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LASER SYSTEMS AND SPECTRAL DEVICES Spectral optimized output We have developed for our Ti:Sapphire lasers a specific cavity with Q-factor matched to spectral gain curve of the active medium. It allows to obtain the utmost wide tuning range and the maximum output for each wavelength. Excellent beam quality Innovative cavity design provides high efficient output with a smooth Gaussian beam profile and ~1mrad divergence in the whole spectral range. High quality of tunable radiation makes our Ti:Sapphire lasers an optimal choice for experiments in non-liner optics and other fields. High reliability Conventional Ti:Sapphire lasers typically operate at high pump intensities close to the damage threshold of their optical components. is results in low reliability of such systems. e Ti:Sapphire lasers developed by SOLAR LS avoid this problem by providing specified output at pump intensities that are much lower than damage threshold for optical components. is leads to high reliability and longer lifetime for key optics utilized in the laser. Harmonic Generators options SOLAR LS Ti:Sapphire lasers have built-in high-efficient SHG. A compensator in the SHG allows to avoid spatial shiſt of the second harmonic beam while changing the wavelength. e fundamental and second harmonic are separated with high spectral purity by means of broadband dichronic mirrors. e lasers have possibilities for both separate and simultaneous fundamental and second harmonic output. THG and FHG units offered by SOLAR LS together with Ti:Sapphire lasers provide high-efficient tunable output within the range from 209nm to 330nm. PC Control option Upon your request all the Ti:Sapphire lasers may be computer controlled. The tunable Ti:Sapphire lasers manufactured by SOLAR LS are the devices integrating more than 15-year experience of SOLAR LS’s engineers and researchers in the field of solid-state tunable lasers. Our Ti:Sapphire lasers offer the user a unique combination of reliable and friendly design with high-quality and high-power output. Compatibility with pump lasers SOLAR LS advanced design solves a typical problem related to compatibility of Ti:Sapphire lasers to a pump source. Either single-mode or multimode Nd:YAG lasers with SHG with the output energy from several mJ till 1J can be used as a pump laser. Easy-to-use and friendly in operation e lasers installation does not take much time. Due to the rigid design, the laser retains the factory alignment even aſter ling transportation. All you need is just to steer properly the pumping beam into the laser and be sure that pump energy is within the specified range.

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LASER SYSTEMS AND SPECTRAL DEVICES

Spectral optimized outputWe have developed for our Ti:Sapphire lasers a specific cavity with Q-factor matched tospectral gain curve of the active medium. It allows to obtain the utmost wide tuning range and the maximum output for each wavelength.

Excellent beam qualityInnovative cavity design provides high efficient output with a smooth Gaussianbeam profile and ~1mrad divergence in thewhole spectral range. High quality of tunable radiation makes our Ti:Sapphire lasers an optimal choice for experiments in non-liner optics and other fields.

High reliabilityConventional Ti:Sapphire lasers typically operate at high pump intensities close to the damage threshold of their optical components. This results in low reliabilityof such systems. The Ti:Sapphire lasersdeveloped by SOLAR LS avoid this problem by providing specified output at pumpintensities that are much lower than damage threshold for optical components. This leadsto high reliability and longer lifetime for key optics utilized in the laser.

Harmonic Generators optionsSOLAR LS Ti:Sapphire lasers have built-in high-efficient SHG. A compensator in theSHG allows to avoid spatial shift of thesecond harmonic beam while changing the wavelength. The fundamental and secondharmonic are separated with high spectral purity by means of broadband dichronic mirrors. The lasers have possibilities for bothseparate and simultaneous fundamental and second harmonic output.THG and FHG units offered by SOLAR LStogether with Ti:Sapphire lasers provide high-efficient tunable output within therange from 209nm to 330nm.

PC Control optionUpon your request all the Ti:Sapphire lasers may be computer controlled.

The tunable Ti:Sapphire lasers manufactured by SOLAR LS are the devices integrating more than 15-year experience of SOLAR LS’s engineers and researchers in the field of solid-statetunable lasers.Our Ti:Sapphire lasers offer the usera unique combination of reliable and friendly design with high-quality and high-power output.

