2D-3D microfabrication with fs laser coupled to a uFAB workstation

2D-3D microfabrication with fs laser

coupled to a uFAB workstation

Stefano Orlando  - stefano.orlando@ism.cnr.it

FemtoLAB in sharing with DiaTHEMA LAb

 
Through the use of fs laser sources it's possible to obtain, with an high reproducibility and periodicity, micro and nano surface structures of materials whose resolution exceeds the diffraction limit. Exceeding this limit makes the technique unique and impracticable with standard optical systems, allowing it to modify in a relatively simple way the chemical-physical properties of the surface of the materials. Laser Induced Periodic Surface Structures (LIPSS) have shown to be effective in varying the optical, mechanical, wettability and electronic properties of the surface (e.g. by introducing defects and electronic states in the semiconductor bandgap), as much as to open up new perspectives for the application of materials which, in their bulk form, have very different properties. In addition to the micro- and nano-structuring of surfaces, this technique allows to create color centers within materials with a wide band gap (e.g. ionic crystals and diamonds) or to create microfabrications or 3D chemical transformations within solids transparent to radiation laser.
 

TECHNICAL SPECIFICATIONS

Spectra Physics Ti:Sa “fs” Laser

  • Spitfire Pro - Regenerative Amplifier  
    • TEM00 
    • ʎ= 800 nm
    • Emax = 4 mJ 
    • RepRate = 1kHz;  
    • timpulso = 120 fs;  
    • ʎSHG = 400 nm;  
    • Emax@400= 1.5 mJ

Newport uFAB Workstation

  • Translation resolution: (x, y) 5 nm; (z) 20 nm;
  • Magnification optics 4x, 20x, 40x

AVAILABLE TECHNIQUES

Use of single or double pulse configurations with time delays ranging from 100 fs to 2 ns

  • Micro and nano-texturing of the surface of any material;
  • microfabrication within the transparent solids
  • creation of color centers in large band gap materials

Scanning electron microscopy images of structures fabricated by 2-photon lithography. All the samples reveal the three-dimensional nature of the microstructures. The scale bars are 20 μm in (a), (c), (d), (e), and 10 μm in (b) and (f)

 

Optical microscopy images of 100 vertical graphitic walls embedded in a diamond plate (left) and a Fresnel lens for far-IR fabricated on a diamond plate surface (right)

 

SAMPLES

  • Max workable size:

    • Software limitation: 50 x 50 mm2 (x,y);  5 mm (z);

    • With manual positioning: 100 x 100 mm2 (x,y); 5 mm (z).

USED FOR

  • surface nanostructuring

  • surface graphitizations

  • internal graphitizations

  • creation of color centers

  • realization of microchannels in bulk materials

  • diffraction gratings

 

CASE STUDIES

Surface nanostructuring to optimize the absorption of light in solar concentrators

The treatment with ultrashort pulse laser of diamond surfaces represents an innovative solution to increase the limited absorbance of the solar spectrum resulting from the wide bandgap of the diamond itself. This treatment is able to produce a material such as black diamond, introducing defects in the bandgap and nanostructuring the surface so as to effectively trap the photons of incident solar radiation.

See:

  • FP7-Energy Collaborative - E2PHEST2US, Grant Agreement n.241270 (2010-2012)
  • FP7-Energy FET - ProME3THE2US2, Grant Agreement n.308975 (2013-2016)
  • H2020 FET-OPEN - AMADEUS, Grant Agreement n.737054 (2017-2020)
  • Daniele M., Trucchi, Advanced Energy Materials 8, 1802310 (2018) DOI: 10.1002/aenm.201802310
 
 
 
 

Creation of color centers in large gap materials (e.g. ionic crystals)

  • Creation of conductive traces within insulating materials (eg graphite traces inside diamond);
  • creation of micro-channels by self-focusing the laser beam using long focal length lenses (> >1 m).

