Patent Application
20220289619
The present disclosure relates to an X-ray shielding glass and a glass component.
In facilities where radiation is handled, including medical facilities such as an X-ray room in the hospital, research facilities, or nuclear power plants, radiation shielding glass is used in terms of the ease of working and in terms of protecting people in the facilities from radiation. Such glass is typically required of high visible light transmissivity (transparency) and high radiation shielding capability (absorption capability). Since the shielding capability is proportional to the mass absorption coefficient and the density of glass, lead glass having high density has been used as radiation shielding glass for a long time.
However, a lead component is a toxic substance. Therefore, when producing, processing, and discarding radiation shielding glass containing a large amount of a lead component, measures need to be taken for environmental protection, resulting in increased cost. Further, for radiation shielding glass containing a large amount of the lead component, when the surface of the glass is cleaned to remove contaminants on the surface, “dimming and staining” of the glass surface occurs, and this “dimming and staining” significantly reduces the transparency of the glass.
To address the above-described problems, radiation shielding glass free of a lead component has been under development.
As such glass, for example, JP H06-127973 A (PTL 1) discloses a SiO2—BaO-based radiation shielding glass having a density of 3.01 g/cm3 or more. Further, J P 2013-220984 A (PTL 2) discloses a P2O5—WO3-based glass having high radiation shielding ability. Moreover, J P 2008-088019 A (PTL 3) and JP 2008-088021 A (PTL 4) disclose a B2O3—La2O3-based glass having high radiation shielding performance.
Furthermore, in recent years, certain medical fields require high shielding capability against radiation especially against X-rays with a tube voltage of 150 kV or less.
However, none of the glasses disclosed in PTLs 1 to 4 above had sufficient shielding capability against X-rays with a tube voltage of 150 kV or less. In particular, the radiation shielding glass disclosed in PTL 1 had low density, so that its X-ray shielding performance was not sufficient. Further, the glass disclosed in PTL 2 was colored yellow or blue and had low visible light transmissivity, so that the inside of a system in which X-rays were used was considered to be hardly observed.
The present disclosure advantageously solves the above problems, and it could be helpful to provide an X-ray shielding glass having high shielding capability against X-rays with a tube voltage of 150 kV or less. Further, it could be helpful to provide a glass component that uses the above-described X-ray shielding glass and has high shielding capability against X-rays with a tube voltage of 150 kV or less.
The inventors of the present disclosure diligently made studies to achieve the above objectives, and found that for example, since the glasses disclosed in PTL 3 and PTL 4 contain a certain amount of ZnO, TiO2, Li2O, etc. having a relatively lower molar weight, the ratio of components contributing to the improvement in the X-ray shielding performance was low and the shielding capability against X-rays, in particular, X-rays with a tube voltage of 150 kV or less was not sufficient.
The present inventors made further studies, and found that a glass having a certain composition including B2O3, La2O3, Gd2O3, and WO3 as essential components and including a predetermined metal oxide had high shielding capability against X-rays with a tube voltage of 150 kV or less. These findings led to the present disclosure.
Specifically, an X-ray shielding glass of the present disclosure has a composition including:
15 mass % to 25 mass % B2O3;
7 mass % to 50 mass % La2O3;
7 mass % to 50 mass % Gd2O3;
10 mass % to 25 mass % WO3;
0 mass % to 7 mass % SiO2;
0 mass % to 10 mass % ZrO2;
0 mass % to 8 mass % Nb2O5;
0 mass % to 10 mass % Ta2O5;
0 mass % to 5 mass % Bi2O3;
0 mass % to 3 mass % CeO2; and
0 mass % to 1 mass % Sb2O3.
The glass does not contain ZnO, and
the total content of La2O3 and Gd2O3 in the glass is 45 mass % to 65 mass %.
When the thickness of the glass is 3 mm, the transmittance of the glass to an X-ray from an X-ray tube with a tube voltage of 60 kV is 0.0050% or less, and the transmittance of the glass to an X-ray from an X-ray tube with a tube voltage of 100 kV is 0.1500% or less. Such an X-ray shielding glass has high shielding capability against X-rays with a tube voltage of 150 kV or less.
The density of the X-ray shielding glass of the present disclosure is preferably 5.00 g/cm3 or more.
The refractive index (nd) of the X-ray shielding glass of the present disclosure is preferably 1.855 or less.
