Liquid Crystal EO Amplitude Modulators, Free Space


  • Liquid Crystal EO Modulator / Variable Attenuator
  • Attenuation Control Using SMA Modulation Input or Potentiometer
  • Models with Wavelength Ranges Covering 425 - 1620 nm Available

Front

Modulation
Input

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Application Idea

NEL02A EO Modulator
with Half-Wave Plate in
CRM1T Rotation Mount

NEL01A

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Noise Eater Max Modulation Depth
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Modulation Performance of Thorlabs' LC EO Modulators/Noise Eaters

Features

  • Modulate the Intensity of Signals Using an Internal Liquid Crystal Variable Waveplate
  • Low, 0 - 2.5 V Modulation Input Voltage Range
  • Ø4 mm Clear Aperture
  • SMA Modulation Input Connector
  • Also Functions as a Noise Eater or Variable Attenuator
  • Models for use at 425 - 650 nm, 475 - 650 nm, 650 - 1050 nm, or 1050 - 1620 nm
  • Maximum Input Power of up to 1.65 W, Depending on Model, Wavelength, and Beam Size
    (See the Operation Tab for Details)

Thorlabs' Noise Eaters are liquid crystal (LC) devices that can function as electro-optic (EO) modulators. They use a liquid crystal retarder and a polarizer with a closed-loop feedback system to precisely and quickly attenuate light with no moving parts. The attenuation can be controlled using the SMA modulation input or an onboard potentiometer. Additionally, the noise eaters' attenuation can be controlled automatically by the feedback loop, allowing them to function as a noise reduction device. These noise eaters/EO modulators are designed for use with light in the 425 - 650 nm [Item # NEL01A(/M)], 475 - 650 nm [Item # NEL02A(/M)], 650 - 1050 nm [Item # NEL03A(/M)], or 1050 - 1620 nm [Item # NEL04A(/M)] wavelength range. We offer noise eater models for low (<60 mW) or high (<1.65 W) power use; see the Specs tab for details.

Power Attenuation and Modulation
These noise eaters are also capable of continuously attenuating and modulating the laser output using the liquid crystal retarder and integrated polarizer. Unlike most attenuators available, Noise Eaters attenuate the laser power rapidly without the use of any mechanical components. The noise eater's attenuation capabilities can be controlled via the onboard potentiometer or electrical modulation input.

Noise Eater Top View
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NEL02A Top View Showing Power Range Adjustment Switches and Modulation Input
Noise Eater Schematic
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Noise Eater Block Diagram

Noise Reduction
Utilizing a liquid crystal amplitude modulator, combined with an internal photodiode for power measurement and a feedback control circuit, these noise eaters can eliminate intensity noise in linearly polarized light, achieving amplitude stabilization of within 0.05% of a selected output power. The input power can be set to one of several ranges using the switches on the top of the unit, which permit the noise eater to remove noise without unnecessarily attenuating the signal power. The potentiometer is then adjusted to select the output power (see the Operation tab for more information). Long-term performance and frequency characterization for each noise eater model are shown on the Performance tab.

Mechanical Compatibility
Thorlabs' Noise Eaters are post mountable in two orientations via 8-32 (M4) tapped holes. They also feature 4-40 tapped holes on the front and back for 30 mm Cage System compatibility and an SM1-threaded (1.035"-40) rear aperture for Ø1" Lens Tube compatibility.

