- Ma~X In this xampl-, the mask compri~ing layer 15 wa~ not depo~lted onto th- workpiece, but lnstead was ~ormed soparately and placed onto the ~urface o~ the workpioce to be otched. A workpiece was rormed of alumina. A base ma~k was ~ormed of generally planar nickel, with opening~ through whlch the workpiece could be expo~ed.

The mask had a thicknes~ o~ about fi~teen microns in the areas ad~acent the openings, and elsewhero a thicXness o~ about 125 micron~, the thick portion providing m-chanlcal sturdlne~ whlle the thin portion allow-d ~or ~etter rosolution in ~llgnment o~ the ~ask over the workpiece.

To prevent chemical interaction between the mas~ and a liguid which might be used, the masX was plated with a ten micron layer of gold.

The masX was then aligned with the worXpiece and both were clamped together in a fixture.

Methylene chloride liguid was then sprayed onto the fixture to form a uniform thin layer on the surface which would receive the laser radiation.

2018~.6~ 17. 83-367CIP-l The workpiec~ was then illuminated by a CO2 laser.

To increase the energy per unit area of the laser (which had about four ~oules per pulse), the laser beam was focu~ed to ~ slz- of about on--fourth inch by one lnch by ~ean~ of len~es, and th- workplec- wa~ ~o~ed under the laser bea~ at a rate o~ ~lx-thousandth~ of an inch per second untll the entire surfac- of the workpiece had been Qxpos~ed through the mask. $he procQs~ was repeated twenty times to for~ recesses in the alumina havlng a depth of approxlmat-ly thirty-five microns .

After the process was concluded, th- mask was removed from th- workpiece by unclamping the flxture.

$he mask could be used in a subsequent etchlng process.

E~a~ g~_l Etchlng o~ High-Denslty Ceramlc A workpiece was fabricated of hlgh-density ceramic having a patterned layer o~ copper to dsfine the pattern to be etched. Carbon dioxide, ruby and Nd:YAG lasers were used to per~orm the etch. When the etch was per~ormsd in air, that is, when no liguid was present, small cracks developed in the ceramic and some ceramic debris ~rom the etch resolidified.

In other trials using high-density ceramic, several liquids were used, including methylene shloride Z~18r~6~ 18 83-367CIP-1 and a solution of potassium hydroxide in water The potassium hydroxide solution was generally ~ati~factory for the Nd YAG and ruby lasers, even though for some depths o~ liquid it absorbed about thirty-rive percent of the radiation o~ th- Nd YAG la~er Th- pr-~-rred concentration o~ th- potaJ~ium hydroxid- wa~ on thorder o~ twelv- normal ~12N) or abovet trial tche~ in solutlon~ having concentrations o~ on the order o~ ~ix normal or le~ xhibitsd some cracking Or th- ceramic ~xa~ple No 4 Etching of Permalloy A workpiece was pr pared comprlJing an Alsimag substrat- on which a three thousand Angstrom thick layer o~ aluminum wa~ deposited by sputt-ring The aluminu~ served ag a etch-stop layer A two thousand Angstrom thick layer o~ permalloy wa~ then platod onto th~ aluminu~ ~heet An aluminum masX was formed on the per~alloy layer using a li~t-ofr technique The workpiece wa~ then irradiated, in air, with a krypton ~luoride laser The permalloy was etched without affecting the aluminum mask or the etch-stop layer In another trial, a solut$on of dilute nitric acid with small amounts of potassium dichromate was used The resulting etch had less resolidification of molten 201~ir~6~2 19. 83-367CIP-l permalloy than had occurred in the etch without thliquid.

ExamDle No. S Etching of Polymer A thin film of copper was deposited on a ilicon 3ubstrat- a~ an tch-stop lay-r ~13, Flg. 1). A lay-r of photoresl-t wa~ deposited on the copp-r lay-r and baked hard. A portion o~ the photoresist layer was exposed to ruby laser radiation through a hole in a ~0 removable ~talnless steel mask.

The laser beam had an ef~ective diameter of about 3 millimeters, and th- holln the mask had a diameter of about 40 microns.

The portion o~ th- photoresist struck by the lasor wa~ectlvely d-composed into volatile parts, and so no resolidification occurred.

