[go: up one dir, main page]

CN102760506A - Phosphor sheet - Google Patents

Phosphor sheet Download PDF

Info

Publication number
CN102760506A
CN102760506A CN2012101304518A CN201210130451A CN102760506A CN 102760506 A CN102760506 A CN 102760506A CN 2012101304518 A CN2012101304518 A CN 2012101304518A CN 201210130451 A CN201210130451 A CN 201210130451A CN 102760506 A CN102760506 A CN 102760506A
Authority
CN
China
Prior art keywords
luminescent material
material plate
projection
protrusions
layer
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
CN2012101304518A
Other languages
Chinese (zh)
Inventor
M.富克斯
K.洛瓦克
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Siemens Corp
Original Assignee
Siemens Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Siemens Corp filed Critical Siemens Corp
Publication of CN102760506A publication Critical patent/CN102760506A/en
Pending legal-status Critical Current

Links

Images

Classifications

    • CCHEMISTRY; METALLURGY
    • C09DYES; PAINTS; POLISHES; NATURAL RESINS; ADHESIVES; COMPOSITIONS NOT OTHERWISE PROVIDED FOR; APPLICATIONS OF MATERIALS NOT OTHERWISE PROVIDED FOR
    • C09KMATERIALS FOR MISCELLANEOUS APPLICATIONS, NOT PROVIDED FOR ELSEWHERE
    • C09K11/00Luminescent, e.g. electroluminescent, chemiluminescent materials
    • C09K11/08Luminescent, e.g. electroluminescent, chemiluminescent materials containing inorganic luminescent materials
    • C09K11/62Luminescent, e.g. electroluminescent, chemiluminescent materials containing inorganic luminescent materials containing gallium, indium or thallium
    • C09K11/626Halogenides
    • C09K11/628Halogenides with alkali or alkaline earth metals
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01TMEASUREMENT OF NUCLEAR OR X-RADIATION
    • G01T1/00Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
    • G01T1/16Measuring radiation intensity
    • G01T1/20Measuring radiation intensity with scintillation detectors
    • G01T1/2012Measuring radiation intensity with scintillation detectors using stimulable phosphors, e.g. stimulable phosphor sheets
    • GPHYSICS
    • G21NUCLEAR PHYSICS; NUCLEAR ENGINEERING
    • G21KTECHNIQUES FOR HANDLING PARTICLES OR IONISING RADIATION NOT OTHERWISE PROVIDED FOR; IRRADIATION DEVICES; GAMMA RAY OR X-RAY MICROSCOPES
    • G21K4/00Conversion screens for the conversion of the spatial distribution of X-rays or particle radiation into visible images, e.g. fluoroscopic screens

Landscapes

  • Chemical & Material Sciences (AREA)
  • High Energy & Nuclear Physics (AREA)
  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Molecular Biology (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Inorganic Chemistry (AREA)
  • Health & Medical Sciences (AREA)
  • Materials Engineering (AREA)
  • Organic Chemistry (AREA)
  • General Engineering & Computer Science (AREA)
  • Measurement Of Radiation (AREA)
  • Conversion Of X-Rays Into Visible Images (AREA)

Abstract

本发明涉及发光材料板,其具有基底(1)和位于其上的附加层(2),在所述附加层(2)上涂覆有发光材料层,其中所述附加层(2)以如下方式格栅化,由此通过沟槽(3-7)生成分离的突起(8),形成发光材料层的发光材料的发光材料针状物生成在突起(8)的表面上,其中第一突起(8)形成第一结构,第二突起(9)形成几何上不同于第一结构的第二结构,并且所述第二结构设置在第一结构之间。这种发光材料板即使在厚度大的发光材料层时也具有好的成像质量。

Figure 201210130451

The invention relates to a phosphor plate with a substrate (1) and an additional layer (2) located thereon, on which a layer of phosphor is applied, wherein the additional layer (2) is as follows gridded in such a way that separate protrusions (8) are generated by the grooves (3-7), the luminescent material needles of the luminescent material forming the luminescent material layer are formed on the surface of the protrusions (8), wherein the first protrusion (8) First structures are formed, the second protrusions (9) form second structures geometrically different from the first structures, and the second structures are disposed between the first structures. Such a phosphor plate has a good imaging quality even with thick phosphor layers.

Figure 201210130451

Description

发光材料板Luminescent material plate

技术领域 technical field

本发明涉及一种发光材料板,其具有基底和位于其上的附加层,在所述附加层上涂覆有发光材料层,其中所述附加层以如下方式格栅化(rastem),由此通过沟槽形成分离的突起,形成发光材料层的发光材料的发光材料针状物生成在突起(Noppe)的表面上。The invention relates to a phosphor plate with a substrate and an additional layer thereon, on which a layer of phosphor is applied, wherein the additional layer is rasterized in such a way that The separate protrusions are formed by the grooves, on the surface of which the phosphor needles of the phosphor forming the phosphor layer are produced.

背景技术 Background technique

在这种发光材料板中,发光材料可以为蓄能型发光材料(Speicherleuchtstoff)或闪烁体(Szintillator)。In such a phosphor plate, the phosphor can be an energy-storage phosphor or a scintillator.

