Interferometric Laser Processing Thin Films

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Solution Overview

Problem

Current laser material processing techniques fail to generate a thin, isolated laser interaction zone within thin films, limiting the creation of new structures and functionalities in materials like CMOS, flexible electronics, and photovoltaic devices, where thin films are crucial.

Innovation Solution

The method involves confining laser-material interaction to an array of narrow zones within transparent films using Fresnel reflections to create a Fabry-Perot intensity modulation, allowing for strong ionization and quantized ejection of film segments or formation of nano-voids at specific fringe maxima, thereby controlling the laser modification process.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Volume of moving object

If laser light is focused onto a thin transparent film, then the laser interaction volume extends through the full depth of focus and full film thickness, but this prevents generation of a thin, isolated laser interaction zone within the film

Engineering Contradiction:
Improvelaser interaction zone thicknessVSAvoidcontrol over laser modification location
Core Design Contradiction:
Volume of moving objectVSManufacturing precision

Solution Approach 1:

The patent segments the continuous laser interaction volume into discrete, thin interaction zones by introducing optical interference fringes within the film. The laser beam is divided into multiple interference patterns with spacing of λ/2n f, creating separate modification locations at each fringe maximum rather than a continuous modified region through the full film thickness.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The patent applies local quality by creating spatially varying interference patterns within the film that produce localized high-intensity regions at specific fringe maxima. Each fringe maximum creates a distinct zone of modified material properties, allowing precise control over where laser modification occurs within the film thickness while maintaining the original beam parameters.

Inventive Principle:
Principle #3Local quality

2Manufacturing precision

If optical interference patterns are generated to create narrow processing zones, then thermal diffusion spreads energy beyond fringe-to-fringe separation, but this washes out process resolution

Engineering Contradiction:
Improveprocess resolutionVSAvoidthermal diffusion
Core Design Contradiction:
Manufacturing precisionVSLoss of energy

Solution Approach 1:

The patent employs periodic action by using ultrashort laser pulses with duration shorter than the thermal diffusion time scale (τ p < τ d =λ 2n f 2). This periodic pulsed delivery allows the laser to deposit energy faster than thermal diffusion can spread it, confining the modification to the fringe width scale (∼λ/4n f ) rather than allowing thermal blurring to expand the affected zone to the beam waist scale.

Inventive Principle:
Principle #19Periodic action

3Manufacturing precision

If the laser pulse duration is shortened to reduce thermal diffusion, then spectral bandwidth increases, but this broadens and merges interference fringes toward a uniform intensity profile

Engineering Contradiction:
Improvefringe contrastVSAvoidlaser pulse duration
Core Design Contradiction:
Manufacturing precisionVSDuration of action of moving object

Solution Approach 1:

The patent applies parameter changes by carefully selecting the laser pulse duration to satisfy the inequality τ p < min(λ 2n f 2, z/c n f ), where z is film thickness and c is light speed. This parameter optimization ensures the pulse is short enough to prevent thermal diffusion but long enough to maintain sufficient spectral coherence for fringe visibility, balancing both requirements through precise temporal parameter control.

Inventive Principle:
Principle #35Parameter changes

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

This approach enables precise internal structuring and quantized ejection of thin film segments, extending control over laser modification and enabling the creation of novel structures and functionalities in thin films, such as nano-voids and blisters, with improved resolution and precision.

Implementation Method 1

A focused laser beam (12) on entering the film (14) from above undergoes Fresnel reflections at the first (air-film) (20) and second (film-substrate) (22) boundary interfaces

Methodology Applied
Scientific EffectFresnel reflections: Reflection

Implementation Method 2

to lead to the formation of a Fabry-Perot interference pattern (18) inside the film (14)

Methodology Applied
Scientific EffectFabry-Perot interference: Fabry-Perot Interferometer

Implementation Method 3

nonlinear optical interactions by the ultrashort duration laser predicts a strong ionization with an electron density profile to follow the shape of the optical interference pattern

Methodology Applied
Scientific EffectIonization: Ionisation

Implementation Method 4

At the threshold exposure for internal material structuring, the electron density reaches a critical threshold at the predicted fringe maxima positions to facilitate the quantized ejection of the film or the formation of thin nano-voids inside the film

Methodology Applied
Scientific EffectLaser ablation: Laser Ablation

Data Source

PatentEP3024569B1Interferometric laser processing
Publication Date: 2019.02.27 KUMAR BV
  • EP3024569B1 patent drawingFigure 1(a)~1(k)
  • EP3024569B1 patent drawingFigure 2(a)~2(c)
  • EP3024569B1 patent drawingFigure 3(a)~3(b)

AI summary

The present disclosure relates to the field of laser induced modification and processing of materials. Modification is achieved by confining laser-material interaction within an array of narrow zones characterizing an optical interference profile. Disclosed is a method of laser induced modification of a material comprising applying at least one laser pulse to the material, the at least one laser pulse being incident on the first interface of the material, wherein the material is selected on the basis that it can support an optical interference pattern such that a thin volume at a site of at least one intensity maxima of the optical interference pattern is characterized by a laser intensity above a threshold value to responsively produce the laser induced modification of the material at a location relative to the first interface.