U.S. Philips Corporation

Johnny W Van Der Velden

Johannes K Colditz

August L Simons

Tiemen Poorter

Martinus A Ligtenberg

Franciscus M Dreesen

Theodorus F Van Bergen

Henricus F Diebels

In an X-ray image intensifier tube an entrance section is optimized in respect of image quality, optical aberrations and efficiency. To achieve this, notably in order to avoid photocathode charging phenomena, a separating layer having an adapted electrical transverse conduction is provided. In order to reduce scattered radiation, an edge portion of the entrance screen is deactivated for relevant examinations. In order to increase efficiency, use is made of a double phosphor layer having different X-ray absorption properties. In order to compensate for vignetting a radial variation of the thickness or of the radiation properties of a separating layer or of the luminescent layer itself is used.

X-ray image intensifier tube with improved entrance section

The entrance screen in an X-ray image intensifier includes an intermediate layer of a material which selectively absorbs photon energy. As a result, the speed of the photo-electrons is substantially reduced, thus improving the imaging. By introducing a radial variation of the absorption in the intermediate layer, vignetting-compensation can also be realized without substantial loss of sensitivity and resolution for the central portion of the tube. The resolution at the periphery of the tube can thus be substantially improved.

X-ray image intensifier tube comprising a selective filter

An x-ray image intensifier including an input screen 3 having a radiation transparent support 7 on which is applied a fluorescence layer 8 of CsI, a translucent conductive barrier layer 9 which replenishes the photocathode 10 with electrons but tends to reflect incident light especially when made of metal, e.g. of aluminum 7 nm thick which reflects about 50% of the incident fluorescence. The improvement adds first and second intermediate layers 21, 22 of metal oxide e.g. respectively TiO.sub.2, MnO, which are semiconductive. The thickness of the first layer 21 adjusts the reflection amplitude to equal that at the photocathode-vacuum interface, and that of the second layer adjusts the relative phase so that the reflections cancel. The first and second layers can be non-conductors such as Al.sub.2 O.sub.3, however the second layer is then made thin enough, e.g. 25 nm or less, to allow electron conduction by tunnelling to occur.

Radiographic image intensifier

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Heerlen, Netherlands

Johnny W Van Der Velden