11QE95 laser energy detectors can measure energy up to 250 J (with attenuator). Low noise level - just 15 µJ. Large effective aperture - 95 mm square. These detectors are convenient to use and can measure relatively wide beams. They are suitable for many OEM, manufacturing and laboratory applications. Specifications
| Detector |
11QE95LP-S-MB |
11QE95LP-H-MB |
11QE95ELP-S-MB |
11QE95ELP-H-MB |
| MAX MEASURABLE ENERGY (WITH ATTENUATOR) |
250 J |
250 J |
250 J |
250 J |
| MAX REPETITION FREQUENCY |
40 Hz |
40 Hz |
10 Hz |
10 Hz |
| EFFECTIVE APERTURE |
95 mm Ø |
95 mm Ø |
95 mm Ø |
95 mm Ø |
| MEASUREMENT CAPABILITY |
| Spectral Range *a |
0.19 – 20 µm |
0.19 – 20 µm |
0.19 – 20 µm |
0.19 – 20 µm |
| Maximum Measurable Energy b,c |
Alone |
Attenuator |
Alone |
Attenuator |
Alone |
Attenuator |
Alone |
Attenuator |
| 1064 nm, 150 ns pulse, single shot d |
70 J |
250 J |
70 J |
250 J |
70 J |
250 J |
70 J |
250 J |
| 1064 nm, 7 ns, 10 Hz |
35 J |
150 J |
35 J |
150 J |
35 J |
150 J |
35 J |
150 J |
| 266 nm, 7 ns, 10 Hz |
30 J |
50 J |
30 J |
50 J |
30 J |
50 J |
30 J |
50 J |
| Noise Equivalent Energy e |
15 µJ |
15 µJ |
30 µJ |
30 µJ |
| Sensitivity f,g |
2 V/J |
2 V/J |
0.6 V/J |
0.6 V/J |
| Max Repetition Frequency |
40 Hz |
40 Hz |
10 Hz |
10 Hz |
| Rise Time (typical 0-100 %) |
1.5 ms |
1.5 ms |
5 ms |
5 ms |
| Maximum Pulse Width (typical) |
2 ms |
2 ms |
6 ms |
6 ms |
| Calibration Uncertainty h |
±3 % |
±3 % |
±3 % |
±3 % |
| Repeatability |
<0.5 % |
<0.5 % |
<0.5 % |
<0.5 % |
| DAMAGE THRESHOLDS |
| Maximum Average Power |
Alone |
Attenuator |
Alone |
Attenuator |
Alone |
Attenuator |
Alone |
Attenuator |
| All Wavelengths |
20 W |
45 W |
40 W |
90 W |
20 W |
45 W |
40 W |
90 W |
| Maximum Energy Density |
Alone |
Attenuator |
Alone |
Attenuator |
Alone |
Attenuator |
Alone |
Attenuator |
| 1064 nm, 150 µs, 10 Hz |
1.2 J/cm2 |
14 J/cm2 |
1.2 J/cm2 |
14 J/cm2 |
1.2 J/cm2 |
14 J/cm2 |
1.2 J/cm2 |
14 J/cm2 |
| 1064 nm, 7 ns, single shot |
0.6 J/cm2 |
16 J/cm2 |
0.6 J/cm2 |
16 J/cm2 |
0.6 J/cm2 |
16 J/cm2 |
0.6 J/cm2 |
16 J/cm2 |
| 1064 nm, 7 ns, 10 Hz |
0.6 J/cm2 |
8 J/cm2 |
0.6 J/cm2 |
8 J/cm2 |
0.6 J/cm2 |
8 J/cm2 |
0.6 J/cm2 |
8 J/cm2 |
| 532 nm, 7 ns, 10 Hz |
0.6 J/cm2 |
6 J/cm2 |
0.6 J/cm2 |
6 J/cm2 |
0.6 J/cm2 |
6 J/cm2 |
0.6 J/cm2 |
6 J/cm2 |
| 266 nm, 7 ns, 10 Hz |
0.5 J/cm2 |
1 J/cm2 |
0.5 J/cm2 |
1 J/cm2 |
0.5 J/cm2 |
1 J/cm2 |
0.5 J/cm2 |
1 J/cm2 |
| Maximum Average Power Density |
10 W/cm2 |
600 W/cm2 |
10 W/cm2 i |
600 W/cm2 |
10 W/cm2 |
600 W/cm2 |
10 W/cm2 i |
600 W/cm2 |
| PHYSICAL CHARACTERISTICS |
| Effective Aperture (with Attenuator) |
95 mm Ø(90 mm Ø) |
| Absorber |
Multi-Band |
Multi-Band |
Multi-Band |
Multi-Band |
| Dimensions |
122H x 122W x 20D mm |
122H x 122W x 98D mm |
122H x 122W x 20D mm |
122H x 122W x 98D mm |
| Weight |
0.78 kg |
1.2 kg |
0.78 kg |
1.2 kg | Specifications are subject to change without notice
* For the calibrated spectral range, see the user manual.
a. 0.308 - 2.1 µm with QED Attenuator.
b. Not exceeding Maximum Average Power.
c. Maximum measurable energy depends on the monitor.
d. Increasing pulse width increases the maximum measurable energy.
e. Nominal value, actual value depends on electrical noise in the measurement system.
f. Load: 1 M&Omh; and ≤ 30 pF.
g. Maximum output voltage = sensitivity x maximum energy.
h. Excludes non-linearities.
i. At 12 W. Maximum Average Power Density is 5 W/cm2 @ 40 W.
More information about QED attenuators
Compatible Monitors:
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