在共振传感器中,复制光谱基线用于明确的频率锁定
Andi Setiono1,2, Nelfyenny2, Wilson Ombati Nyang'au1,3
1Laboratory for Emerging Nanometrology (LENA), Institute of Semiconductor Technology (IHT), Technische Universität Braunschweig, 38106 Braunschweig, Germany.
Sensors (Basel, Switzerland)
|April 13, 2024
概括
本研究介绍了一种消除电热共振传感器中热干扰的方法. 通过减去基线频谱,研究人员实现了准确的频率跟踪,用于实时粒子检测等应用.
科学领域:
- 微电子机械系统 (MEMS) 是一种微电子机械系统.
- 传感器技术 传感器技术
- 纳米技术 纳米技术
背景情况:
- 电热压电阻共振悬臂传感器利用嵌入式加热和压电阻元件进行执行和传感.
- 这些元素的近距离导致热寄生效应,导致不对称的振幅和逆相光谱反应.
- 这些光谱扭曲妨碍了准确的共振频率确定和基于相锁循环 (PLL) 的共振跟踪.
研究的目的:
- 开发和验证一种方法,以减轻电热共振悬臂传感器中的热寄生效应.
- 为了提高传感器应用中的共振频率跟踪的准确性.
- 使用相锁循环技术实现可靠的实时共振跟踪.
主要方法:
- 制造带有集成Wheatstone桥的电热压电阻共振悬臂传感器.
- 开发复制光谱减去技术以数学消除热寄生效应.
- 使用香烟烟雾颗粒进行模拟和实验评估,以优化光谱响应.
主要成果:
- 复制光谱减去方法有效地从传感器共振光谱中消除了热寄生效应.
- 优化的光谱反应表现出对称的振幅和单调的相位过渡.
- 通过粒子检测证明了基于PLL的成功实时频率跟踪,并通过粒子检测进行了验证.
结论:
- 拟议的复制光谱减去技术准确地补偿了共振传感器中的热寄生效应.
- 这种方法显著提高了共振频率确定的精度,并使基于PLL的可靠跟踪成为可能.
- 这些发现为各种环境和工业监测应用中更可靠,更准确的传感器系统铺平了道路.
相关概念视频
Aliasing
133
Accurate signal sampling and reconstruction are crucial in various signal-processing applications. A time-domain signal's spectrum can be revealed using its Fourier transform. When this signal is sampled at a specific frequency, it results in multiple scaled replicas of the original spectrum in the frequency domain. The spacing of these replicas is determined by the sampling frequency.
If the sampling frequency is below the Nyquist rate, these replicas overlap, preventing the original...
If the sampling frequency is below the Nyquist rate, these replicas overlap, preventing the original...
133
Double Resonance Techniques: Overview
200
Double resonance techniques in Nuclear Magnetic Resonance (NMR) spectroscopy involve the simultaneous application of two different frequencies or radiofrequency pulses to manipulate and observe two distinct nuclear spins. One important application of double resonance is spin decoupling, which selectively suppresses coupling with one type of nucleus while observing the NMR signal from another nucleus, simplifying the spectrum and enhancing resolution.
Spin decoupling is usually achieved by...
Spin decoupling is usually achieved by...
200
NMR Spectrometers: Resolution and Error Correction
692
When magnetic nuclei in a sample achieve resonance and undergo relaxation, the signal detected in NMR is an approximately exponential free induction decay. Fourier transform of an exponential decay yields a Lorentzian peak in the frequency domain. Lorentzian peaks in an NMR spectrum are defined by their amplitude, full width at half maximum, and position, where the peak width is governed by the spin-spin relaxation time alone. In real experiments, however, the applied magnetic field is rendered...
692
Bandpass Sampling
175
In signal processing, bandpass sampling is an effective technique for sampling signals that have most of their energy concentrated within a narrow frequency band. This type of signal is known as a bandpass signal. The key principle of bandpass sampling involves sampling the signal at a rate that is greater than twice the signal's bandwidth to prevent aliasing.
A bandpass signal has a spectrum with a lower frequency limit, denoted as ω1, and an upper frequency limit, denoted as ω2....
A bandpass signal has a spectrum with a lower frequency limit, denoted as ω1, and an upper frequency limit, denoted as ω2....
175
Sound Waves: Resonance
2.6K
Resonance is produced depending on the boundary conditions imposed on a wave. Resonance can be produced in a string under tension with symmetrical boundary conditions (i.e., has a node at each end). A node is defined as a fixed point where the string does not move. The symmetrical boundary conditions result in some frequencies resonating and producing standing waves, while other frequencies interfere destructively. Sound waves can resonate in a hollow tube, and the frequencies of the sound...
2.6K
Parallel Resonance
208
The parallel RLC circuit is an arrangement where the resistor (R), inductor (L), and capacitor (C) are all connected to the same nodes and, as a result, share the same voltage across them. The parallel RLC circuit is analyzed in terms of admittance (Y), which reflects the ease with which current can flow. The admittance is given by:
208


