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09.09.2025

How to Choose Pyroelectric Detectors?
Materials, Applications, and Working Principle

LASER COMPONENTS  – Experts in Pyroelectric Detector Manufacturing

Multi channel pyroelectric detectors Multi channel pyroelectric detectors
Multi-channel and single-channel pyroelectric detectors

Pyroelectric detectors are thermal detectors: temperature fluctuations produce a change in surface charge on pyroelectric materials, which produces a corresponding electrical signal This temperature gradient is usually triggered by an absorber that converts incident light into heat. There are various pyroelectric materials available, three of which are commonly used in pyroelectric detectors: DLaTGS, LiTaO₃ (LTO), and PZT. The table below provides an overview of the properties of each material. Simply put, the figures mean the following: 

  • The pyroelectric coefficient determines the ability to produce current from infrared radiation. That is to say: the bigger, the better.
  • The dielectric constant (at room temperature) determines the capacitance, thereby affecting the noise. In voltage operation, the following is true: 
    The larger the capacitance, the lower the noise. The dielectric constant (at room temperature) corresponds in the exact opposite manner.
  • The specific heat capacity determines the temperature increase in the pyroelectric material depending on the absorbed radiation. A low Cv means a larger temperature increase and thus a better signal.
  • The specific AC resistance is coupled with dielectric losses that, in turn, produce a kind of Johnson noise. A pure dielectric would not produce any noise. The lower the AC resistant, the better.

DLaTGS

Pyroelectric coefficient:       4.5 x 10-8
δ [Coul/cm² °K]

Dielectric constant
(at room temperature):         18 
ε

Specific heat capacity:        2.5 
Cv [J/cm3 °K]

Specific AC resistance:      2.4 x 1010
ρ [Ω -cm]


Figure of merit:                  24
δρ/εCv



 

LiTaO3

Pyroelectric coefficient:    1.7 x 10-8
  δ [Coul/cm² °K]

Dielectric constant
(at room temperature):       max. 51 (anisotrope)
  ε

Specific heat capacity:    3.2
  Cv [J/cm3 °K]

Specific AC resistance:   4.2 x 1010
  ρ [Ω -cm]

Figure of merit:               4.3
  δρ/εCv

 

PZT 

Pyroelectric coefficient:          4.4 x 10-8
δ [Coul/cm² °K]


Dielectric constant
(at room temperature):            180
ε

Specific heat capacity:           2.6
Cv [J/cm3 °K]

Specific AC resistance:          4.2 x 109
ρ [Ω -cm]


Figure of merit:                       0.4
δρ/εCv

Fig. 1: Current Response [µA/W] vs. Temp. [°C] (DLaTGS & LTO]

To compare materials in terms of their fundamental suitability for pyroelectric detectors, it makes sense to analyze them using the following parameters: pyroelectric coefficient, specific AC resistance, dielectric constant, and specific heat capacity. DLaTGS and LiTaO₃ achieve the best results and are therefore particularly well suited. 
 
DLaTGS offers the highest performance detectivity (approx. 2 × 10⁹ Jones  @ 10 Hz) and is widely used in IR measurement technology in laboratory settings, especially in routine FTIR applications. Industrial applications are largely the domain of LiTaO₃ due to its favorable thermal behavior (Fig. 1). PZT is primarily used in consumer products.

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How to Choose Pyroelectric Detectors

Current vs Voltage Mode

Fig. 2: Typical VM circuit: Equivalent circuit of a detector in voltage mode (VM)

The IR crystal is modulated as a power source with a parallel capacitance and housed in a TO can with additional electronic components. There are two basic modes of operation of pyro detectors: voltage mode (VM) (Fig. 2) and current mode (CM) (Fig. 3). 

Voltage Mode: Pros and Cons:

JFET-based voltage mode has been widely used in pyroelectric detector applications for many years. However, integration comes with significant challenges and is best suited for experienced users.

Main Voltage Mode Challenges:

  • A relatively low output signal 
  • A strongly temperature-dependent offset 

Advantages of Voltage Mode:

  • It provides flexible amplification options 
  • It enables the highest possible D* value with a simple design (approx. 0.5 × 10⁹ Jones @ 10 Hz)
Fig. 3: Typical CM circuit: Equivalent circuit of a detector in current mode (CM)

Why Current Mode (CM) Detectors?

Current mode (CM) offers several advantages like high responsivity for pyroelectric detector applications. 

Key Benefits of Current Mode:

  • Produces high signal on a low offset, with minimal temperature dependence
  • Requires low-power operational amplifiers (OpAmps)
  • Easy to implement, making it ideal for beginner-level product development
  • Features low output impedance, which improves EMC performance 

D Performance and Design Considerations

  • High D* (detectivity) values in current mode are comparable to those in voltage mode. 
  • The design is slightly more complex than voltage mode because to reach this impressive D* the detector can be connected to a second blind detector element in antiparallel.
  • This design—even though it is not the best term—is commonly referred to as "temperature compensation" (TC)

What Temperature Compensation Really Does

  • The blind detector element reduces unwanted signals caused by fluctuations in ambient temperature. 
  • However, it does not compensate for inherent temperature dependencies of the detector material (see Fig. 1). 
  • A more accurate term would be "temperature fluctuation compensation" (TFC) or signal stabilization

Effect of TFC on Performance

  • In current mode, TFC improves performance by attenuating toward natural oscillations, enabling greater signal amplification
  • In voltage mode, however, TFC can reduce performance by approximately 50%. 

