Triple Beam FIB-SEM-Ar(Xe) Combined System NX2000

Similar documents
SCIENTIFIC INSTRUMENT NEWS. Introduction. Design of the FlexSEM 1000

Introduction of New Products

Low-energy Electron Diffractive Imaging for Three dimensional Light-element Materials

Deliverable 4.2: TEM cross sections on prototyped Gated Resistors

Fabrication of Probes for High Resolution Optical Microscopy

CD-SEM for 65-nm Process Node

New CD-SEM System for 100-nm Node Process

Ion Beam Lithography: faster writing strategies for features between 150nm and 1um

3-7 Nano-Gate Transistor World s Fastest InP-HEMT

Ion Beam Lithography next generation nanofabrication

Inspection-analysis Solutions for High-quality and High-efficiency Semiconductor Device Manufacturing

NanoSpective, Inc Progress Drive Suite 137 Orlando, Florida

PERFORMANCE IN NANOSPACE PRODUCT OVERVIEW

Development of JEM-2800 High Throughput Electron Microscope

Semiconductor Manufacturing and Inspection Technologies for the 0.1 µm Process Generation

Development of SEM for Realtime 3D Imaging and Its Applications in Biology

Measurement of Microscopic Three-dimensional Profiles with High Accuracy and Simple Operation

FEI Helios NanoLab 600 TEM specimen prep recipe Nicholas G. Rudawski (352) (office) (805) (cell) Last updated: 01/19/17

POLYMER MICROSTRUCTURE WITH TILTED MICROPILLAR ARRAY AND METHOD OF FABRICATING THE SAME

Measurement of Surface Profile and Layer Cross-section with Wide Field of View and High Precision

Introduction of ADVANTEST EB Lithography System

40nm Node CMOS Platform UX8

Functions of the SEM subsystems

PicoMaster 100. Unprecedented finesse in creating 3D micro structures. UV direct laser writer for maskless lithography

DualBeam and FIB capability applied to metals research

Medical Imaging. X-rays, CT/CAT scans, Ultrasound, Magnetic Resonance Imaging

MODULE I SCANNING ELECTRON MICROSCOPE (SEM)

JEM-F200. Multi-purpose Electron Microscope. Scientific / Metrology Instruments Multi-purpose Electron Microscope

PERFORMANCE IN NANOSPACE PRODUCT OVERVIEW

Evaluation of Confocal Microscopy. for Measurement of the Roughness of Deuterium Ice. Ryan Menezes. Webster Schroeder High School.

Carbon Nanotube Bumps for Thermal and Electric Conduction in Transistor

STRUCTURE OF THE MICROSCOPE

2014 HTD-E with options

Quick and simple installation and no maintenance needed. 3 Times More affordable Than a normal SEM. Obtaining results in less than 4 minutes

Chapter 1. Basic Electron Optics (Lecture 2)

NANO MODIFICATION OF THE W(100)/ZrO ELECTRON EMITTER TIP USING REACTIVE ION ETCHING

Digital Rock and Fluid Analytics Services From Schlumberger Reservoir Laboratories. Accuracy from Every Angle

S200 Course LECTURE 1 TEM

Development of a Thin Double-sided Sensor Film EXCLEAR for Touch Panels via Silver Halide Photographic Technology

--> Buy True-PDF --> Auto-delivered in 0~10 minutes. JY/T

Schottky Emission VP FE-SEM

Introduction to Scanning Electron Microscopy

Waveguiding in PMMA photonic crystals

Supplementary Figure S1 X-ray diffraction pattern of the Ag nanowires shown in Fig. 1a dispersed in their original solution. The wavelength of the

Design and Application of a Quadrupole Detector for Low-Voltage Scanning Electron Mcroscopy

Microtools Shaped by Focused Ion Beam Milling and the Fabrication of Cylindrical Coils

Chapter 2 The Study of Microbial Structure: Microscopy and Specimen Preparation

INTRODUCTION We believe that every laboratory working in the field of nanotechnology needs an SEM, therefore we would like to introduce to you our IEM

Section 2: Lithography. Jaeger Chapter 2 Litho Reader. The lithographic process

Lithographic Performance and Mix-and-Match Lithography using 100 kv Electron Beam System JBX-9300FS

Development of Orderly Micro Asperity on Polishing Pad Surface for Chemical Mechanical Polishing (CMP) Process using Anisotropic Etching

Section 2: Lithography. Jaeger Chapter 2 Litho Reader. EE143 Ali Javey Slide 5-1

Introduction to Electron Microscopy

Park NX-Hivac The world s most accurate and easy to use high vacuum AFM for failure analysis.

