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    • 1. 发明公开
    • X-ray imaging system
    • Röntgenbildsystem。
    • EP0526921A1
    • 1993-02-10
    • EP92201685.2
    • 1992-06-10
    • Philips Electronics N.V.
    • Jonkman, Rudi
    • H05G1/64H01J31/50
    • H05G1/64H01J31/501H01J2231/50036
    • The invention relates to an X-ray imaging system, comprising an X-ray image intensifier tube in which the electron-optical system can be adjusted to a number of different image formats. By making the image format increase or decrease visibly on the exit screen in the event of a change of image format, annoying visual adjustment effects are avoided and a patient can be continuously observed also in the event of a change of format. Because of the gradual high-voltage variation of the power supply for the electron-optical system, associated with a visible variation of the image format, the output resistance of the power supply circuit may be high. Furthermore, due to the gradual change of the mean intensity on the exit screen of the X-ray image intensifier tube, the control behaviour of the automatic exposure control and the automatic gain control of the X-ray imaging system are influenced in a positive sense.
    • 本发明涉及一种X射线成像系统,其包括X射线图像增强管,其中电子 - 光学系统可被调整到多种不同的图像格式。 在图像格式发生变化的情况下,通过在出口屏幕上使图像格式明显增加或减少,避免了烦琐的视觉调整效果,并且在格式变化的情况下也可以连续观察患者。 由于与图像格式的可见变化相关联的电子 - 光学系统的电源的逐渐高压变化,电源电路的输出电阻可能很高。 此外,由于X射线图像增强管的出射屏幕上的平均强度的逐渐变化,自动曝光控制的控制行为和X射线成像系统的自动增益控制受到正面影响 。
    • 3. 发明公开
    • Magnetic resonance method for obtaining selected spectra
    • Verfahren手套磁铁Resonanz zur ErzielungausgewählterSpektren。
    • EP0385548A1
    • 1990-09-05
    • EP90200444.9
    • 1990-02-26
    • Philips Electronics N.V.
    • Van Vaals, Johannes Jacobus
    • G01R33/48G01R33/56
    • G01R33/4833
    • The method includes a critical time shift of a refocusing pulse between two (90 o ) excitation pulses which produce multiple quantum coherence signals and which are followed by a (90 o ) read pulse (using a critical timing a refocusing pulse serving the same purpose can also be applied between the second excitation pulse and the read pulse). With respect to the centre of the time path between the excitation pulses or between the excitation pulse and the read pulse the time shift is chosen to be such that given resonances do not occur positively or negatively in the spectrum whereas other resonances do occur therein (i.e. at substantially maximum strength). The MRI method can be combined with the use of spatially selective gradients in order to obtain localised spectra or images.
    • 该方法包括在产生多个量子相干信号的两个(90)激励脉冲之间的重聚焦脉冲的临界时间偏移,并且之后是(90)读取脉冲(使用临界定时,重聚焦脉冲服务 也可以在第二激励脉冲和读取脉冲之间施加相同的目的)。 关于激发脉冲之间或激励脉冲与读取脉冲之间的时间路径的中心,时移被选择为使得给定的谐振在频谱中不会正面或负面地发生,而在其中发生其它谐振(即 基本上最大强度)。 MRI方法可以与使用空间选择性梯度组合,以获得局部化的光谱或图像。
    • 9. 发明公开
    • Method of and device for automatic phase correction of complex NMR spectra
    • Verfahren und Anordnung zur automatischen Phasenkorrektur komplexer Kernspinresonanz-Spektren。
    • EP0316991A1
    • 1989-05-24
    • EP88202485.4
    • 1988-11-08
    • Philips Electronics N.V.
    • van Vaals, Johannes Jacobus
    • G01N24/08
    • G01R33/4625
    • A method is proposed for the automatic correction of phase errors in NMR spectra. The phase errors are inter alia due to deficiencies of the NMR hardware, the time-shifted sampling of a magnetic resonance signal after the appearance thereof. The phase correction is performed by first determining peak locations in a modulus spectrum determined from the complex spectrum and by determining the phases in the peak locations, after which the phases in the peak locations are fitted to a predetermined polynomial by means of a least-­squares optimization procedure. The coefficients of the polynomial are thus defined. Subsequently, the NMR spectrum is point-wise corrected by means of the phase polynomial determined. The proposed method can be simply implemented in a NMR device; no severe requirements are imposed as regards the signal-to-noise ratio and the resolution of the spectrum. In practical situations an NMR spectrum usually comprises many spectral lines. Therefore, the method is not susceptible to the effects of overlapping spectral lines.
    • 提出了NMR光谱相位误差自动校正的方法。 相位误差尤其是由于NMR硬件的缺陷,出现之后的磁共振信号的时移采样。 通过首先确定从复谱确定的模式谱中的峰值位置并通过确定峰值位置中的相位来执行相位校正,之后通过最小二乘法将峰值位置中的相位拟合到预定的多项式 优化程序。 因此定义多项式的系数。 随后,NMR谱通过确定的相位多项式逐点校正。 所提出的方法可以简单地在NMR装置中实现; 在信噪比和频谱分辨率方面没有严格的要求。 在实际情况下,NMR谱通常包含许多谱线。 因此,该方法不易受到重叠谱线的影响。
    • 10. 发明公开
    • Method of and device for automatic phase correction of complex NMR spectra
    • Verfahren und Anordnung zur automatischen Phasenkorrektur komplexer Kernresonanzspektren。
    • EP0316041A1
    • 1989-05-17
    • EP88202486.2
    • 1988-11-08
    • Philips Electronics N.V.
    • van Vaals, Johannes Jacobus
    • G01R33/54G01R33/56
    • G01R33/4625
    • A method is proposed for the automatic correction of phase errors in NMR spectra. The phase errors are caused inter alia by deficiencies of the NMR hardware, by the shifted sampling of a magnetic resonance signal after the occurrence thereof. Phase correction is performed by determining first the modulus spectrum from a complex magnetic resonance spectrum, after which in the modulus spectrum there are determined, with discrimination of peaks which are below a given level, the peak parameters of the remaining peaks, such as peak amplitude, peak width at half amplitude and peak position, after which, using the peak parameters determined, a model of the complex spectrum is determined which does not contain phase errors, a phase distortion being subsequently introduced into this model until the phase of the model at the edges of the spectrum corresponds as well as possible to the phase at the edges of the complex spectrum, after which finally the complex spectrum is point-wise corrected with the phase distortion introduced. The proposed phase correction does not impose strict requirements as regards the modeling, because upto a given level variations in the modeling hardly influence the phase variation at the edge of the spectrum.
    • 提出了NMR光谱相位误差自动校正的方法。 通过磁共振信号发生后的移位采样,相位误差尤其由NMR硬件的缺陷引起。 通过首先从复磁共振谱中确定模数谱进行相位校正,之后在确定低于给定水平的峰的模数谱中确定剩余峰的峰值参数,例如峰值振幅 峰值宽度在半幅度和峰值位置之间,之后,使用确定的峰值参数,确定不包含相位误差的复谱的模型,随后将相位失真引入该模型,直到模型的相位 频谱的边缘对应于复谱边缘处的相位,之后最终通过引入的相位失真对复谱进行逐点校正。 所提出的相位校正并没有对建模施加严格的要求,因为建模中给定的水平变化几乎不影响光谱边缘的相位变化。