Photolithographic illuminator device enabling controlled diffraction

Abstract

The invention relates to a photolithographic illuminator device including: a light beam source, a condenser (5), an optical homogenizing system (4) including at least one microlens array, said system being arranged upstream from the condenser, and a shutter (3) arranged at the object focal point of the optical homogenizing system, the illuminator being characterized in that same further comprises a network of aperture diaphragms (8) arranged in the Fourier transform plane of the shutter plane (3). The invention likewise relates to a photolithographic device including such an illuminator.

Claims

1. A photolithographic device illuminator, comprising: a source (1) of a light beam, a condenser (5), an optical homogenizing system (4), comprising at least one array of microlenses (L3, L4), said system being positioned upstream from the condenser, an obturator (3), positioned at the object focus of the optical homogenizing system, and the illuminator being characterized in that it further includes a network of aperture diaphragms (8), positioned in the plane of the Fourier transform of the plane of the obturator (3).

2. The illuminator according to claim 1, wherein the network of aperture diaphragms (8) includes a plurality of diaphragms positioned facing the microlenses of an array (L3, L4) of the optical homogenizing system (4), each diaphragm of the diaphragm network being positioned facing a corresponding microlens.

3. The illuminator according to claim 1, wherein the focal distance f.sub.1 of a first array of microlenses (L3) of the optical homogenizing system (4) with respect to the optical axis, the illumination angle of the obturator, and the aperture diameter b of the diaphragms are adapted so that the light rays passing through the diaphragms have a coherence factor $=\frac{2f_1\sin \left(\right)}{b}$ comprised between 0.2 and 0.8.

4. The illuminator according to claim 3, wherein the aperture diameters of the diaphragms and the coherence factors of the light rays passing through said diaphragms vary from one diaphragm to the other.

5. The illuminator according to claim 4, wherein the aperture diameters of the diaphragms and the coherence factors of the light rays are variable between two adjacent diaphragms.

6. The illuminator according to claim 4, wherein the distribution of the aperture diameters of the diaphragm is random.

7. The illuminator according to claim 4, wherein the variations of the aperture diameters from one diaphragm to the other are comprised between 0 and 50%, and preferably between 0 and 30%.

8. The illuminator according to claim 1, wherein the image focal plane of the optical homogenizing system (4) is positioned in the object focal plane of the condenser (5).

9. A photolithographic device, including a mask (7) and an illuminator according to claim 1, wherein the obturator (3) of the illuminator is positioned in a conjugate plane of the image focal plane of the condenser (5) of the illuminator.

Description

PRESENTATION OF THE FIGURES

(1) Other features, objects and advantages of the invention will become apparent from the description which follows, which is purely illustrative and non-limiting, and which should be read with reference to the appended drawings wherein:

(2) FIG. 1, already described, schematically illustrates an illuminator known from the state of the art;

(3) FIGS. 2a, 2b and 2c schematically illustrate different embodiments of an illuminator according to the invention;

(4) FIG. 3 illustrates the arrangements relative to the arrays of microlenses downstream from the obturator.

(5) FIG. 4 illustrates the image of a slot of the obturator in the object focal plane of the condenser depending on the coherence of light beams crossing a diaphragm network.

DETAILED DESCRIPTION OF AT LEAST ONE EMBODIMENT OF THE INVENTION

(6) General Description of the Illuminator

(7) FIGS. 2a to 2c schematically show a portion of an illuminator according to the invention.

(8) In FIG. 2a, the illuminator includes a source 1 of a light beam 10, for example a laser source, a diffractive element 1 placed at the outlet of the source 1, and a zoom 2 (these elements are not shown in FIGS. 2b and 2c).

(9) It further includes an afocal system L1L2 consisting of a first and second array of microlenses L1 and L2 at the outlet of the zoom 2.

(10) The beam 10 comprises at the outlet of the afocal system L1L2, a plurality of sub-beams 100, forming outlet sub-pupils of the afocal system L1L2.

(11) The illuminator includes an obturator 3, illustrated as two grids 31, 32, and positioned at the outlet pupils of the afocal system L1L2.