常见的闪烁体包括CsI:Tl、CsI:Na、NaI:Tl或类似材料,其含有碱-卤化物,其中CsI特别适合作为闪烁体材料,这是因为其可以长成针状物形状。由此即使在确保X射线最佳吸收的较大层厚时也获得了X射线呈现的好的位置分辨率。好的位置分辨率由所谓的“光导作用”产生,该光导作用通过闪烁体针状物之间的空气间隔实现。Common scintillators include CsI:Tl, CsI:Na, NaI:Tl or similar materials containing alkali-halides, with CsI being particularly suitable as a scintillator material because it can grow into a needle shape. This results in a good spatial resolution of the x-ray representation even with relatively large layer thicknesses which ensure optimal absorption of the x-rays. Good positional resolution is produced by so-called "photoguiding" via the air spaces between the scintillator needles.

将X射线和γ射线转换成光的闪烁体例如在医学成像中,在检测货物和包装体时以及在无破坏材料检测中使用。这些发光物质应当在“更硬”的X射线具有高的吸收,所述“更硬”的X射线由所谓C弧在放射学中增加的3D应用而引起。Scintillators, which convert X-rays and gamma rays into light, are used, for example, in medical imaging, when inspecting goods and packages, and in non-destructive material inspection. These luminescent substances should have a high absorption in the "harder" X-rays caused by the increased 3D use of so-called C-arcs in radiology.

如图1所示,与常见的CsI:Tl-闪烁体的辐射质量比较,在“辐射硬度”增加时,吸收度(Absorption)从RQA3时的87%到RQA9时的44%,几乎减半。As shown in Figure 1, compared with the radiation quality of the common CsI:Tl-scintillator, when the "radiation hardness" increases, the absorption (Absorption) is almost halved from 87% at RQA3 to 44% at RQA9.

RQA表示基于添加了铝的过滤剂(来自标准IEC 61267)的辐射质量。RQA stands for Radiation Quality based on aluminum-added filters (from standard IEC 61267).

作为对比,在图1中除了显示闪烁体CsI:Tl的吸收曲线外,还显示了另外四种闪烁体的吸收曲线,其中该测量分别在20mm直径的混合辐射束条件下进行。For comparison, in addition to the absorption curves of the scintillator CsI:Tl shown in Figure 1, the absorption curves of four other scintillators are also shown, wherein the measurements were performed under the condition of a mixed radiation beam with a diameter of 20 mm.

在图1中示出的吸收曲线A1至A5和所给出的RQA-值表示:The absorption curves A1 to A5 shown in Figure 1 and the given RQA-value represent:

A1未结构化的发光材料UFC的吸收曲线,Absorption curve of A1 unstructured luminescent material UFC,

A2结构化的发光材料UFC的吸收曲线,Absorption curve of A2 structured luminescent material UFC,

A3发光材料CsI:Tl(400μm)的吸收曲线,The absorption curve of A3 luminescent material CsI:Tl (400μm),

A4发光材料GOS的吸收曲线,和Absorption curve of A4 luminescent material GOS, and

A5层厚小于A4的发光材料GOS的吸收曲线,The absorption curve of the luminescent material GOS with A5 layer thickness smaller than A4,

其中UFC表示超快速陶瓷(Ultra Fast Ceramic)和GOS表示氧硫化钆。Among them, UFC means Ultra Fast Ceramic and GOS means gadolinium oxysulfide.

RQA3    50kV/10mmAl,RQA3 50kV/10mmAl,

RQA5    70kV/21mmAl,RQA5 70kV/21mmAl,

RQA7    90kV/30mmAl和RQA7 90kV/30mmAl and

RQA9    120kV/40mmAl。RQA9 120kV/40mmAl.

闪烁体材料UFC必须是结构化的,从而减少侧面的光传播。这降低了各种辐射质量下的吸收度。尽管存在结构化,但是在UFC情况下分辨率通常为1线对/mm(Linienpaar pro mm)。相应地,CsI:Tl在400μm时的分辨率典型为4线对/mm,并且因此是优选的。The scintillator material UFC must be structured so as to reduce light propagation from the sides. This reduces the absorbance at various radiation qualities. Despite the structuring, the resolution is usually 1 line pair/mm (Linienpaar pro mm) in the case of UFC. Correspondingly, the resolution of CsI:Tl at 400 μm is typically 4 line pairs/mm, and is therefore preferred.

为了增加辐射硬度的情况下补偿明显降低的吸收度,在常见的CsI:Tl-闪烁体的情况下必须显著提高发光材料层的厚度。为了在RQA9的情况下实现90%的吸收度,层厚必须为约1.8mm。In order to compensate for the significantly lower absorption with increased radiation hardness, the thickness of the phosphor layer must be significantly increased in the case of conventional CsI:Tl scintillators. In order to achieve an absorption of 90% in the case of RQA9, the layer thickness must be about 1.8 mm.