Item # NEL01A(/M) NEL02A(/M) NEL03A(/M) NEL04A(/M)
Wavelength Range 425 - 650 nm 475 - 650 nm 650 - 1050 nm 1050 - 1620 nm
Switchable High Power Mode - YES! YES! YES!
Noise Attenuation Performance Specs
Output Power Stabilitya ±0.05% (RMS)
Noise Attenuation Frequency Rangeb DC - 1.8 kHz DC - 2.5 kHz DC - 1.4 kHz
Noise Attenuation Amplitude Range 0.1% to 50% of Input Signal
Noise Attenuation Factorc >150 at 10 Hz, 80 at 60 Hz
20 at 400 Hz, 4 at 1 kHz
>150 at 10 Hz, 80 at 60 Hz
10 at 400 Hz, 1.5 at 1 kHz
Effective Output Power Attenuation Ranged 1 - 40 1 - 5
Internal Polarizer Blocking DamageThreshold
(Maximum Power Attenuation)
1 W/cm2 10 W/cm2
Attenuation Control Onboard Potentiometer (10 Turns) or SMA Modulation Input
Optical Specs
Transmission (Click for Plot) >85% at 635 nm >80% at 635 nm >85% at 780 nm >85% at 1550 nm
Power Level Switching Four Position Power Range Switch High/Low Power Mode Switch and Four Position Power Range Switch
Maximum Input Power See the Max Powers at Various Wavelengths Section on the Operation Tab
Minimum Input Power 0.5 mW
Polarization Extinction Ratio at Output >1000:1 Over Wavelength Range
Damage Threshold (CW)e 0.8 W/cm2 8 W/cm2
Input Aperture Ø5 mm
Input Beam Diameterf Ø4 mm (Max)
Output Beam Displacement 1 mm Vertically (in the Direction of Input Polarization)
Beam Divergence 5 mrad (Max)
Angle of Incidence ±2° (Max)
Input Polarization Tolerance ±3°
Wavefront Distortion ≤λ/4 at 635 nm ≤λ/2 at 635 nm
AR Coating Ravg <0.5% from 400 - 650 nm Ravg <0.5% from 650 - 1100 nm Ravg <0.5% from 1050 - 1620 nm
Modulation Performance Specs
Modulation Input SMA Connector, 0 - 2.5 V, 10 kΩ Input Impedance
Extinction Ratiog 512.6 7.7 6.5
Minimum Rise / Fall Timeh 0.65 ms / 7.3 ms 0.75 ms / 11.5 ms 2.8 ms / 25 ms
Pulsed Laser Input Repetition Rate >1 MHz
General Specs
Mounting Options Two 8-32 (M4) Tapped Holes for Post Mounting
30 mm Cage System Compatible via Eight 4-40 Tapped Holes
Ø1" Lens Tube Compatible via 4 mm Deep Internal SM1 Threads on Rear Side
Operating Temperature Range 15 °C to 45 °C
  • RMS value over 8 hours.
  • The maximum of the frequency range is defined as the point where 0 dB noise attenuation is obtained. These noise eaters are designed to operate down to DC frequency. However, due to external factors (e.g. ambient temperature, vibration, spatial and/or polarization stability of the light source), the noise attenuation factor below 10 Hz is difficult to measure and quantify. Therefore our specifications are guaranteed at 10 Hz and above.
  • Noise attenuation factor is the ratio of noise amplitude before and after the noise eater. It was tested at 3 mW input power with a noise amplitude of 5% of the input power level. See detailed noise attenuation plots on the Performance tab for more information.
  • This is the range of output power adjustment where the noise attenuation factor is guaranteed for a given input power level. If the output power is further reduced, the noise eater might not be able to completely reduce the noise in the signal. This specification does not include losses due to absorption.
  • The maximum input power density and laser damage threshold are wavelength-independent. Additionally, the absolute maximum input power varies with wavelength; see the Operation tab for details.
  • Specified for a 1/e2 beam diameter.
  • Extinction ratio is the ratio of the signal power at minimum attenuation to the signal power at full attenuation, regardless of the effective noise attenuation factor, when using the SMA modulation input.
  • Rise time is measured on the rising edge of the output intensity from 10% to 90% of full output power.

Noise Eater Performance Graphs

In the graphs below, noise attenuation was measured as one of three parameters was varied: input power level, input signal modulation (noise) amplitude, and output signal attenuation. The graphs show that the noise eaters provide consistent performance regardless of changes in these parameters.

Graph Definitions

Modulation Performance
In these graphs, a sine wave with a 2.5 V amplitude and an increasing frequency was used to modulate a noiseless input beam. The graphs show that the maximum modulation depth decreases with increasing modulation frequency. Further testing has demonstrated that the modulation performance is consistent for a given noise eater model, regardless of the laser beam's input power.

Noise Attenuation at Various Input Power Levels
Noise attenuation factor is the ratio of noise amplitude before and after the noise eater. In these graphs, the attenuation factor was measured for several different input power levels, with a fixed signal modulation depth (noise amplitude). The graphs below show that the noise eaters provide consistent performance regardless of input power level.

Noise Attenuation at Various Input Signal Modulations
In these graphs, the input signal was modulated with a sine wave to simulate noise. The attenuation factor was measured at a variety of modulation depths (noise amplitudes). The graphs below show that the noise eater provides consistent performance even at large noise levels.

Noise Attenuation at Various Output Signal Power Levels
Since the noise eater uses a liquid crystal modulator as the optical control element, the noise attenuation is achieved by attenuating the laser beam when noise appears. Our noise eaters are carefully designed to optimize the noise attenuation performance without needing to severely attenuate the signal. These graphs demonstrate that the specified noise attenuation can be reached with a cost of only 5% - 10% overall attenuation of the output power, and further increases in attenuation does not significantly improve the noise attenuation.