See: Sergey M., Avanesyan, Appl. Surf. Sci. 248, 129 (2005)
DOI:10.1016/j.apsusc.2005.03.014

 
 

Laser surface treatment of polymers

Polymers are progressively replacing metals and metal alloys in technological applications and there is great interest in physico-chemical treatments for the modification of surface properties. The purpose of these research activities is the modulation of the physical and chemical properties of polymeric surfaces in order to improve their performance in some applications such as solar cells and the automotive sector. Laser treatments are of particular interest to morphologically and chemically modify a polymer. In order to achieve this goal, we use laser sources (al fs or al ns) choosing in the appropriate way the laser parameters such as: pulse energy, laser spot size and distance of the focused laser beam from the sample surface. Processed samples are characterized by scanning electron microscopy (SEM), X-ray diffraction (XRD), u-Raman spectroscopy and wettability measurements. The morphological results obtained so far have shown the formation of periodic structures of micrometric and sub-micrometric dimensions such as to maintain the principal chemical characteristics of the polymer surface but modulating the surface physical properties such as wettability.

  • See: A. Guarnaccio et al., Femtosecond Laser Surface Texturing of Polypropylene copolymer for automotive paint applications (in manuscript).
     
    Contact: Ambra Guarnaccio - ambra.guarnaccio@ism.cnr.it
 
 
 
 

Superficial nanostructuring of materials with various morphologies, also bioinspired and determined by

  • use of two fs laser pulses delayed in time in the interval (100 fs-2 ns): 2D-LIPSS;
  • linear polarization of the two incident beams (vertical-horizontal) or circular polarization (left-handed-right-handed).

Effects of different morphologies at the nanoscale

  • modulable variation of the surface properties of materials (eg chemical-physical, optical, etc.). 

Periodic 2D structures with a pitch of about 80 nm were realized for the first time on monocrystalline diamond surfaces using two linearly polarized and perpendicular to each other ultrashort laser beams (2D-LIPSS) obtained through the development of a Michelson interferometer like experimental set-up and one another optically delayed in the range 100 fs - 50 ps. Through this configuration it has already been shown how it's possible to create periodic surface structures whose pitch ranges from 1/4 to 1/10 of the wavelength of the incident radiation. The extent of the delay between the two pulses in the 2D-LIPSS structuring determines the resulting surface's periodicity. The 2D-LIPSS set up allows to control, in the fs-ps time domain, the interference between the incident laser beam and the induced surface plasmonic polaritons in order to allow, at the nanoscale, the fabrication of 2D surface periodic structures, so as to be able to apply this technique in a versatile way to high band-gap materials by modulating their properties that can be linked to both the dimensional scale and the geometry of the surface's nanostructures generated via 2D-LIPSS.

  • See: M. Mastellone et al., submitted, 00 (2020) 00
    Applicazioni DiaTHEMA Lab

Contact: Antonio Santagata - antonio.santagata@ism.cnr.it

 
 
 
 