此时的一个问题是,尽管在基底温度不是过高的情况下随着层厚的增加,闪烁体-针状物(发光材料针状物)的直径可以保持小于10μm,但是在发光材料层中围绕每个闪烁体-针状物不确定地形成了所需的裂纹。通过这些裂纹在闪烁体-针状物之间产生了受限的间隔,理想情况该间隔具有的间距为闪烁体发射波长的一半。在碘化铯(CsI)的情况下,该间距为约250nm至300nm。A problem here is that, although the diameter of the scintillator-needles (needles of luminescent material) can remain smaller than 10 μm with increasing layer thickness if the substrate temperature is not too high, in the luminescent material layer Around each scintillator-needle formed the desired crack indefinitely. These cracks create a limited spacing between the scintillator-needle, which ideally has a pitch of half the emission wavelength of the scintillator. In the case of cesium iodide (CsI), this spacing is approximately 250 nm to 300 nm.

相反地,由于在冷却蒸镀基底时膨胀系数低,在发光材料层中产生了收缩裂纹。这导致了裂纹宽度在1μm以上的叠加的不规则裂纹结构,其包裹了全部的针状物芯包(Nadelpakete),如图2中所示,其中显示了已知CsI-层在光栅电子显微镜下放大50倍的照片。此时的裂纹间距在0.5mm至1.5mm的尺寸级数上,并且该裂纹具有最高达约10μm的宽度。Conversely, shrinkage cracks are generated in the luminescent material layer due to the low coefficient of expansion when cooling the evaporated substrate. This leads to a superimposed irregular crack structure with a crack width above 1 μm that encloses the entire needle core (Nadelpakete), as shown in Figure 2, which shows the known CsI-layer under a grating electron microscope Enlarge the photo 50 times. The distance between the cracks in this case is on the order of size from 0.5 mm to 1.5 mm, and the cracks have a width of up to about 10 μm.

在晶界、间隔和裂纹处,已知从发光材料层比从发光材料针状物本身输出耦合(auskoppeln)更多的光。因此,聚焦光束的光晕(Lichthof),如图3中所示,显示出清楚的光晕(Halo,即在具有“增亮”针状物边界的非直接照射环境中的较均匀的过度照射的变化(Verlauf)。该问题在增加层厚时也显著加剧,因为需要更多的能量以分离发光材料针状物。At grain boundaries, gaps and cracks, it is known that more light is coupled out of the phosphor layer than from the phosphor needles themselves. Therefore, the halo (Lichthof) of the focused beam, as shown in Fig. 3, shows a clear halo (Halo, i.e. a relatively uniform over-illumination Variation of (Verlauf). This problem is also significantly exacerbated with increasing layer thickness, since more energy is required to separate the phosphor needles.

发光材料层由蓄能型发光材料构成的发光材料板例如由DE10242006A1已知。在衬底上涂覆的附加层用于平衡基底与发光材料层之间不同的热膨胀系数,并且因此由聚合物(例如聚酰亚胺或帕利灵(Parylen))构成,且具有规则的、优选n-角结构。A phosphor plate in which the phosphor layer consists of an energy-storage phosphor is known, for example, from DE 10 24 2006 A1. The additional layer applied on the substrate is used to balance the different coefficients of thermal expansion between the substrate and the layer of luminescent material and therefore consists of a polymer such as polyimide or Parylen and has a regular, An n-angle structure is preferred.

在根据DE10242006A1的发光材料板中,由于具有规则的多角形结构,产生了“线”,沿着该线形成了裂纹并继续,而没有分离成单个的结构元件(线性裂纹扩展)。由于蓄能型发光材料的层厚的增大,加剧了叠加裂纹结构的形成。这不仅仅涉及蓄能型发光材料层如溴化铯(CsBr),而且涉及闪烁体层如碘化铯(CsI)的情况。In the phosphor plate according to DE 10242006 A1, due to the regular polygonal structure, "lines" are produced along which cracks form and continue without separation into individual structural elements (linear crack propagation). Due to the increase in the layer thickness of the energy-storage luminescent material, the formation of superimposed crack structures is aggravated. This is the case not only for layers of energy-storage luminescent materials such as cesium bromide (CsBr), but also for scintillator layers such as cesium iodide (CsI).

在图4和图5中,在例如两个不同多角形结构处的叠加裂纹结构(图4中的四方形和图5中的六角形)在由碘化铯构成的厚度为500μm的发光材料层中已经清楚可见。附加层的结构化导致裂纹的沟渠化(Kanalisierung),由此尽管避免了不期望的宽裂纹,但是裂纹在择优取向(Vorzugsrichtung)上清楚可见。In FIGS. 4 and 5, superimposed crack structures at, for example, two different polygonal structures (squares in FIG. 4 and hexagons in FIG. 5) in a luminescent material layer made of cesium iodide with a thickness of already clearly visible. The structuring of the additional layer results in a channelization of the cracks, so that although undesirably wide cracks are avoided, the cracks are clearly visible in the preferred orientation.

此外,在DE68906478T2中记载了一种具有闪烁体作为发光材料的发光材料板(闪烁体板)。该闪烁体涂覆在铝基底上。该铝基底具有蜂窝形状的表面结构,其通过Eloxal-法(铝的电解氧化)实施。Furthermore, DE 68906478 T2 describes a phosphor plate (scintillator plate) having a scintillator as phosphor. The scintillator was coated on an aluminum substrate. The aluminum substrate has a honeycomb-shaped surface structure, which is carried out by the Eloxal method (electrolytic oxidation of aluminum).