For the X-ray shielding glass of the present disclosure, the total content of La2O3, Gd2O3, and WO3 is preferably 36 mol % or more.
Further, a glass component of the present disclosure uses the X-ray shielding glass described above as a material. Such a glass component has high shielding capability against X-rays with a tube voltage of 150 kV or less.
The present disclosure can provide an X-ray shielding glass having high shielding capability against X-rays with a tube voltage of 150 kV or less. Further, the present disclosure can provide a glass component that uses the above-described X-ray shielding glass and has high shielding capability against X-rays with a tube voltage of 150 kV or less.
(X-Ray Shielding Glass)
An X-ray shielding glass according to one embodiment of the present disclosure (hereinafter may also be referred to as “glass of this embodiment”) will now be described. The requirements for the composition of the glass of this embodiment include that the composition contains:
15 mass % to 25 mass % B2O3;
7 mass % to 50 mass % La2O3;
7 mass % to 50 mass % Gd2O3;
10 mass % to 25 mass % WO3;
0 mass % to 7 mass % SiO2;
0 mass % to 10 mass % ZrO2;
0 mass % to 8 mass % Nb2O5;
0 mass % to 10 mass % Ta2O5;
0 mass % to 5 mass % Bi2O3;
0 mass % to 3 mass % CeO2; and
0 mass % to 1 mass % Sb2O3,
no ZnO is contained, and
the total content of La2O3 and Gd2O3 in the glass is 45 mass % to 65 mass %. Further, property requirements for the glass of this embodiment are that when the thickness of the glass is 3 mm, the transmittance of the glass to X-rays from an X-ray tube with a tube voltage of 60 kV is 0.0050% or less, and the transmittance of the glass to X-rays from an X-ray tube with a tube voltage of 100 kV is 0.1500% or less.
The glass of this embodiment is not only useful for shielding against X-rays from X-ray tubes with tube voltages of 60 kV and 100 kV but also for shielding against X-rays emitted from a tube with a given voltage of 150 kV or less. Further, the tube voltage of the X-ray tube emitting the X-ray which the glass of this embodiment blocks is more preferably 130 kV or less, still more preferably 120 kV or less.
The above glass composition has been found through repeated experiments, and the limitations of the components are based on the following reasons.
<B2O3>
B2O3 is an oxide enabling glass formation, and is an essential component critical for obtaining highly transparent glass without devitrification in the glass of this embodiment that contains a large amount of rare earth oxides such as La2O3 and Gd2O3. Now, when the content of B2O3 is less than 15 mass %, the stability of the glass would not be increased sufficiently, which precludes vitrification. On the other hand, when the content of B2O3 exceeds 25 mass %, the chemical durability of the glass is reduced and the ratio of components contributing to the improvement in the X-ray shielding performance is reduced, which precludes the X-ray shielding performance from being sufficiently improved. Accordingly, for the glass of this embodiment, the content of B2O3 is set in a range of 15 mass % to 25 mass %. In similar terms, the content of B2O3 in the glass of this embodiment is preferably 16 mass % or more and preferably 24 mass % or less.
<La2O3>
La2O3 is an essential component critical for achieving the objectives in the present disclosure, which can increase the density of glass and can impart high X-ray shielding capability to the glass. Further, La2O3 has the effect of improving the chemical durability of glass. Now, when the content of La2O3 is less than 7 mass %, the X-ray shielding capability of the glass cannot be increased sufficiently. On the other hand, when the content of La2O3 exceeds 50 mass %, the effect of an absorption edge in the radiation energy band is greatly exerted, which impairs the X-ray shielding capability. Accordingly, for the glass of this embodiment, the content of La2O3 is set in a range of 7 mass % to 50 mass %. In similar terms, the content of La2O3 in the glass of this embodiment is preferably 10 mass % or more and preferably 49 mass % or less.
<Gd2O3>
Similar to La2O3, Gd2O3 is an essential component critical for achieving the objectives in the present disclosure, which can increase the density of glass and can impart high X-ray shielding capability to the glass. Further, similar to La2O3, Gd2O3 has the effect of improving the chemical durability of glass. Now, when the content of Gd2O3 is less than 7 mass %, the X-ray shielding capability of the glass cannot be increased sufficiently. On the other hand, when the content of Gd2O3 exceeds 50 mass %, the effect of an absorption edge in the radiation energy band is greatly exerted, which impairs the X-ray shielding capability. Accordingly, for the glass of this embodiment, the content of Gd2O3 is set in a range of 7 mass % to 50 mass %. In similar terms, the content of Gd2O3 in the glass of this embodiment is preferably 8 mass % or more and preferably 48 mass % or less.
