Beam Shaper / Top-hat
Top-Hat beam shaper converts a Gaussian input laser beam into a uniform
intensity beam of any shape and size requested by the customer. The beam shaping
element is a diffractive optical element (DOE) used to transform a near-gaussian
incident laser beam into a uniform-intensity spot of either round, rectangular,
square, line or other shape with sharp edges in a specific work plane.
uniform spot enables equal treatment to a surface, excluding over/under-exposure
of specific areas. In addition, the spot is characterized by a sharp transition
region that creates a clear border between the treated and untreated area.
The beam shaping can be a:
(lens) or module which give a Top-Hat intensity distribution at a
specific working distance (BFL of the lens or distance from exit
location of the module to Top-Hat plane).
(window) which gives a Top-Hat intensity distribution at infinity or
focal length of aberration free customer's lens.
(window) which gives a uniform exposure over scanned lines.
Small Angle Top Hat standard
Small Beam Shaper for scanning application (~1.5X Diffraction Limit)
Laser beams with Top-hat energy distribution are being used for different
applications in the laser material processing industry. Most systems in this
industry include scanners and F-θ lenses in order to direct and focus the beam
on the substrate. HoloOr is proud to introduce a new design for
~1.5x(Diffraction limit) beam shapers DOEs (Diffractive Optical Element) which
is considerably cheaper than regular Top-hats.
Those DOEs are specially designed to operate with scanners/F-θ lenses under high
power lasers. Placing the beam shaper DOE before the scanner will create a
top-hat energy distribution at the F-θ lens working plane. The use of this beam
shaper does not affect the focal length of the system.
Homogenizer / Diffuser
Homogenizer product line flexibly converts any collimated input laser beam into
a well-defined beam with homogenized intensity and desired shape.
Using our Beam Homogenizer product, you can convert any collimated input beam
profile into a well-defined beam with homogenized intensity. Any desired shape,
for any wavelength can be achieved.
A Beam Homogenizer is very useful in many applications requiring a well-defined
beam shape with a randomly-diffused intensity profile.
The output of the Beam Homogenizers will depend on the input beam profile:
A multi-mode laser beam actually has an advantage when used with beam
homogenizer, as their degraded coherence will reduce the visibility of speckles
and therefore create a more uniform intensity profile than with single mode
A Beam splitter element converts input laser beam into a 1 or 2-dimensional
array of beamlets according to custom parameters.
The Diffractive Beam Splitter is a diffractive optical element used to split a
single laser beam into several beams, each with the characteristics of the
original beam (except for its power and angle of propagation).
A diffractive beam splitter can generate either a 1-dimensional beam array (1xN)
or a 2-dimensional beam matrix (MxN), depending on the diffractive pattern on
the element. The diffractive beam splitter is used with monochromatic light such
as a laser beam, and is designed for a specific wavelength and angle of
separation between its output beams.
In this section, we present our standard list of 1D, 2D, and custom diffractive
We offer, in addition to standard diffractive beam splitters, the possibility to
choose the number of spots and their locations, as a part of its custom design
and manufacturing capability.
We also offer Binary Phase Gratings, which is a special case of 1D Damman
grating with a duty cycle of 50% within a period. The gratings are transmission
grating. In addition to standard gratings, We offer gratings with custom
specifications (duty cycle, modulation depth, period, reflection or transmission
|Beam splitter 6x8
||Hexagonal Beam Splitter
||Round beam splitter
Vortex lenses convert a Gaussian input laser beam into a donut-shaped energy
A Vortex lens is a unique optic, whose structure is composed of spiral or
helical phase steps.
A Spiral phase plate converts a Gaussian input profile into a donut-shaped
The spiral phase plate is a unique optic, whose structure is composed entirely
of spiral or helical phase steps, whose purpose is to control the phase of the
The topological charge, denoted in the literature as m, refers to the number of
2π cycles (i.e. "staircases") etched around 360° turn of diffractive surface.
One main effect of a higher topological charge is an increase in the angular
momentum of the vortex beam by a factor of m. Another effect is the dimensions
magnification of the ring intensity pattern, by a factor of m.
Multi-focal Diffractive Optical Element (DOE) allows to focus a single incident
beam simultaneously at several focal planes along the propagation axis.
We have a vast variety of solutions for multiple foci along the optical axis:
The Multifocal Diffractive Optical Elements (DOE’s) allow a single incident beam
to focus simultaneously at several focal lengths along the propagation axis.
From a collimated input beam (single mode or multi-mode), the output beams
focussed at a fixed number of focal lengths, predetermined during the design of
the Multifocal DOE based on the customer's system requirements.
The Multifocal DOE comes in two configurations:
A DOE consisting of a Plano-convex lens with predetermined focal length, and a
diffractive pattern, etched on its Plano side.
For more flexibility, a window DOE, thus, to get the foci spots at certain
distances, the user adds a regular focusing lens after the DOE. The lens focal
length determines the working distance (WD).
The Multifocal DOE can also be used as quasi elongated focus elements,
increasing effectively the depth of focus in applications such as laser glass
cutting and laser micro machining.