(12) An optical homogenizing system 4 including a third array L3 of microlenses is placed downstream from the obturator 3, so that the latter is positioned in the object focal plane of the optical homogenizing system 4.

(13) The illuminator also includes a condenser 5 with which it is possible to superpose to a photolithographic mask 7 the sub-beams 100 from the afocal system L1L2, an apodization device 6 being provided between the condenser 4 and the plane in which the mask 7 is positioned.

(14) The object focal plane of the condenser 5 is advantageously positioned in the image focal plane of the homogenizing system 4 in order to ensure the sharpness of the image of the obturator on the mask.

(15) A photolithographic device comprising such an illuminator also comprises a mask 7 positioned on a wafer w to be etched, the obturator being positioned in the conjugate plane of the image focal plane of the condenser 5, it being understood that during use, projection optics produce the image of the mask 7 on the wafer w.

(16) Homogenizing System

(17) The homogenizing system of the illuminator according to the invention gives the possibility of obtaining the sharpness and telecentricity of the illuminator in two distinct directions, orthogonal to the optical axis. These directions are advantageously orthogonal to each other. As a non-limiting example, in FIGS. 2a to 2c, the optical axis is noted as Z, an axis along a first direction orthogonal to the optical axis and orthogonal to the sectional plane of the figures is noted as X, and an axis along a second direction orthogonal to the optical axis and to the X axis is noted as Y.

(18) The homogenizing system allowing this result to be obtained, in addition to the third array of microlenses L3, comprises a fourth array of microlenses L4.

(19) The relative configurations of the arrays of microlenses L3 and L4 are illustrated in FIG. 3. The obturator 3, located at the object focal point P of the homogenizing system, and the image focal plane F of this system, which have to be located in the object focal plane FC of the condenser, in both directions X and Y, are schematically illustrated.

(20) Sharpness and telecentricity conditions are ensured if the optical homogenizing system has the same object and image focal planes in both directions X and Y.

(21) To do this, each array of microlenses appears as a planar plate comprising two faces 310, 320, 410, 420 facing each other, a plurality of cylindrical microlenses being etched on at least one of said faces.

(22) More specifically, the array of microlenses L3 includes microlenses on each of its faces 310, 320, the microlenses being cylindrical, the axes of the microlenses of one face being orthogonal to the axes of the microlenses of the other face.

(23) The axes of the microlenses of both faces are orthogonal to the optical axis so that light rays reach the microlenses through their cylindrical surfaces.

(24) As for the array of microlenses L4, it only includes cylindrical microlenses on its first face 410 relatively to the propagation direction of the light flux, the upper face 420 being planar so as not to divert the light rays in any direction.

(25) The axes of the cylinders of the microlenses are oriented so that, in a first direction, for example the Y direction, the homogenizing system behaves as a convergent lens 31 positioned at the first face of the array L3. The plane of the obturator P is then in the object focal plane of said lens 31, and the object focal plane of the condenser FC is in the image focal plane F of said lens.

(26) In order to obtain this result, the axes of the cylindrical lenses of the first face of the array of microlenses L3 extend orthogonally to the Y direction, while the axes of the other cylindrical lenses (i.e. those of the second face of the array L3 and of the first face of the array L4) extend parallel to the Y direction, so as not to deviate the propagation of the light beams along the Y direction.

(27) This gives the possibility of obtaining the sharpness and the telecentricity of the illuminator in the first direction Y.

(28) As for the second direction, in this case the X direction, the axes of the cylinders of the microlenses are oriented parallel to the first direction Y, so that the homogenizing system 4 behaves as a system comprising: a convergent lens 32 at the second face of the array L3, and a divergent lens D1 at the first face of the array L4,
the plane of the obturator being in the object focal plane of the convergent lens 32, and the object focal plane of the condenser being in the image focal plane F of the system.

(29) The lenses are dimensioned in a way known to one skilled in the art so that their respective focal lengths allow such a result to be obtained.

(30) Thus, the positioning of both arrays of microlenses L3 and L4, and the dimensioning of the lenses making them up, give the possibility of obtaining a homogenizing system 4 having the same focal length in both directions.

(31) Diaphragms

(32) Referring to FIG. 2b, the illuminator comprises, in order to control diffraction phenomena at the outlet of the obturator, a network 8 of aperture diaphragms, positioned in the plane of the Fourier transform, or Fourier plane, of the plane P of the obturator.