The copper efrectively stopped the etch, but was somewhat de~ormed by the high energy o~ the ruby laaer radiation.

Scannina Techniques It has been found to be advantageous in some cases to scan the workpiece under laser irradiation.

Hence, the workpiece scans, for example, horizontally for a selected number of times for each vertical location (where horizontal and vertical describe X and Y locations in a working plane).

This minimizes heat Z01~6~ 83-367C~P-l build up while providing statistically even irradiat~on on a given workpiece A pulsed Co2 laser with cylindrical beam ig preferred The focused cylindrical beam aids in mixing of la~er modes as will yield a homogeniz-d beam by compres~ing the modes ln such a manner as to mix thmod-s Each scan m~y be compris~d o~ a eri-s o~ ovsrlapplng beam pro~ePtions for greater uniformity of illumination Hence, we can avoid uneven etching o~ alumina and can prevent damage to the mask and stop layer For exampl-, we successfully opened bonding pads in aluoina approximat-ly 30~ thick using a C02 laser and a methylen- chloride bath In that cas-, the ~ollowing laser parameters were found to yield desirable resultJ 5 ~oules per pulse, fluence at about S 5 ~/c~2, pulse rate of ~bout 4 hertz, 20 scans p-r address, and scan rate o~ about 0 6 cm/sec our laser beao spot area was about 0 9 cmZ and the bea~ shape was oval The spot was obtained at the focal point of a cylindrical lens of F L 12cm After every set Or 20 ~can~ the beam spot was shifted by 0 35cm so as to insure overlap of the irradiated areas, the length of the beam spot was about 2 cm The total scan time ~or workin~ on a full three inch diameter wa~er 2~18r~ 21. 83-367CIP-1 wa~ about two hours and 50 minutes. These conditions led to co~pleto roooval o~ alumina without reguiring rurther etching, chemical or otherwise. In such case, wire bonding can proceed directly on th- xposed pad ~urfaces.

We move the wor~piece through th- pulsea and already homogonized laser Jpot in a mann-r so as to achi-vo tatistically uniform int-nsity over the ntirsurface to b- etched. This will be appreciated with referenc- to Fig. 2. ~he workpiece fir-t scans horizontally along the x-axis having th- pulsed laser spot imping- upon the workpiece at vertical address A ~on the y-axis). The worXpiece is then incremented to the next addr 8~.

These horizontal scans ~re per~ormed ln step~ or increments, ~long the x-axis. For exampl-, in ono set of scans, the workpiece is moved to the step "1" location, the laser is pulsed, the workpiece is moved ! to the step ~2" location, the laser is pulsed, the workpiece is moved to the step "3" location, the laser is pulsed, and etc., until a ~ull scan of the entire workpiece at address A is completed. In this process, the irradiated areas overlap along the x-axis. Hence it will be appreciated that Fig. 2 shows an incompletely scanned workpiece with areas that have Z~18r~6~2 22 83-367CIP-l been fully overlapped (3X) and partly overlapped (2X) and (lX), in a one-third overlap process, as an example, along address A After a horizontal scan i8 completed, it is preferably repeated another 19 times Whon thl~ sot o~ 20 scan9 ls complete, th- workpi-c- i9 incr mented to vertloal addre~s B, wh-reupon a eaond set of ~cans 1~ p-r~ormed 20 times Th- same occurs at addres~ C, tc Pr ferably vertical addresse~ A, B, C, ar~ cted to achieve a one-third overlap of scan sets Horizontal overlap can b- controlled by scan speed of th- workpiece and vertical overlap by increment ~iz-, for a glven puls- rat- and ~pot ~ize In addition, we were able to reduce scan tine by designing the ~can excursion $n view of th- outer dimensions of the workplece Hence, a workpiece can be scanned with a correspondingly designed or li~ited ~can ex¢ursion Th- rOregoing description has been limited to specific embodiments of this invention It will be understood, however, that variations and modifications may be made to the process, with the attainment of some or all of the advantages of the i-nvention Therefore, it is the object of the appended claims to cover all - 2a~ 3r~6~2 23. 83-367CIP-l such variations and modi~ications as come within the spirit and scope o~ the invention.

We claim: