TECHNICAL FIELD OF THE INVENTION

The present invention relates to lithographic techniques for producing images of masks and, more particularly, . to an apparatus and method for focusing hard X-rays and gamma rays to project a reduced image of a mask.

BACKGROUND OF THE INVENTION

One of the steps in producing integrated circuit semiconductor chips is to project the image defined by a mask onto the surface of a semiconductor wafer. In order to achieve greater miniaturization of the integrated circuits of these chips methods have been sought to project smaller mask images while maintaining sharp and precise circuit lines. To achieve this end, lithographic techniques progressed from the use of visible and ultra-violet electromagnetic energy to "soft X-rays." Soft X-rays occupy that portion of the electromagnetic spectrum just above ultra-violet energy. The shorter wavelength of soft X-rays makes possible the projection of smaller mask images.

^■ Hard X-rays have shorter wavelengths than soft X-rays and occupy that portion of the electromagnetic spectrum above soft X- rays. Gamma rays have wavelengths shorter than hard X-rays and occupy that part of the electromagnetic spectrum above hard X-rays. Thus, it would be desirable to utilize hard X-rays and gamma rays to project mask images to produce more minute chip circuitry. ^{' '} A problem in attempting to use these shorter-wavelength

electromagnetic energies (hard X-rays and gamma rays) is that useful manipulation is difficult because of the shorter wavelengths and high electrical ^' energies involved. Standard focusing mechanisms, such as lenses and prisms, are ineffective.

SUMMARY OF THE INVENTION

It is an object of the invention to provide a means for using hard X-rays and gamma rays to project a mask image onto a surface.

It is a further object of the invention to provide a means to collimate diffuse hard X-ray or gamma ray beams and convergently focus these collimated beams to project a reduced mask image.

The present invention teaches the use of a dislocation-free, composite-substance crystal having a lattice constant which decreases over the length of the crystal to convergently focus beams of hard X-rays or gamma rays. The invention also teaches the use of a dislocation-free, single-substance, crystal to collimate diffuse beams of hard X-rays or gamma rays and, in turn, to project the collimated radiation to the composite crystal. A mask is interposed between the "collimating crystal" and the "focusing crystal." The focusing crystal produces convergent hard X-rays or gamma rays to focus a reduced image of the mask upon a desired surface, namely, a wafer. The invention further teaches as a focusing crystal a substantially dislocation-free silicon-germanium crystal wherein the proportion of germanium to silicon varies over the length of the silicon germanium crystal from about 100 percent germanium to about 100 percent silicon.

Other aspects, objects, features, and advantages of the present invention will become apparent to those skilled in the art upon reading the detailed description of preferred embodiments in conjunction with the accompanying drawings and appended claims.

BRIEF DESCRIPTION OF THE DRAWINGS

Fig. 1 is a representation of a crystal illustrating principles utilized in the teachings of the invention.

Fig. 2 is a representation of a composite-substance crystal illustrating teachings of the invention. Fig. 3 is a schematic representation of an apparatus and method for convergently focusing hard X-rays or gamma rays to project a reduced mask image embodying teachings of the present invention.

DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS OF THE INVENTION

While the specification concludes with claims particularly pointing out and distinctly claiming the subject matter which is regarded as the present invention, the invention will now be described with reference to the following description of an embodiment taken in conjunction with the accompanying drawings. The broad technique taught by the invention is the manipulation of high energy, very small wavelength electromagnetic radiation. While this manipulation is suitable for many uses, it is particularly applicable to further teachings of the invention which are directed to the creation of mask images.

The invention manipulates hard X-rays and gamma rays for useful purposes by collimating and convergently focusing beams of these rays. Although ^' most of the principles which form the foundation for the invention, which are described below, refer to X-ray phenomena, the teachings of the invention are equally applicable to the shorter wavelength radiation of gamma rays. Hard X-rays are considered to be those X-rays having electrical energy in the range of from 1 to 100 keV. The invention utilizes crystals to perform the collimating and focusing functions. For convenience, for the purposes of describing the invention, the crystals are referred to as a collimating crystal and a focusing crystal.

The invention's utilization of crystals as manipulating lenses is based upon the X-ray diffractive-properties of crystals. In general, X-rays striking a crystal are absorbed by the crystal. However, the diffraction of X-rays occurs when they strike a crystal at a particular angle with respect to the lattice structure of the crystal. In such instances, the X-rays are passed through the crystal, exiting at a particular angle. This propagation through the crystal occurs because the rays are internally reflected by the latticework of the crystal. This phenomenon is known as the Bragg condition and is quantitatively expressed as Bragg's Law or the Bragg equation, namely,

(n) (lambda) = 2 (d) sin b where n is an integer,

lambda is the wavelength of the X-ray, d is the lattice constant, or distance between the reflecting layers of the crystal, and b is the angle of incidence of the ray with respect to the lattice layer.

Reference is now made to Fig. 1 in which the operation of the collimating crystal 10 employing the diffraction phenomenon is illustrated. The collimating crystal 10 utilizes the Borrmann effect caused by the Bragg condition in crystals to project a beam of hard X-rays or gamma rays from a diffuse ray source. ^' The Borrmann effect in crystals is also known as anomalous transmission. When the Bragg condition, that is the Bragg equation, is satisfied in dislocation-free crystals, the Borrmann effect is manifested as a drastic reduction (for example by a factor of 200) of the absorption coefficient. A reduction in the absorption coefficient means that more of the electromagnetic energy exits the crystal. The term "dislocation-free" refers to the absence of "dislocations" in the lattice structure. Dislocations are imperfections in the lattice that alter the geometric structure and adversely affect energy propagation therethrough. In Fig. 1, an incident ray 11 is shown entering the crystal 10 at an angle of incidence 13, or b, with respect to the lattice planes or layers 12 of the crystal 10. The lattice layers 12 are separated by the distance referred to above as the lattice constant or lattice spacing d or 14. When the Bragg condition is satisfied, the angle of incidence b, or 13, may also be referred to

as the Bragg angle. The Borrmann effect is demonstrated by the transmission of beams shown in positions 15, 17 and 19. The transmitted radiation is split into two equal intensity parts separated by the angle 2b . Beams at positions 15 and 17 are the anomalously-transmitted radiation. Those positions are known as the rearward diffracted beam and forward diffracted beam, respectively. The third component 19 is unaltered transmitted radiation. It is weak compared with the anomalously transmitted radiation. The angular width of the Borrmann effect is about 10 ^*5 radians, or about one arc second. Therefore, the anomalous transmission of hard X-rays or gamma rays through a dislocation free crystal produces a very well collimated beam of radiation 11' . The above principles and phenomena are also utilized in the teachings of the invention directed to focusing hard X-rays and gamma rays. The teachings directed to the use of a focusing crystal are based upon a further phenomenon associated with the above Borrmann and Bragg principles, namely, that when a crystal is distorted the propagated X-radiation may produce a converging or diverging beam. The mechanical flexing of a crystal produces a cylindrically-focused beam. The crystal lattice may also be distorted by heating one end and cooling the other end of the crystal, or by mechanical force, such as the application of radial force on one end of the crystal. For a crystal 10 cm in length, " the effects produced would be small, that is, approximately 10 ^'3 radians for a pressure of 1,000 atmospheres applied to one end of the crystal, or 10 ^"4 radians for a 400 degree temperature difference

along the crystal. Another effective way to convergently or divergently focus short wavelength radiation is to produce a crystal with a varying lattice constant, or spacing between planes. Referring now to Fig. 2, therein is represented an example of a focusing crystal 20 which has a varying lattice constant over its length. Radiation entering a focusing crystal 20 according to the teachings herein emerges as either a diverging beam of radiation or a converging beam of radiation. The crystal 20 shown tapers from top to bottom, representing a decreasing lattice constant from top to bottom. Properly aligned radiation entering the top exits as a converging beam. Conversely, radiation entering the top of a crystal which tapers from bottom to top produces a diverging beam. The teachings of the invention may be illustrated using the substances silicon and germanium. The lattice constant of silicon is 5.43 Angstroms and the lattice constant of germanium is 5.66 Angstroms. Solid state solubility of germanium in silicon covers the complete range from 0% germanium to 100% germanium. In Fig. 1, the top of the crystal is represented as being composed of 100% germanium and, thus, 0% silicon. The bottom of the crystal is represented as being composed of 100% silicon, and, thus, 0% germanium. The concentration proportions vary continuously over the length of the crystal 20. By growing a crystal with a continuously varying concentration of silicon in germanium, the lattice constant varies by about 4%. If the crystal 20 has a linear concentration gradient of about 4% per cm, over the length of 10 cm the dimension of the crystal lattice would decrease by

about .04 cm. This would result in a convergence angle 25 of

0.04/10 = 4 milliradians. The crystal 20 thus has a focal length f of 1/0.004 = 250 cm. The diffraction limited size of the focal spot (at 250 cm) is given by the diffraction equation: (1.22) (lambda) _s = _ff

D where s is the diameter of the focal spot, 1.22 represents a proportionality constant, D is the diameter of the end of the crystal 20 which first receives radiation, lambda is the wavelength of radiation and f is the focal length. The following example illustrates the applicability of these teachings. 60 keV gamma rays from the decay of Am ²¹ have a wavelength (lambda) of 0.17 Angstroms. The size of the focal spot for the crystal 20 illustrated having a diameter D of 2 cm would then be:

1.22 X 1.7 X 10 ^"9 s = x 250

2

= 26 X 10 ^"8 cm. This would be the typical size accuracy or definition of a nanoelectronic feature. Therefore, the focusing crystal 20 could be used to extend the range of lithography for electronics down into the nanometer range.

Referring now to Fig. 3, therein is schematically illustrated an apparatus for convergently focusing hard X-rays and gamma rays

30 in accordance with the teachings of the invention. A diffuse ray source 32 emits diffuse hard X-ray or gamma ray beams 11. A

8

collimating crystal 34, operating like the collimating crystal 10 described above propagates a collimated hard X-ray or gamma ray beam 11'. A mask 36 defining the circuit patter which is to placed upon a chip is positioned to receive the collimated beam 11*. The collimated radiation 11* ' which exits the mask now carries the image of the mask 36. The collimated beam 11' ' enters the focusing crystal 38. The focusing crystal 38 is a composite crystal having a lattice constant which decreases over the length of the crystal 38. A converging beam 11' ' ' , carrying the image of the mask, exits the focusing crystal 38. A wafer 39 which is to be manufactured into semiconductor chips is placed in the path of the converging beam 11' ' ' . The image of the mask which strikes the wafer 39 is a reduced version of the image which enters the focusing crystal 38 because of the convergence of the carrying radiation beam 11' ' ' . The reduced image irradiates the photosensitive layer 41 of the wafer 39 which is supported by a substrate 43. Conventional chip production methods may then be used to produce integrated circuits having the degree of miniaturization and definition made possible by the invention. The focusing crystal 20 or 38 can also receive radiation at its narrow, or smaller-lattice-structure, end. Radiation exiting the crystal 20 or 38 would then be diverging because of the dynamics described above.

As stated above, the lattice constant may be made to vary by several methods; however, the use of a composite-substance crystal is a simple, practical method.

As should be apparent from the foregoing specification, the invention is susceptible of being modified with various alterations and modifications which may differ from those which have been described in the preceding specification and description. Accordingly, the following claims are intended to cover all alterations and modifications which do not depart from the spirit and scope of the invention.

10