独立于发光材料的类型,即在蓄能型发光材料板的情况下以及在闪烁体板的情况下,出于上述原因,应当尽可能避免叠加裂纹结构的形成。Independently of the type of phosphor, ie in the case of energy-storage phosphor plates as well as in the case of scintillator plates, the formation of superimposed crack structures should be avoided as much as possible for the above reasons.

发明内容 Contents of the invention

本发明的目的在于,提供一种发光材料板,其在发光材料层厚度大的情况下也具有好的成像质量

Figure BDA0000158629350000031
The object of the present invention is to provide a phosphor plate which has a good image quality even with large phosphor layer thicknesses
Figure BDA0000158629350000031

该目的根据本发明通过根据权利要求1的发光材料板得以解决。根据本发明的发光材料板的有利的实施方案分别为其他权利要求的主题。This object is solved according to the invention by a phosphor plate according to claim 1 . Advantageous embodiments of the phosphor plate according to the invention are in each case the subject-matter of the further claims.

权利要求1的发光材料板包括基底和位于其上的附加层,在该附加层上涂覆有发光材料层,其中所述附加层以如下方式格栅化:通过沟槽形成分离的突起,形成发光材料层的发光材料的发光材料针状物生成在突起的表面上,其中第一突起形成第一结构,第二突起形成几何上不同于第一结构的第二结构,并且所述第二结构设置在第一结构之间。The luminescent material plate of claim 1 comprising a substrate and an additional layer thereon, on which the luminescent material layer is applied, wherein the additional layer is gridded in such a way that separate protrusions are formed by grooves forming Luminescent material needles of the luminescent material of the luminescent material layer are produced on the surface of the protrusions, wherein the first protrusions form a first structure, the second protrusions form a second structure geometrically different from the first structure, and the second structure disposed between the first structures.

本发明方案的特征在于,第一突起形成第一结构,第二突起形成第二结构,其中所述第一结构和第二结构以几何上不同的方式形成,并且所述第二结构设置在第一结构之间。由此,第一突起和第二突起分别具有比第一突起相互之间和第二突起相互之间更短的距离。The solution of the present invention is characterized in that the first protrusion forms a first structure, and the second protrusion forms a second structure, wherein the first structure and the second structure are formed in a geometrically different manner, and the second structure is arranged at the second between a structure. As a result, the first protrusions and the second protrusions each have a shorter distance than the first protrusions and the second protrusions from each other.

该附加层使得本发明结构化可以简单的方式通过对聚合物、氧化物和金属常见的结构化方法实现。This additional layer enables the structuring according to the invention to be realized in a simple manner by the usual structuring methods for polymers, oxides and metals.

术语“形成几何上不同的结构”可以理解为所形成的结构具有例如不同的大小和/或不同的形状。这可以是第一结构内部和/或在第二结构内部的情况,而且也可以是第一结构和第二结构进行比较的情况(权利要求8和/或权利要求9)。The term "forming geometrically different structures" is understood to mean that the formed structures have, for example, different sizes and/or different shapes. This can be the case within the first structure and/or within the second structure, and it can also be the case when the first structure and the second structure are compared (claim 8 and/or claim 9).

由于第一突起和第二突起彼此直接相邻设置,所以由第一突起形成的沟槽被第二突起“干扰”。Since the first protrusion and the second protrusion are arranged directly adjacent to each other, the groove formed by the first protrusion is "interfered" by the second protrusion.

通过本发明的方案能够可靠地防止附加层中不期望的叠加裂纹结构,并因此可靠地防止破坏成像性质,取而代之的是确保有利的裂纹围绕发光材料针状物形成。本发明的发光材料板因此在发光材料层的层厚大的情况时也具有好的成像质量。Undesirable superimposed crack structures in the additional layer and thus damage to the imaging properties can be reliably prevented by the solution according to the invention, and instead favorable crack formation around the phosphor needles is ensured. The phosphor plate according to the invention therefore has a good image quality even in the case of large layer thicknesses of the phosphor layer.

有利的是,由第一突起形成的第一结构构成格栅结构,和/或由第二突起形成的第二结构构成格栅结构(权利要求2和3)。Advantageously, the first structure formed by the first protrusions constitutes a lattice structure and/or the second structure formed by the second protrusions constitutes a lattice structure (claims 2 and 3).

在本发明的范围内,在突起上可以形成一个或多个分离的发光材料针状物(权利要求4)。Within the scope of the invention, one or more separate phosphor needles may be formed on the protrusion (claim 4).

根据发光材料板的一个有利的实施方案,附加层的厚度为约10μm至50μm(权利要求5)。According to an advantageous embodiment of the phosphor plate, the thickness of the additional layer is approximately 10 μm to 50 μm (claim 5 ).

所述结构的格栅尺寸优选在10μm至100μm的范围,优选在20μm至50μm之间(权利要求6)。The grid size of the structure is preferably in the range of 10 μm to 100 μm, preferably between 20 μm and 50 μm (claim 6 ).

根据本发明的发光材料板的一个有利的实施方案,沟槽的宽度在10μm至50μm的范围(权利要求7),其中通过该沟槽各突起彼此分开。According to an advantageous embodiment of the phosphor plate according to the invention, the groove has a width in the range of 10 μm to 50 μm (claim 7 ), wherein the protrusions are separated from one another by the groove.

在具有上文所述缺点的附加层中可通过以下方式避免(erreichen)不期望的叠加裂纹结构的形成:The formation of undesired superimposed crack structures can be avoided in the case of additional layers with the above-mentioned disadvantages by:

-第一结构至少部分具有规则的形状,第二结构至少部分具有规则的形状(权利要求10),和/或- the first structure is at least partly of regular shape, the second structure is at least partly of regular shape (claim 10), and/or

-第一结构至少部分具有不规则的形状,第二结构至少部分具有不规则的形状(权利要求11),和/或- the first structure has an at least partially irregular shape, the second structure has an at least partially irregular shape (claim 11), and/or

-第一结构至少部分具有规则的形状,第二结构至少部分具有不规则的形状(权利要求12),和/或- the first structure has an at least partially regular shape and the second structure has an at least partially irregular shape (claim 12), and/or

-第一结构至少部分具有不规则的形状,第二结构至少部分具有规则的形状(权利要求13)。- The first structure has an at least partially irregular shape and the second structure has an at least partially regular shape (claim 13).

由突起形成的结构和/或突起本身可以具有例如n-角的(n-eckig)结构或形状。这对第一突起和第一结构以及第二突起和第二结构都成立(权利要求14至17)。The structures formed by the protrusions and/or the protrusions themselves may have, for example, an n-eckig structure or shape. This holds for both the first protrusion and the first structure and the second protrusion and the second structure (claims 14 to 17).

本发明的方案可以有利地在蓄能型发光材料板(权利要求18)实现,同样可以在闪烁体板(权利要求19)实现。The solution according to the invention can advantageously be realized in panels of energy-storage luminescent materials (claim 18 ), as well as in scintillator panels (claim 19 ).

附加层可以例如通过PVD-法(物理气相沉积)或通过CVD-法(化学气相沉积)涂覆。此外,溶胶凝胶法和旋涂法(Spin-On-Verfahren)(离心涂料(Lack))适于制备中间层。Additional layers can be applied, for example, by PVD methods (Physical Vapor Deposition) or by CVD methods (Chemical Vapor Deposition). Furthermore, the sol-gel method and the spin-on-coating method (spin-on-coating) are suitable for producing the intermediate layer.

附加层的结构化可以例如通过具有后续分解

Figure BDA0000158629350000051
的光刻法而生成。根据附加层的组成,借助激光或腐蚀的结构化为其他的结构化方法。Additional layers of structuring can be achieved, for example, by having a subsequent decomposition
Figure BDA0000158629350000051
produced by photolithography. Depending on the composition of the additional layer, structuring by means of laser or etching are other structuring methods.

附图说明 Description of drawings

下面参考附图更详细地解释本发明的示意性实施方式,但是对本发明没有限制作用。在附图中:Schematic embodiments of the invention are explained in more detail below with reference to the drawings, without however restricting the invention. In the attached picture:

图1显示了在不同闪烁体的情况下X射线依赖于辐射质量的吸收度,Figure 1 shows the radiation mass-dependent absorption of X-rays in the case of different scintillators,

图2显示了已知CsI:Tl-层在光栅电子显微镜下放大50倍的照片,用于显示裂纹间距,Figure 2 shows a 50X magnification of the known CsI:Tl-layer under a grating electron microscope to show the crack spacing,

图3显示了CsI:Tl-层光晕的显微照片,Figure 3 shows a photomicrograph of a CsI:Tl-layer halo,

图4显示了已知的具有四方形结构化的CsI:Tl-层在光栅电子显微镜下放大50倍的照片,Figure 4 shows a known CsI:Tl-layer with a tetragonal structure under a grating electron microscope at 50X magnification,

图5显示了已知的具有六角形结构化的CsI:Tl-层在光栅电子显微镜下放大50倍的照片,Figure 5 shows a 50x magnification photograph of a known hexagonal structured CsI:Tl-layer under a grating electron microscope,

图6显示了根据本发明结构化的第一实施方案的部分俯视图,Figure 6 shows a partial top view of a first embodiment structured according to the invention,

图7显示了根据本发明结构化的第二实施方案的部分俯视图。Figure 7 shows a partial top view of a second embodiment structured according to the invention.

具体实施方式Detailed ways

在CsI:Tl-闪烁体的情况中,由于已经解释的吸收度(图1)的原因,层厚必须显著地增加。这种增加导致了叠加的不规则的裂纹结构(图2)以及明显的光晕(图3)。尽管DE10242006A1中建议的n-角结构化的附加层在n=4和n=6时已经抑制了不期望的宽裂纹,但是裂纹在择优取向上还是清楚可见的(图4和5)。In the case of CsI:Tl scintillators, the layer thickness has to be significantly increased due to the already explained absorbance ( FIG. 1 ). This increase resulted in a superimposed irregular crack structure (Fig. 2) and a pronounced halo (Fig. 3). Although the n-corner structured additional layer proposed in DE 10242006 A1 already suppresses the undesirably wide cracks at n=4 and n=6, the cracks are still clearly visible at the preferred orientation ( FIGS. 4 and 5 ).

