微波旋转扭矩纳米振荡器的相互相锁
Shehzaad Kaka1, Matthew R Pufall, William H Rippard
1Electromagnetic Technology Division, National Institute of Standards and Technology, Boulder, Colorado 80305, USA. shehzu21@gmail.com
Nature
|September 16, 2005
概括
两个旋转扭矩纳米振荡器 (STNOs) 可以同步,提高微波信号功率. 在STNO阵列中这种相锁定可以使新的纳米传递器和接收器用于无线通信.
科学领域:
- 这就是Spintronics.
- 非线性动力学是一种非线性动力学.
- 微波工程 微波工程 微波工程
背景情况:
- 在磁性多层中,旋转扭矩效应会从直流电流中产生微波信号.
- 磁电子设备通常用于传感和记忆.
- 单旋转扭矩纳米振荡器 (STNOs) 发射的微波功率低 (<1 nW).
研究的目的:
- 调查STNO阵列对增加微波输出功率的潜力.
- 为了证明附近的STNO之间相互相锁定和同步.
- 探索相锁STNO阵列在无线通信中的应用.
主要方法:
- 实验设置两个紧密放置的STNO.
- 在直流电流下观察信号特征.
- 在同步状态下对线宽缩小和功率增加的分析.
主要成果:
- 在两个相邻的STNO之间证明了相互相锁定 (同步).
- 观察到一个明显的相锁状态,其特点是线宽缩小和功率增加.
- 确认同步是相互作用的非线性振荡器系统的自然趋势.
结论:
- 阶段锁定STNO的阵列可以达到更高的微波功率水平.
- 阶段锁定STNO阵列显示出作为纳米尺度参考振荡器的潜力.
- 阶段性STNO阵列可以实现纳米尺度的定向发射器和接收器.
相关概念视频
Atomic Nuclei: Larmor Precession Frequency
3.8K
The earth's gravitational field produces a 'twisting force' perpendicular to the angular momentum of a spinning mass (such as a spinning top) that causes the mass to 'wobble' around the gravitational field axis in a phenomenon called precession. Similarly, the magnetic moment (μ) of a spinning nucleus precesses due to an external magnetic field directed along the z-axis. The precession of the magnetic moment vector about the magnetic field is called Larmor precession,...
3.8K
Atomic Nuclei: Nuclear Relaxation Processes
1.4K
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
1.4K
NMR Spectroscopy: Spin–Spin Coupling
3.9K
The spin state of an NMR-active nucleus can have a slight effect on its immediate electronic environment. This effect propagates through the intervening bonds and affects the electronic environments of NMR-active nuclei up to three bonds away; occasionally, even farther. This phenomenon is called spin–spin coupling or J-coupling. Coupling interactions are mutual and result in small changes in the absorption frequencies of both nuclei involved. While nuclei of the same element are involved...
3.9K
Spin–Spin Coupling Constant: Overview
1.7K
In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
1.7K
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)
2.0K
Two NMR-active nuclei bonded to a central atom can be involved in geminal or two-bond coupling. Geminal coupling is commonly seen between diastereotopic protons in chiral molecules and unsymmetrical alkenes, among others.
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
2.0K
Time and frequency -Domain Interpretation of Phase-lag Control
452
Phase-lag controllers are widely used in control systems to improve stability and reduce steady-state errors. A dimmer switch controlling the brightness of a light bulb serves as a practical example of phase-lag control, gradually adjusting the bulb's brightness. Mathematically, phase-lag control or low-pass filtering is represented when the factor 'a' is less than 1.
Phase-lag controllers do not place a pole at zero, but instead influence the steady-state error by amplifying any...
Phase-lag controllers do not place a pole at zero, but instead influence the steady-state error by amplifying any...
452


