X-ray mirror and material

Abstract: The object of the present invention is to provide an x-ray mirror material of high reflectance having a surface roughness which is very small and further that the film density is large. A Pt alloy film is provided as a mirror surface. A reflecting surface material for an x-ray mirror is expressed as the general formula Pt 1-x M x . This is deposited on a levelly polished surface of a substrate. Where M indicates one or more substances of Mo, Ru, Rh, Pd, Ta, W, and Au, and X lies in the range 0.005 ≦ x ≦ 0.10.

Description: The present invention relates to an x-ray mirror and material and in particular to, but not exclusively to, a total reflection mirror and a multilayer mirror for use with x-ray radiation. In a catoptric system wherein radiation having a wave length in an x-ray region, 0.01 to 20 x 10 -9 m (0.1 to 200 Å), is employed, a total reflecting mirror, a multilayer mirror, and so on are used depending on the use and the particular wave length. If an oblique incident angle is small, the mirror of the catoptric system increases in area. On the other hand, the area of an optical system for focusing and an imaging mirror reduces in aperture and thereby increases in aberration. Therefore, it is preferable to ensure that a critical angle between incident x-rays and the mirror surface for total reflection is large. A reflecting material is important because the critical angle of total reflection is proportional to a density of the reflecting material. Thus, a high density substance, such as gold (Au) and platinum (Pt) is often used. Au and Pt are chemically quite stable and thereby utilised for the reflecting surface in addition to their excellent reflecting properties. In these reflecting mirrors, material such as Au and Pt, are deposited on a surface of material, such as quartz glass, single silicon, and SiC, which can be polished to obtain a very level surface, by physical or chemical vapour deposition, such as vacuum deposition and sputtering or plating. Such mirrors are for instance known from JP-A-63266398 or JP-A-1309000. An x-ray has a relatively short wave length, which is about 1/10-1/1000 of that of visible light. So in order to obtain highly efficient reflectance in this wave length region, the roughness of the reflecting surface and the interface must be reduced to about 1/10-1/1000 of that of visible light. Also, when using a substrate, such as quartz glass, which is polished level, the roughness of the film surface can increase at deposition. Particularly, substances such as Pt and Au, have a low Debye temperature and so the mobility of the atoms at room temperature is large. As a result, the crystal grains grow during vacuum deposition and sputtering which results in the roughness of the surface increasing. Moreover, a film which is 10-100 x 10 -9 m (100-1000 Å) thick is deposited to form a total reflecting mirror. The film thickness of one layer constituting a multilayer mirror is between 1 and 10 x 10 -9 m (10 Å and 100 Å). If the film is formed by the above-mentioned method, the density of the film is inclined to reduce by about 5-30% as compared to that of a bulk material within the above film thickness. Therefore, a sufficient x-ray reflecting performance cannot be obtained. An object of the present invention is to reduce the surface roughness of a film formed by the above deposition method and provide a reflecting material for an x-ray mirror which has almost equal density to a pure film and which is superior in reflecting properties and is further chemically stable. According to the present invention, there is provided an x-ray mirror for reflecting x-ray radiation comprising, a reflecting material formed on a substrate and comprising Pt and characterised by a material chosen from Mo, Ru, Rh, Pd, Ta, W and Au. Also, the present invention uses an alloy film expressed as a general formula Pt 1-x M x , for a mirror surface of an x-ray mirror so as to reduce the surface roughness without reducing the film density so much. M may be selected from one or more of the following substances; Mo, Ru, Rh, Pd, Ta, W and Au. x, in order to satisfy the equation; should fall in the range 0.005 ≤ x ≤ 0.10. If x is indicated by percentage, x should fall between 0.5% and 10% and the formula is expressed as Pt 100-x M x . When the above-described additions to the Pt material of 0.5-10%, the crystal grain size of an alloy film according to the present invention gets much smaller than that of a conventional pure Pt film. Further, dispersion of the crystal