<La2O3+Gd2O3>
As described above, both La2O3 and Gd2O3 are components that can increase the density of glass, and can impart high X-ray shielding capability to glass; using considerable amounts of those components can more effectively improve X-ray shielding capability and devitrification resistance of glass than using one of the components alone. For the glass of this embodiment, in terms of achieving such an effective improvement, the total content of La2O3 and Gd2O3 is set in a range of 45 mass % to 65 mass %. Further, the total content of La2O3 and Gd2O3 in the glass of this embodiment is preferably 50 mass % or more and preferably 62 mass % or less.
<WO3>
WO3 is an essential component critical for achieving the objectives in the present disclosure, which can increase the shielding capability against X-rays with a tube voltage of 150 kV or less. Further, WO3 is significantly effective in improving stability and chemical durability of glass. Now, when the content of WO3 is less than 10 mass %, the shielding capability against X-rays with a tube voltage of 150 kV or less cannot be increased sufficiently. On the other hand, a content of WO3 exceeding 25 mass % rather reduces the stability of glass, which precludes vitrification. Accordingly, for the glass of this embodiment, the content of WO3 is set in a range of 10 mass % to 25 mass %. In similar terms, the content of WO3 in the glass of this embodiment is preferably 24 mass % or less.
<La2O3+Gd2O3+WO3 (mol %)>
For the glass of this embodiment, the total content of La2O3, Gd2O3, and WO3 is preferably 36 mol % or more. When the above total content is 36 mol % or more, both mass ratio and molar ratio of La2O3, Gd2O3, and WO3 that contribute to the improvement in the X-ray shielding performance are sufficiently high, which can further improve the X-ray shielding capability of the glass. In similar terms, the total content of La2O3, Gd2O3, and WO3 in the glass of this embodiment is more preferably 36.5 mol % or more.
<SiO2>
SiO2 is an oxide enabling glass formation, and is a component that can improve the stability against devitrification and can improve the chemical durability of glass. However, when the content of SiO2 exceeds 7 mass %, fusibility is degraded and unmelted materials are likely to remain. Accordingly, for the glass of this embodiment, the content of SiO2 is set in a range of 0 mass % to 7 mass %. In similar terms, the content of SiO2 in the glass of this embodiment is preferably 6 mass % or less, more preferably 5 mass % or less. Further, the content of SiO2 in the glass of this embodiment is preferably more than 0 mass %, more preferably 1 mass % or more, still more preferably 2 mass % or more in terms of improving the fusibility, stability, and chemical durability of the glass.
<ZrO2>
ZrO2 is a component that can be used for the glass of this embodiment, since it has the effect of improving X-ray shielding capability and chemical durability. However, when the content of ZrO2 exceeds 10 mass %, the stability against devitrification would be degraded. Accordingly, for the glass of this embodiment, the content of ZrO2 is set in a range of 0 mass % to 10 mass %. In similar terms, the content of ZrO2 in the glass of this embodiment is preferably 9 mass % or less, more preferably 8 mass % or less. Further, the content of ZrO2 in the glass of this embodiment is preferably more than 0 mass %, more preferably 1 mass % or more, still more preferably 2 mass % or more in terms of further improving the X-ray shielding capability and the chemical durability of the glass.
<Nb2O5>
Nb2O5 is a component that can be used for the glass of this embodiment, since it has the effect of improving X-ray shielding performance. However, when the content of Nb2O5 exceeds 8 mass %, the stability against devitrification would be degraded. Accordingly, for the glass of this embodiment, the content of Nb2O5 is set in a range of 0 mass % to 8 mass %. In similar terms, the content of Nb2O5 in the glass of this embodiment is preferably 7 mass % or less, more preferably 6 mass % or less. Further, the content of Nb2O5 in the glass of this embodiment is preferably more than 0 mass %, more preferably 0.5 mass % or more, still more preferably 1 mass % or more in terms of further improving the X-ray shielding capability.