fs-PLD (@ 800-400 nm) in HV or gaseous atmosphere

fs-PLD (@ 800-400 nm) in HV or gaseous atmosphere

Antonio Santagata  - antonio.santagata@ism.cnr.it

FemtoLAB

 
By focusing a high power pulsed laser beam onto the surface of a solid (target) the ablation process is generated. This is characterized by the formation of a plasma containing a high density of electrons, atoms, ions and clusters, or also, when ultrashort fs pulsed lasers are used, nanoparticles (NPs), are ejected whose compositional features are typical of the ablated material. The technique can be applied for the "vaporization", in the form of plasma, of any material (e.g. oxides, carbides, nitrides, alloys such as quasicrystals, biocompatible materials, etc.) which, through their subsequent deposition, whose process is characterized by complex phenomena taking place and controlling the stoichiometric ratios of the various species present, allow the formation and growth of innovative thin films, or new nanostructures, that could be challenging to be obtained by other methods. The properties of the species deposited depend on the operating conditions employed such as the laser pulse duration as well as its energy density (fluence: J/cm2), the background gas present in the ablation chamber and its pressure, or otherwise vacuum, and the temperature of the substrate on which the ablated species are deposited. Two different laser pulses are available: one having pulse duration of 7ns and the other of 120 fs, which in turn allow the occurrence of different ablation processes. Although their description can be quite complex, these can roughly be distinguished in thermal and non-thermal ablation, respectively. In practical terms, fs laser pulses induce an ablation process that can be modeled in different ways (e.g. Coulomb explosion, photomechanical fragmentation etc.) leading to the formation of two components, 10-20% of plasma and 80-90% of hot NPs whose temperature can be determined, even at high temporal resolutions, by their blackbody-like Planck’s emission (Vis-NIR). On the contrary, when ns pulsed lasers are used just the plasma due to the radiative decay of the electronic excited species emitting in the UV-Vis region, takes place. Because of the laser ablation and deposition system apparatuses available, temporally characterizations of both the induced plasma and blackbody like emissions of the NPs produced, can be performed. It is, therefore, feasible to correlate them to the features of the thin films or nanostructured materials deposited.
 

TECHNICAL SPECIFICATIONS

  • Spectra Physics Ti:Sa “fs” Laser
    Spitfire Pro - Regenerative Amplifier (120 fs; 1kHz; 4 mJ @ 800 nm; SH: 1.5 mJ @ 400 nm)
  • Quanta System Nd:YAG “ns” Laser
    Prototype (7 ns; 10 Hz; 100 mJ @ 532 nm)
  • Time-resolved spectroscopy and imaging
    • Andor iStar “Inductively Charge Couple Device – ICCD” camera (t ≥ 2 ns; Spectral range = 250-900 nm, Pixeldim = 13 μm x 13 μm)
    • ARC SpectraPro 300i monochromator (Spectral range = 200-1000 nm; ʎ/Δʎ = 10000)
  • Vacuum chamber
    • pmin = 10-7 mbar;  
    • Tmax (substrate holder) = 800 °C

AVAILABLE TECHNIQUES

  • Deposition at RT or high temperature (eg. (max 800°C) in HV or controlled gaseous environment (es. Ar, N2, He, O2) of various kind thin films and nanostructured inorganic materials:
    • Carbides, oxides, nitrides, borides, etc.
    • Noble metals (e.g. for plasmonic applications)
  • The PLD activities are also carried out in collaboration with the Physical-Chemistry Laser Laboratory of the University of Basilicata which expands the offer by the availability of other experimental equipments and techniques for characterizing the obtained deposits (e.g. HR-TEM).

 

SAMPLES

  • Solid and flat samples with side dimensions 10 mm x 10 mm (minimum) and 25 mm x 25 mm (maximum); thickness 20 mm (maximum).

USED FOR

  • Optoelectronics

  • Optical components

  • Thermoelectric devices

  • Tribological coatings

  • Magnetic devices

  • Semiconductors

  • Microbattery electrodes

  • Biosensors

  • Biocompatible coatings

  • Plasmonic systems

  • Superconductors

  • Thermionic systems

 
 

CASE STUDIES

Features of the NPs deposited by fs-PLD

The laser ablation and deposition performed by fs pulses allows the direct deposition of NPs:
* having an initial temperature of approximately 3500 K which decays exponentially over time;
* that during their flight towards the substrate onto which they deposit, a variation of their stoichiometry can take place as a consequence of a differential evaporative cooling of the involved species;
* form nanostructured deposits which, compared to the starting target, may miss part of the most volatile components;
* whose initial dimensions are centered around 5-10 nm giving rise, for long deposition times, to agglomerations having dimensions up to a few hundred nm 
* which can give crystalline structures by increasing the substrate temperature although, however, it can affect to a further stoichiometry variation of the final deposit.