图6显示了本发明发光材料板的基底1的第一实施方案的俯视图。该发光材料板包括基底1,在该基底1上涂覆有附加层2。该附加层2以如下方式格栅化,通过沟槽3至7形成分离的突起8,在其表面上在另一工艺步骤中蒸镀形成发光材料层的发光材料的发光材料针状物。该附加层2使得可以借助常见的结构化方法以简单的方式实现本发明提供的结构化。FIG. 6 shows a plan view of a first embodiment of a substrate 1 of an inventive phosphor plate. The phosphor plate comprises a substrate 1 on which an additional layer 2 is applied. The additional layer 2 is gridded in such a way that the trenches 3 to 7 form separate protrusions 8 , on the surface of which the phosphor needles of the phosphor forming the phosphor layer are evaporated in a further process step. This additional layer 2 makes it possible to implement the structuring provided by the invention in a simple manner by means of conventional structuring methods.

在所述的实施方案中,突起8各具有八角形基面。In the embodiment described, the protrusions 8 each have an octagonal base.

根据本发明,通过沟槽3至7分离的突起8形成了第一突起,并限定了第一结构。第二突起9,在所示实施方案中例如各具有四角形基面,形成了第二结构。According to the invention, the protrusions 8 separated by the grooves 3 to 7 form a first protrusion and define a first structure. The second protrusions 9 , each having, for example, a quadrangular base in the embodiment shown, form the second structure.

根据本发明,由第一突起8形成的第一结构和由突起9形成的第二结构以几何上不同的方式形成。此外,第二结构设置在第一结构之间。由此第一突起8和第二突起9分别具有短于第一突起8彼此之间和第二突起9彼此之间的间距。为此,所述第二突起9设置在沟槽3至7中。由此,由突起8形成的沟槽3至7被第二突起9“干扰”。According to the invention, the first structure formed by the first protrusion 8 and the second structure formed by the protrusion 9 are formed in a geometrically different manner. Furthermore, a second structure is disposed between the first structures. As a result, the first protrusions 8 and the second protrusions 9 each have a shorter distance than the distances between the first protrusions 8 and the second protrusions 9 . To this end, the second protrusions 9 are arranged in the grooves 3 to 7 . As a result, the grooves 3 to 7 formed by the protrusion 8 are “interrupted” by the second protrusion 9 .

图7显示了本发明发光材料板的基底1的第二实施方案的俯视图。该基底1的结构与图6中所示基底1的结构基本一致。仅仅是第二突起9相对于根据图6的基底1而言旋转了45°的角。由此,突起9的角靠近突起8。FIG. 7 shows a plan view of a second embodiment of a substrate 1 of an inventive phosphor plate. The structure of the substrate 1 is basically the same as that of the substrate 1 shown in FIG. 6 . Only the second protrusion 9 is rotated by an angle of 45° relative to the base 1 according to FIG. 6 . As a result, the corners of the protrusions 9 approach the protrusions 8 .

在图6和7以具有八角形基面的突起8和具有四角形基面的突起9(规则设置的两个多角形)为例描述了本发明。在本发明的范围中,针对所述第一结构和所述第二结构,还可以通过以其他方式成型的第一突起8和/或以其他方式成型的第二突起9实现其他的结构。在此,所述第一突起8和所述第二突起9可以具有任意结构,并且可以规则或不规则设置。此外,第一突起8和/或第二突起9还可以设置为一个结构,其在附加层2的整个表面上变化。The invention is described in FIGS. 6 and 7 using the example of a protrusion 8 with an octagonal base and a protrusion 9 with a quadrangular base (two polygons arranged regularly). Within the scope of the invention, further configurations can also be realized for the first configuration and the second configuration by means of a differently shaped first protrusion 8 and/or a differently shaped second protrusion 9 . Here, the first protrusions 8 and the second protrusions 9 may have any structure, and may be arranged regularly or irregularly. Furthermore, the first protrusions 8 and/or the second protrusions 9 can also be provided as a structure which varies over the entire surface of the additional layer 2 .

通过这两个实施方案说明的本发明方案可靠地防止了附加层2中的不期望的叠加裂纹结构,并且因此可靠地防止了破坏成像性质,取而代之的是确保有利的裂纹形成和发光材料针状物。因此,本发明的发光材料板即使在发光材料层的层厚大时也具有好的成像质量。The inventive solution illustrated by these two embodiments reliably prevents an undesired superimposed crack structure in the additional layer 2 and thus reliably prevents damage to the imaging properties and instead ensures favorable crack formation and acicular shape of the luminescent material thing. The phosphor plate according to the invention therefore has a good imaging quality even with a large layer thickness of the phosphor layer.

从而通过本发明的措施在附加层2的情况中注意到了“线自由度(Linienfreiheit)”。这表明例如在规则设置的多角形结构(由第一突起8形成)之间的“干扰元素”(由第二突起9形成)阻碍了线性裂纹扩展的“途径”,并由此迫使裂纹改变方向。因此可靠地防止了在附加层2中形成叠加裂纹结构。The measures according to the invention thus take into account the "linear degrees of freedom" in the case of the additional layer 2 . This suggests that for example "interfering elements" (formed by second protrusions 9) between regularly arranged polygonal structures (formed by first protrusions 8) block the "path" of linear crack propagation and thereby force the crack to change direction . The formation of superimposed crack structures in the additional layer 2 is thus reliably prevented.

