High-Speed Optical Shutter/Switch

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Specifications^a
Item #	SOA1013SXS	BOA1004PXS
Operating Wavelength	1528 - 1562 nm	1500 - 1600 nm
Optical Isolation (P_IN / P_OUT)^b	≥42 dB	≥40 dB
Extinction Ratio^c	60 dB	70 dB
Switching Speed	1 ns	1 ns
Max Output Power for CW Input Signal	17 dBm	18 dBm
Max Output Power for Modulated Input Signal	9 dBm	10 dBm

Typical values. For complete specifications, please see Specs tab.
At 0 mA and 1550 nm
At P_IN = -20 dBm and 1550 nm

Features

High Switching Speed of <1 ns
FC/APC Connectors with Key Aligned to Slow Axis on BOA1004PXS
Typical Applications Include LIDAR Systems, Remote Sensing Systems, and Cavity Ring-Down Sensors
Case Temperature Control via Internal Thermoelectric Cooler (TEC) Element

The SOA1013SXS and BOA1004PXS Optical Switches are designed specifically for applications requiring an optical shutter with operation around 1550 nm. Both the polarization-independent SOA1013SXS and the polarization-dependent BOA1004PXS provide an extinction ratio greater than 60 dB. The devices are based on our semiconductor amplifier platform consisting of a highly efficient InP/InGaAsP Multiple Quantum Well (MQW) layer structures grown on an InP wafer and processed into a proven and reliable ridge waveguide. The device can operate as a lossless, high-speed, optical isolation switch, a full-range variable optical attenuator (VOA), or an optical shutter for protection of delicate optical equipment.

The SOA1013SXS polarization-independent switch features the right combination of low polarization sensitivity, wide optical bandwidth, and high extinction ratio for an optical isolation switch. Using the gain/absorption properties of the MQW structure, the device can function as an optical blocking shutter with no reflections. In addition, the switch is also designed to support the highest gain and signal levels, allowing it to function reliably at signal levels of 15 dBm and above. The SOA1013SXS is also ideal for applications where the input signal polarization is unknown or fluctuates. The device comes in an industry-standard 14-pin butterfly package with single mode fiber (SMF) pigtails that are terminated with FC/APC connectors.

The BOA1004PXS polarization-dependent switch offers the user full control of the power level making it ideal for high-power laser pulse generation systems like cavity ring-down sensors and LIDAR systems. The device comes in an industry-standard 14-pin butterfly package with polarization-maintaining fiber (PMF) pigtails that are terminated with FC/APC connectors and key aligned to the slow axis. The BOAs can be customized upon request to have isolators on the input, output, or both. Please contact Tech Support for help customizing a device for your application.

Driver Option
The CLD1015 Compact Controller with Mount can be used to drive these optical switches, however, this controller will only be able to achieve switching speeds of around 4 µs. For information on compatible drivers that can achieve switching times up to the specified 1 ns time scale, please contact Tech Support.

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Item	SOA1013SXS			BOA1004PXS
Parameter	Min	Typical	Max	Min	Typical	Max
Operating Current	-	500 mA	600 mA	-	600 mA	750 mA
Operating Wavelength	1528 nm	-	1562 nm	1500 nm	-	1600 nm
Optical Isolation (P_IN/P_OUT) @ 0 mA and 1550 nm	42 dB	-	-	40 dB	-	-
Extinction Ratio (On/Off @ P_IN = -20 dBm and 1550 nm)	-	60 dB	-	-	70 dB	-
Switching Speed	-	1 ns	-	-	1 ns	-
Max Output Power for CW Input Signal	-	17 dBm	-	-	18 dBm	-
Max Output Power for Modulated Input Signal	-	9 dBm	-	-	10 dBm	-
Saturation Output Power (@ -3 dB)	12 dBm	14 dBm	-	13 dBm	15 dBm	-
Noise Figure	-	8.0 dB	9.5 dB	-	8.0 dB	9.5 dB
Small Signal Gain Across BW (@ P_IN = -20 dBm)	10 dB	13 dB	-	22 dB	25 dB	-
Polarization Dependent Gain	-	1 dB	1.8 dB	-	-	-
Forward Voltage	-	1.6 V	1.8 V	-	1.6 V	1.8 V
Thermoelectric Cooler (TEC) Current^a	-	0.23 A	1.5 A	-	0.23 A	1.5 A
Thermoelectric Cooler (TEC) Voltage^a	-	0.5 V	4 V	-	0.5 V	4 V
Thermistor Resistance^a,b	-	10 kΩ	-	-	10 kΩ	-
Chip Length	-	1.5 mm	-	-	1.5 mm	-
Waveguide Refractive Index	-	3.2	-	-	3.2	-
Fiber Type	SMF-28-J9 (Single Mode Fiber)			PMF-1550 (Polarization-Maintaining Fiber)
Fiber Length	1.5 ± 0.1 m			1.5 ± 0.1 m
Fiber Connector	FC/APC			FC/APC, Key Aligned to Slow Axis