Diffractive beam samplers are used to monitor high power lasers where optical
losses and wavefront distortions of the transmitted beam need to be kept to a
minimum. In most applications, most of the incident light must to continue
forward, "unaffected," in the "zero order" while a small amount of the beam is
diffracted into a higher order, providing a "sample" of the beam. By directing
the sampled light in the higher order(s) onto a detector, it is possible to
monitor, in real time, not only the power levels of a laser beam, but also its
profile. A Laser Beam Sampler allows the high power beam (zero order) to
propagate undisturbed along the optical axis, but produces two side beams with
low energy. These two sample beams are located to the left and right of the main
beam (-1 and +1 orders), and are characterized by a given separation angle
between them and by a sample power ratio. It is relatively easy to modify the
sampling ratio upon a request of the customer.
A Ring generator transforms a laser beam into a ring (Diffractive axicon) or
into a multi-rings (Multi-Circles).
A laser concentric circles pattern transforms a laser beam into multiple
A concentric circles light pattern can be used for certain 3D mapping
applications, especially within pipe/tube objects.
A concentric circles pattern was recently proved to be the most appropriate
light pattern for certain 3D mapping applications, especially with pipe/tube
Each laser concentric circles is defined by its full angle and its number of
We offer, in addition to its standard products, the possibility to design and
manufacture a number of circles, separation angle between the circles and full
angle as requested by the customer, as a part of its custom design and
We also design and manufacture diffractive axicon which is a DOE that splits an
input beam to a single ring.
An Axicon transforms a laser beam into a ring shape (a Bessel intensity
The ring's thickness will be equivalent to the diffraction-limited-spot size (of
the input laser beam).
An Axicon also images a point source into a line along the optical axis and
increases the Depth Of Focus (DOF). Each diffractive Axicon product is defined
by its ring propagation angle.
Dual wavelength beam combiners are diffractive optical elements used to combine
two incident beams with different wavelengths into the same focal point.
In multi-wavelength light beams the dual wavelengths are diffractive optical
elements used to combine two incident beams with different wavelengths into the
same focal point.
In particular, this focus combiner is used for combining CO2 laser focus and
visible aiming beam focus into a single focal point.
The Dual wavelength corrects the strong chromatic aberrations between a CO2
laser and its visible aiming beam.
This hybrid element, is based on a Plano convex lens with corresponding
diffractive pattern on its Plano side.
The focal length for both wavelengths is determined during the design, according
to the customer's application
masks are glass substrates that have a very thin (~1um) reflective patterned
coating. The coated part reflects the incoming beam while the uncoated part
transmits the beam. The output in the near field will be very close to the shape
of the pattern. In the far field some diffraction patterns may appear. One
should not see significant diffraction, if one projects with a lens the output
of the mask to an image plane, as shown in the figure below.
One can narrow the transition region from a beam-shaper by using the Dielectric
mask as in the figure below.
One can also create any pattern that will be imaged with a lens. One cannot
manage the intensity profile within a spot.
We offers customers the opportunity to obtain custom solutions such as:
DOE for spectral dispersion of focal plane
In applications requiring multi-spectral focal
dispersion, we offer a flexible and compact diffractive solution. A refractive
lens alone has a small dispersive component, due to slight spectral dependence
of the lens material optical index. As a result, the spectral foci are discreet
but very close to one another. A diffractive surface is a compact effective
solution for "stretching out" or expanding the inter-focal distance between two
or more spectral foci.
On the other hand, a diffractive surface is also an effective solution for
combining foci of assorted wavelengths to a single focal point.
Diffractive lenslet arrays are substrates covered
with a set of micro diffractive lenses. The arrays perform as diffusers or for
local focusing and sampling. A diffractive lenslet array has the advantage of
100% fill factor, much higher than refractive lenslet array. Aberration
corrected micro lenses for imaging systems are easily designed and fabricated.
We also offer 1-D micro lens arrays, lenslet arrays with shifted center.
Wavefront corrector (i.e. for aberrations
When the wavefront is different from the desired
shape, a DOE element can be used to correct the deviation. The wavefront
deviation from desired shape must be constant in time, because each part of the
element introduces a specific phase correction.
Diffractive lens and Zone Plate Lens [ZPL]
Diffractive lenses are used to focus monochromatic
light (often laser light). A diffractive lens consists of a series of radial
rings or "zones" of decreasing width (known also as Fresnel zones). The
diffractive lens is a perfect lens which include spherical aberration
correction. As a general rule, diffractive elements work best at a single
wavelength. At any other wavelength the efficiency as well as image contrast are
reduced. However, the diffractive lens can be used also as chromatic aberration
corrector and, in this case, the image contrast will not be reduced. The
diffractive lens can be used also to reduce the number of elements in a system.
DOE Tuner for wavelengths range from 266nm to 1064nm
To answer the demand for fine-tuning abilities of various output parameters when
using a DOE, as: shape/spot size, separation/divergence angle, etc. our designed
a variable beam tuner, optimized for use with Top-Hat beam shaper, Homogenizer,
MultiSpot, and other DOE products. Another application is the fine-tuning of
incident beam size before DOE for Top-Hat application, where precision of
incident beam size is important.
