Laser Speckle Reducer

Laser Speckle Reducer

Keywords: laser speckle reducers, speckle reducers, optotune,de-speckle
Aug 18, 2021 View: 6890 Data Sheet

Our laser speckle reducers are nothing other than moving diffusers. But the way they are actuated is absolutely unique. Two innovative tehttp://www.sintec.sg/sintec/images/button_ok.gifchnologies are offered, each with its own advantages.

STF Series Fiber De-Speckler

Our proprietary De-Speckler technology averages the modal noise within an optical fiber. This reduction in speckle is an ideal choice for fiber assemblies used in the Life Sciences, Digital Laser Projection, Interferometry, Laser Beam Homogenization, Lithography, and Metrology. For many fiber coupled applications, modal noise interferes with optimal performance. We have developed a small, simple and integrated de-speckling system which maximizes performance and reliability in illumination, with no optical loss.

de-speckler

Features and Benefits

Speckle is a random granular pattern commonly observed in the output beam of a laser. It is characterized by many dark and light spots of different intensities visible in a given cross section of the laser beam. This effect occurs as a result of interference between various propagation modes of the light.

The reduction of speckle is important for applications where a homogeneous laser output of uniform intensity is ideal, such as laser-scanning microscopy, flow cytometry, and DNA sequencing. By using the De-Speckler to average the modal noise and greatly reduce speckle, maximized performance can be achieved. Other benefits resulting from speckle reduction can include faster integration times, improved signal-to-noise ratios, and higher throughput.

Our speckle reduction solution has a small form factor and is in-line with a customizable fiber assembly. The fiber size, core shape, jacketing, connectors, and length can all be customized to perfectly suit your application. Please view the product specifications for more information.

This product is popularly paired with our square core fiber and RARe Motheye anti-reflection technology.

de-speckler de-speckler

Applications

  • Life sciences: bioanalytical instrumentation, flow cytometry, gene sequencing, microscopy, spectroscopy

  • Digital laser projection

  • Interferometry

  • Laser beam homogenizers

  • Lithography

  • Metrology

Specifications

  • Power supply: +5 Volts

  • Power consumption:  < 1 Watt

  • Wavelength range: 400nm – 1550nm

  • Fiber core size: 100μm – 400μm

  • De-speckling rate: up to 5000 Hz

Customization Options

  • Fiber types: all Silica optical fiber; plastic clad fiber; round or square core fiber; RARe Motheye available.

  • Jacket types: acrylate, nylon, polyimide, Tefzel

  • Assembly types: single fiber assemblies

  • Connector types: 905 SMA; 906 SMA; FC/PC; FC/UPC; FC/APC; ST/PC; ST/UPC; ST/APC; cleaved ends; polished ends; round 2.5mm ferrule; custom connectors

de-speckler

de-speckler  de-speckler

Reluctance Force-based Laser Speckle Reducer STOT-LSR-4C

LSR4C1.jpg

A way to reduce speckle noise from a laser-based system is by dynamically diffusing the laser beam. Our STOT-LSR-4C speckle reducer averages multiple speckle patterns by dynamically displacing a diffuser, and by doing so creates a more homogeneous, speckle-free beam. The STOT-LSR-4C has an aperture of 18.5x18.5 mm and is especially suitable for laser-based cinema projectors where high laser powers and large beam diameters are used. The diffusor is mounted in a metallic frame and is set into motion by the reluctance force generated in the oscillating magnetic field of a driving coil.

If required, STOT-LSR-4C can combine two oscillating diffusors rotated by 90°, realizing optimized despeckling in both directions. The compact driving electronics, assembled on a flexible plastic substrate, stabilizes the resonance Frequency in closed-loop mode and includes an error signal.

Mechanical specifications

Clear aperture

18.5 x 18.5

mm

External dimensions

35.2 x 37.9 x 5.8

mm

Housing diameter

30.0

mm

Height

14.5

mm

Weight

Full device: 11.0 

Diffuser: 0.29

g

Mechanical clamping

2x M2 screws


Minimal weight of anchor mass

500

g

Performance specifications

Oscillation amplitude (peak to peak)

Min: 0.6

Typical:   0.8

Max: 2.0

mm

Oscillation frequency

120 ± 10

Hz

Device start-up time (typical)

20

s

Optical specifications

Material

Fused silica


Diffusion angle (FWHM)

8.5 (up to 20 on request)

°

Transmission wavelength

VIS coated: 440-660

Uncoated: approx. 200-2200

nm

Transmission

VIS coated: >98

Uncoated: >94

%

Depolarization

< 0.1

%

Coating

High power, double-sided


Damage threshold

> 600

W/cm2

Scratch/dig

60/40

Over full clear aperture of diffuser

Electrical specifications

Power supply (micro-USB or solder pads)¹

3.4-5

VDC

Power consumption (with std. electronics

50 mW

mW

Environmental specifications

Operating temperature at fixed startup temperature Ts²

Ts-5 to Ts+55

°C

Storage temperature

-40 to +85

°C

Start-up temperature

-30 to +85

°C

Mechanical shock

500

g

Cycle life

>40 000

hours

Overview of available standard products

Standard Product

Coating

Diffusion angle

STOT-LSR-4C-L-18x18-9-T2-VIS

VIS-coated

8.5°

STOT-LSR-4C-L-18x18-9-T2-NOC

uncoated

8.5°

Accessories

Description

Bracket kit STOT-LSR-4

Bracket for single and double diffusor configuration

STOT-LSR-4C-LL-mounting kit

Mounting kit for double diffusor configuration

PS-5V-US

5V DC micro-USB power supply with US plug

PS-5V-EU

5V DC micro-USB power supply with EU plug

Assemblies

Components to order

STOT-LSR-4C-L (no bracket)

1x STOT-LSR-4C, 1x Power supply

STOT-LSR-4C-L (with bracket)

1x STOT-LSR-4C, 1x Bracket-kit LSR-4, 1x Power supply

STOT-LSR-4C-LL (double diffusor configuration with bracket)

2x STOT-LSR-4C, 1x Bracket-kit LSR-4,

1x STOT-LSR-4C-LL-mounting kit, 2x Power supply

Control

The STOT-LSR-4C is driven using a 5V DC power supply. No further driver electronics are needed; the device settles into its optimal trajectory once powered on.

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