grain size reduces and besides the surface roughness reduces. Thus the film density does not decline so much, since the quantity of additions is small. Hence, the x-ray reflecting performance is improved. If the additions are added at more than 10% the surface roughness deteriorates and the film density also deteriorates. Consequently the x-ray reflecting performance declines. Embodiments of the present invention will now be described with reference to the accompanying drawings, of which: Figure 1 is a graph showing the relationship between the surface roughness and the concentration of M in the inventive alloy film when M comprises Pd, both on a glass substrate and a Si substrate; Figure 2 is a graph giving the x-ray reflectance of the inventive alloy film against the CuK α x-ray incident angle when the film comprises Pt-Pd; and Figure 3 is a graph showing the x-ray reflectance against the incident angle of the multilayered x-ray mirror comprising a combination of the inventive Pt-Pd alloy film and a carbon film. Hereinafter, the present invention will be described with reference to the preferred embodiments. (Embodiment 1) A Pt-Pd film used for an x-ray mirror material of the present invention can be deposited in the following method. Deposition is performed by sputtering. However, many other deposition techniques can be also utilised. When sputtering is performed, the substrate temperature is kept at almost room temperature. In the present invention, both single silicon and BK7 glass are employed as a substrate. However, any other materials, which can be polished to be very level, can be also used. This embodiment discloses a Pt-Pd film in a total reflecting mirror which is used for the x-ray wave length region of 0.07 to 0.02 x 10 -9 m (0.7-2 Å). As for a target, a composite target in which a Pd chip is disposed on a Pt target is used so as to control precisely the quantity of Pd. The film thickness of the Pt-Pd alloy film is approximately 50 x 10 -9 m (500 Å). Pd content is adjusted between 1 atomic percent and 10 atomic percent. Conventionally, the crystal grain size of a pure Pt film is between 10 and 50 x 10 -9 m (100 Å and 500 Å) and each crystal grain size varies differently. The size is 20 x 10 -9 m (200 Å) on average. On the other hand, the crystal grain size of the Pt-Pd alloy film, to which Pd is added at 1-2 atomic percent, is between 5 and 15 x 10 -9 m (50 Å and 150 Å). That is to say, a pretty small crystal grain size can be obtained. Further, the dispersion of the crystal grain size can be suppressed. The crystal grain size is about 9 x 10 -9 m (90 Å) on average. The upper limit of Pd is 10 atomic percent for suppressing the dispersion and reducing the crystal grain size. Figure 1 is a graph showing the relationship between the quantity of Pd and a rms (root mean square) of the surface roughness. Adding Pd reduces considerably the surface roughness as compared to a pure Pt sputtering film. The same effect can be obtained in single silicon and a BK7 glass substrate. The Pd content at which the surface roughness of the Pt-Pd alloy film becomes a minimum, is 3-4 atomic percent. Figure 2 is a graph showing the x-ray reflectance measured against a CuK α x-ray (i.e., one whose wave length is 0.154 x 10 -9 (1.54 Å). The curve indicated with a solid line shows the theoretical reflectance when a Pt film has an ideal surface (i.e. roughness = 0) and has a density equal to a bulk state of Pt. As shown in Figure 2, the x-ray reflectance which is actually measured, is smaller than the theoretical reflectance. This is due to the surface roughness and a low density of the Pt film, which is lower than that of the bulk state Pt. Most of Pt-Pd alloy films to which Pd is added, can obtain a higher reflectance than that of a pure Pt film at an oblique incidence angle of less than 0.5°. On the other hand, a critical angle of total reflection deteriorates because adding Pd at more than about 3 atomic percent reduces the density considerably. As long as Pd is added at less than 3 atomic percent, the density of the Pt-Pd film is almost the same value as a pure Pt film. Further, a high reflectance than a pure Pt film can be achieved. The same effect can also be achieved when using a Pt 1-x M x film and as deposited as described above, where M is another substance rather than Pd from among Mo, Ru, Rd, Ta, W. (Embodiment 2) According to the result shown in Embodiment 1, an x-ray multilayer mirror having high reflectance can be produced utilising an alloy film expressed as the general formula; Pt 1-x M x . M represents one or more substances of Mo, Rh, Pd, Ta, W and Au, and further, x satisfies the following formula 0.005 ≤ x ≤ 0.10. The x-ray multilayer mirror is constituted of the combination of a high density metal and low density material, wherein approximately 10-200 layers are laminated and each layer has the thickness of 1-10 x 10 -9 m (10-100 Å), The x-ray multilayer mirror is produced by vacuum deposition. The following two multilayered films are produced. One is comprised of Pt and carbon, C; the other is comprised of Pt containing Pd at 1 atomic percent and C. The thickness of one layer is 2.5 x 10 -9 m (25 Å). Figure 3 is a graph showing x-ray reflectance of a Pt/C x-ray multilayer mirror and Pt containing Pd at 1 atomic percent/C. The x-ray multilayer mirror is measured with an AIK α x-ray having a wave length of 0.834 x 10 -9 m (8.34 Å). As shown in Figure 3, the peak x-ray reflectance is between 2% and 3 %. When a multilayered film comprising Pt and C has an ideal surface and an ideal interface (roughness = 0) and is equal to a bulk state in density, the theoretical reflectance of the Pt/C x-ray multilayer mirror is 32%. The difference with ideal reflectance is caused by the roughness of the surface and the interface and the decline of film density. In the produced multilayered film the Pt/C x-ray multilayer mirror, it can be estimated that the rms surface roughness and the interface roughness is between 0.45 and 0.55 x 10 -9 m (4.5 Å and 5.5 Å) and that the film density of Pt and C is approximately 80% of the density in a bulk state. On the other hand, in the x-ray multilayer mirror comprising the combination of Pt containing Pd at 1 atomic percent and C, peak reflectance is about 15% and the roughness of the film surface and the interface is 0.25 - 0.3 x 10 -9 m (2.5-3 Å). Even if the thickness of one layer of a multilayered film is between 1 and 10 x 10 -9 m (10 Å and 100 Å), a similar effect can be obtained on reducing the roughness of the film surface and the interface. Figure 3 shows a multilayered film comprising the combination of Pt containing Pd at 1 atomic percent and C as an example. However, a similar effect can be gained as long as the alloy film is expressed as the general formula Pt 1-x M x and constitutes one element of a combination constituting a multilayered film. The M represents one or more substances of Mo, Ru, Rh, Pd, Ta, W, and Au, and X satisfies the formula: 0.005 ≤ x ≤ 0.10. (Embodiment 3) According to embodiment 1, the crystal grain is miniaturised in order to reduce the surface roughness. In Embodiment 3, an alloyed amorphous film is employed for reducing the surface roughness. A diffraction peak to an x-ray cannot be seen in an alloy film expressed as the general formula Pt 1-x M x so that the above alloy film is an amorphous film. The M represents one or more substances of Mo, Rh, Ta, and W, and X satisfies the formula 0.10 ≤ x ≤ 0.20. As described above, the alloy film used for a reflecting surface of an x-ray mirror expressed as a general formula Pt 1-x M x can reduce the roughness of the surface and the interface but hardly reduces the density. Namely, the present invention can provide a stable reflecting material for an x-ray mirror. M represents one or more substances of Mo, Ru, Rh, Pd, Ta, W, and Au, and X satisfies the formula 0.005 ≤ x ≤ 0.10. The aforegoing description has been given by way of example only and it will be appreciated by a person skilled in the art that modifications can be made without departing from the scope of the present claims.

Claims: An X-ray mirror for reflecting X-ray radiation, comprising a layer of reflecting alloy formed on a substrate, the reflecting alloy being characterised by the formula Pt 1-x M x wherein M represents a metal chosen from M o , R u , Rh, Pd, Ta, W and Au and 0.005 ≤x≤ 0.10. An X-ray mirror according to claim 1, wherein said alloy has an average grain size of less than 15 nanometres. An X-ray mirror according to claim 1 or claim 2, wherein M represents Pd and x≤0.03. An X-ray mirror according to any preceding claim in which the X-ray mirror is a multi-layered mirror comprising alternate layers of said alloy and a low density material. An X-ray mirror according to claim 4, wherein said low density material is carbon.

Inventors: NAKAJIMA KUNIO, SUDO SHUZO, NAKAJIMA, KUNIO, SUDO, SHUZO, NAKAJIMA, KUNIO, C/O SEIKO INSTRUMENTS INC., SUDO, SHUZO, C/O SEIKO INSTRUMENTS INC.
Applicants: SEIKO INSTR INC, SEIKO INSTRUMENTS INC.
Application year: 1993
Main classification: G21K1
IPC codes: C22C5, C23C14, G21K1