IMP EPD End Point Detector

Similar documents
Advanced Sensor Fabrication Using Integrated Ion Beam Etch and Ion Beam Deposition Processes

Differentially pumped quadrupole SIMS probe on FIBbased and two-beam microscopes

Precision Without Compromise

Wavelength Dispersive XRF Spectrometer

Specimen Preparation Technique for a Microstructure Analysis Using the Focused Ion Beam Process

In-Situ Low-Angle Cross Sectioning: Bevel Slope Flattening due to Self-Alignment Effects

A discussion of crystal growth, lithography, etching, doping, and device structures is presented in

RIX3100. Fully Automated Sequential X-ray Spectrometer System. Product Information

High-Energy Resolution Microcalorimeter EDS System for Electron Beam Excitation

Layer Thickness Analysis of Thin Metal Coatings with. Bruker Nano Analytics, Berlin, Germany Webinar, June 8 th 2017

INA-X System for SNMS and SIMS

X-RAY DIFFRACTION IN SEMICONDUCTOR INDUSTRY AND RESEARCH

2008 Summer School on Spin Transfer Torque

2006 UPDATE METROLOGY

In-line Hybrid Metrology Solutions

Chapter 4 Fabrication Process of Silicon Carrier and. Gold-Gold Thermocompression Bonding

ise J. A. Woollam Ellipsometry Solutions

S. Gupta. The University of Alabama

Electrodeposition of Magnetic Materials

Sputtering Targets for Microelectronics. Sputtering Targets for Semiconductor Applications

Lecture 5. SOI Micromachining. SOI MUMPs. SOI Micromachining. Silicon-on-Insulator Microstructures. Agenda:

Oxidation behavior of Cu nanoclusters in hybrid thin films

We get small. Micron-scale Circuits and Structures from Prototype through Production

METHOD FOR IMPROVING FIB PREPARED TEM SAMPLES BY VERY LOW ENERGY Ar + ION MILL POLISHING

Advanced Materials Analysis with Micro-XRF for SEM

Thin Film Gas Sensor. Nanoelectronics and MEMS Laboratory National Electronics and Computer Technology

SUB-Programs - Calibration range Fe Base for "PMI-MASTER Pro" Spark - mode Fe 000

Why Probes Look the Way They Do Concepts and Technologies of AFM Probes Manufacturing

In-situ Heating Characterisation Using EBSD

Lecture Day 2 Deposition

Fabrication Process. Crystal Growth Doping Deposition Patterning Lithography Oxidation Ion Implementation CONCORDIA VLSI DESIGN LAB

Chapter 1.6. Polished Single-Crystal Silicon, Prime Wafers (all numbers nominal) Wafer Specification Table. Diameter 100 mm 4-inch 150 mm 6-inch

Activities in Plasma Process Technology at SENTECH Instruments GmbH, Berlin. Dr. Frank Schmidt

GDMS. High Resolution GDMS.

COMPATIBILITY OF THE ALTERNATIVE SEED LAYER (ASL) PROCESS WITH MONO- Si AND POLY-Si SUBSTRATES PATTERNED BY LASER OR WET ETCHING

S8 TIGER Series 2. Lab Report XRF 144. Innovation with Integrity. Accurate Quality Control of Tool Steels XRF

h Reclamation Center Lot Number List

General Introduction to Microstructure Technology p. 1 What is Microstructure Technology? p. 1 From Microstructure Technology to Microsystems

SUPPLEMENTARY INFORMATIONS

1 MARCH 2017 FILM DEPOSITION NANOTECHNOLOGY

Development of different copper seed layers with respect to the copper electroplating process

Acoustic Characterization of Materials

Platypus Gold Coated Substrates. Bringing Science to the Surface

Advanced Analytical Techniques for Semiconductor Assembly Materials and Processes. Jason Chou and Sze Pei Lim Indium Corporation

Supporting Information

Nanoscale Imaging, Material Removal and Deposition for Fabrication of Cutting-edge Semiconductor Devices

SEMASPEC Test Method for Metallurgical Analysis for Gas Distribution System Components

In operandi observation of dynamic annealing: a case. Supplementary Material

Epitaxy and Roughness Study of Glancing Angle Deposited Nanoarrays. Hamid Alouach and G. J. Mankey

