DIEGO TONINI MORPHOLOGY OF NIOBIUM FILMS SPUTTERED AT DIFFERENT TARGET SUBSTRATE ANGLE



Similar documents
MORPHOLOGY OF NIOBIUM FILMS SPUTTERED AT DIFFERENT TARGET SUBSTRATE ANGLE

Sputtered AlN Thin Films on Si and Electrodes for MEMS Resonators: Relationship Between Surface Quality Microstructure and Film Properties

X-ray diffraction techniques for thin films

X-Ray Diffraction HOW IT WORKS WHAT IT CAN AND WHAT IT CANNOT TELL US. Hanno zur Loye

X-ray thin-film measurement techniques

The study of structural and optical properties of TiO 2 :Tb thin films

2. Deposition process

Stress and Microstructure of Sputter Deposited Thin Copper and Niobium Films

Coating Technology: Evaporation Vs Sputtering

Optical Properties of Sputtered Tantalum Nitride Films Determined by Spectroscopic Ellipsometry

Dependence of the thickness and composition of the HfO 2 /Si interface layer on annealing

THIN FILM MATERIALS TECHNOLOGY

Laboratorio Regionale LiCryL CNR-INFM

Burcu Saner, Firuze Okyay, Fatma Dinç, Neylan Görgülü, Selmiye Alkan Gürsel and Yuda Yürüm*

BIOACTIVE COATINGS ON 316L STAINLESS STEEL IMPLANTS

Experiment: Crystal Structure Analysis in Engineering Materials

Characterization of sputtered NiO thin films

Chapter 4 Indium Tin Oxide Films Deposited by d.c. Sputtering

Glancing XRD and XRF for the Study of Texture Development in SmCo Based Films Sputtered Onto Silicon Substrates

Characterization of surfaces by AFM topographical, mechanical and chemical properties

X-ray Diffraction and EBSD

OPTIMIZING OF THERMAL EVAPORATION PROCESS COMPARED TO MAGNETRON SPUTTERING FOR FABRICATION OF TITANIA QUANTUM DOTS

" {h k l } lop x odl. ORxOS. (2) Determine the interplanar angle between these two planes:

COMPARISON OF TEXTURE IN COPPER AND ALUMINUM THIN FILMS DETERMINED BY XRD AND EBSD *

NANOSTRUCTURED ZnO AND ZAO TRANSPARENT THIN FILMS BY SPUTTERING SURFACE CHARACTERIZATION

Spectroscopic Ellipsometry:

EXPERIMENTAL STUDY OF STRUCTURAL ZONE MODEL FOR COMPOSITE THIN FILMS IN MAGNETIC RECORDING MEDIA APPLICATION

New CNLS software for analysis of impedance spectra Outline

Electrochemical Impedance Spectroscopy (EIS): A Powerful and Cost- Effective Tool for Fuel Cell Diagnostics

Effect of the oxide film formed on the electrical properties of Cu-Zn alloy electric contact material

Reactive Sputtering Using a Dual-Anode Magnetron System

TEM study of the sol-gel oxide thin films

BNG 331 Cell-Tissue Material Interactions. Biomaterial Surfaces

Amorphous Transparent Conducting Oxides (TCOs) Deposited at T 100 C

Chapter types of materials- amorphous, crystalline, and polycrystalline. 5. Same as #3 for the ceramic and diamond crystal structures.

Lecture 12. Physical Vapor Deposition: Evaporation and Sputtering Reading: Chapter 12. ECE Dr. Alan Doolittle

STRUCTURAL STUDIES OF MULTIFERROIC THIN FILMS

Crystal Structure of High Temperature Superconductors. Marie Nelson East Orange Campus High School NJIT Professor: Trevor Tyson

Ion Beam Sputtering: Practical Applications to Electron Microscopy

Acoustic GHz-Microscopy: Potential, Challenges and Applications

Atomic Force Microscope and Magnetic Force Microscope Background Information

Bourns Resistive Products

Introduction to X-Ray Powder Diffraction Data Analysis

Cathodic Arc Deposition of superconducting thin films of MgB 2 for RF cavities*

HPPMS/DC-MSIP (Cr,Al,V)N and (Cr,Al,W)N Thin Films for High Temperature Application

SPM 150 Aarhus with KolibriSensor

Neuere Entwicklungen zur Herstellung optischer Schichten durch reaktive. Wolfgang Hentsch, Dr. Reinhard Fendler. FHR Anlagenbau GmbH

DOE Solar Energy Technologies Program Peer Review. Denver, Colorado April 17-19, 2007

Surface characterization of oxygen deficient SrTiO 3

Preparation of ZnS and SnS Nanopowders by Modified SILAR Technique

An Introduction to Electrochemical Impedance Spectroscopy (EIS)

POWDER X-RAY DIFFRACTION: STRUCTURAL DETERMINATION OF ALKALI HALIDE SALTS

SALES SPECIFICATION. SC7640 Auto/Manual High Resolution Sputter Coater

Structure Factors

Improvement of surface porosity and properties of alumina films by incorporation of Fe micrograins in micro-arc oxidation

Module 7 Wet and Dry Etching. Class Notes

Crystal Structure Determination I

For Touch Panel and LCD Sputtering/PECVD/ Wet Processing

SUPERCONDUCTIVITY. PH 318- Introduction to superconductors 1

Chapter 7: Basics of X-ray Diffraction

Microhardness study of Ti(C, N) films deposited on S-316 by the Hallow Cathode Discharge Gun

Optical Properties of Thin Film Molecular Mixtures

Physics 441/2: Transmission Electron Microscope

ELECTROMAGNETIC ANALYSIS AND COLD TEST OF A DISTRIBUTED WINDOW FOR A HIGH POWER GYROTRON

CIRICULUM VITAE 1. PERSONAL. Date of Birth-Place : March 2 nd Balikesir, Turkey

Applications of New, High Intensity X-Ray Optics - Normal and thin film diffraction using a parabolic, multilayer mirror

Laser sintering of greens compacts of MoSi 2

Thermal Resistance, Power Dissipation and Current Rating for Ceramic and Porcelain Multilayer Capacitors

Near-field scanning optical microscopy (SNOM)

and LUMINOUS CHEMICAL VAPOR DEPOSITION INTERFACE ENGINEERING HirotsuguYasuda University of Missouri-Columbia Columbia, Missouri, U.S.A.

Keysight Technologies How to Choose your MAC Lever. Technical Overview

1. PECVD in ORGANOSILICON FED PLASMAS

Current and Temperature Ratings

ISSN X CODEN (USA): PCHHAX

X-Ray Study of Soft and Hard Magnetic Thin Films

X-ray diffraction in polymer science

Nanoelectronics 09. Atsufumi Hirohata Department of Electronics. Quick Review over the Last Lecture

Matter Waves. Home Work Solutions

Al 2 O 3, Its Different Molecular Structures, Atomic Layer Deposition, and Dielectrics

Interfacial thermal resistance of Au/SiO 2 produced by sputtering method

MOLECULAR DYNAMICS INVESTIGATION OF DEFORMATION RESPONSE OF THIN-FILM METALLIC NANOSTRUCTURES UNDER HEATING

6) How wide must a narrow slit be if the first diffraction minimum occurs at ±12 with laser light of 633 nm?

Introduction to VLSI Fabrication Technologies. Emanuele Baravelli

Micro-Power Generation

Ultra-High Density Phase-Change Storage and Memory

Etudes in situ et ex situ de multicouches C/FePt

X-ray Diffraction (XRD)

Metrology of silicon photovoltaic cells using coherence correlation interferometry

How To Understand Light And Color

5. Scanning Near-Field Optical Microscopy 5.1. Resolution of conventional optical microscopy

O6: The Diffraction Grating Spectrometer

Basic Properties and Application Examples of PGS Graphite Sheet

Deposition of Silicon Oxide, Silicon Nitride and Silicon Carbide Thin Films by New Plasma Enhanced Chemical Vapor Deposition Source Technology

High Rate Oxide Deposition onto Web by Reactive Sputtering from Rotatable Magnetrons

OLED display. Ying Cao

Laboratory #3 Guide: Optical and Electrical Properties of Transparent Conductors -- September 23, 2014

Transcription:

UNIVERSITÀ DEGLI STUDI DI PADOVA SCIENCE FACULTY MATERIAL SCIENCE DEGREE INFN LABORATORI NAZIONALI DI LEGNARO DIEGO TONINI MORPHOLOGY OF NIOBIUM FILMS SPUTTERED AT DIFFERENT TARGET SUBSTRATE ANGLE

2 QUESTIONS What is the effect of target substrate angle on the film properties? How the film morphology varies changing target substrate angle?

DEPOSITIONS MADE AT DIFFERENT TARGET SUBSTRATE ANGLE FILM MORPHOLOGY CRYSTAL STRUCTURE THICKNESS AFM IMAGING ELECTROCHEMICAL IMPEDANCE SPECTROSCOPY SUPERCONDUCTING PROPERTIES T C MEASURE RRR MAGNETO-OPTICAL X-RAY DIFFRACTION TEXTURE ANALYSIS

MULTI-ANGLE SAMPLE HOLDER 7 substrates coated in the same run Almost identical process conditions for each sample

DC MAGNETRON SPUTTERING LOWER T C AND RRR INCREASING TARGET SUBSTRATE ANGLE

PULSED MAGNETRON SPUTTERING BETTER PROPERTIES FOR PULSED CURRENT DEPOSITION THERE IS STILL THE SAME ANGLE DEPENDENCE OF T C AND RRR

DC MAGNETRON SPUTTERING WITH SUBSTRATE HEATING T RRR C (K) 25 9.6 9.4 20 9.2 15 9.0 8.8 10 8.6 5 8.4 Substrate temperature kept at 600 C during process 1. Better properties 2. Less angle sensitivity 8.2 0 00 15 15 30 30 45 45 60 60 75 75 90 90 deposition angle (degrees)

XRD SPECTRA OF FILM DEPOSITED AT DIFFERENT TARGET SUBSTRATE ANGLE 100 110 Relative Intensity 80 60 40 20 200 211 220 310 222 321 15 degrees 0 20 40 60 80 100 120 140 2 Theta (degrees) 75 degrees 60 degrees 45 degrees 30 degrees

ESTIMATED GRAIN DIMENSION crystallite dimension (Angstrom) D = 0.9λ cos( θ ) (2θ ) 140 120 100 80 60 15 30 45 60 75 deposition angle (degrees)

d 110 OF CRYSTAL PLANES 3,0 2 ( ) d sin = hkl θ nλ 2,8 2,6 2,4 d 110 (Angstrom) 2,2 2,0 1,8 1,6 1,4 1,2 1,0 15 30 45 60 75 deposition angle (degrees)

TEXTURE ANALYSIS

DC MAGNETRON SPUTTERING 0 gradi 15 gradi 30 gradi 45 gradi 60 gradi 75 gradi

PULSED MAGNETRON SPUTTERING 0 gradi 15 gradi 30 gradi 45 gradi 60 gradi 75 gradi

TEXTURE ANALYSIS DC VS PULSED MAGNETRON SPUTTERING 50 DC PULSED Φ max counts (degrees) 40 30 20 10 0 0 15 30 45 60 75 90 deposition angle (degrees)

ATOMIC FORCE MICROSCOPY TOPOGRAPHIC IMAGES 15 gradi 30 gradi 45 gradi 60 gradi 75 gradi 90 gradi