 


NEL01A(/M): Low Power Noise Eater for Visible (425 - 650 nm)

Click here to download raw data.

Item # Modulation
Performance
Noise Attenuation Long-Term
Noise Attenuation
Transmission
vs. Input Power vs. Noise Amplitude vs. Signal Attenuation
NEL01A(/M)

 


NEL02A(/M): High/Low Power Noise Eater for Visible (475 - 650 nm)

Click here to download raw data.

Item # Modulation
Performance
Noise Attenuation Long-Term
Noise Attenuation
Transmission
vs. Input Power vs. Noise Amplitude vs. Signal Attenuation
NEL02A(/M)  

 


NEL03A(/M): High/Low Power Noise Eater for NIR (650 - 1050 nm)

Click here to download raw data.

Item # Modulation
Performance
Noise Attenuation Long-Term
Noise Attenuation
Transmission
vs. Input Power vs. Noise Amplitude vs. Signal Attenuation
NEL03A(/M)

 


NEL04A(/M): High/Low Power Noise Eater for IR (1050 - 1620 nm)

Click here to download raw data.

Item # Modulation
Performance
Noise Attenuation Long-Term
Noise Attenuation
Transmission
vs. Input Power vs. Noise Amplitude vs. Signal Attenuation
NEL04A(/M)

Operation

Thorlabs' Liquid Crystal EO Modulators/Noise Eaters are precision instruments for modulating, stabilizing, and attenuating laser power. The modulator consists of a variable attenuator (liquid crystal wave plate and polarizer), a calibrated beamsplitter, and a servo controller to control the modulator, as depicted in the block diagram to the right.

Linearly polarized light is input into the liquid crystal retarder, which, together with the output polarizer, acts as a variable retarder. A beamsplitter then sends a small part of the beam to a feedback loop consisting of a photodiode and control servo. The servo compares the optical signal to a preset signal level and applies the appropriate adjustment voltage until the optical signal reaches the desired level.

The noise eater can also be used as a variable attenuator, even without the presence of noise. By adjusting the resistance of the potentiometer, the user can set the desired output power level.

Noise Eater Mounting Options
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The Noise Eater can be post mounted in two different orientations to match the input light's direction of polarization. A CRM1T(/M) Cage Rotation Mount and four 30 mm Cage Rods can mount a half-wave plate for fine tuning the polarization alignment.

Mounting and Alignment

The noise eater is designed to work with linearly polarized input light aligned with the direction of the arrow engraved on the noise eater near the input aperture. Linearly polarized light and proper alignment of the direction of polarization are important for achieving the best results from the noise eater.

In order to minimize optical losses, the noise eater does not have an input polarizer. If the incident light is not linearly polarized, a linear polarizer must be placed before the noise eater to polarize the incident light.

If the incident light is linearly polarized but is not aligned exactly vertically or horizontally, a half-wave plate can be used before the noise eater to rotate the polarization axis. As shown in the photo to the right, the noise eater's cage mount can be used along with a CRM1T(/M) cage rotation mount to rotate the half-wave plate, thus aligning the polarization axis with the noise eater.

For post mounting, the noise eater is equipped with two 8-32 (M4) threaded holes. These holes are offset by 90° so that light with a vertical or horizontal polarization axis can be aligned with the noise eater. The four 4-40 holes on the front of the noise eater can also be used to mount the noise eater in either a horizontal or vertical orientation using the Thorlabs 30 mm Cage System.

For best performance of the noise eater, it is recommended that the beam be well centered within the input aperture. Due to the optical path inside the noise eater, the output beam will be shifted down by 1.0 mm if the noise eater is mounted vertically, as shown in the left view in the figure to the right. Similarly, the output beam will be shifted sideways by 1.0 mm if the noise eater is mounted horizontally, as shown in the right view in the figure to the right.

Noise Eater Feedback Detector Normalized Responsivity
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In the data plotted above, a sine wave with a 2.5 V amplitude and an increasing frequency was used to modulate a noiseless input beam.
Noise Eater SMA Modulation Input Jack
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SMA Modulation Input Jack

Modulation

There is an SMA interface at the right side of the noise eater, which can be used to modulate the attenuation of the noise eater. The modulation input has a 10 kΩ input impedance. A voltage ranging from 0 to 2.5 V can be input to modulate the output power from 0 to full output. Before modulating the output power, first turn the output power level knob clockwise to the end of its travel (minimum output power setting).

