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STATE-OF-THE-ART DEVELOPMENTS B.I.Stepanov Institute of Physics National Academy of Sciences of Belarus ifanbel.bas-net.by
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Page 1: STATE-OF-THE-ART DEVELOPMENTS

STATE-OF-THE-ART

DEVELOPMENTS

B . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

ifanbel.bas-net.by

Page 2: STATE-OF-THE-ART DEVELOPMENTS

DIODE PUMPED SOLID STATE LASERS

B . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

Page 3: STATE-OF-THE-ART DEVELOPMENTS

Erbium lasers

Model IFL-E23-P IFL-E53-P IFL-E83-P Operating wavelength, nm 1535 1535 1535 Output pulse energy, mJ 2 5 8 Pulse repetition rate, Hz 3 3 3

2 Beam quality factor, M < 1.3 < 1.3 < 1.3

0Operating temperature interval, C - 40 ÷ + 50 - 40 ÷ + 50 - 40 ÷ + 50

0.2 Dimensions, mm 60×30×30 75×35×30 75×45×30

Lasing pulse duration, ns < 20 < 20 < 20

Type of Q-switch passive passive passive

Weight, kg 0.2 0.2

APPLICATIONS:

range-finding target designating systems environmental monitoring material processingmedicinelaser spectroscopy

B . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

Page 4: STATE-OF-THE-ART DEVELOPMENTS

APPLICATIONS:

range-finding target designating systems environmental monitoring material processingmedicinelaser spectroscopy

Model IFL-E2020-EO Operating wavelength, nm 1535 Output pulse energy, mJ 20 Pulse repetition rate, Hz 20 Lasing pulse duration, ns < 30

0Operating temperature interval, C + 10 ÷ + 30 Cooling method air cooling

300×120×123

Beam diameter, mm 2.2

Weight, kg 5 Dimensions, mm

Erbium lasers withhigh energy

B . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

Page 5: STATE-OF-THE-ART DEVELOPMENTS

Diode-pumpedNd:YAG laser

APPLICATIONS:

range-finding target designating systems environmental monitoring material processingmedicinelaser spectroscopy

Model IFL–N(150)20030-EO Operating wavelength, nm 1064 Output pulse energy, mJ 150 / 200 Pulse repetition rate, Hz 30 Beam diameter, mm < 5 Beam divergence, mrad <1.2

0Operating temperature interval, C + 10 ÷ + 30 Cooling method air cooling

350×200×100

Lasing pulse duration, ns 7 ÷ 10

Weight, kg 5 Dimensions, mm

B . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

Page 6: STATE-OF-THE-ART DEVELOPMENTS

Eye-safe OPO based on Nd:YAG laser

APPLICATIONS:

range-finding remote sensingmaterial processinglaser spectroscopy

Model IFL-N5030- OPO Operating wavelength, nm 1570 Output pulse energy, mJ 50 Pulse repetition rate, Hz 30 Beam diameter, mm 5

0Operating temperature interval, C + 10 ÷ + 30 Cooling method air cooling

285×110×120

Lasing pulse duration, ns 7 ÷ 10

Weight, kg 5 Dimensions, mm

B . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

Page 7: STATE-OF-THE-ART DEVELOPMENTS

APPLICATIONS:

scientific research

explosives detecting devices

medicineenvironmental monitoring

Model IFL–N18030-4H Operating wavelength, nm 1064, 532, 355, 266

90 (532 ) 45 (355 ) 20 (266 nm)

Pulse repetition rate, Hz 30 Beam diameter, mm < 5

Cooling method air cooling

222×440×155

Output pulse energy, mJ 180 (1064 nm) nm nm

with amplifier, J 0.4 / 1 (1064 nm)

Lasing pulse duration, ns 7 ÷ 10 (1064 nm)

Beam divergence, mrad <1.2

Weight, kg 10 Dimensions, mm

Diode pumped Nd:YAG laser with harmonics

B . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

Page 8: STATE-OF-THE-ART DEVELOPMENTS

Portable double pulselaser for LIBS applications

APPLICATIONS:

laser induced breakdown spectroscopy

Model IFL-N50(100)10-DPLOperating wavelength, nm 1064 Output pulse energy Pulse repetition rate, Hz 1

Pulse-to-pulse delay, s 1Cooling method air cooling

Dimensions with power supply , mm 510×200×230

for each channel, mJ 50 / 100 ÷ 10

Lasing pulse duration, ns 8 ÷ 12μ ÷ 100

Weight, kg 18

B . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

Page 9: STATE-OF-THE-ART DEVELOPMENTS

All-solid-state picosecondand femtosecond lasers

APPLICATIONS:

time-resolved spectroscopymaterial processingtwo-photon microscopytissue ablationnonlinear optics researchlaser-matter interaction research

Model IFL-F1100 Operating wavelength, nm 760-830 Output pulse energy, mJ 1 Pulse repetition rate, MHz up to 100 Lasing pulse duration, fs < 50

Model IFL-P20100Operating wavelength, nm 1064

p

Output pulse energy, µJ 20 Pulse repetition rate, kHz 10 ÷ 100Lasing pulse duration, s < 20

Average power, W 2 2

Beam quality, M < 1.5

B . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

Page 10: STATE-OF-THE-ART DEVELOPMENTS

OPTOELECTRONIC

Page 11: STATE-OF-THE-ART DEVELOPMENTS

SYSTEMS

B . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

Page 12: STATE-OF-THE-ART DEVELOPMENTS

Night vision system at reducedtransparency of the atmosphere

B . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

Page 13: STATE-OF-THE-ART DEVELOPMENTS

Night vision system

Model NVS S500-10 Distance of the boundary of the observation zone , m

÷ Operating

0Operating temperature interval, C - 40 ÷ + 50

120×120×280

minimal 10 maximal 500

Angle of view 10°х х Magnification 1 3

voltage, V 12

Consumption power, W < 10 Weight, kg < 2.5

Dimensions, mm

B . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

Page 14: STATE-OF-THE-ART DEVELOPMENTS

Model NVS M11000-10 Distance of the boundary of the observation zone , m minimal 10

maximal 1000 Angle of view 20°

х Magnification 10 Operating voltage, V 12, 24

0Operating temperature interval, C - 40 ÷ + 50 Consumption power, W < 20 Weight, kg < 5