<Ta2O5>
Ta2O5 is a component that can be used for the glass of this embodiment, since it has the effect of improving X-ray shielding performance. However, since Ta2O5 is an extremely expensive material, it is not suitable for use in large quantity. Accordingly, for the glass of this embodiment, the content of Ta2O5 is set in a range of 0 mass % to 10 mass %. In similar terms, the content of Ta2O5 in the glass of this embodiment is preferably 8 mass % or less.
<Bi2O3>
Bi2O3 is a component that can be used for the glass of this embodiment, since it has a high shielding effect particularly against X-rays with a tube voltage of more than 100 kV. However, although Bi2O3 is used in large quantity, the shielding capability against X-rays with a tube voltage of 150 kV or less is not significantly improved. Further, when the content of Bi2O3 exceeds 5% mass %, the transmittance of light in the ultraviolet range to the visible range is reduced. Accordingly, for the glass of this embodiment, the content of Bi2O3 is set in a range of 0 mass % to 5 mass %.
<CeO2>
CeO2 is a component that can be used for the glass of this embodiment, since it has the effect of reducing coloration of glass due to X-ray irradiation. However, when CeO2 is used in large quantity, the absorption edge of the glass in the ultraviolet range to the visible range is shifted to the long wavelength side, which reduces the visible light transmissivity. Accordingly, for the glass of this embodiment, the content of CeO2 is set in a range of 0 mass % to 3 mass %.
<Sb2O3>
Sb2O3 is a component that can be used in order to perform degassing during the glass melting. Accordingly, for the glass of this embodiment, the content of Sb2O3 is set in a range of 0 mass % to 1 mass % in terms of obtaining the degassing effect with the minimum essential amount.
<Other Components>
The glass of this embodiment may contain components other than the above components, for example, CsO2, SrO, BaO, Y2O3, Yb2O3, etc. as appropriate without departing from the objectives.
Although ZnO is a component that effectively improves the fusibility of glass, it has been found not to greatly contribute to the improvement in the X-ray shielding performance of the glass of this embodiment. Further, since the molecular weight of ZnO is relatively low, the ratio of La2O3, Gd2O3, and WO3 that contribute to the improvement in the X-ray shielding performance is undesirably reduced even when ZnO is used in small quantity. Therefore, in terms of maintaining the ratio of La2O3, Gd2O3, and WO3 that contribute to the improvement in the X-ray shielding performance, ZnO is not contained in the glass of this embodiment.
Further, components containing transition metals (excluding La, Gd, W, Zr, Nb, Ta, and Ce) such as Ti, V, Cr, Mn, Fe, Co, Ni, Cu, Ag, and Mo color the class and allow the absorption of light with a certain wavelength in the visible range even when the components are used alone or in combination in small quantity. In particular, since the molecular weight of Ti, V, Cr, Mn, Fe, Co, Ni, and Cu is relatively low, the ratio of La2O3, Gd2O3, and WO3 that contribute to the improvement in the X-ray shielding performance is undesirably reduced even when those elements are used alone or in combination in small quantity. Accordingly, it is preferred that the glass of this embodiment does not substantially contain components having the above-described transition metals.
In this specification, “does not substantially contain” means to include cases where the components concerned are inevitably contained as impurities, specifically, where the relevant components are contained in a ratio of 0.2 mass % or less.
Further, in recent years, there are tendencies to avoid the use of components having Pb, Th, Cd, Tl, or Os as hazardous chemical substances; therefore, measures are required to be taken for environmental protection when glass using those components is produced, processed, and discarded. Accordingly, it is preferred that the glass of this embodiment does not substantially contain any component having Pb, Th, Cd, Tl, or Os.
Further, fluorine components would be volatilized when glass is melted, and are further likely to cause striae. Accordingly, it is preferred that the glass of this embodiment does not substantially contain fluorine components.
Further, since the molecular weight of Li, Na, K, Be, Mg, and Ca is low, the ratio of La2O3, Gd2O3, and WO3 that contribute to the improvement in the X-ray shielding performance is undesirably reduced greatly even when those elements are used alone or in combination in small quantity. Accordingly, it is preferred that the glass of this embodiment does not substantially contain any component having Li, Na, K, Be, Mg, or Ca.
In terms of further ensuring the desired properties to be obtained, the glass of this embodiment preferably has a composition consisting only of the essential components described above and optional components (a composition that may contain only B2O3, La2O3, Gd2O3, and WO3 as the essential components and components selected from SiO2, ZrO2, Nb2O5, Ta2O5, Bi2O3, CeO2, and Sb2O3).
In this specification, “consist only of the above components” include cases where impurity components other than the components concerned are inevitably contained, specifically case where the ratio of the impurity components is 0.2 mass % or less.
The following describes the properties of the glass of this embodiment.
The density of the glass of this embodiment is preferably 5.00 g/cm3 or more. Since the X-ray shielding capability is likely to be higher as the density of the glass is higher, a glass density of 5.00 g/cm3 or more results in better X-ray shielding capability. In similar terms, the density of the glass of this embodiment is more preferably 5.05 g/cm3 or more and still more preferably 5.10 g/cm3 or more.
The density of the glass may be, for example, controlled by appropriately selecting the kind and/or the content of the components to be contained in the glass. Further, a glass having a density of 5.00 g/cm3 or more can be usually obtained by fulfilling the requirements for the glass composition described above.
The above-described density can be measured by the method to be described in Examples.
For the glass of this embodiment, when the thickness of the glass is 3 mm, the transmittance of the glass to X-rays from an X-ray tube with a tube voltage of 60 kV is 0.0050% or less, and the transmittance of the glass to X-rays from an X-ray tube with a tube voltage of 100 kV is 0.1500% or less. The glass of this embodiment has the above-described properties, so that high shielding capability can be brought out against X-rays from an X-ray tube with a tube voltage of 150 kV or less.
The transmittance of the glass to X-rays from an X-ray tube with a tube voltage of 60 kV and the transmittance to X-rays from an X-ray tube with a tube voltage of 100 kV may be, for example, controlled by appropriately selecting the kind and/or the content of the components to be contained in the glass. Further, a glass having a transmittance of 0.0050% or less to X-rays from an X-ray tube with a tube voltage of 60 kV and a transmittance of 0.1500% or less to X-rays from an X-ray tube with a tube voltage of 100 kV can usually be obtained by fulfilling the requirements for the glass composition described above. In particular, a glass having a transmittance of 0.0050% or less to X-rays from an X-ray tube with a tube voltage of 60 kV and a transmittance of 0.1500% or less to X-rays from an X-ray tube with a tube voltage of 100 kV satisfies the above-described glass composition requirements and can be more reliably obtained when the total content of La2O3, Gd2O3, and WO3 is 36 mol % or more.
The above-described X-ray transmittance can be measured by the method to be described in Examples.
The glass of this embodiment with a thickness of 10 mm preferably has a transmittance of 40% or more to light with a wavelength of 400 nm. When the glass has the above-described transmittance, better visible light transmissivity can be brought out. In similar terms, the glass of this embodiment more preferably has a transmittance of 50% or more, more preferably 55% or more, to light with a wavelength of 400 nm.
The glass of this embodiment with a thickness of 10 mm preferably has a transmittance of 80% or more to light with a wavelength of 550 nm. When the glass has the above-described transmittance, better visible light transmissivity can be brought out.
The visible light transmittance described above may be, for example, controlled by appropriately selecting the kind and/or the content of the components to be contained in the glass. Further, a glass having a transmittance within the preferred range mentioned above can be usually obtained by fulfilling the requirements for the glass composition described above.
The above-described visible light transmittance can be measured by the method to be described in Examples.
The refractive index (nd) of the glass of this embodiment is preferably 1.855 or less. The glass having the above refractive index is more useful, since the surface reflection of light incident upon the glass can be sufficiently reduced.
The refractive index of the glass may be, for example, controlled by appropriately selecting the kind and/or the content of the components to be contained in the glass. Further, a glass having a refractive index (nd) of 1.855 or less can be usually obtained by fulfilling the requirements for the glass composition described above.
The above-described refractive index can be measured by the method to be described in Examples.
<Method of Producing Glass>
The following describes a method of producing the glass of this embodiment.
The method of producing the glass of this embodiment is not limited as long as the glass satisfies the above-described composition requirements and property requirements, and the glass can be produced in accordance with a conventional production method.
For example, as the raw material of each component that may be contained in the glass of this embodiment, oxides are prepared to have a weight at a predetermined ratio, and the oxides are fully mixed to obtain a preparation raw material. Next, the preparation raw material is charged into a melting container (for example, a crucible made of precious metal) that is not reactive with the material concerned, and the material is heated and melted at 1100° C. to 1500° C. in an electric furnace. During the heating, the material is stirred at the appropriate times to be refined and homogenized. Subsequently, the melt is cast into a metal mold preheated to an appropriate temperature, and was then allowed to cool slowly, thereby eliminating strains, thus the glass of this embodiment can be obtained.