Noise Eater Feedback Detector Normalized Responsivity
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The dotted lines represent operating wavelength regions for each of the noise eaters.
Noise Eater Top View
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Top View Showing Power Range Adjustment Switches

Power Range Adjustment

The selection switch(es) at the top of the noise eater are used to select the input power range. The power selector should be set to the lowest value that is still higher than the actual power of the laser. For example, if the NEL01A(/M) is being used with a beam power of 8 mW at 635 nm, the selector should be set to position 3, which represents 10 mW. For specifications, refer to the Max Power tables below.

The NEL02A(/M), NEL03A(/M), and NEL04A(/M) noise eaters have two selection switches at the top of the case, which are used to select the input power range. When the low/high power switch is set to "LOW", the input power range can be set to one of the lower set of powers; when the status switch set to "HIGH", the input power range can be set to one of the higher set of powers. For specifics, refer to the Max Power tables below. Note that the NEL01A noise eater has only one selection switch.

The NEL01A(/M), NEL02A(/M), and NEL03A(/M) noise eaters use a silicon detector as part of the feedback loop, while the NEL04A noise eater uses a germanium detector. The responsivity of the detectors is different for different wavelengths, and so the power settings on the selector only correspond to the design wavelength of the detector [635 nm for Item #s NEL01A(/M) and NEL02A(/M), 780 nm for Item # NEL03A(/M), 1550 nm for Item # NEL04A(/M)]. The power range at a given wavelength is inversely proportional to the responsivity (a higher responsivity value will result in a lower power range value). The graph to the right shows the relative responsivity of both detectors at a range of wavelengths. The tables below show a rough estimate of the power settings at various wavelengths for each model.

The noise eater operates by varying how much of the signal is attenuated in order to reach the target output power and attenuate the noise. Since the noise eater can attenuate the signal but not amplify it, the clean output beam can only have a power as high as the minimum power level of the noisy signal. In practice, to remove all noise without unnecessarily attenuating the signal power, the output power level should be set to slightly lower than the minimum power of the noisy signal. See the manual for more information.

Max Powers at Various Wavelengths

The tables below list the maximum input powers for each noise eater, specified for a variety of input wavelengths and switch settings. Please note that these maximum power levels correspond to the feedback electronics of the noise eater, and in some cases, the actual maximum input power is instead limited by the damage threshold of the noise eater. For the high power noise eaters [Item #s NEL02A(/M), NEL03A(/M), and NEL04A(/M)], this damage threshold is 8 W/cm2, which corresponds to a maximum input power of 1 W if the input power is distributed evenly across the Ø4 mm clear aperture. For the low power NEL01A(/M) noise eater, the damage threshold is 0.8 W/cm2, which corresponds to a maximum input power of 100 mW if the input power is again distributed evenly across the Ø4 mm clear aperture.

