Method for reducing reflection of grazing incident p-polarized ultraviolet light from a surface of a substrate

Abstract: Multilayer antireflection coatings are disclosed for grazing incident ultraviolet light having a large angle of incidence. The coatings comprise, from the medium side, layers of high-refractive-index material alternating with layers of low-refractive-index material. Each layer of the high-refractive-index material has the same optical thickness, and each layer of the low-refractive-index material has the same optical thickness. The multilayer antireflection coatings are effective in preventing reflection of p-polarized light, from optical elements coated with such a coating, having a wavelength of 150 nm ≤ λ ≤ 250 nm in a range of angle of incidence of 70° ≤  ≤ 80°.

Description: Field of the Invention The present invention relates to multilayer antireflection coatings for optical elements and the like, the antireflection coatings serving to inhibit refelection from the optical elements of grazing incident light, especially ultraviolet light from excimer lases and the like. Background of the Invention The recent development of lasers such as excimer lasers has increased the demand for optical systems and components that can transmit ultraviolet light. Such optical systems and components typically require antireflection coatings effective against incident light , including "grazing" incident light (i.e., incident light having a high angle of incidence θ of generally 70° or greater). An excimer laser produces linearly polarized light. Depending upon the placement of the optical system relative to the excimer laser, light from the laser enters the optical system as either p-polarized light or s-polarized light. Conventional multilayer antireflection coatings consist of stacked layers in which layers of high-refractive-index material and low-refractive-index material are altematingly arranged. For example, EP-A-0 814 350 describes multilayer antireflection coatings the include multiple stacked layers of high-refractive-index material and a low-refractive-index material that are altematingly arranged. JP-A-07 244 217 describes an antireflection coating that includes three low-index layers and two intermediate-index layers and that is configured to have a reflectance of 0.5% or less over a 70 nm spectral bandwidth. A larger number of layers is required as the angle of incidence is increased (e.g., whenever θ ≤ 70°. the number of layers is four or more). Conventional multilayer antireflection coatings also typically have a non-periodic multilayer structure in which the optical thickness of each layer is different. Hence, the optical thickness of each layer must be precisely controlled when forming such an antireflection coating. Also, for each incidence angle, the optical thickness of each layer and the number of layers in the antireflection coating must be different. In making a conventional multilayer antireflection coating for grazing incident light (the coating being made with a non-periodic structure), the following difficulties are encountered: (1) During formation of each of the stacked layers, variations in layer thickness frequently arise; such variations cause corresponding unplanned variations in re-fractive index over the antireflective coating. Hence, it is necessary to evaluate the refractive index of each layer before deposition. (2) If the optical performance of a coating is different from ideal performance, it is difficult to identify the specific culprit layer(s) in the coating because the optical thickness of each layer is different. Consequently, obtaining a coating that is entirely within specification requires a trial-and-error approach. (3) Parameters that must be controlled to controllably form the correct optical thickness of each layer of the multilayer antireflection coating are complicated. (4) For each angle of incidence, both the optical thickness of each layer and the total number of layers in the multilayer antireflection coating must be different. Generalized Brewster-angle conditions for quarter-wave multilayers at non-normal incidence" by H.F. Mahlein, Journal of the Optical Society of America, Volume 64, no. 5, pp. 647-653, May 1974, discloses a method of reducing reflection of polarized UV light by alternatively depositing high and low refractive index layers having the same effective optical thickness of a quarter wavelength of the incident radiation. Summary of the Invention In view of the foregoing shortcomings of conventional multilayer antireflection coatings for grazing incident light, an object of the present invention is to provide effective multilayer antireflection coatings for grazing incident light for ultraviolet light having a larger range of angle of incidence. According to the invention, a method is provided as defined in claim 1. Preferred embodiments of the invention are indicated in the dependent claims. The high-refractive-index material preferably comprises a substance selected from the group consisting of lanthanum fluoride (LaF 3 ), gadolinium fluoride (GdF 3 ), neodymium fluoride (NdF 3 ), dysprosium fluoride (DyF 3 ), yttrium fluoride (YF 3 ), and mixtures and compounds of such compounds. The low-refractive-index material preferably comprises a substance selected from the group consisting of aluminum fluoride (AlF 3 ), magnesium fluoride (MgF 2 ), calcium fluoride (CaF 2 ), sodium fluoride (NaF), cryolite (Na 3 AlF 6 ), thiolite (Na 5 Al 3 F 14 ), and mixtures and compounds of such compounds. The total number N of layers comprising the antireflection coating is preferably within a range of 5 ≤ N ≤ 17. The foregoing and additional features and advantages of the invention will be more readily apparent from the following detailed description, which proceeds with reference to the accompanying drawings. Brief Description of the Drawings FIG. 1(a) is a sectional schematic diagram of a multilayer antireflection coating for grazing incident light made in accordance with the present invention when the number of stacked layers is odd. FIG. 1(b) is a sectional schematic diagram of a multilayer antireflection coating for grazing incident light made in accordance with the present invention when the number of stacked layers is even. FIG. 2 is a plot of antireflection performance versus angle of incidence of p-polarized light at λ = 193.4 nm for multilayer antireflection coatings according to Example Embodiment 1 having 7, 9, 13, 15, and 17 layers. FIG. 3 is a plot of antireflection performance versus angle of incidence of p-polarized light at λ = 193.4 nm for multilayer antireflection coatings according to Example Embodiment 2 having 5, 7, 9, and 11 layers. FIG. 4 is a plot of antireflection performance versus angle of incidence of p-polarized light at λ = 248 nm for multilayer antireflection coatings according to an example having 9, 11, 13, 15, and 17 layers. Detailed Description The following description is directed to representative embodiments of a multilayer antireflection coating for grazing incident light, representing the current best mode of method according to the invention. A schematic elevational sectional diagram of a multilayer antireflection coating for grazing incident light, made according to the invention, is shown in FIG. 1. The antireflection coating comprises, from a medium side, a high-refractive-index layer 1, a low-refractive-index layer 2, a high-refractive-index layer 1, and additional such layers in an alternating superposed manner on a substrate 3. The refractive index of a "high-refractive-index" material is higher than the refractive index of the substrate material. The refractive index of a "low-refractive-index" material is lower than the refractive index of the substrate material. Whenever the number of stacked layers is odd, a high-refractive-index layer 1 preferably contacts the substrate (FIG. 1(a)). Whenever the number of lamination layers is even, a low-refractive-index layer 2 preferably contacts the substrate (FIG. 1(b)). Each high-refractive-index layer 1 has the same optical thickness; similarly, each layer of the low-refractive-index layer 2 has the same optical thickness. If each high-refractive-index layer is made of the same high-refractive-index material, and each low-refractive-index layer is made of the same low-refractive-index material, then the optical thickness of each pair of adjacent layers (consisting of a high-refractive-index layer 1 and a low-refractive-index layer 2) is fixed at a value (representing the "optical period length") that is the same for all such pairs. Thus, a multilayer-antireflection coating for grazing incident light in accordance with the present invention has a periodic structure. The substrate 3 is typically a material that transmits ultraviolet light, such as (but not limited to) silica glass, calcium fluoride, and magnesium fluoride. The high-refractive-index layers are preferably made of a material selected from a group consisting of lanthanum fluoride: (LaF 3 ), gadolinium fluoride (GdF 3 ), neodymium fluoride (NdF 3 ), dysprosium fluoride (DyF 3 ), yttrium fluoride (YF 3 ), and mixtures and compounds of these materials. The low-refractive-index layers are preferably made of a material selected from a group consisting of aluminum fluoride (AlF 3 ), magnesium fluoride (MgF 2 ), calcium fluoride (CaF 2 ), sodium fluoride (NaF), cryolite (Na 3 AlF 6 ), thiolite (Na 5 Al 3 F 14 ), and mixtures and compounds of these materials. The sum of the optical thickness of a high-refractive-index layer 1 and an adjacent low-refractive-index layer 2 is termed the "optical period length" nd. The optical period length nd = n H d H + n L d L , wherein n H is the refractive index and d H is the physical thickness of the high-refractive-index material, n H d H is the optical thickness ofthe high-refractive-index material, n L is the refractive index and d L is the physical thickness of the low-refractive-index material, and n L d L is the optical thickness of the low-refractive-index material. The optical period length satisfies the following relationship: 0.6 λ o ≤ nd ≤ 0.65 λ o The ratio of the optical thickness of the high-refractive-index layer to the optical period length (also termed the "optical thickness ratio" r = n H d H /nd) satisfies the following relationship: 0.38 ≤ Γ ≤ 0.73 The total number of layers N of the antireflective coating preferably satisfies the following relationship: 5 layers ≤ N ≤ 17 layers The multilayer antireflection coating can be made by any suitable method such as (but not limited to) vacuum vapor deposition, sputtering, ion plating, chemical vapor deposition (CVD). To begin formation of the multilayer antireflection coating, a pair of stacked layers consisting of a high-refractive-index layer and a low-refractive-index layer is deposited on the substrate; deposition parameters under which the pair of layers is formed are such that the optical thickness of each layer satisfies the parameters noted above. Additional layers are added in an alternating manner according to fixed deposition parameters for the high-refractive-index layers and the low-refractive-index layers. The resulting multilayer antireflection coating comprises a different number of layers depending upon the anticipated angle of incidence. A multilayer antireflection coating that satisfies the foregoing parameters exhibits a satisfactory antireflection effect when p-polarized light in the wavelength range of 150 to 250 nm enters the coating at an angle of incidence of 70 to 80°. Example Embodiment 1 In this example embodiment, attemating layers of lanthanum fluoride (LaF 3 ) as the high-refractive-index layer and magnesium fluoride (MgF 2 ) as the low-refractive-index layer were formed on a substrate of synthetic silica glass. The optical thickness of each resulting layer was n H d H = 0.322λ o for each of the LaF 3 layers, and n L d L = 0.322λ o for each of the MgF 2 layers. The optical period length nd (i.e., the sum of the optical thickness of the high-refractive-index layer and the optical thickness of the low-refractive-index layer) was 0.644λ o (wherein λ o = 193.4 nm), and the ratio of the optical thickness of the high-refractive-index layer to the optical period length was r = 0.5. Each layer was deposited by vacuum vapor deposition. Eleven separate antireflective coatings were prepared, with the number N of stacked layers ranging from 7 to 17 (i.e., N = 7, 8, 9, 10, 11, 12, 13, 14, 15, 16, 17). With respect to each antireflective coating, the materials from which the layers were formed, the optical period length, and the ratio of the optical thickness of the high-refractive-index layer to the optical period length were the same. Formation of each antireflective coating was started by depositing a first pair of stacked layers on the substrate wherein one layer was lanthanum fluoride (LaF 3 ) and the other layer was magnesium fluoride (MgF 2 ). Alternating layers of these materials were applied to this initial two-layer structure until the desired number of layers was reached. The coating-deposition parameters were set such that the respective optical thicknesses were as described above. The angular characteristics of the multilayer antireflection coatings made according to this example embodiment were.measured using p-polarized incident light at λ = 193.4 nm. Table 1 shows, for each value of N from 7 to 17, the angle of incidence at which reflectance was minimized and the value of the reflectance under such conditions. FIG. 2 shows incidence-angle characteristics for certain of the multilayer antireflection coatings according to this example embodiment (i.e., for coatings in which N = 7, 9, 13, 15, and 17). The data shown in Table 1 and FIG. 2 indicate that the multilayer antireflection coatings according to this example embodiment have a full antireflection effect with transmittance of 99 % or greater when the angle of incidence is in the range 70° ≤ θ ≤ 80°. (For the synthetic silica glass substrate alone, reflectance R = 4 % at θ = 70° and R = 23:3 % at θ = 80°). These data also indicate that the angle of incidence at which reflectance is minimized is changed simply by changing the number of stacked layers. Table 1 Number of Layers (N) Angle of Incidence θ at which Reflectance is Minimized (°) Minimum Reflectance R (%) 7 72.1 0.3 8 73.0 0.3 9 74.4 0.2 10 74.7 0.2 11 75.5 0.1 12 76.0 0.1 13 76.7 0.1 14 77.0 0.1 15 77.6 0.1 16 77.8 0.2 17 78.2 0.4 Example Embodiment 2 In this example embodiment, alternating layers of lanthanum fluoride (LaF 3 ) as the high-refractive-index layer and cryolite (Na 3 AlF 6 ) as the low-refractive-index layer were formed on a substrate of calcium fluoride. The optical thickness of each resulting layer was n H d H = 0.3 λ o for each of the LaF 3 layers, and n L d L = 0.35λ o for each of the Na 3 AlF 6 layers. The optical period length nd (i.e., the sum of the optical thicknesses of the high-refractive-index layer and the low-refractive-index layer) was 0.65 λ o (wherein λ o = 193.4 nm), and the ratio of the optical thickness of the high-refractive-index layer to the optical period length was r = 0.46. Each layer was deposited by vacuum vapor deposition. Seven separate antireflective coatings were prepared, with a number N of stacked layers ranging from 5 to 11 (i.e., N = 5, 6, 7, 8, 9, 10, 11). With respect to each antireflective coating, the materials from which the respective layers were formed, the optical period length, and the ratio of the optical thickness of the high-reflective-index layer to the optical period length were the same. Formation of each antireflective coating was started by forming a pair of stacked layers on the substrate, wherein one layer was lanthanum fluoride (LaF 3 ) and the other layer was cryolite (Na 3 AlF 6 ). The coating-deposition parameters were such that the respective optical thicknesses were as described above. The angular characteristics of the multilayer antireflection coatings made according to this example embodiment were measured using p-polarized incident light at λ = 193.4 nm. Table 2 shows, for each value of N from 5 to 11, the angle of incidence at which reflectance was minimized and the value of the reflectance under such conditions. FIG. 3 shows incidence-angle characteristics for certain of the multilayer antireflection coatings according to this example embodiment (i.e., for N = 5, 7, 9, and 11). The data shown in Table 2 and FIG. 3 indicate that the multilayer antireflection coatings according to this example embodiment have a full antireflection effect with transmittance of 99 % or greater when the angle of incidence is in the range 70° ≤ θ ≤ 75°. (For the calcium fluoride substrate alone, reflectance R = 4.3 % at θ = 70° and R = 10.7 % at θ = 75°). These data indicate that the angle of incidence at which reflectance is minimized is changed simply by changing the number of stacked layers. Table 2 Number of Layers (N) Angle of Incidence θ at which Reflectance is Minimized (°) Minimum Reflectance R (%) 5 70.0 0.1 6 70.7 0.1 7 72.4 0.1 8 72.8 0.1 9 74.0 0.1 10 74.2 0.1 11 75.0 0.4 Example In this example, alternating layers of lanthanum fluoride (LaF 3 ) as the high-refractive-index layer and cryolite (Na 3 AlF 6 ) as the low-refractive-index layer were deposited on a substrate of calcium fluoride. The optical thickness of each resulting layer was n H d H = 0.35λ o for each of the LaF 3 layers, and n L d L = 0.31λ o for each of the Na 3 AlF 6 layers. The optical period length nd (i.e., the sum of the optical thickness of the high-refractive-index layer and the optical thickness of the low-refractive-index layer) was 0.66λ o (wherein λ o = 248 nm), and the ratio of the optical thickness of the high-refractive-index layer to the optical period length was Γ = 0.53. Each layer was deposited using vacuum vapor deposition. Five separate antireflection coatings were prepared, with a number N of layers ranging from 9 to 17 (i.e., N = 9, 11, 13, 15, 17). With respect to each antireflection coating, the materials from which the layers were formed, the optical period length, and the ratio of the optical thickness of the high-refractive-index layer to the optical period length were the same. Formation of each antireflection coating was started by forming a pair of layers on the substrate, wherein one layer was lanthanum fluoride (LaF 3 ) and the other layer was cryolite (Na 3 AlF 6 ). The coating-deposition parameters were such that the respective optical thicknesses were as described above. The angular characteristics of the multilayer antireflection coatings made according to this example were measured using p-polarized incident light at λ = 248 nm. Table 3 shows, for each value of N, the angle of incidence at which reflectance was minimized and the reflectance under such conditions. FIG. 4 shows incidence-angle characteristics for each of the multilayer antireflection coatings according to this example. The data shown in Table 3 and. FIG. 4 indicate that the multilayer antireflection coatings according to this example have a full antireflection effect with transmittance of 99 % or greater when the angle of incidence is in the range 72° ≤ θ ≤ 76°. (For the calcium fluoride substrate alone, reflectance R = 4.4 % at θ = 70° and R = 10.8 % at θ = 75°). These data also indicate that the angle of incidence at which reflectance is minimized is changed simply by changing the number of stacked layers. Table 3 Number of Layers (N) Angle of incidence θ at