通过光源的离心作用通过速度诱导的光束偏转打破对称性
Breaking symmetry through speed-induced beam-deflection via centrifugation of the light source
摘要:
提出的实验旨在证明和测量由源速度引起的光线在发射时的偏转,并将其与由观察者速度引起的光线的像差区分开。该方法主张在光源的速度和观察者的速度之间产生速度不对称,并且依赖于光源以1000米的速度离心。当源和观测器具有相同的速度时,例如当源和观测器都在同一惯性系统上时,偏转和像差补偿并且它们的净效应为零。因此,为了限制惯性系统的几率并隔离这些速度引起的效应,人们转而求助于离心系统,因为它允许破坏源速度和观测者速度之间的对称性。三种情况被认为是。(a)源固定在转子臂的一端,而探测器固定在转子轴上。实验的这种配置旨在揭示,由于源的圆周速度,光束向前偏转,因此它撞击在中心检测器上,当系统不旋转时,它的位置略有偏移。(b)源和检测器的位置互换,因此源的圆周速度为零,因此没有速度引起的偏转,但是由于观察者的圆周速度,存在速度引起的像差,因为在射束飞行时间期间,检测器稍微侧向移动。然而,这一次斑点在相反方向上移动,因此离心的效果不是相互的。(c)源和探测器固定在转子臂的两端。在这种情况下,光束偏转和像差增加,因为它们的速度矢量具有相反的方向,并且由于飞行时间是两倍,所以检测器上的光斑的每次移位是两倍。
英文摘要:
The experiment proposed aims to evidence and to measure the deflection of light rays induced by the source speed upon emission, and to discern it from the aberration of light rays induced by the observer speed. The method stands in creating a speed asymmetry between that of the source and that of the observer, and relies on the centrifugation of a light source at ultrahigh speed. When source and observer have the same speed, such as when being both on the same inertial system, the deflection and the aberration compensate and their net effect is null. So, in order to circumscribe the odds of inertial systems and to isolate these speed-induced effects it has instead been appealed to a centrifugal system, since it allows infringing symmetry between the source and the observer speeds. Three cases are considered. (a) Centrifugation of the source fixed at one end of the rotor arm, while the detector is fixed on the rotor axis. This configuration of the experiment aims to unveil that due to the peripheral speed of the source the beam is deflected forward, so it impinges on the centric detector slightly shifted from its position when the system was not rotating. (b) The positions of the source and the detector are interchanged, so the source peripheral speed is then null and thus no speed-induced deflection ensues, but due to the observer peripheral speed there is a speed-induced aberration since during the beam time-of-flight the detector has slightly moved side-way. However, this time the spot shifts in opposite direction and hence the effect of centrifugation is not reciprocal. (c) The source and the detector are fixed at the two ends of the rotor arms. In this case the beam deflection and aberration add, since their speed vectors have opposite directions and each shift of the spot on the detector is double since the time-of-flight is double.
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