ATOMIC FORCE MICROSCOPY DC MAGNETRON SPUTTERING 20 20 18 18 16 16 14 14 roughness (nm) 12 10 8 6 roughness (nm) 12 10 8 6 4 4 2 2 0 0 15 30 45 60 75 90 0 0 15 30 45 60 75 90 deposition angle (degrees) deposition angle (degrees) Variable thickness Uniform thickness

ATOMIC FORCE MICROSCOPY PULSED MAGNETRON SPUTTERING I campioni depositati in corrente pulsata sono sistematicamente più rugosi

ELECTROCHEMICAL IMPEDANCE SPECTROSCOPY V ( t) = V0 cos( ωt) I( t) = I 0 cos( ωt ϕ ) Z = V ( t) I( t) = Z 0 cos( ωt) cos( ωt ϕ) Z = Z 0e jϕ

ELECTROCHEMICAL IMPEDANCE SPECTROSCOPY NYQUIST PLOT FLAT ELECTRODE: 6 ideally flat electrode porous electrode Real part of impedance represents R s at any frequency Im(Z) /arbitrary units 4 2 Immaginary part does not vary with frequency NYQUIST PLOT IS A VERTICAL LINE POROUS/ROUGH ELETRODE: 0 0 2 4 6 Re(Z) / arbitrary units The apparent capacity C dl depends on frequency because the penetration length of electric field inside the pores raises when decreasing frequency. NYQUIST PLOT IS A 45 INCLINED LINE

ELECTROCHEMICAL IMPEDANCE SPECTROSCOPY DC MAGNETRON SPUTTERING VARIABLE FILM THICKNESS Up to 45 there is porous electrode behaviour Film deposited at higher angles are less thick so resistence is greaer

ELECTROCHEMICAL IMPEDANCE SPECTROSCOPY DC MAGNETRON SPUTTERING COMPARISON BETWEEN FILM WITH DIFFERENT THICKNESS AND FILM WITH CONSTANT THICKNESS Films with the same thickness have the same resistance There is a maximum in capacity at 60 target substrate angle

ELECTROCHEMICAL IMPEDANCE SPECTROSCOPY DC MAGNETRON SPUTTERING Films with the same thickness measures in passivaton condition Imposed potential to create a passivation layer on the film Oxide tichkness depends only on applied potential Oxide growth follows niobium film morphology Capacity shows the same angle dependence of non oxidized films

ELECTROCHEMICAL IMPEDANCE SPECTROSCOPY PULSED MAGNETRON SPUTTERING R = C cont ac C C pulsed ac pulsed ac 100

MAGNETO-OPTICAL ANALYSIS OFHC copper substrate (not electropolished) Target substrate angle: 0 Good connectivity respect to vortex penetration Target substrate angle: 45 Vortex penetrate along substrate discontinuity

SIMULATION OF THIN FILM GROWTH 0 15 30 45 60 75 85

CONCLUSIONS s.c. and transport properties 9.625 9.4 9.220 DC DC PULSED PULSED HEATED HEATED T C (K) RRR 9.0 15 8.8 8.6 10 8.4 8.2 5 8.0 7.80 0 15 30 45 60 75 90 0 15 30 45 60 75 90 deposition angle (degrees) deposition angle (degrees) Properties depend on target substrate angle Pulsed magnetron sputtering and heating of the substrate reduce the angle dependence

CONCLUSIONS Crystal structure Films deposited at higher angles tend towards amorphization Lattice parameter has a maximum at 60 target subtrate angle (110) crystal planes of the growing film orient along niobium atoms arrival direction This effect is reduced using pulsed magnetron deposition

CONCLUSIONS morphology 1.4 1.2 Impedance spectroscopy AFM simulated normalized intensity 1.0 0.8 0.6 0.4 0.2 0.0 0 15 30 45 60 75 90 deposition angle There is a maxmum in roughness between 60 and 75 target substrate angle This is not a thickness effect but is due to deposition dynamics

Fine.