Low Power Thermopile Sensors are the choice for measuring laser beam powers up to 50 Watts. We offer two types that are calibrated for use with Ophir Power Meters. High Sensitivity Thermal Laser Sensors are very low noise and drift sensors that accurately measure low laser powers in the 30uW to 12W range over a wide range of wavelengths. They can also measure low single shot laser energies down to tens of uJ. Low Power Thermal Sensors accurately measure power in the 20 mW to 50 W range as well as single shot laser energy. All low power sensors are calibrated for use with standard ophir power and energy meters. We also offer Medium Power Thermopile Sensors, and Water Cooled Thermopile Sensors for higher power measurement requirements.
Thermopile Sensor Overview
The thermopile sensor has a series of bimetallic junctions. A temperature difference between any two junctions causes a voltage to be formed between the two junctions. Generally, Ophir specifies ±2% uniformity of reading over the surface or better. Thermal sensors are for use from fractions of a milliwatt up to thousands of watts.
Although Ophir thermal power sensors are used primarily to measure power, they can measure single shot energy as well where they integrate the power over time flowing through the disc and thus measure energy. Since the typical time it takes for the disc to heat up and cool down is several seconds, these thermal sensors can only measure one pulse every several seconds at most. Thus they are suitable for what is called single shot measurement. Although the response time of the sensor discs is slow, there is no limit to how short the pulses measured are since the measurement is of the heat flowing through the disc after the pulse.
Ophir has developed several types for different applications, such as long pulses (0.1-10ms), short pulses (<1µs) and continuous radiation. Absorbers optimized for long pulses and CW are characterized by thin, refractory materials, since the heat can flow through the coating and into the disc during the pulse. On the other hand, heat cannot flow during short pulses, and all the energy is deposited in a thin (typically 0.1µm) layer near the surface. This causes vaporization of the surface which ruins the absorber. Instead, a volume absorber that is partially transparent and absorbs over a distance of 50µm -3mm is used. This spreads the heat over a larger volume allowing much higher energies.
Compaible Power Meters
NOVA-II-OP Optical Power and Energy Meter
VEGA-OP Optical Power and Energy Meter
NOVA-OP Optical Power and Energy Meter
JUNO-OP Virtual Optical Power and Energy Meter
USBI-OP Virtual Optical Power and Energy Meter
JUNO-OP 2 Channel Virtual Optical Power and Energy Meter
High Sensitivity Thermal Sensors
|
Model |
3A-OP
|
3A-P-OP
|
3A-FS-OP
|
12A-V1-OP
|
| Absorber Type |
Broadband (general purpose) |
P Type (short pulses) |
With removeable window |
Broadband (general purpose) |
| Spectral Range (µm) |
0.190 to 20 |
0.150 to 6 |
0.190 to 20(b) |
0.190 to 20 |
| Active Diameter (mm) |
9.5 |
12 |
9.5 |
16 |
| Power Mode |
| Power Range (W) |
60 µW - 3 W |
30 µW - 3 W |
2mW - 12 W |
| Power Scales (µW) |
3 W to 300 µW |
12W to 20 mW |
| Noise Equivalent Power (µW) |
2 |
4 |
2 |
50 |
| Thermal Drift (30 mnin) % (a) |
5 - 20 µW |
5 - 30 µW |
2 - 10 µW |
10 - 150 µW |
| Power Density, Maximum Average (W/cm2) |
200 |
50 |
200 |
25,000 |
| Rise Time (s) with Meter (0-95%) typ |
1.8 |
2.5 |
1.8 |
2.5 |
| Power Accuracy +/-% |
3 |
| Linearity with Power +/- (%) |
±1.5 |
| Energy Mode |
| Energy Range |
20 µJ - 2 J |
15 µJ - 2 J |
1 mJ - 30 J |
| Energy Scales (µJ) |
2 J to 200 µJ |
30J to 30 mJ(c) |
| Minimum Energy |
20 µJ |
15 µJ |
1mJ |
| Max Energy Density (J/cm2) |
<100 ns, 0.3 J/cm2 0.5 ms, 1 J/cm2 2 ms, 2 J/cm2 10 ms, 4 J/cm2 |
<100ns, 1 J/cm2 0.5ms, 1 J/cm2 2ms, 1 J/cm2 10ms, 1 J/cm2 |
<100ns, 0.3 J/cm2 0.5ms, 1 J/cm2 2ms, 2 J/cm2 10ms, 4 J/cm2 |
<100ns, 0.3 J/cm2 0.5ms, 5 J/cm2 2ms, 10 J/cm2 10ms, 30 J/cm2 |
| Cooling Method |
Sensor Body |
| Weight (kg) |
0.2 |
0.35 |
| Fiber Adapters Available |
FC |
|
|
FC |
(a) Depending on room airflow and temperature variations.
(b) Remove window for measurement beyond 2.2 µm.
(c) For the 30 mJ energy scale measurements it is recommended to use the screw on barrel supplied with the sensor to protect from direct air flow.
Low Power Thermal Sensors
|
Model |
10A-OP
|
30A-BB-18-OP
|
L30A-10MM-OP
|
| Absorber Type |
Broadband (low power) |
Broadband (general purpose) |
Broadband (thin profile) |
| Spectral Range (µm) |
0.190 to 20 |
0.190 to 20 |
0.150 to 20 |
| Active Diameter (mm) |
16 |
17.5 |
26 |
| Power Mode |
| Power Range (W) |
20 mW - 10 W |
20 mW - 30 W |
80 mW - 8 W free standing 30 W heat sinked |
| Power Scales (W) |
10 W to 0.5 µW |
30 W , 5 |
30 W, 3 |
| Noise Equivalent Power (mW) |
1 |
1 |
4 |
| Power Density, Maximum Average (W) |
28 |
20 kW/cm2 at 30W, 28 kW/cm2 at 10 W |
20 kW/cm2 at 30 W, 28 kW/cm2 at 10 W |
| Rise Time (s) with Meter (0-95%) typ (b) |
0.8 |
0.8 |
1.5 |
| Power Accuracy +/-% |
3 |
| Linearity with Power +/- (%) |
±1 |
±1 |
| Energy Mode |
| Energy Range |
6 mJ - 2 J |
6 mJ - 30 J |
20 mJ - 60 J |
| Energy Scales (mJ) |
2 J, 200 µJ |
30 J, 3 J, 300 mJ |
60 J to 20 mJ |
| Minimum Energy |
6 mJ |
20 µJ |
| Max Energy Density (J/cm2) |
<100 ns, 0.3 J/cm2 0.5 ms, 2 J/cm2 2 ms, 2 J/cm2 10 ms, 2 J/cm2 |
<100 ns, 0.3 J/cm2 0.5 ms, 5 J/cm2 2 ms, 10 J/cm2 10 ms, 30 |
| Cooling Method |
Sensor Body |
Heat Sink |
Sensor Body |
| Weight (kg) |
0.2 |
0.3 |
0.1 |
| Fiber Adapters Available |
FC |
|
|