Compatibility with pump lasersSOLAR LS advanced design solves a typical problem related to compatibility of Ti:Sapphire lasers to a pump source.Either single-mode or multimode Nd:YAG lasers with SHG with the output energy from several mJ till 1J can be used as a pump laser.

Easy-to-use and friendly in operationThe lasers installation does not take muchtime. Due to the rigid design, the laser retains the factory alignment even afterling transportation. All you need is just to steer properly the pumping beam into the laser and be sure that pump energy is within the specified range.

SOLAR Laser Systems ▪ 4 Stebenev lane, Minsk 220024 ▪ BELARUS ▪ fax: 375(17)2019596 ▪ phone: 375(17)2019590 ▪ e-mail: [email protected] ▪ www.solarlaser.com

High Output Versions

Maximum output and extremely wide tuning range of the Ti:Sapphire laser are the key points for most of users. SOLAR LS offers the models providing the output ofmore than 150mJ and the tuning range from 690nm to 1000nm at fundamental for such applications. The conversion efficiency of pump radiation to the tunable output for these models exceeds 25…30%.

Narrow Linewidth Versions

For many applications wide tuning range and efficiencyare not so important as narrow linewidth. In these cases SOLAR LS offers Ti:Sapphire lasers which providespectral linewidth at 10pm level with acceptable efficiency and tuning range.

High Pulse Repetition Rate Versions

SOLAR LS offers a laser optimized for efficientoperation at high repetition rate from 1 to 20kHz. Upon your request a fiber output option is available.Such configuration provides additional advantageswhile using the laser in medicine and photobiology.

Custom Laser System

While developing custom systems, SOLAR LS’s specialists take into consideration specific requirementsof the customers and provide users with optimal cost and time effective solutions of the challenges they face.

Please visit our website www.solarlaser.com or contact us to get more detailed information and specifications.

LASER SYSTEMS AND SPECTRAL DEVICES

Laser tattoo removal and pigmented lesion treatment are non-invasive procedures that completely remove skin defects leaving one’s skin looking scarless and, most importantly, spotless.

In the past, tattoos were removed through methods such as dermabrasion, salabrasion, cryosurgery, or acid injections. All of these approaches left either seriousscarring on the skin or unpigmented, “blotchy” areas where tattoo used to be.

Lasers for tattoo removal eliminate these unfortunate side effects. The Q-switchedNd:YAG laser is the newest system in this class of lasers. The laser system offered bySOLAR LS can treat everything from very small tattoos to large multicolored tattoos and pigmented lesions. This feature isprovided due to the possibility of choosing the optimal laser radiation wavelength and the spot size during treatment.

The laser system provides high poweroutput at special selected wavelengths, which pass through the skin but absorbed by ink or pigment. The rapid selectiveabsorption of light energy by ink or pigment causes their fragmenting into thousands of tiny particles, where they are then removed by the body’s natural filteringsystems.

The use of optimized wavelengths, pulsewidth, variable fluencies and spot sizesresults in tattoo removal and pigmented lesion treatment without any skin damage.

The handpiece has a unique spot-size sensorwhich provides automatic measuring of fluence whenever the spot-size is changed

The colour touch-screen display allows easyselection of optimal wavelength and other treatment parameters

Multilingual interface menu

Superior articulated arm to enhance treatment procedure

Compact, mobile, quiet

Single-phase electrical main, no external water requirements

Laser Type Q-switched Frequency Doubled Nd:YAG Laser

Laser Wavelength 1064 nm 532 nm

Maximum Energy delivered to tissue 400 mJ 200 mJ

Pulse width 7 nsec 6 nsec

Fluence 0.4 to13 J/cm2 0.2 to 7 J/cm2

Spot Size 2 to 6 mm

Repetition Rate Single shot, 1, 2, 5, 10 Hz

Beam Delivery System Articulated arm

Aiming Beam Red laser diode (630…675 nm)

Control Panel 8.4’’ colour touch screen

Cooling Self contained, water-to-air

Dimension (without arm) 35 cm (W) x 70 cm (D) x 90 cm (H)

Electrical Main 100 V or 120 V +/- 10%; </= 12 A 220 V or 240 V +/- 10%; </= 9 A

Ambient 12…27°C

Chromophore black blue green red orange pigment

Q-Sw Nd:YAG (1064 nm) OK OK OK OK

Frequency Doubled Nd:YAG (532 nm) OK OK OK

SOLAR Laser Systems ▪ 4 Stebenev lane, Minsk 220024 ▪ BELARUS ▪ fax: 375(17)2019596 ▪ phone: 375(17)2019590 ▪ e-mail: [email protected] ▪ www.solarlaser.com

SPECIFICATIONSSpecifications are subject to change without notice

The laser provides two proven Q-switched wavelengths for the most effective treatment ofpigmented lesions and all colours of tattoos.

SOLAR Laser Systems also offers other aesthetic laser systems:

Multifunctional Nd:YAG Laser Systems for aesthetics Ruby laser for treatment of pigmented lesions CW Nd:YAG laser for surgery Alexandrite aesthetic laser system

CW Nd:YAG laser for surgery

Ruby laser for treatment of pigmented lesions

Multifunctional Nd:YAG Laser Systems for aesthetics

LASER SYSTEMS AND SPECTRAL DEVICES

The DeLight laser - offers to customersunprecedented multifunctionality and enables medical personnel to perform three most popular types of treatment in laser cosmetology: hair removal, vascular lesion treatment, noninvasive skin rejuvenation and toning.

This advantage of the device is provided bya plenty of tunable parameters of laser radiation and extremely wide range of their variation. To switch from one treatment to another and, accordingly, to change the laser operation mode fundamentally physician just needs to attach one of three smart handpieces, which is appropriate to the treatment chosen.

Hair removalUnlike radiation of other types of hair removal laser and lamp epilators, the DeLight operates at 1064nm and can be used for treatment of patients with skin of any type according to Fitzpatrick’s classification and any depth offollicles’ bedding and its use has no limitations imposed by racial peculiarities.

Vascular lesion treatmentDeLight ensures successful treatment, practically painless and harmless for skin, of undesirable vascular formations not only in the facial area but also for rather large veins up to 5 mm in diameter on legs.

Noninvasive skin rejuvenationThe optimum matching of pulse duration andpower parameters of DeLight with a thermal relaxation time of microvessels allows to achive effective smoothing of the most diverse types ofskin due to a growth and tightening of collagen. Smoothing of small and moderately large wrinkles is accompanied by significant improvement ofskin’s tone and texture that increases considerably cosmetologic effect of treatment. The operationdoes not require anesthesia and skin cooling, moreover patient needs no special subsequent care and recovery time.

Easy to use

Large area treatment

Skin cooling option

Small foot print design

No external water, single phase mains operation

Low maintenance

SOLAR Laser Systems ▪ 4 Stebenev lane, Minsk 220024 ▪ BELARUS ▪ fax: 375(17)2019596 ▪ phone: 375(17)2019590 ▪ e-mail: [email protected] ▪ www.solarlaser.com

Laser type Variable pulse width Nd:YAG laser

Wavelength, nm 1064

Max output energy, J 80

Application Hair removal Vascular lesion treatment Skin rejuvenation

Pulse width, msec 7…50 7…50 0.3

Max fluence, J/cm2 100 300 18

Spot size, mm 7, 10, 13 5 5

Repetition rate single shot, 0.5 to 2 Hz

single shot, 0.5 to 2 Hz

single shot, 1 to 10 Hz

Beam delivery system ∅800μm x 2.5m optical fiber

Aiming beam red laser diode

Control panelLCD screen, touch panel;

fluence, pulse width, spot size, repetition rate set up;real time output monitoring

Calibration internal calibration port

AccessoriesPeltier skin cooler;

air skin cooler; integrated with handpiece Peltier or air skin cooler

Cooling self-contained water-air cooling system

Environmental conditions (15…27)°C ambient temperature

Dimensions (H x W x D), mm 775 x 330 x 650

Power requirements 220V ±10%, single phase, 50/60 Hz, < 9A

Weight, kg 70

SPECIFICATIONSSpecifications are subject to change without notice

SOLAR Laser Systems also offers other aesthetic laser systems:

Ruby laser for treatment of pigmented lesions CW Nd:YAG laser for surgery Nd:YAG Tatoo Removal Laser System Alexandrite aesthetic laser system