See: Angela, De Bonis et al. Appl. Surf. Sci. 258, 9198 (2012)
DOI: 10.1016/j.apsusc.2011.07.077

 
 
 

Deposition of Ag nanoparticles for SERS applications

The direct deposition of NPs by fs-PLD is immediately exploitable for getting nanostructured films which can be extremely beneficial for several applications. For instance, by fs-PLD of Ag, it has been demonstrated how the surfaces obtained, due to their localized surface plasmon resonance (LSPR) properties, are straightforward operating efficiently for enhancing the electromagnetic Raman scattering for the Surface Enhanced Raman Scattering (SERS) technique, whose signal amplification effect can exceed ten orders of magnitude.

See: Angela, De Bonis et al. Surf. Coat. Tech. 207, 279 (2012)   
DOI: 10.1016/j.surfcoat.2012.06.084

 
 

Plasmonic angular tunability of Cu, Ag and Au nanoparticles generated by fs PLD

Noble metals NPs’ angular distribution induced by fs PLD plays a relevant role in providing spatially resolved NPs distribution on top of substrates and characterizing the resulting thin films' properties. As demonstrated by our published study, different grade of Au NPs’ agglomeration follows the NPs’ angular distribution which leads to spatially resolved plasmonic tunability of the obtained deposits offering new perspectives for their application in several fields such as biosensors and optoelectronic devices.

See: Maria Lucia, Pace et al., Appl. Surf. Sci. 374, 397 (2016)
DOI:10.1016/j.apsusc.2016.02.111

Contatto: Ambra Guarnaccio - ambra.guarnaccio@ism.cnr.it

 
 
 
 

Micro- and nano-technological treatments of materials

The Synthesis’ researchers’ knowhow and instrumental facilities available at ISM offer different treatments such as micro and nanostructuring and creation of microchannels and color centers of materials whose are located onto the surface or inside the material, respectively.
The Surface nanostructures obtained on large band gap systems, such as diamond films, have allowed: 1) the modulation of optical properties (e.g. blackdiamond) which have enhanced the absorption of solar radiation used in conversion modules of solar concentrators based on new generation thermionic and thermoelectric technologies, or, 2) the creation of metamaterials obtained as a result of surface graphitization that find application for THz spectral range components. Different treatment processes can be carried out by the use of a micro and nanofabrication workstation µFAB, managed jointly by the DiaTHEMA Lab and Tito Scalo FemtoLab, whose coupling with a Ti:Sa fs laser source, can provide micro and nanometric scale fabrications (micromachining, and internal micro and nanostructuring of materials’ surfaces, etc.). These, as a consequence of their high 1D, 2D or 3D achievable periodicity, can allow the manipulation and control of materials’ optical, electronic, charge transport and electromagnetic radiation – matter interaction, reactivity or more generally chemical-physical properties and therefore their peculiar behaviors (e.g. creation of color centers of high band gap systems, variation of refractive indices and/or surface wettability of materials etc.). In general, due to local features that can be designed and realized at the nanoscale, innovative technological systems that find application in areas such as: photonics, microfluidics, micro and nanoelectronics, optoelectronics, optimization in processes chain such as painting of aesthetic polymeric systems used in the automotive industry, can be obtained.

