Patent Number: 053393465
Section: description

DEFINITIONS Plasma Source--A thermally-produced plasma for yielding x-ray radiation--generally pumped by a high power pulsed laser. PA0 Illumination Radiation--The delineating radiation as incident on and producing an PA0 Illumination Field on the mask, characterized by intensity, direction, divergence and spectral width. PA0 Divergence--As used by itself, the term refers to mask divergence, i.e., the largest angle about the axis of the cone of radiation as incident on the mask. In projection, the axis is generally a few degrees off normal incidence as required for reflection masking. The magnitude of divergence required in projection is that needed to reduce ringing at feature edges to the extent necessary for desired resolution and contrast. In full-field exposure, divergence should be similar at every illumination point. In scanning, some non-uniformity in the scanning direction may be averaged out. PA0 Condenser--Optical system for collecting radiation from the plasma source, for processing the radiation to produce a ringfield illumination field, and for illuminating the mask. PA0 Collecting Optics (or Collector)--The Optics within the condenser responsible for collecting the plasma-derived radiation. The collector has a focus. PA0 Processing Optics--Optics, in addition to the collecting optics, within the condenser for processing collected radiation for delivery to the mask. PA0 Imaging Optics--Optics following the condenser responsible for delivering mask-modulated radiation to the wafer, i.e. the camera optics. PA0 Camera Pupil--Real or virtual aperture which defines the position through which illumination radiation must enter the camera, of angular size defining the diffraction limit of the camera. Its physical size is that of an image of the real limiting aperture of the camera. PA0 Lens--The term is used in this description to define any optical element which causes x-ray radiation to converge or diverge. "Lenses", in x-ray systems, are generally reflecting--are sometimes referred to as "mirrors". contemplated lenses may be multi-faceted or may be non-faceted, i.e. continuous--e.g., of ellipsoidal or other curvature. The convergence or divergence is a result of action analogous to that of a transmission optical lens. PA0 Facet--Individual segment of a lens--either a separate element, or part of a monolithic structure, which, generally in concert with other facets, is responsible for convergence or divergence of the radiation. Individual facets may be planar or curved. PA0 Scatter Plate--Optical element for increasing divergence. Divergence may be in one or two dimensions. PA0 General--There is a continuing effort directed to development of x-ray plasma sources for pattern delineation at feature sizes .ltoreq.0.25 .mu.m. See, W. T. Silfvast, M. C. Richardson, H. Binder, A. Hanzo, V. Yanovsky, F. Jin, and J. Thorpe, "Laser-Produced Plasmas for Soft-X-ray Projection Lithography" J. Vac. Sci. Tech. B 106, Nov./Dec. 1992, pp. 3126-3133. By its nature, emission from a plasma source is omnidirectional. Device fabrication of this invention depends upon a condenser designed to capture this omnidirectional emission and to shape it to produce a high-aspect ratio illumination field for ringfield projection lithography. PA0 The Drawing--Detailed design and processing information is discussed in conjunction with the figures. DETAILED DESCRIPTION In addition to shaping, directing, and tailoring divergence, the condenser must filter the natural plasma spectrum of perhaps .lambda.=50 .ANG.-400 .ANG. to yield the favored ringfield wavelength range within a spectrum of .lambda.=100 .ANG.-200 .ANG. (at this time the preferred spectral range is .lambda.=125 .ANG.-140 .ANG.). Use of this "soft x-ray projection lithography" (SXPL) takes advantage of ability to make high reflectivity normal incidence mirrors. It also expedites use of glancing mirror optics, in permitting larger angles of incidence than those required for the "hard x-ray" used in proximity printing. Filtration, to yield the desired x-ray spectrum, will likely use multi-layer reflectors (MLR) operating on the Distributed Bragg Reflector (DBR) principle. In FIG. 1a YAG or excimer laser 11 emits a beam 12 which is focused by lens 13 to heat a spot 14 on target material 15, thereby yielding plasma ball 16 which emits x-rays 17. Radiation is emitted over an entire 180.degree. half sphere. FIG. 2 is a perspective view of a state-of-the-art system for using a plasma source for powering a projection camera. Plasma source 21 emits a half sphere of x-ray radiation shown as rays 22. An MLR 23 focuses radiation at focus 24 on mask 25. The illumination field is an image of the source. As depicted, the illumination field is a spot 24 incident on mask 25, where the radiation is either transmitted or reflected to be introduced into camera 26 by partially filling entrance pupil 27. For the proper pupil fill shown only a relatively small cone of radiation is collected, and