TEC Operation (Typ/Max @ TCASE = 25/70 °C)
See the plot to the right for the relation between the thermistor temperature and resistance.

This is plotted using the Steinhart-Hart equation,

, where A = 1.129241 x 10^-3, B = 2.341077 x 10^-4, and C = 8.775468 x 10^-8.

SOA1013SXS Charts

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BOA1004PXS Charts

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Posted Comments:

Jeffrey Lee (posted 2019-05-08 14:45:32.847)

I just wanted to let you know that if these could be made to work at 780nm (and other common wavelengths for atomic physics), I and a lot of my colleagues would be very very interested in them.

YLohia (posted 2019-05-08 02:56:30.0)

Hello, thank you for contacting Thorlabs. I have reached out to you directly to discuss the possibility of offering this.

marco.brunero (posted 2018-11-12 10:09:14.437)

Dear Mr/Mrs, is it possible to directly modulating the SOA1013SXS with electrical pulses of 10 ns and repetition rate of 20 us? If the input CW signal will have a power of few milliwatts, what will be the maximum peak power of the output pulses? Thank you, Marco Brunero.

YLohia (posted 2018-11-12 08:56:14.0)

Hello Marco, thank you for contacting Thorlabs. It is possible to directly modulate this SOA with such pulses, provided that the proper drive electronics are utilized. The output power depends on the wavelength, peak current, and input power. I will reach out to you directly to discuss this further.

hnguyen43 (posted 2018-05-07 08:13:50.987)

Would this product work for the wavelength 1130 nm range? If not, can I get a customized one for that wavelength?

YLohia (posted 2018-05-07 11:37:37.0)

Hello, thank you for contacting Thorlabs. I will reach out to you directly regarding the possibility of offering this.

marian.kreyer (posted 2017-10-04 10:52:29.123)

We would like to use this product as a shutter in an automatic power loss protection for our fiber amplifier. Can you tell me a bit more about the properties of the input signal? Do i need the TEC element when i operate it as a shutter? What is the expected delay of the shutter? Thanks in advance!

tfrisch (posted 2017-12-06 01:15:36.0)

Hello, thank you for contacting Thorlabs. The internal TEC should be used, yes. The switching speed is 1ns, but if you want to use this as a shutter failsafe, the control electronics would likely be the limiting factor of the speed. For example CLD1015 would achieve only 4us. We will reach out to you directly to discuss the details your application and the input signal.

brad.m.gibson (posted 2016-12-14 17:35:47.78)

Would it be possible to get a unit centered near 1391 nm?

tfrisch (posted 2016-12-19 04:07:46.0)

Hello, thank you for contacting Thorlabs. I will reach out to you directly on the availability of a 1391nm version.

felix.schmieder (posted 2016-12-07 17:39:16.043)

Like one of the previous posters I find this is a very interesting product. However, an operation at 532nm would be crucial to my application.

tfrisch (posted 2016-12-15 09:53:40.0)

Hello, thank you for contacting Thorlabs. I will reach out to you directly about this.

cong_du (posted 2015-10-16 15:03:39.55)

