Related Experiment Video
Updated: Jul 27, 2025

08:25
Construction of a Wireless-Enabled Endoscopically Implantable Sensor for pH Monitoring with Zero-Bias Schottky Diode-based Receiver
Published on: August 27, 2021
2.6K
PT-Symmetric LC Passive Wireless Sensing
Dong-Yan Chen1, Lei Dong1, Qing-An Huang1
1Key Laboratory of MEMS of the Ministry of Education, Southeast University, Nanjing 210096, China.
Sensors (Basel, Switzerland)
|June 10, 2023
Summary
Parity-time (PT) symmetry in inductor-capacitor (LC) sensors enhances sensitivity and sensing distance. This review explores PT-symmetric LC sensors, highlighting non-Hermitian advantages over classical principles.
Area of Science:
- Quantum mechanics
- Electrical engineering
- Sensor technology
Background:
- Parity-time (PT) symmetry challenges the Hermitian operator requirement in quantum mechanics.
- Non-Hermitian Hamiltonians with PT symmetry exhibit real energy spectra.
- PT symmetry is applied to inductor-capacitor (LC) passive wireless sensors to boost performance.
Purpose of the Study:
- To review the research status of PT-symmetric LC sensors.
- To demonstrate the advantages of non-Hermitian sensing principles.
- To analyze sensor performance in exact phase, exceptional point, and broken phase working areas.
Main Methods:
- Systematic review of PT-symmetric LC sensor research.
- Analysis of higher-order PT symmetry and divergent exceptional points (EPs).
- Comparison of non-Hermitian sensing with classical LC sensing.
Main Results:
- PT symmetry enables multi-parameter sensing, ultrahigh sensitivity, and longer interrogation distances in LC sensors.
- Higher-order PT symmetry and divergent EPs offer enhanced sensitivity and spectral resolution via drastic bifurcation.
- Controversies exist regarding noise and precision in EP sensors.
Conclusions:
- PT-symmetric LC sensors offer significant advantages over classical LC sensing.
- Further research is needed to address noise and precision limitations in EP sensors.
- Non-Hermitian sensing principles provide a promising avenue for advanced LC sensor development.
Related Concept Videos
Passive Filters
562
Passive filters are utilized to shape the frequency spectrum of signals across a diverse array of applications. These filters, using only passive elements like resistors (R), inductors (L), and capacitors (C), are capable of selectively allowing or blocking certain frequency ranges without the need for external power sources.
Low-Pass Filters
Low-pass filters are designed to transmit signals with frequencies lower than the cutoff frequency, ωc, and attenuate those above it. The cutoff...
Low-Pass Filters
Low-pass filters are designed to transmit signals with frequencies lower than the cutoff frequency, ωc, and attenuate those above it. The cutoff...
562
Parallel RLC Circuits
930
Street lamps equipped with RLC surge protectors are an excellent example of applying circuit analysis in practical scenarios. These surge protectors safeguard the lamp's components against sudden voltage spikes.
A simplified parallel RLC circuit model with a DC input source generating a step response is employed in this context. When the switch is turned on, Kirchhoff's current law is applied, leading to a second-order differential equation.
A simplified parallel RLC circuit model with a DC input source generating a step response is employed in this context. When the switch is turned on, Kirchhoff's current law is applied, leading to a second-order differential equation.
930
LC Circuits
2.6K
An LC circuit consists of an inductor and a capacitor, either in series or parallel. Consider a charged capacitor connected with an inductor in series. Before the switch is closed, all the energy of the circuit is stored in the electric field of the capacitor. When the switch is closed, the capacitor begins to discharge, producing a current in the circuit. The current, in turn, creates a magnetic field in the inductor. Because of the induced emf in the inductor, the current cannot change...
2.6K
Oscillations In An LC Circuit
2.3K
An idealized LC circuit of zero resistance can oscillate without any source of emf by shifting the energy stored in the circuit between the electric and magnetic fields. In such an LC circuit, if the capacitor contains a charge q before the switch is closed, then all the energy of the circuit is initially stored in the electric field of the capacitor. This energy is given by
2.3K