(33) Preferably, this network comprises a plurality of diaphragms 80, each diaphragm 80 being positioned facing a corresponding microlens 40 of an array adjacent to the homogenizing system.

(34) In FIG. 2b, the homogenizing system 4 comprises only one array L3 of microlenses; the diaphragm network is then found in the image focal plane of the array L3 of microlenses, the diaphragms facing the microlenses of this array L3.

(35) In FIG. 2c, the use of a network 8 of diaphragms was combined with a homogenizing system 4 comprising two arrays of microlenses L3 L4 as described earlier with reference to FIG. 2a.

(36) In this case, the diaphragm network 8 is positioned between both arrays of microlenses L3 and L4, in the plane of F, this plane being the Fourier plane of the plane of the obturator. The diaphragms are found facing the microlenses of the arrays L4 and L3 of microlenses.

(37) Thus, in the case of diffraction at the outlet of the obturator 3, the presence of diaphragms gives the possibility of avoiding crosstalk phenomena between the sub-beams 100 of the light beam. With the network 8 of diaphragms, it is also possible to sufficiently increase the field depth so as to make the accuracy of the illuminator less sensitive to defocusing of the obturator relatively to the object focal plane of the homogenizing system, and thereby facilitate manufacturing and adjustment of the illuminator.

(38) Advantageously, the aperture diameter of a diaphragm is of the order of magnitude of a microlens. For example, a microlens may have a diameter of the order of 0.5 mm, and an aperture diameter may be of the order of 0.1 mm.

(39) The correction of the diffraction resulting from the presence of the obturator by the network of aperture diaphragms depends on certain parameters of the illuminator. Notably, the sharpness of the image depends on the coherence factor of the illumination of the diaphragm network.

(40) With reference to FIG. 4, the image of an edge of a slot of the obturator in the image focal plane of the condenser is shown, for different coherence factors. In the figure: the curve plotted for a coherent beam corresponds to a coherence factor of zero, the curve plotted for a partly coherent beam corresponds to a coherence factor of 0.3, and the curve plotted for an incoherent beam corresponds to a coherence factor equal to 1.

(41) A geometrical position in millimeters with respect to the slot is given in abscissae. The slot is positioned at 25 mm, the transparent portion of the slot being found at less than 25 mm, and the opaque portion being found after 25 mm.

(42) The light intensity is illustrated in ordinates as a percentage of the intensity of the incident beam. Theoretically, this intensity is equal to 100% in the transparent portion of the slot and falls to 0% in the opaque portion.

(43) Now, for a totally coherent beam, interference patterns appear on the transparent side of the slot, giving the sinusoidal appearance of the intensity at this level.

(44) These interferences disappear in the case when the beam is totally incoherent, this improvement however occurring to the detriment of the transition between the opaque portion and the transparent portion of the slot at 25 mm.

(45) The case when the beam is partly coherent is an intermediate case, providing a good compromise between both previous cases. More specifically, an advantageous configuration is ensured when the beam has a coherence factor comprised between 0.2 and 0.8.

(46) The coherence factor is written as

(47) $=\frac{2f_1\sin \left(\right)}{b},$
wherein f.sub.1 is the focal length of the array of microlenses L3 of the homogenizing system, is the illumination angle of the obturator with respect to the optical axis, and b the aperture diameter of the diaphragms. Thus the value of the coherence factor is obtained by adjusting the values of these three parameters.

(48) However it is observed in FIG. 4 that light intensity oscillations subsist in the transparent portion of the slot. In order to average out these oscillations, provision is advantageously made for varying the aperture diameters of the diaphragms, modifying the coherence factor by doing this. Preferably, the diameters of the diaphragms vary, including between two adjacent diaphragms.

(49) The variations of the aperture diameters from one diaphragm to another are comprised between 0 and 50%, and preferably between 0 and 30%.

(50) Further, the aperture diameters of the diaphragms advantageously follow a random statistical distribution and this regardless of the illumination of the obturator. This allows averaging out of the diffraction phenomena, for example even locally for a given sub-beam 100.