OptoSigma

LensesGradient Index Microlenses

  • Cylindrical shape is easy to mount, easy to align
  • Available with both plano and convex end profiles
  • Available for popular visible and IR laser wavelengths
  • Perfect solution for optical data transmission applications
  • Also available with the focal plane falling outside the lens for non-contact use

P35,Lense,gim,Gw/on

Optical glass with a refractive index gradient provides a very efficient and simple way to produce high quality imaging lenses. The material used in these Microlenses is Selfoc®. This material has a radial index gradient which causes focusing to occur within the material. The index variation is defined by and is normally specified by the constant (check)A. The simplest form of gradient index lens is a simple cylinder of Selfoc®. Collimated light incident on one end of the lens will be focused as it travels along the length of the cylinder. These Microlenses are particularly useful for fiber and diode coupling since they can be mounted in close proximity to the source. They are ideal for use in optical data transmission. We offer gradient index Microlenses with Plano end faces and also in a convex configuration for greater imaging power. The convex lenses have a spherical radius on one end only. Normally these lenses are a quarter pitch so that they focus a collimated input at the remote face of the lens. However, we also offer lenses having slightly less than 1/4 pitch so that they focus just outside the lens. This is often more convenient since contact with the source or detector may be physically impossible. Two different numerical apertures are offered, 0.46 and 0.6. These lenses are wavelength specific. They are supplied for the wavelengths 633, 830, 1300 and 1560 nm and are anti-reflection coated for these wavelengths. They will work at other wavelengths but their focusing characteristics will vary from the published figures and the coatings will not be optimized.


Specifications & Tolerances

Diameter:

±0.02mm

Parallelism:

<10arcmin

Aperture:

70% of diameter

Length:

+0, -0.04mm

Index gradient:

±0.75%

Material:

Doped borosilicate glass

Coating:

NMAR V-coat


Gradient index material provides the focusing capabilities of a lens by providing a continuously variable index of refraction across the profile of a cylindrical rod. In other words, a spherical (or even aspherical lens) can be replicated with a cylindrical rod of glass.

Light Path

Gradient index Microlenses (convex or plano) are easy to mount, easy to use, and are most effective in fiber optic coupling arrangements where only on-axis aberrations need to be addressed.

Graphic of Data Info

 

Gradient Index Convex Microlenses

Range (nm)

N.A.

Diameter, D

Length, L (mm)

Pitch

Refractive Index (axial)

Index Constant A (mm-1)

Price

Availability

Product Number

(inch)

(mm)

830

0.46

0.07

1.8

4.7

0.25

1.60

0.33

 

from stock

024-1110

830

0.60

0.07

1.8

3.0

0.20

1.65

0.42

 

from stock

024-1130

1300

0.46

0.07

1.8

4.8

0.25

1.59

0.33

 

from stock

024-1140

-

-

-

-

-

-

-

-

 

-

-

1300

0.60

0.07

1.8

3.0

0.20

1.64

0.42

 

from stock

024-1160

1560

0.46

0.07

1.8

4.8

0.25

1.59

0.33

 

from stock

024-1170

1560

0.60

0.07

1.8

3.0

0.20

1.63

0.42

 

from stock

024-1190

® Selfoc is a registered trademark of Nippon Sheet Glass Company.


Gradient index material provides the focusing capabilities of a lens by providing a continuously variable index of refraction across the profile of a cylindrical rod. In other words, a spherical (or even aspherical lens) can be replicated with a cylindrical rod of glass.

Light Path

Gradient index microlenses (convex or plano) are easy to mount, easy to use, and are most effective in fiber optic coupling arrangements where only on-axis aberrations need to be addressed.

Graphic of Data Info

 

Gradient Index Plano Microlenses

Range (nm)

N.A.

Diameter, D

Length, L (mm)

Pitch

Refractive Index (axial)

Index Constant A (mm-1)

Price

Availability

Product Number

(inch)

(mm)

633

0.46

0.04

1.0

2.6

0.25

1.61

0.61

 

from stock

024-0130

633

0.46

0.07

1.8

4.6

0.25

1.61

0.40

 

from stock

024-0140

633

0.46

0.07

1.8

4.3

0.23

1.61

0.40

 

from stock

024-0160

633

0.60

0.07

1.8

3.7

0.25

1.66

0.40

 

from stock

024-0180

633

0.46

0.08

2.0

5.2

0.25

1.61

0.30

 

from stock

024-0220

-

-

-

-

-

-

-

-

 

-

-

830

0.46

0.04

1.0

2.6

0.25

1.60

0.60

 

from stock

024-0330

830

0.46

0.07

1.8

4.7

0.25

1.60

0.33

 

from stock

024-0340

830

0.46

0.07

1.8

4.4

0.23

1.60

0.33

 

from stock

024-0360

830

0.60

0.07

1.8

3.7

0.25

1.65

0.33

 

from stock

024-0380

-

-

-

-

-

-

-

-

 

-

-

830

0.46

0.08

2.0

5.3

0.25

1.60

0.30

 

from stock

024-0440

1300

0.46

0.04

1.0

2.6

0.25

1.59

0.60

 

from stock

024-0460

1300

0.46

0.07

1.8

4.8

0.25

1.59

0.33

 

from stock

024-0470

1300

0.46

0.07

1.8

4.4

0.23

1.59

0.33

 

from stock

024-0490

1300

0.60

0.07

1.8

3.8

0.25

1.64

0.33

 

from stock

024-0560

-

-

-

-

-

-

-

-

 

-

-

1300

0.46

0.08

2.0

5.3

0.25

1.60

0.30

 

from stock

024-0580

1560

0.46

0.04

1.0

2.6

0.25

1.59

0.60

 

from stock

024-0660

1560

0.46

0.07

1.8

4.8

0.25

1.59

0.33

 

from stock

024-0670

1560

0.46

0.07

1.8

4.4

0.23

1.59

0.33

 

from stock

024-0690

1560

0.60

0.07

1.8

3.8

0.25

1.63

0.33

 

from stock

024-0780

1560

0.46

0.08

2.0

5.3

0.25

1.59

0.29

 

from stock

024-0880

 

Merci de contacter Infos Photon Lines pour tout renseignement complémentaire.