The DOE tuner presents the following features:
Very low wavefront error
Beam expander x0.8-x1.2
No need to change module direction
Constant mechanical size
Fused Silica lens material
Input and output clear aperture = 23 [mm]
Module length = 120 [mm]
Max. Input Beam Diameter (1/e2): Ø8.4 mm (0.8X), Ø7.0 mm (1.2X)
Max. output beam size = 8.4 [mm]
*Max. incident angle = 0.5o
Wavelength range = 266-1064 [nm]
Other wavelengths upon request
*Defines angular limitation for Top Hat Beam Shaper or Beam Splitter usage.
Different configurations for using the DOE-Tuner module:
Placing the DOE-Tuner before a DOE
Purpose – Fine tuning for input beam size
For Top-Hat beam shaper – achieves nominal beam size
For Beam-Splitters, Multi-Focal and Vortex phase plate – controls spot size
||Magnification < 1
||Magnification > 1
Figure 1: DOE-Tuner module placed before DOE
Placing the DOE-Tuner after a DOE
Purpose – controlling divergence of the output beam, allows to vary key
parameters of DOE in range of 80-120 %
Multi-Spot – controls the separation angle
Multifocal – controls the separation between foci
Top-Hat , Homogenizer & others – controls the image size
||Magnification < 1
||Magnification > 1
Figure 2: DOE-Tuner module placed after DOE and
before focus lens (or objective)
Module for blocking unwanted spots \ energy
For applications as metrology and sensitive material processing, our designed a
compact universal module for blocking undesired spots of Multi-Spots or
parasitic energy of Homogenizers.
The module contains 6 lenses and a mask/aperture in the middle.
Each DOE design requires a certain mask/aperture according to customer’s specs.
Parameters and features of the module:
Max input beam diameter = 12 [mm]
Max full angle of DOE for 12 [mm] input beam dia = 5 [deg]
Input beam smaller than 12[mm] enables larger than 5 [deg] full angle for DOE
Module length = 90 [mm] (not includes DOE and focusing lens)
Outer diameter of module = 30.5 [mm] (lens diameter = 25.4 [mm])
Lenses material = N-SF11
Simulation results of two DOEs with the module (right) and without (left):
Focusing Module Optimized for Beam Shaper
For applications requiring an aberration-free image in focus plane, with a high
precision, we developed a new optimized focusing module to be used with our Beam
Shapers. A standard focusing lens (or objective) is normally optimized for
focusing a Gaussian beam and is not optimized to work with a Beam Shaper. Thus,
the use of standard focusing lens with Beam-Shapers often causes aberrations of
the Top-Hat image and requires special design of a focusing lens or module.
These aberrations will normally occur at small focal lengths, short wavelength
and large input beam. In order to solve this problem, we designed a focusing
module (with focal length 50 [mm]) adapted to our Beam Shaper working at 355
[nm]. The module contains 5 lenses, and the Top-Hat output is obtained at the
back focal length of the module. We offers customization of the module for other
wavelengths and focal length. The focusing module presents the following
Focal lengths: 30 and 50 [mm]
Wavelength (optimized): 355 [nm]
Material: Fused Silica
Max. input beam size = 12 [mm]
Optional - Objective correction collar
Comparison between Square Top-Hats result at image
plane obtained by different focusing elements:
results for a Square Top-Hat 100x100[μm2] in size, with (from left to
right): perfect lens (not real lens) for ideal spot, aspheric lens,
standard focusing module not optimized for use with a Beam Shaper and
our focusing module optimized for use with Beam Shapers.
We introduce a new module for modifying certain output parameters of a
Diffractive Optical Element (DOE).
The module reduces or expands the full angle of a DOE output by a magnification
Unlike standard beam expander, our module takes into considerations the
characteristics of our beam shaping, beam splitting and beam foci elements, thus
achieving superb results with minimal aberrations.
The module can be beneficial/suitable in the following cases:
Using the module together with a DOE, to create an overall function that would
be hard to manufacture by a single element
Adding our module to a standard, semi-standard or in-stock DOE with specific
full angle to change the full angle of the DOE thus avoiding any NRE payment,
and shortening delivery time
our is also able to customize the module according to the customer’s system and
|Fixed Expansion factor:
||x5 and x9.4
|Product categories to be
used with the DOE expander:
||Beam Splitter, Homogenizer / Diffuser,
Top-Hat Beam Shaper, Vortex Spiral Phase Plate, Diffractive Axicon,
|DOE expander optimized for:
||Square shape beam (as Top-Hat square or
Beam Splitter 2D square [9x9 spots for example])
||266nm to 1550nm
|Without DOE Expander
||With DOE Expander x5
||With DOE Expander x9.4
|Far-field simulation results for a Square Top-Hat, from
left to right, without DOE expander 1.5x1.5[deg], with DOE expander x5
7.5x7.5[deg] and with DOE expander x10 ~14x14[deg].
Comparison between Square Top-Hats result at image
plane obtained by different expander module elements: