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首页> 外文期刊>International Journal of Quantum Chemistry >Single-Photon and Multiphoton Processes Causing Resonance in the Transmission of Electrons by a Single Potential Barrier in a Radiation Field
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Single-Photon and Multiphoton Processes Causing Resonance in the Transmission of Electrons by a Single Potential Barrier in a Radiation Field

机译:单光子和多光子过程通过辐射场中的单个势垒在电子传输中引起共振。

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Simulations of electrons tunneling in a barrier for which the height varies sinusoidally with time show resonances increasing the transmitted current. For square barriers, these resonances occur when electrons are promoted above the barrier by absorbing quanta from the barrier oscillations, and the barrier length is an integer multiple of one-half of the de Broglie wavelength. For several barriers having other profiles, we find that there is a single broad resonance centered at a wave length equal to 0.9 times the wavelength for a photon having the energy to take the particle exactly to the top of the barrier. We attribute this difference to the fact that quanta may only be exchanged at the ends of a square barrier, whereas quanta are exchanged throughout the full length of barriers having other profiles-especially in regions of high electric field intensity. A Floquet expansion is used to examine the change in transmission caused by barrier modulation for electrons at the different energies caused by the exchange of quanta. We find that the wavelengths of resonance are proportional to the number of quanta absorbed by the particles, and attribute this observation to the requirement that specific values of absorbed energy are necessary for resonance. The increase in transmission caused by absorbing M quanta is proportional to the Mth power of the power flux density of the radiation causing barrier modulation. Thus, as the power is increased, the total transmission (including all energies) shows greater structure due to multiphoton processes.
机译:在势垒高度随时间呈正弦变化的势垒中电子隧穿的模拟表明,共振会增加传输电流。对于方形势垒,当通过吸收势垒振荡中的量子将电子提升到势垒上方时,就会发生这些共振,势垒长度是德布罗意波长的二分之一的整数倍。对于具有其他轮廓的几个势垒,我们发现存在一个单一的宽共振,其中心波长等于光子波长的0.9倍,该光子具有将粒子恰好带到势垒顶部的能量。我们将这种差异归因于以下事实:量子只能在方形势垒的末端交换,而量子在具有其他轮廓的势垒的整个长度上交换,尤其是在高电场强度的区域中。 Floquet展开用于检查由量子交换引起的不同能量下的电子的势垒调制所引起的传输变化。我们发现共振的波长与粒子吸收的量子数量成正比,并将这种观察归因于共振所必需的特定吸收能量值。吸收M量子引起的传输增加与引起势垒调制的辐射功率通量密度的Mth功率成正比。因此,随着功率的增加,由于多光子过程,总传输(包括所有能量)显示出更大的结构。

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