当激光作为信息发射器时,充当电容器或电感的电子芯片

Mashair Ahmed Mohammed Yousef, A. Alsubaie, Z. Saad, M. D. Abd-Alla
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引用次数: 0

摘要

为了提高电子设备中信息流动的速度和存储容量,可以用激光代替电流来传输信息。由于光子比电子快,人们期望当光子取代电子时,信息通过互联网传输的速度会非常快。这需要寻找充当电容器、电感或电阻的芯片。为了做到这一点,我们使用了麦克斯韦电场强度方程和电子运动方程。假设电子在有局部电场和磁场存在的摩擦介质中自然振动。这些方程已被用来求出吸收系数的有用表达式。发现吸收系数除了依赖于内部电场和磁场外,还依赖于摩擦系数的激光和固有频率。这些参数可以微调,使芯片作为一个电容器,电感或电阻。激光强度随吸收系数的增大而减小。因此,吸收系数起着电阻的作用。因此,如果吸收系数随频率降低而增加,则芯片充当电容器。但随着激光频率的增加,吸收系数增大,芯片就会起到电感的作用。在吸收系数随着载流子浓度的增加而增加的情况下,它在这种情况下充当电阻器。对于磁通密度可以抵消摩擦力的磁性材料,当激光频率接近原子的固有频率时,材料就会起到电感的作用。但当内外部电场相同时摩擦力较低时,这种材料就起到了电容器的作用。然而,当没有电偶极子存在,当内部磁场力与摩擦力平衡时,它作为一个电阻的固有频率可以忽略不计。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Electronic Chips Acting as Capacitors or Inductors when Laser Act as Information Transmitter
To increase the speed of information flow and storage capacity in electronic devices laser can be used to carry information instead of electric current. Since the photon is faster than electrons, one expects information to be transmitted very fast through the internet when photons replace electrons. This requires searching for chips that act as capacitors, inductors or resistors. To do this Maxwell's equation for the electric field intensity beside the electron equation of motion were used. The electron is assumed to vibrate naturally inside a frictional medium in the presence of a local electric and magnetic fields. These equations have been used to find a useful expression for the absorption coefficient. The absorption coefficient was found to be dependent on the laser and natural frequencies beside the coefficient of friction in addition to the internal electric and magnetic fields. These parameters can be fine-tuned to make the chip act as a capacitor, inductor or resistor. The laser intensity decreases when the absorption coefficient inecreases. Thus, the absorption coefficient acts as an electic resistor. Therefore, if the absorption coefficient inecreases upon decreasing the frequency the chip acts as a capacitor. But when the absorption coefficient inecreases when the laser frequency inreases the chip acts as an inductor. In the case that the absorption coefficient inecreases with the concentration of the carriers it acts in this situation as a resistor. For magnetic materials with magnetic flux density that cancels the frictional force, when the laser frequency is equal nearly to the atom’s natural frequency the material acts as an inductor. But when the frictional force is low with the internal and external electric fields in phase, the material acts as a capacitor. However, it acts as a resistor for negligible natural frequency, when no electric dipoles exist and when the internal magnetic field force balance the frictional force.
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