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ADVANCES IN PRODUCTION AND CHARACTERIZATION OF NEAR CRITICAL CARBON FOAM TARGETS Andrea Pazzaglia 1 , David Dellasega 1 , Alessandro Maffini 1 , Valeria Russo 1 , Irene Prencipe 2 , Matteo Passoni 1 1 Dipartimento di Energia, Politecnico di Milano, Milan, Italy 2 Institute of Radiation Physics, Helmholtz–Zentrum Dresden–Rossendorf, Dresden, Germany INTRODUCTION n< n c Undercritical regime n> n c Overcritical regime n~n c Near critical regime Electromagnetica wave propagation Wave damping, high reflection High laser-plasma coupling 2 4 CRITICAL DENSITY PRODUCTION CHARACTERIZATION FOAM SIMULATION LASER-DRIVEN ION ACCELERATION RESULTS CONCLUSION AND FUTURE PERSPECTIVE www.ensure.polimi.it Substrate Plasma Plume Rotating Target Laser Beam Pulsed Laser Deposition (PLD) of nanostructured targets Deposition of different morphologies: Low density Carbon foam Intermediate density Carbon trees Functionally graded Carbon coating Buffer Gas: Ar λ = 532 nm E = 130 mJ P = 50 Pa Gas flow = 80 sccm Substrate-Target distance = 4.5 cm Buffer Gas: Ar λ = 532 nm E = 130 mJ P = 500 Pa Gas flow = 1.4 sccm Substrate-Target distance = 4.5 cm Buffer Gas: Ar λ = 532 nm E = 150 mJ P = 100->700 Pa (linear) Gas flow = 0 sccm Substrate-Target distance = 4.5 cm ~ 10 mg/cm 3 (8 times air density) ~ 150 mg/cm 3 (1/10 bulk density) Gradient from 150 to 10 mg/cm 3 Diffusion Limited Cluster-Cluster Aggregation (DLCA) Brownian motion of nanoparticles (15 nm diameters) in the plasma plume Irreversible sticking of nanoparticles Formation of clusters (from tens to thousands of particles) Deposition of clusters on substrate Passoni, Matteo, et al. "Energetic ions at moderate laser intensities using foam-based multi-layered targets." Plasma Physics and Controlled Fusion 56.4 (2014): 045001. Prencipe, I., et al. "Development of foam-based layered targets for laser-driven ion beam production." Plasma Physics and Controlled Fusion 58.3 (2016): 034019. Passoni, M., et al. "Toward high-energy laser-driven ion beams: Nanostructured double-layer targets." Physical Review Accelerators and Beams 19.6 (2016): 061301 Carbon Foam 1.2 – 4 n c Al 0.75 – 1.5 μm ions n c =5.7 mg/cm3 laser Ion acceleration experiments: - Performed at SLIC (France) in 2014 - Performed at GIST (Rep. of Korea) in 2015-2016 - Performed at HZDR (Germany) in 2017 + 30% enhancement! Zani, A., et al. "Ultra-low density carbon foams produced by pulsed laser deposition." Carbon 56 (2013): 358-365. Raman Spectroscopy SEM & HR-TEM Density measurement = Thickness with SEM Areal Density with new technique based on Energy Dispersive X-ray Spectroscopy (EDS) Semiempirical model Density-pressure measures A new Theoretical Model (solution of transport equation for electron) is under validation → more reliable Prencipe, Irene, et al. "Energy dispersive x-ray spectroscopy for nanostructured thin film density evaluation." Science and Technology of Advanced Materials 16.2 (2015): 025007. We are able to: Produce C coating with tunable ultra-low density (10-150 mg/cm 3 ) on every kind of substrate Produce functionally graded coatings Simulate the material at the mesoscale (>10 nm) Measure the mean density with novel method based on EDS Design the foam based target for laser-driven enhaced ion acceleration ERC - 2014 - CoG No. 647554 Advances in production, characterization and simulation of of ultra-low density carbon CARBON FOAM @ Micro and Nano-structured Materials Laboratory (Nanolab) (Politecnico di Milano) Exploited as a near critical coating enhanced laser-driven ion acceleration γ= 0.723 10 18 Τ 3 λ 2 2 +1 γ ≈ 4.6 = 10 20 Τ 3 λ = 532 nm ≈ 5.7 Τ 3 C fully ionized (γ=1) Relativistc transparency FOAM BASED TARGET The C foam che be deposited on every kind of substrate The foam suffer from laser damaging designed foam based target Cardioid Laser Focusing Damage Necessity of: 1. not reflecting holder 2. high shot distance Different Solutions In the future we will be able to: Produce C coatings with femtoseconds laser PLD and High Power Impulse Magnetron Sputtering Increse the control on the C foam parameters (lower density, designed gradients ) Use laser-driven ion for applied science (ion beam analysis, neutron imaging , ion implantation, radiation damaging) Heigh [μm] 0 8 4

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Page 1: ADVANCES IN PRODUCTION AND CHARACTERIZATION OF NEAR … · ADVANCES IN PRODUCTION AND CHARACTERIZATION OF NEAR CRITICAL CARBON FOAM TARGETS Andrea Pazzaglia1, David Dellasega1, Alessandro

ADVANCES IN PRODUCTION AND CHARACTERIZATION OF NEAR CRITICAL CARBON FOAM TARGETS Andrea Pazzaglia1, David Dellasega1, Alessandro Maffini1, Valeria Russo1, Irene Prencipe2, Matteo Passoni1

1Dipartimento di Energia, Politecnico di Milano, Milan, Italy2Institute of Radiation Physics, Helmholtz–Zentrum Dresden–Rossendorf, Dresden, Germany

INTRODUCTION

n<nc

Undercritical regimen>nc

Overcritical regimen~nc

Near critical regime

Electromagnetica wave propagation

Wave damping, high reflection

High laser-plasma coupling

𝑛𝑐 = γ𝑚𝑒𝜔

2

4𝜋𝑒

CRITICAL DENSITY

PRODUCTION CHARACTERIZATION

FOAM SIMULATION

LASER-DRIVEN ION ACCELERATION RESULTS

CONCLUSION AND FUTURE PERSPECTIVE

www.ensure.polimi.it

Substrate

Plasma Plume

Rotating

TargetLaser Beam

Pulsed Laser Deposition (PLD) of nanostructured targets

Deposition of different morphologies:

• Low density Carbon foam

• Intermediate density Carbon trees

• Functionally graded Carbon coating

Buffer Gas: Arλ = 532 nmE = 130 mJP = 50 PaGas flow = 80 sccmSubstrate-Target distance = 4.5 cm

Buffer Gas: Arλ = 532 nmE = 130 mJP = 500 PaGas flow = 1.4 sccmSubstrate-Target distance = 4.5 cm

Buffer Gas: Arλ = 532 nmE = 150 mJP = 100->700 Pa (linear)Gas flow = 0 sccmSubstrate-Target distance = 4.5 cm

~ 10 mg/cm3 (8 times air density)

~ 150 mg/cm3 (1/10 bulk density)

Gradient from 150 to 10 mg/cm3

Diffusion Limited Cluster-Cluster Aggregation (DLCA)

• Brownian motion of nanoparticles (15 nm diameters) in the plasma plume

• Irreversible sticking of nanoparticles• Formation of clusters (from tens to thousands of

particles)• Deposition of clusters on substrate

Passoni, Matteo, et al. "Energetic ions at moderate laser intensities using foam-based multi-layered targets." Plasma Physics and Controlled Fusion 56.4 (2014): 045001.

Prencipe, I., et al. "Development of foam-based layered targets for laser-driven ion beam production." Plasma Physics and Controlled Fusion 58.3 (2016): 034019.

Passoni, M., et al. "Toward high-energy laser-driven ion beams: Nanostructured double-layer targets." Physical Review Accelerators and Beams 19.6 (2016): 061301

Carbon Foam1.2 – 4 nc

Al 0.75 – 1.5 μm

ions

nc=5.7 mg/cm3laser

Ion acceleration experiments:- Performed at SLIC (France) in 2014- Performed at GIST (Rep. of Korea) in 2015-2016- Performed at HZDR (Germany) in 2017

+ 30% enhancement!Zani, A., et al. "Ultra-low density carbon foams produced by pulsed laser deposition." Carbon 56 (2013): 358-365.

Raman Spectroscopy SEM & HR-TEMDensity measurement

𝜌 = 𝜏 𝑡Thicknesswith SEM

Areal Density with new techniquebased on Energy Dispersive X-raySpectroscopy (EDS)

Semiempirical model Density-pressure measures

A new Theoretical Model (solution of transportequation for electron) isunder validation → more reliable

Prencipe, Irene, et al. "Energy dispersive x-ray spectroscopy for nanostructured thin film density evaluation." Science and Technology of Advanced Materials 16.2 (2015): 025007.

We are able to:• Produce C coating with tunable ultra-low density (10-150 mg/cm3) on every kind of substrate• Produce functionally graded coatings• Simulate the material at the mesoscale (>10 nm)• Measure the mean density with novel method based on EDS• Design the foam based target for laser-driven enhaced ion acceleration

ERC-2014-CoG No. 647554

• Advances in production, characterization and simulation of of ultra-low density carbon CARBON FOAM

• @ Micro and Nano-structured Materials Laboratory (Nanolab) (Politecnico di Milano)

• Exploited as a near critical coating enhanced laser-driven ion acceleration

γ = 0.723 𝐼 1018 Τ𝑊 𝑐𝑚3 λ2 𝜇𝑚2 + 1

γ ≈ 4.6𝐼 = 1020 Τ𝑊 𝑐𝑚3

λ = 532 nm 𝑛𝑐 ≈ 5.7 Τ𝑔 𝑐𝑚3C fully ionized (γ=1)

Relativistc transparency

FOAM BASED TARGET• The C foam che be deposited on every kind of substrate• The foam suffer from laser damaging designed foam based target

Cardioid Laser Focusing Damage

Necessity of:1. not reflecting holder2. high shot distance Different Solutions

In the future we will be able to:• Produce C coatings with femtoseconds laser PLD and High Power Impulse

Magnetron Sputtering• Increse the control on the C foam parameters (lower density, designed

gradients)• Use laser-driven ion for applied science (ion beam analysis, neutron

imaging, ion implantation, radiation damaging)

Heigh [μm] 0

8

4