radiation outside this cone is wasted. If the size of the condenser is increased in order to collect the relatively large angle radiation represented rays 28, the camera pupil is greatly overfilled as shown by field 29, produced by the condenser-emitted rays shown as broken lines. Energy is wasted and the image is degraded. Neither arrangement produces a ringfield illumination field. FIGS. 3 and 4 show an illustrative system for effectively producing the high-aspect ratio illumination field for ringfield projection. FIG. 3, an "elevational" view illustrates processing to deliver the short dimension of the high-aspect-ratio field. Plasma 31, produced by laser beam 30 emits x-rays 32 over a wide angle, near-half sphere, which is captured by lens facets 33. While not seen in this view, most or all of facets 33 are members of paired complementary facets, common to all collectors used in the inventive processing. An aperture can be placed in the beam path, either at position 91 or 92 in FIG. 3, (.about.93 or 94 in FIG. 4). The aperture can block part of the beam to produce greater uniformity in intensity on the mask, if needed. If ellipsoidal, the first focus may conveniently correspond with the source, and the second focus may correspond with the image. The curved facet surface may be of "Lopez" form. The Lopez mirror is explicity designed to produce a single focus for many-angled emission. Its use for the individual facets of the multi-faceted collector lens may be justified. Each of the facets may be viewed as having an effective height comparable to that of mirror 23 in FIG. 2 to produce a field dimension in the scanning direction which is the same as that of a spot 24. Each of the facets focuses an image of source 31 as image 34 on lens 35. Lens 35 is a many-faceted mirror which directs reflected radiation and overlaps individual beams at processing optic 36. Mirror 37, likely a single, continuous surface, concave lens, is a redirecting optic. The several images are brought to a common focus at or near mask 38 and are directed to enter camera pupil 39. Companion FIG. 4 shows illumination of the transverse (or long dimension) of the high-aspect-ratio ringfield. Laser plasma radiation from source 40 is collected by the array of ellipsoidal mirrors, here shown as paired facets 41a-41b. The collector focuses an image of the source to a series of spots on processing lens (mirror array) 42, with individual spots made incident on individual facets of lens 42. The facets of lens 42 are oriented such that the center ray of the reflected beam strikes the center of the processing lens 43 which is again a multi-faceted array in this example, but may be a continuous curved surface such as a cylindrical mirror or an ellipsoidal or toroidal mirror. The distance between the processing lens 42 and processing lens 43 is such that the processed radiation emitted by lens 42 covers the length of lens 43. Lens 43 in conjunction with lens 37 of FIG. 3, together, shape the beam to produce the proper arc shape illumination field 44 as incident on mask 45. The same optics introduce the convergence shown upon reflection from mask 45 to produce the desired fill of entrance pupil 46. The multi-faceted lens 50 shown in FIG. 5 is illustrative of optics serving the function of lens 42 of FIG. 4. Lens 50 is constituted of 8 facets 51 oriented such that incoming cones of radiation 52 are reflected as cones 54 toward the processing optics. The aspect-ratio of facets 51 may approximate that of the desired illumination field--image dimension 53 corresponding with the long dimension of facet 51. In FIG. 6a, collector facets 60 are arranged to have a quadrupole distribution, to focus into two series of spots on multi-faceted lens 61 (e.g. corresponding with lens 42 of FIG. 4). In FIG. 6b, it is seen that facets 61 are split along their length so that each consists of two facets 62, oriented at different angles to result in radiation being reflected in two slightly different directions 63 in the vertical or scanning direction. Viewed from FIG. 6c, radiation upon reaching the pupil is split into four separate multi-image fields 64, 65, 66 and 67. FIGS. 7a-7d show various collector lens designs, always including paired complementary facets. Discrete compensating facets separate lens functions and facilitate design. Members of pairs, always producing equal and opposite intensity gradients, to, together, produce a composite image which is evenly illuminated in the compensating direction, are independently directed to suit the camera optics. Illumination in the compensating direction is at least .+-.15%. Careful facet placement results in .+-.5% or even .+-.1% or better. In FIG. 7a, the lens array 70 is constituted primarily of paired facets 71a-71b. Facets 71c, positioned at the extremities of the emission sphere, are not paired. Pairing, here to, is preferred in principle, but any intensity gradients may be small enough to be ignored. In general, single-faceted mirrors over the final 65.degree.