涂覆在基底1上的附加层2中可以任意设置不同形式的多角形或不规则的结构。在本发明的范围中,术语“多角形”包括任意成型的具有边长a的n-角,其中n≥3。当n→∞(即a→0)时,可以得到近圆形。在由第一突起8形成第一结构的情况下以及在由第二突起9形成第二结构的情况下,本发明还包括其他几何形状,如椭圆形或星形结构。Various forms of polygonal or irregular structures can be arranged arbitrarily in the additional layer 2 coated on the substrate 1 . Within the scope of the present invention, the term “polygon” includes arbitrarily shaped n-angles with side length a, where n≧3. When n→∞ (that is, a→0), a nearly circular shape can be obtained. In the case of the first structure formed by the first protrusions 8 and in the case of the second structure formed by the second protrusions 9, the invention also includes other geometries, such as elliptical or star-shaped structures.

可以此方式结构化的发光材料不仅局限于闪烁体(例如,CsI:Tl,CsF,CsI:Na,NaI:Tl),还扩展到蓄能型发光材料(例如CsBr:Eu)。The luminescent materials that can be structured in this way are not limited to scintillators (eg CsI:Tl, CsF, CsI:Na, NaI:Tl), but also extend to energy-storage luminescent materials (eg CsBr:Eu).

通过在基底1上选择合适的结构化附加层2,闪烁体层或蓄能型发光材料层可以在合适的参数(压力、基底温度)下蒸镀后进行冷却时以所需的方式不仅在第一突起8和/或第二突起9的粗结构化设置时而且在第一突起8和/或第二突起9的细结构化设置时实现。By selecting a suitable structured additional layer 2 on the substrate 1, the scintillator layer or the energy-storage luminescent material layer can be evaporated under suitable parameters (pressure, substrate temperature) and cooled in the desired manner not only at the The coarser structuring of the first protrusions 8 and/or the second protrusions 9 takes place as well as the finer structuring of the first protrusions 8 and/or the second protrusions 9 .

Claims (19)

1. luminescent material plate; It has substrate (1) and position extra play (2) on it; On said extra play (2), be coated with luminous material layer, wherein said extra play (2) gridding as follows generates the projection (8) of separating through groove (3-7); The luminescent material spicule that forms the luminescent material of luminous material layer is created on the surface of projection (8); Wherein first projection (8) forms first structure, and second projection (9) forms second structure that is different from first structure on how much, and said second structure is arranged between first structure.
2. according to the luminescent material plate of claim 1, it is characterized in that said first structure that is formed by first projection (8) constitutes cell structure.
3. according to the luminescent material plate of claim 1 or 2, it is characterized in that said second structure that is formed by second projection (9) constitutes cell structure.
4. according to the luminescent material plate of claim 1, it is characterized in that, in projection (8,9) but go up to form the luminescent material spicule of the separation of predetermined quantity.
5. according to the luminescent material plate of claim 1, it is characterized in that thick about 10 μ m to the 50 μ m of said extra play (2).
6. according to the luminescent material plate of claim 1 or 2, it is characterized in that the grid size of said structure is in the scope of 10 μ m to 100 μ m, preferably between 20 μ m to 50 μ m.
7. according to the luminescent material plate of claim 1, it is characterized in that the width of said groove (3-7) is in the scope of 10 μ m to 50 μ m.
8. according to the luminescent material plate of claim 1, it is characterized in that said first structure and second structure are of different sizes.
9. according to the luminescent material plate of claim 1, it is characterized in that said first structure has different shapes with second structure.
10. according to the luminescent material plate of claim 1, it is characterized in that said first structure part at least has regular shape, and said second structure at least partly has the shape of rule.
11. the luminescent material plate according to claim 1 is characterized in that, said first structure part at least has irregular shape, and said second structure at least partly has irregular shape.
12. the luminescent material plate according to claim 1 is characterized in that, said first structure part at least has regular shape, and said second structure at least partly has irregular shape.
13. the luminescent material plate according to claim 1 is characterized in that, said first structure part at least has irregular shape, and said second structure at least partly has the shape of rule.
14. the luminescent material plate according to claim 1 is characterized in that, said first structure that is formed by first projection (8) has the structure at n-angle.
15. the luminescent material plate according to claim 1 is characterized in that, said second structure that is formed by second projection (9) has the structure at n-angle.
16. the luminescent material plate according to claim 1 is characterized in that, said first projection (8) has the n-angular shape.
17. the luminescent material plate according to claim 1 is characterized in that, said second projection (9) has the n-angular shape.
18. the luminescent material plate according to claim 1 is characterized in that said luminous material layer is made up of the accumulating type luminescent material.
19. the luminescent material plate according to claim 1 is characterized in that said luminous material layer is made up of scintillator.
CN2012101304518A 2011-04-29 2012-04-28 Phosphor sheet Pending CN102760506A (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
DE102011017789.2 2011-04-29
DE201110017789 DE102011017789B3 (en) 2011-04-29 2011-04-29 Phosphor sheet comprises a substrate and an overlying additional layer, on which a phosphor layer is applied, where the additional layer is girdded such that it forms first and second nubs separated by grooves