which Reflectance is Minimized (°) Minimum Reflectance R (%) 9 72.6 0.3 11 73.8 0.2 13 74.8 0.1 15 75.4 0.1 17 75.9 0.2 Although vacuum vapor deposition is the preferred technique for applying each of the layers of a multilayer antireflection coating, alternative techniques, such as sputtering, ion plating or chemical vapor deposition, can be used in the method according to the invention. Thus, the method according to the invention provides multilayer antireflection coatings for grazing incident light. The coatings have a periodic structure (alternating layers of high-refractive-index material and low-refractive-index material) in which each layer of the high-refractive-index material has the same optical thickness, and each layer of the low-refractive-index material has the same optical thickness (which can be different than the optical thickness of the high-refractive-index material). Production is preferably initiated by forming a two-layer structure on a substrate, the structure comprising a high-refractive-index layer and a low-refractive-index layer under known coating-deposition parameters. Subsequent alternating layers are added under the same coating-deposition parameters. The resulting multilayer antireflection coating has a fixed optical-period length and optical-period ratio; by varying the number of stacked layers it is possible to obtain an antireflection effect for any of various angles of incidence in the range 70° ≤ θ ≤ 80° with p-polarized light having a wavelength in the range 150 nm ≤ λ ≤ 250 nm. Optical systems comprising optical elements having a multilayer antireflection coating according to the invention exhibit superior optical performance. Whereas the invention has been described in connection with preferred embodiments, it will be understood that the invention is not limited to those embodiments. On the contrary, the invention is intended to encompass all alternatives, modifications, and equivalents as may be included within the scope of the invention as defined by the appended claims.

Claims: A method for reducing reflection of grazing incident p-potarized ultraviolet light from a surface of a substrate (3) by applying to the surface first and second stacked layers (1, 2), the first layer being a high-refractive index layer (1) and the second layer being a low-refractive-index layer (2), applying to the first and second layers additional high-refractive-index layers and low-refractive-index layers (1, 2) in an alternating manner to produce a multilayer antireflection coating on the substrate (3), the antireflection coating having a total number of layers N within the range of 5≤ N ≤ 17, wherein each alternaung high-refractive-index layer (1) has the same optical thickness, and each alternating low-refractive-index layer (2) has the same optical thicknesss, wherein further: (a) the sum of the optical film thicknesses of a high-refractive-index layer (1) and a low-refractive-index layer (2) defines an optical period length nd, wherein 0.6 λ o ≤ nd ≤ 0.65 λ o , wherein λ o is the wavelength of incident radiation such that 150nm ≤ λ o ≤ 250nm; and (b) the ratio Γ of the optical thickness of the high-refractive-index layer (1) and the optical period length nd is such that 0.38 ≤ Γ ≤ 0.73 wherein deposition parameters under which each pair of layers (1,2) is formed are such that the optical thickness of each layer satisfies the above parameters; whereby the transmittance of the coating at an incidence angle between 70° and 80° is 99% or greater. The method of claim 1, wherein N is even and the second layer (2) contacts the surface of the substrate (3). The method of claim 1, wherein N is odd and the first layer (1) contacts the surface of the substrate (3). The method of any one of claims 1 to 3, wherein: the high-refractive-index layers (1) comprise a substance selected from the group consisting of lanthanum fluoride (LaF 3 ), gadolinium fluoride (GdF 3 ), neodymium fluoride (NdF 3 ), dysprosium fluoride (DyF 3 ), yttrium fluoride (YF 3 ), and mixtures and compounds of such compounds, and the low-refractive-index layers (2) comprise a substance selected from the group consisting of aluminium fluoride (AlF 3 ), magnesium fluoride (MgF 2 ), calcium fluoride (CaF 2 ), sodium fluoride (NaF), cryolite (Na 3 AlF 6 ). thiolite (Na 5 Al 3 F 14 ), and mixtures and compounds of such compounds. The method of any one of claims 1 to 4, wherein the substrate (3) is transmissive to light having a wavelength λ such that 150 nm ≤ λ ≤ 250 nm. The method of claim 5, wherein the substrate (3) is selected from the group consisting of silica glass, calcium fluoride , and magnesium fluoride.

Inventors: NAKAMURA HIROSHI, SHIRAI TAKESHI, NAKAMURA, HIROSHI, SHIRAI, TAKESHI
Applicants: NIPPON KOGAKU KK, NIKON CORPORATION
Application year: 1998
Main classification: G02B1
IPC codes: B32B7, B32B9, G02B1, G02B5, C03C17