Segmented Diffractive Beamforming for Elongated Laser Focus Zones

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Solution Overview

Problem

Existing radiation shape elements for laser processing of transparent materials struggle to produce elongated, slim radiation profiles with high aspect ratios that are diffraction-free in the direction of propagation.

Innovation Solution

A diffractive optical radiation forming element with a flat grid structure is used to impose a two-dimensional phase distribution on a laser beam, creating a phase distribution that generates a long, drawn-out focus zone in the material, free from diffraction effects in the propagation direction.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Shape

If conventional beam shaping elements are used, then the laser beam can be focused, but the focus zone is not elongated and diffraction-free in the propagation direction

Engineering Contradiction:
Improvebeam profile shapeVSAvoidfocus zone precision
Core Design Contradiction:
ShapeVSManufacturing precision

Solution Approach 1:

The beam shaping element is divided into multiple angular segments with different azimuthal segment widths. Each segment is assigned a specific phase shift value to create a two-dimensional phase distribution that generates an elongated, diffraction-free focus zone in the propagation direction, resolving the contradiction between achieving proper beam shaping and maintaining focus precision.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

Different regions of the beam shaping element (angular segments) are assigned different phase shift values and segment widths to create localized variations in the phase distribution. This local differentiation enables the formation of an elongated focus zone with precise control over the intensity distribution in the propagation direction.

Inventive Principle:
Principle #3Local quality

2Device complexity

If the azimuthal segment widths of all angular segments are the same, then the phase profiles are uniform, but the focus zone cannot be elongated with high aspect ratio

Engineering Contradiction:
Improvephase distribution uniformityVSAvoidfocus zone aspect ratio
Core Design Contradiction:
Device complexityVSShape

Solution Approach 1:

The invention introduces asymmetry by assigning different azimuthal segment widths to different angular segments. This asymmetric segmentation, combined with specific phase shift values, creates a two-dimensional phase distribution that generates an elongated focus zone with high aspect ratio in the propagation direction, overcoming the limitation of uniform segment designs.

Inventive Principle:
Principle #4Asymmetry

Solution Approach 2:

The invention transitions from one-dimensional radial phase profiles to two-dimensional phase distributions by incorporating azimuthal segment width variations. This dimensional expansion enables control over the focus zone shape in both radial and longitudinal directions, achieving elongated, diffraction-free focus zones with high aspect ratios.

Inventive Principle:
Principle #17Another dimension (Dimensionality change)

3Adaptability or versatility

If elongated focus zones are created in transparent materials, then volume absorption can be tailored, but control over modification geometry becomes difficult

Engineering Contradiction:
Improvevolume absorption controlVSAvoidmodification geometry control
Core Design Contradiction:
Adaptability or versatilityVSManufacturing precision

Solution Approach 1:

The invention enables independent control of multiple parameters including phase shift values, azimuthal segment widths, and segment grating phases. By adjusting these parameters, the two-dimensional phase distribution can be optimized to achieve both tailored volume absorption and precise control over modification geometry in transparent materials.

Inventive Principle:
Principle #35Parameter changes

Solution Approach 2:

The invention replaces mechanical control methods with optical phase modulation. By using a diffractive optical beam shaping element to impose phase distributions, the system achieves precise control over focus zone geometry and volume absorption without mechanical adjustments, improving both adaptability and manufacturing precision.

Inventive Principle:
Principle #28Mechanics substitution (Replace mechanical system)

Applied Scientific Principles

This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.

Function Achieved in This Case

The solution enables the creation of elongated, diffraction-free focus zones in transparent materials, allowing for precise and efficient laser processing with tailored volume absorption, thereby improving the control over geometry and modification types in laser processing.

Implementation Method 1

diffractive optical beam shaping element for imprinting a phase distribution onto a transverse beam profile of a laser beam

Methodology Applied
Scientific EffectDiffraction: Diffraction

Implementation Method 2

imposing a two-dimensional phase distribution on the laser beam, wherein the two-dimensional phase distribution causes the formation of the elongated focal zone

Methodology Applied
Scientific EffectPhase modulation: Phase Modulation

Implementation Method 3

focusing the laser beam with the focusing lens

Methodology Applied
Scientific EffectFocusing: Focusing

Data Source

PatentEP4049071B1Segmented beamforming element and laser working system
Publication Date: 2025.05.14 TRUMPF LASER & SYSTEMTECHNIK SE
  • EP4049071B1 patent drawingFigure 1A~1B
  • EP4049071B1 patent drawingFigure 2A~2B
  • EP4049071B1 patent drawingFigure 2C

AI summary

The invention relates to a diffractive optical beamforming element (15) for applying a phase distribution to a transverse beam profile of a laser beam (5). Said beamforming element comprises mutually adjacent planar elements (15A), which compose a planar grid structure, in which each planar element (15A) is assigned a phase shift value and the phase shift values define a two-dimensional phase distribution (25). The planar elements (15A) are assigned to a plurality of angle segments (31, 31'; 33, 33'), each angle segment (31, 31'; 33, 33') having an azimuthal segment width (Δβj) with respect to the beam center position (23). The phase shift values form, in the angle segments (31, 31'; 33, 33'), respective phase progressions which are radially symmetrical with respect to the beam center position (23), which radially symmetrical phase progressions form grid functions in the radial direction, which grid functions have the same grid period (Tr). Each of the grid functions is assigned a segment grid phase (Θ). The azimuthal segment widths (Δβj) of at least two adjacent angle segments (31, 31'; 33, 33') differ. Alternatively or additionally, the segment grid phases (Θj) of at least two adjacent angle segments (31, 31'; 33, 33') have a segment grid phase difference (ΔΘj) between 0 and 2π.