(Glass Component)
A glass component of this embodiment (hereinafter may also be referred to as “glass component of this embodiment”) uses the X-ray shielding glass described above as a material. In other words, the glass component of this embodiment includes the above-described X-ray shielding glass. The glass component of this embodiment uses the above-described X-ray shielding glass as a material, thus it has high shielding capability against X-rays from an X-ray tube with a tube voltage of 150 kV or less.
Examples of glass components include, but not limited to, lenses such as spherical lenses, aspherical lenses, microlenses, and rod lenses; arrays of lenses such as microlens arrays; preform materials; and fiber materials.
X-ray shielding glasses of the present disclosure will be described in more concrete terms using Examples and Comparative Examples below; however, the present disclosure is not limited to Examples below.
Glasses according to Examples and Comparative Examples were produced by the following method.
For the raw material of each component in the composition given in Table 1 and Table 2, an oxide corresponding to each component was used; the oxides were prepared to have a weight at the desired ratio, and the oxides were fully mixed to obtain preparation raw materials. Next, the preparation raw materials were charged into a platinum crucible and were melted at temperatures of 1100° C. to 1500° C. in an electric furnace for several hours and were meanwhile stirred with a platinum stirring rod at the appropriate times, thereby performing homogenization and refinement. After that, the materials were cast into a metal mold having been preheated to an appropriate temperature and were allowed to cool slowly, thus transparent and homogenous glasses were obtained (note however that glass was not obtained in Comparative Example 5 and Comparative Example 8).
Note that Comparative Examples 1 and 2 were examples corresponding to the compositions of Examples 1 and 2 in PTL 3 (JP 2008-088019 A), respectively; and Comparative Example 3 was an example corresponding to the composition of Example 1 in PTL 4 (JP 2008-088021 A).
Further, Table 1 and Table 2 give the compositions by mass, and the compositions were converted into the composition by mol for reference and the results are given in Table 3 and Table 4, respectively.
Each of the obtained glasses, was subjected to the calculation of X-ray transmittances (tube voltage of the X-ray tube: 60 kV and 100 kV), and the measurements of the density, the refractive index (nd), and the visible light transmittance (wavelength: 550 nm and 400 nm) by the following procedure The results are given in Table 1 and Table 2 (and Table 3 and Table 4).
<X-Ray Transmittance>
When X-ray were incident on a glass, part of the X-rays was absorbed by the glass, and the rest was transmitted to exit; the X-ray transmittance was calculated as the ratio of the intensity of the exiting X-ray to the intensity of the incident X-rays. More specifically, the incident X-ray spectrum was calculated using the formula found by Tucker, et al., and the attenuation coefficient per energy was then calculated based on the information of the percentage by mass and the density of the elements forming the object to be measured (glass) with reference to the data specified by the National Institute of Standards and Technology (NIST). For the calculated incident X-ray spectrum, the X-rays transmitted through the measurement object was taken as transmitted X-rays, and (transmitted X-rays/incident X-rays)×100 was defined as X-ray transmittance (%).
Note that in the calculation of the X-ray transmittance, a glass having been worked to have a thickness of 3 mm was used, and the transmittance was calculated for X-rays from X-ray tubes with a tube voltage of 60 kV and 100 kV.
<Density>
The density of the glass was measured using “ED-120T” manufactured by Mirage Trading Co., Ltd. in accordance with “JIS Z 8807: 2012 Methods of measuring density and specific gravity of solid”.
<Refractive Index (nd)>
The refractive index (nd) of the glass was measured using “KPR-2000” manufactured by Kalnew Optical Industrial Co., Ltd. in accordance with “JIS B 7071-2: 2018 Measuring method for refractive index of optical glass—Part 2: Vee block refractometers method”.