2D-3D microfabrications by a fs pulsed laser coupled to a uFAB workstation

Deposition of thin films by CVD

Together with the production of thin films and heterostructures, the Synthesis units offers the opportunity of depositing thin films by the Chemical Vapour Deposition – CVD technique.
Since last decade or so ISM has enhanced a state-of-the-art knowhow for the formation and growth of carbon-based materials such as synthetic diamond, amorphous carbon, Diamond-Like Carbon (DLC), nanotubes and graphene, in the form of thin layers suitable for electronic, optical, mechanical, thermal and optoelectronic applications.
At the DiaTHEMA Lab at ISM Montelibretti branch, thin carbon-based layers are deposited using CVD such as the MicroWave-Enhanced (MW-CVD) and the Hot-Filament CVD (HF-CVD) together with the employment of gaseous mixtures of hydrogen, methane, argon and / or nitrogen.
Diamond layers, in particular, are the main topic research which regards their production and optimization in the form of polycrystalline or nanocrystalline deposits performed onto silicon substrate surfaces, as well as carbides and nitrides deposited either over large areas (heteroepitaxy) or monocrystalline onto HPHT (high pressure high temperature) diamond substrates or CVD synthetic ones.
With regard to MW-CVD technique it differs from HF-CVD one in the control of the process, which gives advantages for the growth of a material having a low concentration of defects and impurities which suitable for either electronic devices or for the detection of ionizing radiations. The advantage of the HF-CVD technique is, on the contrary, related to its ability in providing, over large areas, uniform deposition of diamond layers. The applications carbon-based layers obtained by CVD span from the coating of cutting tools to heat dissipation, from radiation detection to power electronics, from nuclear to solar energy conversion and from optoelectronics to quantum computers.

Microwave enhanced CVD Hot-filament CVD

Deposition and growth of materials by PVD

Since the late 1980s, ISM has developed activities and skills regarding the deposition and growth for Physical Vapor Deposition of superconducting, semiconductor, magnetic, and ceramic thin films that are of interest for electronics, sensors, optoelectronics, data storage, ICT and biomedicine applications.
The techniques used range from thermal evaporation and RF-Sputtering to Laser Ablation and Deposition (Pulsed Laser Deposition - PLD). Thanks to the numerous laser sources available and the consolidated experiences acquired over the years by the ISM researchers, PLD represents a technique that can be used in different operating conditions, regulated by both the wavelength of the laser beam and the duration of its pulse as well as by the surrounding environment, that is the presence of: a background gas, a reactive atmosphere or high vacuum. For instance, this technique, whose laser-matter interaction processes and, for sufficiently long pulses (e.g. ns) also those interactions occurring between the laser induced plasma and the laser itself, are strongly dependent on the laser parameters used. The process is based on the "vaporization", in the form of plasma and even nanoparticles when ultrashort pulses, that is in the range of tens of fs are used. PLD can be applied to any inorganic, organic or biological material (e.g. oxides, carbides, nitrides, metals, alloys, polymers, biological materials, etc.) whose subsequent deposition on a support (substrate) is characterized by a complex control of the stoichiometric ratios and properties and dynamics of the various species involved making the laser source parameters and experimental conditions used the key factors for the deposited materials’ features. It follows that the deposition onto the surface of suitable and properly chosen substrates of the vaporized species provide the growth of innovative thin films, or new nanostructured materials. These can be obtained in either as a single or multilayer form or also, when in combination with other techniques such as RF-Sputtering, in order to deposit heterostructure that are otherwise difficult to be grown. ISM has five laboratories employing state-of-the-art PLD which are located at both its Roman branches of Tor Vergata and Montelibretti and at the Southern Italy branch of Tito Scalo (PZ). Because of the different experimental configurations available, the PLD typology to be employed can be chosen on both the laser source features (e.g. pulse duration: 120fs - 30ns, and wavelengths which spans from UV to NIR spectrum interval) or even in case other co-deposition systems or in-situ treatments are required (i.e. occurrind in the same deposition and growth chamber where the thin films or nanostructured materials under study are generated).  To complete the variety of the PVD technique features offered, an electron beam evaporation system, valuable for the development of ultra-thin layers of fluorides, nitrides, carbides and borides, it is also available.

ns-PLD (@532 nm) ns-PLD (@193 nm) ns-PLD (@248 nm) ns-PLD (@1064-532-355-266 nm) Electron beam evaporator fs-PLD (@800-400 nm) Leybold-Heraeus Low Vacuum Evaporator

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