Publications (1)

Publication Number Publication Date
CN102760506A true CN102760506A (en) 2012-10-31

Family

ID=45832821

Family Applications (1)

Application Number Title Priority Date Filing Date
CN2012101304518A Pending CN102760506A (en) 2011-04-29 2012-04-28 Phosphor sheet

Country Status (2)

Country Link
CN (1) CN102760506A (en)
DE (1) DE102011017789B3 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104217778A (en) * 2013-05-30 2014-12-17 柯尼卡美能达株式会社 Radiographic image conversion panel and radiographic image detector
CN106459743A (en) * 2014-06-23 2017-02-22 圣戈班晶体及检测公司 Luminescent material with a textured photonic layer

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5171996A (en) * 1991-07-31 1992-12-15 Regents Of The University Of California Particle detector spatial resolution
EP0573879A2 (en) * 1992-06-12 1993-12-15 Siemens Aktiengesellschaft Manufacturing process of a structured phosphor layer
DE4219347A1 (en) * 1992-06-12 1993-12-16 Siemens Ag Alkali metal halide phosphor layer prodn. - by inclined vapour deposition to obtain layer island regions
CN1422441A (en) * 2000-04-04 2003-06-04 浜松光子学株式会社 Semiconductor energy detector
JP2011137665A (en) * 2009-12-26 2011-07-14 Canon Inc Scintillator panel, radiation imaging apparatus, method of manufacturing scintillator panel and radiation imaging apparatus, and radiation imaging system
CN201966252U (en) * 2011-02-23 2011-09-07 华映视讯(吴江)有限公司 Organic light-emitting diode packaging structure

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5171996A (en) * 1991-07-31 1992-12-15 Regents Of The University Of California Particle detector spatial resolution
EP0573879A2 (en) * 1992-06-12 1993-12-15 Siemens Aktiengesellschaft Manufacturing process of a structured phosphor layer
DE4219347A1 (en) * 1992-06-12 1993-12-16 Siemens Ag Alkali metal halide phosphor layer prodn. - by inclined vapour deposition to obtain layer island regions
CN1422441A (en) * 2000-04-04 2003-06-04 浜松光子学株式会社 Semiconductor energy detector
JP2011137665A (en) * 2009-12-26 2011-07-14 Canon Inc Scintillator panel, radiation imaging apparatus, method of manufacturing scintillator panel and radiation imaging apparatus, and radiation imaging system
CN201966252U (en) * 2011-02-23 2011-09-07 华映视讯(吴江)有限公司 Organic light-emitting diode packaging structure

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104217778A (en) * 2013-05-30 2014-12-17 柯尼卡美能达株式会社 Radiographic image conversion panel and radiographic image detector
CN106459743A (en) * 2014-06-23 2017-02-22 圣戈班晶体及检测公司 Luminescent material with a textured photonic layer

Also Published As

Publication number Publication date
DE102011017789B3 (en) 2012-04-05

Similar Documents

Publication Publication Date Title
US9110176B2 (en) Radiation detecting element
US8669527B2 (en) Scintillator having phase separation structure and radiation detector using the same
JP6066608B2 (en) Scintillator having phase separation structure and radiation detector using the same
US6784432B2 (en) X-ray detector module
US9315919B2 (en) Scintillator plate and radiation detector
JP2011021924A (en) Scintillator panel, radiation detection device, and method of manufacturing scintillator panel
JP2011007552A (en) Scintillator panel, radiation detection device, and method of manufacturing the scintillator panel
US10281591B2 (en) Ceramic scintillator array, X-ray detector, and X-ray inspection device
JP2006153874A (en) Scintillator layer for X-ray detector and manufacturing method thereof
CN1790054A (en) Radiation detector, in particular for x- or gamma radiation, and method for producing it
CN102760506A (en) Phosphor sheet
EP2775319B1 (en) Scintillator having a phase separation structure and radiation detector using the same
JP6771981B2 (en) Scintillator plate and radiation detector using it
JP2011232197A (en) Scintillator panel and radiation image detection device
WO2014128957A1 (en) Scintillator and radiation detector
JP6356352B2 (en) Pixelated scintillator with optimized efficiency
JP6985882B2 (en) Scintillator material and radiation detector
WO2021145260A1 (en) Scintillator and method for producing scintillator
JP2004117347A (en) Phosphor sheet
US8624194B2 (en) Radiation detecting device and method of manufacturing the same
US11644605B2 (en) Polarizing element having alternately laminated dielectric layers and conductive layers and method for manufacturing polarizing element
KR20120122950A (en) Florescent plate
US11947055B2 (en) Multilayer reflector for high efficiency and high spatial resolution pixelated x-ray scintillators and fabrication method
JP2004233343A (en) Radiological image conversion panel
JP7661243B2 (en) Scintillator and method for producing the same

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C02 Deemed withdrawal of patent application after publication (patent law 2001)
WD01 Invention patent application deemed withdrawn after publication

Application publication date: 20121031