Electrical and Fluidic Microbumps and Interconnects for 3D-IC and Silicon Interposer

Introduction to CMOS VLSI Design. Layout, Fabrication, and Elementary Logic Design

FRONT END PROCESSES - CLEANING, LITHOGRAPHY, OXIDATION ION IMPLANTATION, DIFFUSION, DEPOSITION AND ETCHING

Oerlikon PVD production solutions for piezoelectric materials

Perpendicular Magnetic Multilayers for Advanced Memory Application

Physical Vapor Deposition (PVD) Zheng Yang

Microanalysis with high spectral resolution: the power of QUANTAX WDS for SEM

Today s Class. Materials for MEMS

Atomic Layer Deposition (ALD)

Progress in Monolithic III-V/Si and towards processing III-V Devices in Silicon Manufacturing. E.A. (Gene) Fitzgerald

Plasma Quest Limited

1. Scope :- 2. Referenced Documents :-

The Physical Structure (NMOS)

Precision Micro-Aperture Catalog

National Nano Fabrication Centre (NNFC)

Transzmissziós és pásztázó elektronmikroszkópos minták készítése ionsugaras vékonyítással

Thermal Evaporation. Theory

CMOS Fabrication. Dr. Bassam Jamil. Adopted from slides of the textbook

Quantitative X-ray Microanalysis Of Submicron Carbide Formation In Chromium (III) Oxide Rich Scale

HIGH SPATIAL RESOLUTION AND HIGH ENERGY RESOLUTION AUGER DEPTH PROFILING

Chapter 3 Silicon Device Fabrication Technology

Title Ta, and Au for 28.8 MeV Alpha Parti. Author(s) Ishiwari, Ryutaro; Shiomi, Naoko; S.

Direct Analysis of Photoresist by ICP-MS. Featuring the Agilent Technologies 7500s ICP-MS

Analysis of steel and its alloys using the GB/T standard and an Agilent 5100 ICP-OES in dual view mode

Overview of CMP for TSV Applications. Robert L. Rhoades, Ph.D. Presentation for AVS Joint Meeting June 2013 San Jose, CA

Electron Beam Induced Processes and their Applicability to Mask Repair

EECS130 Integrated Circuit Devices

the surface of a wafer, usually silicone. In this process, an oxidizing agent diffuses into the wafer

STRUCTURAL ANALYSIS OF TSVS

Application of sprayed carbon nanotubes to light detectors

MODEL PicoMill TEM specimen preparation system. Achieve ultimate specimen quality free from amorphous and implanted layers

Recent Progress on LAPPD

1 nanometer can be the difference ELECTRONICS COATINGS XRF ANALYZERS

Chapter 4: Imperfections (Defects) in Solids

Characterization of Surface Metals on Silicon Wafers by SME-ICP-MS. Featuring the Agilent Technologies 7500s ICP-MS

Analysis of Copper and Copper Base Alloys, Using Shimadzu PDA-7000

Effects of Thin Film Depositions on the EUV mask Flatness

Fundamentals of X-ray diffraction and scattering

Synchrotron X-Ray Topography Measurements on 4H-SiC Epitaxial Layer

UT Austin, ECE Department VLSI Design 2. CMOS Fabrication, Layout Rules

CERTIFIED REFERENCE MATERIALS (CRM)

Analysis of inhomogeneous samples and trace element detection in alloys using QUANTAX Micro-XRF on SEM

What s Hot in Heat Assisted Magnetic Recording (HAMR)

JSM-7800F Field Emission Scanning Electron Microscope

Improving coupling coefficient distribution on BAW filters manufactured on 200mm wafers

A New Development to Eliminate Artifacts during TEM Sample Preparation in the FIB

Applications. SIMS successfully applied to many fields. Catalysts, metals, ceramics, minerals may primarily use imaging

Alloy Steels. Engineering Materials. Introduction : Msc. Shaymaa Mahmood

Managing Anode Effects and Substrate Heating from Rotatable Sputter Targets

O2 Plasma Damage and Dielectric Recoveries to Patterned CDO Low-k Dielectrics

Performance, Reliability, and Versatility. Transpector CPM. Fast, Field-ready Process Monitoring System

Transcription:

IMP EPD End Point Detector An overview of the Hiden Analytical SIMS end point detector system for ion beam etch applications

IMP-EPD Presentation Topics The topics covered in the presentation include: A description of the Hiden IMP end point detector system Example data Hardware and software Integration with process tools

Hiden IMP EPD The Hiden IMP EPD is used for the precise end point detection in the ion beam etch step of the fabrication of thin film devices The Hiden IMP is a differentially pumped, ruggedized secondary ion mass spectrometer for the analysis of secondary ions and neutrals from the ion beam etch process

The IMP EPD system comprises: Stainless Steel Shroud with Sampling Orifice IMP-EPD Ion Optics with Energy Analyser and integral ioniser Triple filter Quadrupole mass analyser Pulse Ion Counting Detector Differentially Pumped Manifold With Mounting Flange to Process Chamber Data System with integration to the process tool

IMP-EPD Photo courtesy of: http://www.ifixit.com/teardown/apple+a6+teardown/10528

Inside a typical ion beam etch chamber IMP- EPD Analyser Photo and Diagram courtesy of EPFL

End Point Detection Mask Mask Material A Mat. A Substrate Mat. B Substrate Mat. B Primary Ion Beam Secondary Ions Mat. A Secondary Ions Mat. B

IMP EPD end point data The data from the IMP end point detector provides a trend analysis for each component of the etch stack. The trend analysis provides a real time display of the entire etch process. The etch resolution combined with the sensitivity of the SIMS technique provides for end point detection to within +/- 5Å. The signals for each layer of the stack materials are coupled with algorithms and data I/O interfaces to provide for automated end point for a broad range of etch end point criteria including rising and falling edge.

Data Output Each peak corresponds to a layer. Each colour corresponds to a metal or other element. A wide peak corresponds to a thick layer When you etch through a layer the signal goes up.

Signal collection

Front end detail

Angle of acceptance b a +/- 5deg ~50% of signal -80-60 -40-20 0 20 40 60 80 100 Relative angular acceptance

Example data - 30 Angstrom Tantalum Layers 14000 Ta / NiFe /Ta 13000 12000 11000 Tantulum 10000 9000 SEM : c/s 8000 7000 6000 5000 4000 3000 Nickel 2000 1000 0 00:00 03:20 06:40 10:00 13:20 16:40 20:00 Time MM:SS The IMP EPD data shows the depth resolution achieved in an ion mill of a: tantalum / nickel iron / tantalum stack where the tantalum layers are 30 Angstroms.

Example Data 100000 Multilayered Sample: FeMn/NiFe/Co/Cu/Co/NiFe/Ta Data Zoom Iron 10000 Copper SEM : c/s 1000 Manganese Cobalt 100 Nickel Tantalum 10 00:00 01:40 03:20 05:00 06:40 08:20 10:00 11:40 13:20 15:00 Time MM:SS

Data Zoom in showing signal variation due to wafer rotation Multilayered Sample: FeMn/NiFe/Co/Cu/Co/NiFe/Ta 16000 15000 14000 Iron 13000 12000 11000 Copper SEM : c/s 10000 9000 8000 Manganese 7000 6000 Cobalt 5000 4000 3000 Nickel 2000 1000 Tantalum 0 04:50 05:10 05:30 05:50 06:10 06:30 06:50 07:10 07:30 07:50 08:10 Time MM:SS

4 Wafers run sequentially: Wafer number 3 has an imperfection recorded The data shows the consistency of analysis in production. Tantalum, Nickel and Silicon are monitored. The third wafer has an imperfection in the recorded silicon signal.

IMP EPD Materials Guide- SIMS analyses all elements dopants and clusters INTERFACE Si/Ga Au/Cr/Al Au/Ti/Ga Mo/Ge Al/In Al/Ga Y/Ba/Cu/MgO NiCr/Cu/NiFe/SiO2 APPLICATION EXAMPLE Identification of SiO2 interface on III-V semiconductor. Au/Cr track identification on aluminium substrates. Precise definition of Au/Ti electrical contacts in GaAs. Precise definition of Mo/Ge interfaces in multifilm Mo/Ge structures. Identification of the interface between two semiconductors Al In As/InP. To etch down to the interface between two layers of AlGaAs separated by a 79 Å GaAs well. The Al signal clearly identified the sandwich. Identification of separate layers in multilayer superconductor materials. Magnetic disc sensor head manufacture.

Layer Mass to monitor Mass number AlTiC Ti 48 CoFe Co 59 Al 2 O 3 Al / AlO 27 / 43 Mass Channels For Layer Materials Ta Ta 181 NiFe Ni 58 Cu Cu 63 FeMn Mn 55 Co Co 59 Ca Ca 40 Ti Ti 48 Cr Cr 52 Ag Ag 107 Au Au 197 Pt Pt 195 Si Si / SiO 28 / 44

Process Variables that affect angle of acceptance include: Wafer tilt The IMP end point detector probe operates over a wide range of wafer tilt angles Surface roughness Primary ion beam energy The sensitivity of the Hiden IMP-EPD is sufficient to provide end point control on 99.9% masked wafers.

End Point Control The end point is controlled with the following criteria: Rising edge or Falling edge with variables: Mass channel Percentage over etch Timed over etch Time out over etch

End Point Control Parameters Endpoint detection is based on a falling or rising trend in the signal; signal intensities and change rates must be entered into the endpoint template for the EPD to operate correctly. Values are needed for the initial delay, slope, limit, falling, % fall, over-etch-time, and % over-etch parameters, which are defined as follows: Initial-delay The delay, in seconds, after the start of the run until end-point detection is enabled. This may be used to ensure endpoint detection ignores any layers above the endpoint layer. slope limit falling Minimum slope value for the rising edge of the endpoint layer. This value is the minimum difference required between the signals read in the current and previous (normally 5 cycles earlier) scan cycles before a trace maximum (and, therefore, an endpoint) will be detected. A suitable value for this parameter can compensate for noise or sample rotation. A minimum intensity limit for the endpoint layer. Signals below this level are regarded as noise or background and are not used for endpoint detection. Set true (1) if the endpoint is to be a falling edge, otherwise set false (0). Falling edge detection is recommended as it allows a level relative to the layer maximum to be used (see % fall). % fall Determines how far below the maximum the signal must fall before the endpoint is signalled. over-etch The time, in seconds, after the endpoint is detected before the endpoint signal is set true. Determines time how long the etc continues after the endpoint. % over-etch Over-etch time as a percentage of the run time. This is the delay after the endpoint is detected before the endpoint signal is set true. It can compensate for varying etch rates. max_over The maximum time, in seconds, that a percentage over-etch may take. This time will not be exceeded etch even if a calculated percentage over-etch time is longer.

IMP EPD end point control HAL4 PP-EPD #10620 SEM : c/s 60000 50000 40000 30000 20000 Endpoint ion signal 100% %fall 10000 limit 0 00:00 00:10 00:20 00:30 00:40 00:50 01:00 01:10 01:20 01:30 01:40 Time mm:ss L1/L3 L2 Substrate Start Endpoint set clear set clear initial-delay over-etch-time or %over-etch Normal endpoint max_over-etch Endpoint set clear Endpoint where max_over-etch time exceeded

The IMP provides End Point Control- What else does the IMP do? Target Impurity Determination At the start of the etch the ion milling probe provides high sensitivity SIMS spectra for the identification of impurities from surface and primary ion source contamination Residual Gas Analysis The integral electron impact ioniser of the IMP allows for operation as a conventional differentially pumped RGA, with software control for leak detection and gas analysis included

Hiden IMP-EPD users The IMP EPD was developed in the 1980 s for researchers working on new devices based on thin film technology. The research devices of the 1990 s have become full production applications. The 2007 Nobel Prize in Physics was awarded to Albert Fert and Peter Grünberg for the discovery of the Giant magnetoresistance GMR effect. The IMP-EPD is currently in use 24/7 for production of HDD read/write heads based on GMR technology at Seagate, Western Digital, Toshiba and Hitachi Global Storage. The IMP-EPD is currently used in the development of the next generation of devices at the worlds leading research centres including:

Summary IMP EPD for end point detection in ion beam etch processes: End Point resolution; +/- 5 Angstroms IMP-EPD Sensitivity sufficient to work with 99.9% masked wafers Sensitivity sufficient to work with small samples from 6mm 2 to large scale. Process control for production Adaptable to large and small ion beam etch chambers Operates as a residual gas analyzer, RGA