<Visible Light Transmittance>
The glass obtained was worked into an opposite surface parallel polished product having a thickness of 10 mm, and the visible light transmittance of the glass was measured using “U-4100” manufactured by Hitachi, Ltd. in accordance with “JOGIS 02-2003 Measuring Method for Color-Degree of Optical Glass” of the Japan Optical Glass Industrial Standards. Note however that in this disclosure, the transmittance is specified instead of the color degree. Specifically, the spectral transmittance for 200 nm to 800 nm was measured in accordance with JIS Z 8722, and the transmittance for 400 nm and the transmittance for 550 nm were sought. Such transmittances being high indicate that the visible light transmissivity is high.
Table 1 demonstrates that all the glasses of Examples 1 to 14 according to the present disclosure satisfied the predetermined requirements for the glass composition, and had an X-ray transmittance of 0.0050% or less to X-rays from an X-ray tube with a tube voltage of 60 kV and had an X-ray transmittance of 0.1500% or less to X-rays from an X-ray tube with a tube voltage of 100 kV. Thus, the glasses of Examples 1 to 14 were found to bring out high shielding capability against X-rays with a tube voltage of 150 kV or less. Note that all of the glasses of Examples 1 to 14 successfully had a density of 5.00 g/cm3 or more, and a refractive index (nd) of 1.855 or less.
On the other hand, Table 2 demonstrates that the transmittance of the glass of Comparative Example 1 to X-rays from an X-ray tube with a tube voltage of 100 kV exceeded 0.1500%. This may be because since ZnO, TiO2, etc. having a low molecular weight were contained in the glass, the ratio of La2O3, Gd2O3, and WO3 contributing to the improvement in the X-ray shielding performance was low. Further, since the glass of Comparative Example 1 had a refractive index (nd) exceeding 1.855, there was a possibility of the surface reflection of incident light. This is considered to have been due to TiO2 contained in the glass.
The glass of Comparative Example 2 had a transmittance of more than 0.0050% to X rays from an X-ray tube with a tube voltage of 60 kV and a transmittance of more than 0.1500% to X rays from an X-ray tube with a tube voltage of 100 kV. Further, the glass of Comparative Example 2 had a density of less than 5.00 g/cm3. This may be because since ZnO, TiO2, Li2O etc. having a low molecular weight were contained in the glass, the ratio of La2O3, Gd2O3, and WO3 contributing to the improvement in the X-ray shielding performance was low.
The glass of Comparative Example 3 had a transmittance of more than 0.0050% to X rays from an X-ray tube with a tube voltage of 60 kV and a transmittance of more than 0.1500% to X rays from an X-ray tube with a tube voltage of 100 kV. Further, the glass of Comparative Example 3 had a density of less than 5.00 g/cm3. This may be because since ZnO etc. having a low molecular weight were contained in the glass, the ratio of La2O3, Gd2O3, and WO3 contributing to the improvement in the X-ray shielding performance was low.
The transmittance of the glass of Comparative Example 4 to X-rays from an X-ray tube with a tube voltage of 100 kV exceeded 0.1500%. This may be because the content of B2O3 was excessively high.
In Comparative Example 5, no vitrification occurred. This might have been due to the excessively low content of B2O3 and the excessively high content of SiO2.
The transmittance of the glass of Comparative Example 6 to X-rays from an X-ray tube with a tube voltage of 100 kV exceeded 0.1500%. This may be attributed to that for example, since the content of La2O3 was excessively high (and the content of Gd2O3 was excessively low), the effect of the absorption edge of the radiation energy band of La2O3 was greatly exerted.
The transmittance of the glass of Comparative Example 7 to X-rays from an X-ray tube with a tube voltage of 60 kV exceeded 0.0050%. This may be attributed to that for example, since the content of Gd2O3 was excessively high (and the content of La2O3 was excessively low), the effect of the absorption edge of the radiation energy band of Gd2O3 was greatly exerted.
In Comparative Example 8, no vitrification occurred. This may be because the content of WO3 was excessively high.
The glass of Comparative Example 9 had a transmittance of more than 0.0050% to X rays from an X-ray tube with a tube voltage of 60 kV and a transmittance of more than 0.1500% to X rays from an X-ray tube with a tube voltage of 100 kV. This may be because the content of WO3 was excessively low.
The present disclosure provides an X-ray shielding glass having high shielding capability against X-rays with a tube voltage of 150 kV or less. Further, the present disclosure provides a glass component that uses the above-described X-ray shielding glass and has high shielding capability against X-rays with a tube voltage of 150 kV or less.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2019-180546 | Sep 2019 | JP | national |
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/JP2020/034794 | 9/14/2020 | WO |
