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Periodic Structures via Laser Matter Interaction. Alika Khare Physics Department Indian Institute of Technology Guwahati. Layout. Introduction    Lithography using high power laser Interferometry Manipulation of atomic trajectories via dipole force Future Scope Conclusion

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periodic structures via laser matter interaction

Periodic Structures via Laser Matter Interaction

Alika Khare

Physics Department

Indian Institute of Technology Guwahati

layout
Layout
  • Introduction   
  • Lithography using high power laser Interferometry
  • Manipulation of atomic trajectories via dipole force
  • Future Scope
  • Conclusion
  • Acknowledgement
introduction
Introduction

Need for small sized periodic structures?

Example: Information technology

Demand: High Speed>>10Gb/s

Small storage space

Limitations:

1. Material Limitation

Bulk material: Slow response

2. Fabrication Limitation

VLSI 80nm

remedy
Remedy
  • Optical technologies
  • Information carriers: Photons

Photonics devices

Fast Optical devices

Tunability over wide spectrum of parameters

Temporal response <10-12 s

Size nanometer

what is to be done
What is to be done?
  • Synthesis of new Materials
  • Materials having periodic structures dimensions <100nm
  • Quantum confinement effect

Drastic changes in optical, electrical mechanical, thermal and magnetic characteristics of the materials from its bulk behaviour and offers the tremendous scope in microelectronics, optoelectronics and Photonics industries.

manipulation of the materials via laser matter interaction
Manipulation of the materials via Laser Matter Interaction
  • Modification into surface morphology via selective laser ablation of thin films
  • Modification into the trajectories of atom via dipole force
lithography using high power laser interferometry
Lithography using High Power Laser Interferometry
  • Selective ablation of Thin films

Modification into the surface morphology of the orders of tens of nm.

Two step process 

  • a.    Deposition of thin films

b. Selective ablationSingle step

Simple set-up

a deposition of thin film
a. Deposition of thin film
  • Techniques used
  • Thermal Evaporation technique
  • Pulsed Laser Deposition Technique
thin films used
Thin films used
  • Thermal evaporation

Indium and chromium thin films

pulsed laser deposition technique for thin films
Pulsed Laser deposition technique for thin films
  • Schematic of experimental set-up
advantages of pld
Advantages of PLD
  • Applicable to any material
  • Applicable to any form of the target material: Solid

Liquid

Gas

  • By controlling the environment any composition can be deposited
pulsed laser deposition
Pulsed Laser deposition
  • Laser:
  • 2nd harmonic of Q switched Nd: YAG laser

10ns, 10pps, 400mJ in fundamental

  • Deposition time 5 minutes to 30 sec.
  • Vacum 10-5-10 –6 Torr
  • Deposition thickness 200nm-2m
target material
Target Material
  • Copper
  • Silicon wafer
  • Zinc Oxide
b selective ablation of thin films by high power laser interferometry
b. Selective Ablation of thin films by High Power Laser Interferometry
  • The thin films can be selectively ablated by illumination with the interference pattern form by High power laser Interferometer.
selective ablation
Selective Ablation
  • Part of the thin film illuminated by the bright fringe will be ablated
  • The dark fringe region will remain un effected
  • Thus selective ablation results into the series of periodic lines of the materials
  • (grating Structure)
afm image of selectively ablated cu film
AFM image of selectively ablated Cu film

Three dimensional view

Periodicity 50 m

Minimum Line width ~5 m

Scale in m

Two dimensional view

Ref: AKhare et.al, Rad Phys and chem, 70,553-558 (2004)

afm image with improved laser mode structure
AFM image with (improved laser mode structure)

Indium thin film in air

Scale nm

further reduction into size
Further reduction into size
  • By focusing the interference pattern on to the thin film

L

micrograph of selectively ablated film via focusing of interference pattern
Micrograph of selectively ablated film via focusing of interference pattern

Line Thickness< 1 m

formation of two dimensional arrays
Formation of two dimensional arrays
  • Two interferometer in tandem
  • Out put of one interferometer illuminates the second stage of interferometer

Four beam interference

Square arrays of two dimensional light spot

recorded ccd image of tiny arrays of light spot from four beam interferometer
Recorded CCD image of tiny arrays of light spot from four beam interferometer

On illumination with such patterns, in the region of maximum intensity tiny holes will be drilled

Ref: A S Patra and Alika Khare, Optics and Laser technology, (in press)

square matrix of tiny holes
Square matrix of tiny holes

Sample: Indium thin film placed in air for selective ablation via four beam interference

Micrograph after selective ablation

Scale 20 mX20 m

results when the films were placed under vacuum
Results when the films were placed under vacuum

After illumination with the interfernce pattren directly, beam energy~20mJ

Scale in nm

advantage of the technique
Advantage of the technique
  • Applicable to any material
  • Complete writing in Single step, Single shot
  • Structure size tens ofnanometer
  • Relatively simple
what is to be done to reduce the periodicity
What is to be done to reduce the periodicity?
  • Manipulation of Atomic Trajectories using Dipole force
origin of dipole force
Origin of dipole force

Interaction of induced dipole moment with non-uniform near resonant light distribution.

dipole force
Dipole force
  • Classically an atom placed in an electromagnetic field is equivalent to a dipole of dipole moment

p E(electric field)

Results into a force

F= -(p.E)

Hence F  I (intensity of the field)

dipole force1
Dipole force
  • Using Semi classical approach, expression for the dipole force:
configuration details
Configuration details

·    Mono energetic Collimated and diverging Atomic Beams both

Laser fieldAtomic Beam

     Standing wave   Single beam

      Gaussain Beam Arrays of Beams

simulated results
Simulated results
  • Example Rubidium
  • Energy level diagram
standing wave configuration
Standing Wave configuration

Atomic Beam

Standing wave

simulated results for standing wave
Simulated Results for Standing wave
  • One Dimensional focused pattern of atoms

First Focus

Multiple focus

Ref. A Khare, et al, Radiation Physics and Chemistry, 70, 553 (2004)

limitation
Limitation
  • Periodicity /2
arrays of micro oven
Arrays of micro-oven
  • New scheme:
  • Laser produced neutral atomic beams
  • Arrays of Micro-ovens in square geometry
  • Technique: Selective ablation of thin films via four beam interferometer

Illumination from the rear side

  •  Large number of atomic beams in square geometry
cross section of arrays of atomic beams
Cross-section of arrays of Atomic beams
  • Location of atoms in the launching plane
future scope
Future Scope

Selective ablation technique is very general and can be applied on any material with any high power laser

 Formation of

  • Tiny Arrays of laser
  • Wave guide
  • Optocoupler
  • Photonic band gap material
future scope1
Future scope
  • The manipulation of atoms via dipole force is a coming up field where the process has to be understood fully, involving the atom laser interaction. The concept of series of micro-oven is yet to be perfected experimentally. Periodicity and line width both can be reduced by appropriate choice of atomic beam system and laser field.
conclusion
Conclusion
  • Two schemes based on Laser matter interaction for the generation of periodic small structures
  • Selective ablation via high power laser interferometer periodicity  1m
  • Simulated pattern for the dipole force using multiple atomic beam
  • Periodicity as well as spot size ~tens of nm
acknowledgement
Acknowledgement
  • 1.  Research Scholars
  • Mr AS Patra and Mr Kamlesh Alti
  • 2. Partial financial assistance from
  • i. CSIR, New Delhi, India,

Scheme No. 03(831)/98/EMR-II

  • ii. MHRD, New Delhi, India

Scheme No. F.26-1/2000/TSV

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