Nd:YAG Tatoo Removal Laser System

CW Nd:YAG laser for surgery

Ruby laser for treatment of pigmented lesions

RUBY LASER SYSTEM FOR AESTHETICSModel R15

SPECIFICATIONS

Laser type Ruby laserApplication Pigmented lesion treatmentWavelength, nm 694Pulse width, μsec 450Max output energy, J 6Spot size, mm 5Max fluence, J/cm2 30Repetition rate single shot; 1HzBeam delivery system ∅1mm x 2.5m optical fiberAiming beam red laser diode

Control panelLCD screen, touch panel;

fluence, repetition rate set up;real time output monitoring

Calibration internal calibration port

AccessoriesPeltier skin cooler;

air skin cooler; integrated with handpiece Peltier or air skin cooler

Cooling chillerEnvironmental conditions (15…27)°C ambient temperatureDimensions (H x W x D), mm 1000 x 510 x 630

Power requirements 220V ±10%, single phase, 50/60 Hz, ≤ 7A100V ±10%, single phase, 50/60 Hz, ≤15A

Weight, kg 115

Specifications are subject to change without notice

Ruby laser beam is an optimal choice for treatment of pigmented lesion originating in melanin. The reason is that ruby laser beam undergoes minimal absorption in collagen and so it influences melanin selectively leaving all other tissues intact.

Applications:

Nevus Cell Nevus

Spilus Nevus

Becker’s Nevus

Senide Pigmented Freckle

Freckles

Seborrheic Keratosis

Lentigo

SOLAR Laser Systems • 4 Stebenev lane., Minsk 220024 • BELARUSfax: 375 17 2019596 • phone: 375 17 2019590 • E-mail: [email protected] • www.solarlaser.com

ISO 9001 Certified

Laser type CW Nd:YAG laser

Output modes continuous / repeated pulses / single pulse

Output power (CW mode), W 1…100

Output power stability, % ± 5

Repeated pulse mode, sec pulse width: 0.02…60interval: 0.02…10

Beam delivery gas cooled optical fiber, SMA905 connector

Aiming beam red laser diode

Control panel

8 programs;monitoring of output power, pulse duration, repetition interval;

indication of cumulative energy, applied to tissue;error monitoring

Power consumption,(single phase, 220V ± 10%, 50/60Hz), kVA

≤ 4

Cooling self-contained water-air cooling system

Environmental conditions (15…27)°C ambient

Dimensions, mm 920 x 495 x 620

Weight, kg 76

* Specifications are subject to change without notice.

Nd:YAG LASER FOR SURGERY Model J100

Applications:

Urology

Gynecology

General Surgery

Dermatology

Plastic Surgery

Gastroenterology

Pulmonary

Laser application in surgery allows not only to perform unique and delicate operations with minimal traumatism of tissue, but also ensures effective coagulation.

• The J100 laser delivers the power you need for a variety of surgical procedures with the precision you wish for the optimal tissue effect. It is the system that can operate either in continuous wave or various pulse modes at your choice. Pulse mode provides protection from tissue overheating and extends optical fiber lifetime.

• Ergonomical control panel design provides easy and comfortable laser operation.

• The doctor can store his own treatment parameters by means of up to 8 settings for different applications.

• For your applications the laser provides up to 100W continuous power and does not require either city water for cooling or any other special conditions. You only have to connect it to the single-phase electrical main.

SOLAR Laser Systems • 4 Stebenev lane., Minsk 220024 • BELARUSfax: 375 17 2019596 • phone: 375 17 2019590 • E-mail: [email protected] • www.solarlaser.com

ISO 9001 Certified

SPECIFICATIONSSpecifications are subject to change without notice

RAMAN SHIFTERModel LZ221

SPECIFICATIONS*

Pump laser type Pump wavelength, nm Active medium**Output wavelength, nm

1st Stokes 2nd Stokes 3rd Stokes

Nd:YAG

532

1

2

3

555559563

579588599

606621639

1064

1

2

3

115911771197

127213171369

140914941598

1318

1

2

3

146614961529

165217291820

———

Ruby 694

1

2

3

733740748

777793812

826854887

Ti:Sapphire 750…950

1

2

3

796…1025804…1039814…1055

848…1112867…1146890…1186

907…1216941…1279981…1354

Forsterite 1200…1300

1

2

3

1322…14441346…14731372…1505

1471…16241531…16981603…1786

———

Dimensions — (323 x 91 x 65) mm* Specifications are subject to change without notice.** 1 – KGdWO4 crystal, shift 767.3 cm-1

2 – KGdWO4 crystal, shift 901.5 cm-1

3 – Ba(NO3)2 crystal, shift 1047 cm-1

SOLAR Laser Systems • 4 Stebenev line., Minsk 220024 • BELARUSfax: 375 17 2019596 • phone: 375 17 2019590 • E-mail: [email protected] • www.solarlaser.com

The Solid State Raman Shifter LZ series uses innovative technology Ba(NO3)2 and KGdWO4 crystals. Unique crystal properties and optimal cavity design allow to obtain Raman frequency conversion with more than 50% efficiency.

Unlike gas Raman Shifters using high pressure cells, the LZ221 is characterized by complete safety in operation and low operating densities of pump radiation, what leads to additional advantages and facilitates the operation.

LP Series, pulsed DPSS lasers Low repetition rate, high energy

Specification examples: Please inquire for other variations Third harmonic systems also available

Elforlight Ltd, 65 Byfield Rd, Woodford Halse, Northants NN11 3QR, UK Tel 01327 263994, Fax 01327 263973, e-mail info @ elforlight.com www.elforlight.com

Model LP-5-10-532 Wavelength 532nm Pulse energy >5mJ per pulse Repetition rate Up to 20Hz Pulse width <20ns FWHM (typically 10-15ns) Mode Low order multimode, approx. top hat profile Beam diameter <4mm Divergence <3mRad Polarisation 100:1 Head size 400 x 135 x 70 mm PSU size 3U high 19 rack Power requirement 110 to 240VAC, 50/60 Hz, 300 Watts max.

LP Series, pulsed DPSS lasers Low repetition rate, high energy

Elforlight Ltd 4B Brunel Close DAVENTRY Northants NN11 5RB UK Tel +44 1327 300069 Fax +44 1327 300076 e-mail [email protected] www.elforlight.com

Model LP-10-10-1064 Wavelength 1064nm Pulse energy 10mJ Pulse width 8-12ns Repetition rate 10Hz Mode Low order multimode, approx. top hat profile Beam diameter <4mm Divergence < 6mRad Polarisation 100:1 Head size 335 x 100 x 60 mm PSU size 3U high 19 rack Power requirement 110 to 240VAC, 50/60 Hz, <400 Watts

Short Pulse Optical Technology

Elforlight SPOT lasers provide a source of short optical pulses at infrared and green wavelengths. IR pulses are specified at <2ns (typically 1.5ns) and green pulses at < 1.5ns (typically 1ns) at repetition rates up to 20kHz.

Standard products offer IR energies of 10 J (200mW average power at 20 kHz) and green average powers of 80mW. Other specifications to special order - please enquire.

The short pulses are created by a combination of short cavity lengths and a novel fast electro-optic q-switching technique. Repetition rate is continuously variable from single shot to >40KHz.

Applications include micromachining, ranging, nonlinear optics, plasma generation and for seeding laser amplifiers. In short SPOT is suitable for any application where short pulses or high peak powers are important.

Model SPOT 100-1064

SPOT 20-532

Maximum pulse energy 10 J 4 J

Minimum pulse width 2ns <2ns Repetition rate single shot to >40kHz Mode TEM00, M

2<1.2 Beam diameter (at waist) ~100 m Pulse to pulse stability (1 sec) <5% RMS <5% RMS

Laser head size 120x65x40mm 140mm x 65mm x 40 mm

Controller size 220mm wide x 300mm deep x 130mm high Cooling Air cooled PSU, conduction through base of laser head (20W) Power requirement 100 - 240 VAC, 50 / 60 Hz Universal input <100 Watts Frequency control TTL trigger input required at up to 40kHz

Elforlight Ltd, 65 Byfield Rd, Woodford Halse, Northants NN11 3QR, UK Tel +44 1327 263994, Fax +441327 263973, e-mail info @ elforlight.com www.elforlight.com

Short Pulse Optical Technology

Elforlight SPOT lasers, previously only available at 1064nm and 532nm, now has a UV version, at 355nm. SPOT-UV produces pulses at <1.5ns (typically 1ns) at repetition rates from single shot up to 10kHz.

