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Quartz-Enhanced Photoacoustic Spectroscopy

Related products: MFLI, VHFLI

Application Description

Sketch – Quartz-Enhanced Photoacoustic Spectroscopy

Photoacoustic spectroscopy (PAS) is a high-sensitivity technique for trace gas quantification based on the photoacoustic effect: a gas sample absorbs modulated light and releases energy as heat via non-radiative relaxation. This periodic heating generates acoustic pressure waves traditionally measured using microphones. However, microphone-based PAS is susceptible to external noise and imposes strict constraints on the design and size of the gas cell. Quartz-enhanced photoacoustic spectroscopy (QEPAS) overcomes these hurdles by using a quartz tuning fork (QTF) as a high-Q acoustic transducer, providing superior noise immunity, a compact footprint, and enhanced sensitivity.

Measurement Strategies

QEPAS utilizes wavelength modulation spectroscopy (WMS) for high-sensitivity trace gas sensing. As shown in the figure, a sinusoidal signal at frequency f is superimposed on the laser's DC drive current to modulate the wavelength while scanning the absorption line. The resulting photoacoustic excitation between the QTF prongs generates a piezoelectric current. This signal is converted to voltage via a transimpedance amplifier (TIA) and synchronously demodulated by a lock-in amplifier; the gas concentration is then derived from the 2f signal amplitude.

QTF characterization: resonance frequency (f0​ ​) and quality factor (Q)

The resonance frequency (f0​) dictates the required modulation frequency (f=f0​/2) for maximum signal enhancement. The quality factor (Q) governs both the signal gain and the QTF’s response time, τ=Q/(πf0​).

The LabOne Sweeper tool automates the measurement and fitting of these parameters to streamline system setup.

Laser control: ramping rate and modulation depth

The laser's DC ramp rate must be aligned with the QTF time constant (τ) to avoid line-shape distortion. Additionally, the AC modulation depth must be optimized to maximize the 2f response.

The LabOne Sweeper facilitates this by providing automated parametric sweeps for both the scanning range and modulation amplitude.

Piezoelectric current: transimpedance amplifier

The TIA is a critical component in the QEPAS signal chain; its ultra-low input referred noise directly limits the system's minimum detection limit. Furthermore, programmable gain stages are essential to maintain high sensitivity across a wide dynamic range.

The MFLI and VHFLI address these requirements with an integrated, low-noise TIA, providing the high-performance current-to-voltage conversion without the need for external preamplifiers.

Long-term stability and minimum detection limit: Allan deviation analysis

Allan deviation (ADEV) analysis is performed to identify noise sources, verify long-term stability, and accurately determine the minimum detectable concentration limit. This requires continuous, uninterrupted data acquisition over extended periods.

LabOne simplifies this through one-click data streaming and API support, providing the seamless data sequences necessary for ADEV characterization.

Product Highlights

MFLI 500 kHz / 5 MHz Lock-in Amplifier

VHFLI 50 MHz / 200 MHz Lock-in Amplifier

Zurich Instruments MFLI 500 kHz / 5 MHz Lock-in Amplifier front
VHFLI 50 MHz / 200 MHz Lock-in Amplifier
  • DC - 500kHz/5MHz 16 bit Current and Voltage Inputs
  • Ultra-low and flat Input Voltage Noise: < 2.5 nV/√Hz (> 1kHz)
  • Short time constants: 337 ns to 83 s
  • High Dynamic Reserve: 120 dB
  • API programming support for Python, MATLAB, LabVIEW, C, .NET
  • DC - 50 MHz/200 MHz 14-bit Current and Voltage Inputs
  • Ultra-low and flat Input Voltage Noise: < 3 nV/√Hz (> 50kHz)
  • Short time constants: 14 ns to 21 s
  • High Dynamic Reserve: 120 dB
  • API programming support for Python, MATLAB, LabVIEW, C, .NET

The Benefits of Choosing Zurich Instruments

  • Superior Sensitivity & Throughput: The ultra-low noise floor of the MFLI and VHFLI translates directly into higher sensitivity, significantly accelerating data acquisition and experimental throughput.
  • Full Development Cycle Support: From component-level QTF characterization to full system-level validation, Zurich Instruments lock-in amplifiers provide a versatile platform for every stage of sensor development.
  • Automated Optimization: The LabOne Sweeper automates routine tasks, such as resonance parameter fitting (f0​ and Q) and modulation depth optimization, ensuring rapid and repeatable results.
  • Integrated TIA Reduces Complexity: The built-in, high-performance TIA eliminates external preamplifiers, simplifying wiring while maintaining signal integrity.
  • Streamlined Data Workflow: One-click data streaming ensures a stable data flow for long-term analysis, such as Allan Deviation, without requiring external acquisition hardware.

Related Publications

Ma, H., Chen, Y., Qiao, S., He, Y., & Ma, Y.

A high sensitive methane QEPAS sensor based on self-designed trapezoidal-head quartz tuning fork and high power diode laser

Photoacoustics 42, 100683 (2025)

Shi, J., Zhao, J., Zhang, H., Fu, Y., Qin, L., Zhao, Y., Feng, Y., Chen, D., & Wang, Z.

Signal enhancement of the gas detection based on quartz-enhanced photothermal spectroscopy technology

Optics express, 32(16), 27176–27187 (2024)

Zhang, H., Wang, Z., Wang, Q., Borri, S., Galli, I., Sampaolo, A., Patimisco, P., Spagnolo, V. L., De Natale, P., & Ren, W.

Parts-per-billion-level detection of hydrogen sulfide based on doubly resonant photoacoustic spectroscopy with line-locking

Photoacoustics, 29, 100436 (2023)

Wang, Z., Wang, Q., Zhang, H., Borri, S., Galli, I., Sampaolo, A., Patimisco, P., Spagnolo, V. L., De Natale, P., & Ren, W.

Doubly resonant sub-ppt photoacoustic gas detection with eight decades dynamic range

Photoacoustics, 27, 100387 (2022)