I will purchase your High-Speed Optical Shutter/Switch BOA1004PXS or SOA1013SXS Do you provide optical switch driver with above switch so I can set up the time and speed/frequence of off-on switch freely ？

besembeson (posted 2015-10-27 05:25:49.0)

Response from Bweh at Thorlabs USA: For low speed modulation (up to couple of hundred kHz), you can use our CLD1015. We don't have suitable driver at this time for high-speed switching. I will follow-up with some possible external suggestions.

dangerous46 (posted 2015-02-18 18:25:26.64)

Is this product capable of acting as a high extinction ratio modulator? The application I am interested in will cycle on/off up to a rate of 100 MHz.

jlow (posted 2015-02-25 03:15:03.0)

Response from Jeremy at Thorlabs: You can use this to switch on/off an optical signal quickly. I will contact you directly to discuss more about your application.

user (posted 2014-03-29 09:41:21.71)

This looks like a very nice product. Like the other commenters in the feedback section, I would also be interested in seeing a similar device with such fast switching times, but at a different wavelength, 532nm.

jlow (posted 2014-03-31 04:31:58.0)

Response from Jeremy at Thorlabs: Thank you for providing your feedback regarding this. I have added this additional request in our internal forum and we will look into this possibility.

biver (posted 2012-12-04 08:21:12.973)

Hello, I would like to know if the same device is available for UV wavelength! I am working with a fast UV pulsed laser (wavelength: 343nm; repetition rate: 200kHz-2MHz; beam size: ~3mm) and want to be able to discriminate between pulses. The idea is to have a sequence of 3 pulses, the first acting as a trigger to open a shutter and let the 2 following pulses pass (the first pulse triggers also an imaging system to visualize the impact of the 2 pulses on a given substrate). Mechanical shutters seem to be too slow for this application, and I am considering using an optical shutter, a Pockels cell or an acousto-optic modulator. Thank you in advance, Emeric Biver

tcohen (posted 2012-07-03 10:56:00.0)

Response from Tim at Thorlabs: The semiconductor optical amplifiers (SOAs/BOAs) that we currently provide are all single-mode devices. The optical amplifier semiconductor chip itself is a single-mode waveguide device. So, the input optical coupling efficiency to a multi-mode fiber would be very poor. We could make a multi-mode semiconductor optical amplifier chip and couple it to large-core, multi-mode fiber. This would work, however, multi-mode optical amplifiers have a higher noise figure than single-mode amplifiers (the noise figure is directly proportional to the number of modes). The noise figure may or may not be important depending on the application.

roger.pilkington (posted 2012-07-01 04:32:23.0)

Can this be done for larger fibers as well. Such as a 200um core?

bdada (posted 2011-03-04 18:46:00.0)

Response from Buki: The semiconductor optical amplifier operates as a classic intensity amplifier, with a minimum theoretical noise figure of 3 dB. The statistics of the coherent stimulation process as well as the presence of spontaneous emission at the signal wavelength would make it impossible to be used with a single-photon input. A phase sensitive, parametric amplifier, which does not have spontaneous emission at the signal wavelength and can have 0 dB noise figure would be more appropriate for single photon. In terms of wavelength range, our existing product lines covers from 1 um to 2 um. We are working on expanding to wavelengths shorter than 1 um. We will contact you directly to learn more about your wavelength needs.

till.weinhold (posted 2011-03-03 23:05:09.0)

Two questions regarding the SOA1013SXS unit. Can it be operated with gated single photon inputs or does it require a minimum input power. What is the loss through the system? And any view to expanding the wavelength range? Cheers Till

Adam (posted 2010-05-13 10:32:33.0)

A response from Adam at Thorlabs to Pascal: At this time, we do not work with the material system that would allow us to make a custom semiconductor optical amplifier at 670nm. Therefore, we cannot produce custom versions at this time. I will make a suggestion to our engineers for this customer inspired new product idea. I will contact you directly to find out your exact application.

pascal.deladurantaye (posted 2010-05-13 08:54:02.0)

Could you provide a custom version that would work at 670 nm?

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High-Speed Optical Shutter/Switch

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SOA1013SXS Charts

BOA1004PXS Charts