Good to Know

What is D*?

Detectivity D*

“D* represents the signal-to-noise ratio (SNR) for a certain electrical frequency and bandwidth if 1 watt of radiation power reaches a detector surface of 1 cm2. The higher the D* value, the better the detector.”

D*[cHzW-1] =activedetectorareaNEP

Original from October 2018
Last revision September 2025

Components Ranging from Standard to OEM

Find the Right Part or We Make It

The LASER COMPONENTS Detector Group manufactures pyroelectric detectors based on both DLaTGS and LiTaO3. Our portfolio ranges from all commercially available options, from multicolor and miniaturized versions to detectors with a low-microphonic effect, and continues to expand so that LASER COMPONENTS can be your one source for detection solutions. 

For detailed information about the products listed below, or to discuss custom components tailored for specific applications, our product engineers are ready to help. Just fill out the form below to get in contact. 

Infrared Components Infrared Components
55+ Series: IR Components for 5Hz / 5µm

Complete with selected filter and other accessories.

A perfect match: The ideal emissivity of Infrasolid emitters complement the high dynamic range and low noise of our custom-made pyrodetectors.
ALUT3151X1300-k2 ALUT3151X1300-k2
Advanced LTO Infrared Detectors

Advanced single channel voltage mode detectors for FTIR instruments.

Excellent linearity and fast response to IR flux change.
Choice of Filters for Pyroelectric Detectors

An IR filter makes all the difference. Thermal detectors are naturally polychromatic, and a filter is needed to detect specific gases/wavelengths.

Differential Pyroelectric Detector Differential Pyroelectric Detector
Differential Pyroelectric Detector

Pyroelectric crystals generate positive and negative charge carriers simultaneously on opposing sides.

The LD21XX and DD31XX series are exclusive pyroelectric detectors in which both crystal sides are amplified separately.
Differential Pyroelectric Detector Differential Pyroelectric Detector
Differential Pyroelectric Detector

Pyroelectric crystals generate positive and negative charge carriers simultaneously on opposing sides.

The LD21XX and DD31XX series are exclusive pyroelectric detectors in which both crystal sides are amplified separately.
Multi channel pyroelectric detectors Multi channel pyroelectric detectors
Multi-channel LiTaO3 Pyroelectric Detectors

Multi-channel pyrodetectors: dual-channel, triple-channel and quad-channel versions are available.

Multi channel pyroelectric detectors Multi channel pyroelectric detectors
Multi-channel LiTaO3 Pyroelectric Detectors

Multi-channel pyrodetectors: dual-channel, triple-channel and quad-channel versions are available.

Single Channel Current Mode Pyroelectric Detector Single Channel Current Mode Pyroelectric Detector
One-Channel LiTaO3 Pyroelectric Detector

Single channel pyroelectric detectors made of LiTaO3 are available for current mode (CM). They are used for gas detection and flame detection.

Single Channel Current Mode Pyroelectric Detector Single Channel Current Mode Pyroelectric Detector
One-Channel LiTaO3 Pyroelectric Detector

Single channel pyroelectric detectors made of LiTaO3 are available for current mode (CM). They are used for gas detection and flame detection.

LT0102X-k2 LT0102X-k2
Pyroelectric DLaTGS Detectors

DLaTGS detectors exhibit the most effective pyroelectric effect known. Their major application is FTIR.

DLaTGS = Deuterated Lanthanum α Alanine doped TriGlycine Sulphate 
LT0102X-k2 LT0102X-k2
Pyroelectric DLaTGS Detectors

DLaTGS detectors exhibit the most effective pyroelectric effect known. Their major application is FTIR.

DLaTGS = Deuterated Lanthanum α Alanine doped TriGlycine Sulphate 
What Kind of Customized Detector do you need to design innovative products for the future? 
Employee of LASER COMPONENTS US Employee of LASER COMPONENTS US
Jim Dell
LASER COMPONENTS USA Inc.

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Welcome to LASER COMPONENTS USA, Inc., your expert for photonics components. Each product in our wide range of detectors, laser diodes, laser modules, optics, and more is worth every Dollar ($/USD). Our customized solutions cover all conceivable areas of application: from sensor technology to medical technology. You can reach us here:

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Phone: +1 603 821 7040
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Jim Dell
LASER COMPONENTS USA Inc.
03110 Bedford, NH
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116 South River Road
Building C
Bedford, NH 03110
USA

Phone: +1 603 821 7040

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