NEL01A(/M) Max Power at Various Wavelengths
Switch
Position
Max Power
at 450 nm
Max Power
at 550 nm
Max Power
at 635 nm
1 mW 2 mW 1.5 mW 1 mW
3 mW 6 mW 4.5 mW 3 mW
10 mW 20 mW 15 mW 10 mW
30 mW 60 mW 45 mW 30 mW
NEL02A(/M) Max Power at Various Wavelengths
Switch
Position
Max Power
at 450 nm
Max Power
at 550 nm
Max Power
at 635 nm
L 1 2 mW 1.5 mW 1 mW
L 2 6 mW 4.5 mW 3 mW
L 3 20 mW 15 mW 10 mW
L 4 60 mW 45 mW 30 mW
H 1 200 mW 150 mW 100 mW
H 2 600 mWa 450 mW 300 mW
H 3 1000 mWa 750 mWa 500 mW
H 4 N/Ab
  • The maximum power levels specified here are for the feedback electronics, but the maximum input power at these settings is limited by the damage threshold of the liquid crystal retarder, which is 8 W/cm2. See the section "Max Powers at Various Wavelengths," above, for details.
  • This setting is not recommended. If used, do not exceed the power level for the H – 3 setting.
NEL03A(/M) Max Power at Various Wavelengths
Switch
Position
Max Power
at 650 nm
Max Power
at 700 nm
Max Power
at 780 nm
Max Power
at 900 nm
Max Power
at 1000 nm
Max Power
at 1100 nm
L 1 1.2 mW 1.1 mW 1 mW 0.9 mW 0.9 mW 3.3 mW
L 2 3.5 mW 3.3 mW 3 mW 2.6 mW 2.7 mW 10.0 mW
L 3 11.8 mW 11.1 mW 10 mW 8.8 mW 8.9 mW 33.3 mW
L 4 35.5 mW 33.3 mW 30 mW 26.3 mW 26.8 mW 100 mW
H 1 120 mW 111 mW 100 mW 86.0 mW 89.3 mW 333 mW
H 2 355.5 mW 333 mW 300 mW 258.0 mW 268 mW 999 mWa
H 3 600 mWa 500 mW 500 mW 430.0 mW 446.6 mW 1650 mWa
H 4 N/Ab
  • The maximum power levels specified here are for the feedback electronics, but the maximum input power at these settings is limited by the damage threshold of the liquid crystal retarder, which is 8 W/cm2. See the section "Max Powers at Various Wavelengths," above, for details.
  • This setting is not recommended. If used, do not exceed the power level for the H – 3 setting.
NEL04A(/M) Max Power at Various Wavelengths
Switch
Position
Max Power
at 1050 nm
Max Power
at 1150 nm
Max Power
at 1250 nm
Max Power
at 1350 nm
Max Power
at 1450 nm
Max Power
at 1550 nm
Max Power
at 1620 nm
L 1 1.9 mW 1.6 mW 1.4 mW 1.2 mW 1 mW 1 mW 1.6 mW
L 2 5.8 mW 4.8 mW 4.1 mW 3.5 mW 3.1 mW 3 mW 4.8 mW
L 3 19.2 mW 16 mW 13.7 mW 11.7 mW 10.4 mW 10 mW 16 mW
L 4 57.6 mW 48 mW 41.1 mW 35.1 mW 31.3 mW 30 mW 48 mW
H 1 190 mW 160 mW 137 mW 117 mW 104.7 mW 100 mW 160 mW
H 2 500 mW 480 mW 411 mW 351 mW 313.4 mW 300 mW 480 mW
H 3 835 mWa 800 mWa 685 mWa 585 mWa 520 mWa 500 mW 800 mWa
H 4 N/Ab
  • The maximum power levels specified here are for the feedback electronics, but the maximum input power at these settings is limited by the damage threshold of the liquid crystal retarder, which is 8 W/cm2. See the section "Max Powers at Various Wavelengths," above, for details.
  • This setting is not recommended. If used, do not exceed the power level for the H – 3 setting.

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EO Amplitude Modulators / Noise Eaters for 425 - 650 nm or 475 - 650 nm

  • NEL01A(/M) is a Low-Power Noise Eater (0.5 mW to 60 mW) with a Modulation Input and 425 - 650 nm Wavelength Range
  • NEL02A(/M) is a Switchable Low/High-Power Noise Eater (0.5 mW to 1000 mW) with a Modulation Input and 475 - 650 nm Wavelength Range
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Imperial Price Available
NEL01A Support Documentation
NEL01ANoise Eater / EO Modulator for 425 - 650 nm, 8-32 Taps
$1,882.90
3-5 Days
NEL02A Support Documentation
NEL02AHigh-Power Noise Eater / EO Modulator for 475 - 650 nm, 8-32 Taps
$2,442.33
3-5 Days
+1 Qty Docs Part Number - Metric Price Available
NEL01A/M Support Documentation
NEL01A/MNoise Eater / EO Modulator for 425 - 650 nm, M4 Taps
$1,882.90
3-5 Days
NEL02A/M Support Documentation
NEL02A/MHigh-Power Noise Eater / EO Modulator for 475 - 650 nm, M4 Taps
$2,442.33
3-5 Days
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EO Amplitude Modulator / Noise Eater for 650 - 1050 nm

  • NEL03A(/M) is a Switchable Low/High-Power Noise Eater (0.5 mW to 1650 mW) with a Modulation Input
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Imperial Price Available
NEL03A Support Documentation
NEL03AHigh-Power Noise Eater / EO Modulator for 650 - 1050 nm, 8-32 Taps
$2,442.33
3-5 Days
+1 Qty Docs Part Number - Metric Price Available
NEL03A/M Support Documentation
NEL03A/MHigh-Power Noise Eater / EO Modulator for 650 - 1050 nm, M4 Taps
$2,442.33
3-5 Days
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EO Amplitude Modulator / Noise Eater for 1050 - 1620 nm

  • NEL04A(/M) is a Switchable Low/High-Power Noise Eater (0.5 mW to 835 mW) with a Modulation Input
Based on your currency / country selection, your order will ship from Newton, New Jersey  
+1 Qty Docs Part Number - Imperial Price Available
NEL04A Support Documentation
NEL04AHigh-Power Noise Eater / EO Modulator for 1050 - 1620 nm, 8-32 Taps
$2,696.57
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NEL04A/M Support Documentation
NEL04A/MHigh-Power Noise Eater / EO Modulator for 1050 - 1620 nm, M4 Taps
$2,696.57
3-5 Days