-75.degree. of emission in this direction are tolerable. (Consistent with usual practice, angles are measured relative to the optic axis.) As in all arrangements, members of paired facets are symmetrically placed about source 75. In FIG. 7b, collector lens 72 is constituted of five pairs of facets 72a-72b. This arrangement may result in a somewhat smaller aspect-ratio slit than the 7-tier arrangement of FIG. 7a. The variations of FIGS. 7c and 7d are trivial. For the four-tier arrangement of facets 73a-73b, the horizontal center line of spot source 75 is naturally located at the intercept of two pairs. It is of little importance that source-to-facet spacing is different in the two dimensions--it is desirable only that each dimension spacing by symmetrical. Collector lens 74 is a three-tier array of paired facets 74a-74b. Illustrative facet aspect-ratio may be suited to a similarly shaped illumination field. FIG. 7e is an elevational (or side) view of the arrangement of FIG. 7b, showing stacked facets 72a. The facet arrangements shown are based on minimal facet count. The inventive requirements may be met by higher count arrangements. As an example, lateral faceting may involve four rather than two facets, providing that inner and outer pairs produce the required evenly-illuminated composite field image. Should there be reason to do it, it is required only that the entire lateral set produce such a field image (so that neither the inner nor the outer pair is completely self-compensating). FIGS. 8a and 8b are plan and vertical views, respectively, showing a three-lens condenser system used as the basis for Example 1. Collector includes five paired facets of the arrangement shown in FIG. 7b. The facets are MLRs, consisting e.g. of 40 paired Mo-Si layers. The radiation passes through a window 88 that keeps dirt produced by the plasma from damaging the mirrors of the camera 86. The first processing lens 81, a grazing incidence multi-faceted mirror, directs the radiation to processing lens 82 which combines the functions of vertical processing lens 37 of FIG. 3, and horizontal processing lens 43 of FIG. 4. Processed radiation as leaving lens 82 produces arc-shaped illumination field 83 on mask 84, which in turn, creates an image of the arc on wafer 87 via reflection into camera pupil 85 of camera 86. Device Fabrication--Basic device fabrication is not otherwise altered. Reference may be made to a number of texts, e.g. Simon Sze, VLSI Technology, McGraw Hill, 1983. The following examples 1 and 2 are directed to the critical window level in MOS VLSI device fabrication. Example 1--Fabrication of a 256 mbit, 0.1 .mu.m design rule MOS device is illustrated by fabrication at the window level as follows: The apparatus of FIGS. 8a and 8b is provided with a plasma source of 500 watt emission consisting of a 500 watt YAG laser-pumped tin source. The collector lens of the arrangement of lens 80 consists of eight 35 mm.times.90 mm multi-layered facets, each containing 40 pairs of successive Mo-Si layers, to result in focused beams of .lambda.=135.+-.3 .ANG. of total power 2.5 watts. As received by wafer 87, the ringfield scanning line is of dimensions. 1 mm in the scanning direction and 25 mm as measured along the chord of the arcuate line. Example 2--The x-rays projection camera is of the family designed by Jewell. (See U.S. patent application Ser. No. 07/732,559, filed Jul. 16, 1991.) It has a numerical aperture of 0.1 and is capable of printing 0.1 micron lines. In the first applications it will be used only for the critical levels, e.g. the gate and the contact windows. Other printers, e.g., deep UV, will print other levels. In later models, when the numerical aperture has been increased to 0.2, it will print critical levels with 0.05 micron features and also many other levels--the other levels will have 0.1-0.15 micron features that are too small to be printed even by Deep UV. Suppose 1 watt strikes the mask of the gate level. Due to losses in the mirrors of the camera, a thin silicon window (0.3 .mu.m thick) between the wafer and the camera, only 75 .mu.m (or less, depending on how much of the mask is reflective) arrive on the wafer. The wafer has patterning from previous levels. Immediately before the lithography, the wafer was coated with a very thin oxide layer, a polysilicon conductor and on top, a thick oxide layer. An x-ray resist covers the whole wafer. The wafer is placed under the x-ray projector, aligned, and exposed. If the resist has a sensitivity of 15 mj/cm.sup.2, 5 cm.sup.2 will be exposed each second. The resist is developed, and, where there is no resist, the top oxide and polysilicon layers are removed by dry etching, leaving the very thin oxide layer on the bottom intact. Later an ion beam implants dopants through the thin oxide into the silicon, forming conductive layers that act as source and drain regions. The region of silicon under the polysilicon gate remains resistive, and will conduct only when a voltage is applied to the gate.