Dimensions, mm 110×110×370

Night vision systemB . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

Page 15: STATE-OF-THE-ART DEVELOPMENTS

Night vision systemB . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

Model NVS SH700-30 Distance of the boundary of the observation zone, m minima 40

maximal 700 Angle of view 2 ÷ 5°

Angle of survey 30°х Magnification 10

Operating voltage, V 12, 240Operating temperature interval, C - 40 ÷ + 50

Consumption power, W < 100 Weight of flight glasses, kg 0.5 Weight of laser searchlight, kg 3.5 Flight glasses dimensions, mm 155×55×75 Laser searchlight dimensions, mm 165×145×80

Page 16: STATE-OF-THE-ART DEVELOPMENTS

B . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

Distance = 60 m Distance = 250 m Distance = 4700 m

Page 17: STATE-OF-THE-ART DEVELOPMENTS

B . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rusNight vision system

Model NVS L7000-06 Distance of the boundary of the observation zone , m minimal 100

maximal up to 7000 Angle of view 0.6°

х Magnification 100 Operating voltage, V 12, 220

0Operating temperature interval, C - 40 ÷ + 50 Consumption power, W < 500

Weight, kg < 80 Dimensions, mm 380×710×1020

Page 18: STATE-OF-THE-ART DEVELOPMENTS

Mobile laser spectrometer

APPLICATIONS:

Metals CoatingsMinerals SoilCement PlantsPharmaceuticals BiologicalExplosives Food stuff

B . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

ADVANTAGES:Laser-induced breakdown spectroscopy (LIBS)is a simple, rapid, real-time analytical technique of .nondestructive testing

Model MLS-50-200-DP Operating wavelength, nm 1064 Output pulse energy Pulse repetition rate, Hz 1

Pulse-to-pulse delay, s 1 Cooling method air cooling

Dimensions of laser module 510×200×230 Type of spectrograph Czerny-Turner Focal length, 200 Usable wavelength range, 200-1200 Simultaneous registered range, nm 120 nm Wavelength resolution, 0,12 nm

for each channel, mJ 50 / 100 ÷ 10

Lasing pulse duration, ns 10μ ÷ 100

Weight of laser module, kg 18

, mm

mm nm

nmWeight of spectrograph, kg 10

Dimension of spectrograph, mm 320×300×160

Page 19: STATE-OF-THE-ART DEVELOPMENTS

Laser examination andcleaning of historical and artistical values

APPLICATIONS:

Cultural heritage

ADVANTAGES:, microanalysis, no sample preparation nondestructive testing and cleaning.

B . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

Modeloperating wavelength, nm

pulse-repetition rate, Hzpulse duration, nspulse energy, mJ

LС MW5-8001064, 532, 355, 266, 2131 - 515 – 20up to 550 (1064 nm)up to 800 (532 nm)up to 400 (355 nm)up to 300 (266 nm)up to 100 (213 nm)

Page 20: STATE-OF-THE-ART DEVELOPMENTS

High-speed laser marker

ModelLaser type

Laser radiation wavelength, nmPulse-repetition rate, kHz

Pulse duration, nsPulse energy, mJ

Average output power, WLaser life time, hour

Power consumption, WMarking area, mm x mm

Beam movement rate, m/sOutput image type

Weight, kgDimensions, mm

LM HS10(20/50)-8air-cooled pulsed ytterbium fiber laser(LD pumped Nd:YAG laser)1060 ± 1020 10100 ± 100.510 / 20 / 50> 30 000120 / 150 / 24060x60 / 110x110 / 175x175 up to 8 contour, graphic, text, and other images. 35640x500x600

÷

B . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

Page 21: STATE-OF-THE-ART DEVELOPMENTS

High-speed laser marker

APPLICATIONS

Precision laser marking of:

industrial goodssouvenir productionjewelleryaward productions

Laser cutting

MATERIALS: Metals very good Alloys very good Semiconductors good Plastics good Ceramic good

B . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

technology of halftone images

Page 22: STATE-OF-THE-ART DEVELOPMENTS

LidarsB . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

MEASUREMENTS- concentration of gases and aerosols;

ModelBackscattering at wavelengths, nm

Raman scattering at wavelengths, nmDepolarization at wavelength, nm

0Scanning in azimuth,0

Elevation scanning ,Distance, km

Spacial resolution, m Dimensions, mm

Weight, kg

L MW6R355, 532, 1064387, 407, 607532±1800 ÷ 9035151500x1500x2000200

Page 23: STATE-OF-THE-ART DEVELOPMENTS

Optical elementsLaser optics & coatings

Optical windows

Dielectric mirrors & AR coatings

Interference filters

Fabri-Perot interferometers

Polarization optics

Prisms

Lenses

Deep optical contact elements

Spectral region: 250 nm ÷ 2.7 µm

B . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

Page 24: STATE-OF-THE-ART DEVELOPMENTS

B . I . S t e p a n o v Institute of PhysicsNat iona l Academy o f Sc iences o f Be la rus

68, Nezalezhnasti ave, Minsk, Belarus 220072phone: +375 17 2841755, 284-04-27; fax: +375 17 [email protected]://ifanbel.bas-net.by