The short pulses are created by a combination of short cavity lengths and a novel fast electro-optic q-switching technique.

The laser output may be single wavelength, by utilizing a blocking filter for 1064 and 532nm, or can be supplied with simultaneous outputs at 1064, 532 and 355nm

Applications include laser induced fluorescence, time resolved fluorescence, micromachining, biotechnology, plasma generation and remote sensing.

Model SPOT 10-1-355

Maximum pulse energy 1 J

Minimum pulse width <1.5ns Repetition rate single shot to >10kHz Mode TEM00, M

2<1.2 Beam diameter (at waist) ~100 m Pulse to pulse stability (1 sec) <5% RMS

Laser head size 233mm x 121mm x 81 mm

Controller size 250mm wide x 250mm deep x 90mm high (includes 40mm heatsink) Cooling Air cooled PSU, conduction through base of laser head (20W) Power requirement 100 - 240 VAC, 50 / 60 Hz Universal input <100 Watts Frequency control TTL trigger input required at up to 20kHz

Elforlight Ltd, 4b Brunel Close, Daventry, Northants NN11 5RB, UK

Tel +44 1327 300069, Fax +44 1327 300076, e-mail [email protected]

Product Note PolarOnyx

PolarOnyx, Inc., 562 Weddell Drive, Suite 8, Sunnyvale, CA 94089 Tel: 408 734 3038. Fax: 408 734 3045. Web: www.polaronyx.com. Email: [email protected]

Broadband C + L ASE Source

Based on our patent pending proprietary technology and expertise on specialty fiber optics, PolarOnyx has

launched a series of broadband ASE sources covering S, C, L, C+L, and S+C+L bands to meet the requirements

of various applications. Various power levels are available from 5 dBm to 14 dBm. Turn key solution eases

operation.

Figure 1 Broadband ASE source and spectrum stability over 15 minutes

Key features

> 80 nm wide band Excellent power stability Flat and stable spectrum Low cost Low power consumption

Applications

Instrumentation and measurement Fiber sensor systems Fiber Gyro systems Telecom system monitoring Optical Coherence Tomography Near-Infrared Spectroscopy

Specifications

Item Min Typical Max Unit

Output power 5 12 14 dBm

Output power stability15 min. + 0.005 + 0.01 dB

Output power stability8 hrs + 0.02 + 0.05 dB

Wavelength range 1525 1610 nm

Gain Flatness 5 dB

Return loss 30 dB

Operating temperature 0 40 oC

Pump 980 nm

Power consumption 1 4 W

Electronic Interface

Size 24x24x9 cm

Note: Stability test is at room temperature 25 +/- 0.5oC

Product Note PolarOnyx

PolarOnyx, Inc., 562 Weddell Drive, Suite 8, Sunnyvale, CA 94089 Tel: 408 734 3038. Fax: 408 734 3045. Web: www.polaronyx.com. Email: [email protected]

Order Information

ASE XXXX-Y XXXX: C band instrument 3000. L band instrument 3500. C+L band instrument 4000. Y: Grade A or B

Grade (affix Y) Catalog No. Description

A B

ASE3000-Y C band ASE instrument Total output power stability +/- 0.005 dB

(15 min.) and +/- 0.02 dB (8 hrs).

Total output power stability +/- 0.05

dB (15 min.) and +/- 0.2 dB (8 hrs).

ASE3500-Y L band ASE instrument Total output power stability +/- 0.005 dB

(15 min.) and +/- 0.02 dB (8 hrs). Total output power stability +/- 0.05

dB (15 min.) and +/- 0.2 dB (8 hrs).

ASE4000-Y C+L band ASE instrument Total output power stability +/- 0.005 dB

(15 min.) and +/- 0.02 dB (8 hrs). Total output power stability +/- 0.05

dB (15 min.) and +/- 0.2 dB (8 hrs).