Supporting Information

2009 International Workshop on EUV Lithography

Spectroscopy in the UV and Visible: Instrumentation. Spectroscopy in the UV and Visible: Instrumentation

Scanning electron microscope

Unpolarized Cluster, Jet and Pellet Targets

Scanning Electron Microscopy. EMSE-515 F. Ernst

MCR Scanning Electron Microscopy Laboratory Portfolio

MICRO YAW RATE SENSORS

event physics experiments

PICO MASTER 200. UV direct laser writer for maskless lithography

Strata DB235 FESEM FIB

Transmission electron Microscopy

Etch, Deposition, and Metrology Options for Cost-Effective Thin-Film Bulk Acoustic Resonator (FBAR) Production

Characterization of e-beam induced resist slimming using etched feature measurements.

A process for, and optical performance of, a low cost Wire Grid Polarizer

SECONDARY ELECTRON DETECTION

Lecture 7. Lithography and Pattern Transfer. Reading: Chapter 7

IDENTIFICATION OF FISSION GAS VOIDS. Ryan Collette

Project Staff: Feng Zhang, Prof. Jianfeng Dai (Lanzhou Univ. of Tech.), Prof. Todd Hasting (Univ. Kentucky), Prof. Henry I. Smith

Advanced Plasma Technology. High precision film thickness trimming for the TFH industry. Roth & Rau AG September 2009

Development of a Small Residual Gas Analyzer Utilizing the Quadrupole Array Structure Micropole System ~ QL Series ~

Development of Nanoimprint Mold Using JBX-9300FS

Leading in Desktop SEM Imaging and Analysis

Observing Microorganisms through a Microscope LIGHT MICROSCOPY: This type of microscope uses visible light to observe specimens. Compound Light Micros

Demo Pattern and Performance Test

SUPPLEMENTARY INFORMATION

ESCALAB 250: High Performance Imaging XPS

Scanning Electron Microscopy Basics and Applications

NANO 703-Notes. Chapter 9-The Instrument

Hybrid Integration Technology of Silicon Optical Waveguide and Electronic Circuit

Fabrication of a submicron patterned using an electrospun single fiber as mask. Author(s)Ishii, Yuya; Sakai, Heisuke; Murata,

Defense Technical Information Center Compilation Part Notice

Keysight Technologies Why Magnification is Irrelevant in Modern Scanning Electron Microscopes. Application Note

Layout Analysis Floorplan

450mm patterning out of darkness Backend Process Exposure Tool SOKUDO Lithography Breakfast Forum July 10, 2013 Doug Shelton Canon USA Inc.

Upgrade of the ultra-small-angle scattering (USAXS) beamline BW4

Fastest high definition Raman imaging. Fastest Laser Raman Microscope RAMAN

Lecture 5. Optical Lithography

Low Voltage Electron Microscope

High-yield Fabrication Methods for MEMS Tilt Mirror Array for Optical Switches

Basics and applications in nanolithography. E-beam lithography. David López-Romero CRESTEC-ISOM JACA CRESTEC Corp.

Near-field optical photomask repair with a femtosecond laser

Unit Two Part II MICROSCOPY

A NEW TECHNIQUE TO RAPIDLY IDENTIFY LOW LEVEL GATE OXIDE LEAKAGE IN FIELD EFFECT SEMICONDUCTORS USING A SCANNING ELECTRON MICROSCOPE.

Nature Methods: doi: /nmeth Supplementary Figure 1. Resolution of lysozyme microcrystals collected by continuous rotation.

Transcription:

SCIENTIFIC INSTRUMENT NEWS 2017 Vol. 8 M A R C H Technical magazine of Electron Microscope and Analytical Instruments. Technical Explanation Triple Beam FIB-SEM-Ar(Xe) Combined System NX2000 Masahiro Kiyohara *1, Takahiro Sato *2, Shota Torikawa *1 1. Introduction FIB-SEM Systems (FIB: Focused Ion Beam; SEM: Scanning Electron Microscope) are widely used as tools for preparing thin samples for analysis by Transmission Electron Microscope (TEM) and other applications. In recent years, the increasing diversity and miniaturization of structures to be analyzed have spurred researchers to conduct higher-precision analyses. This has resulted in a demand for higher-quality sample preparation techniques, including FIB-SEM systems. To realize this objective requires surmounting a number of challenges, including the following: 1. Nominal thickness for analytical samples have decreased. Consequently, induced damage has increased in significance when structures are observed at the atomic scale. Sample preparation for reducing these effects must be developed. 2. An increasing number of samples require high-resolution analysis by TEM or similar methods. High-quality sample preparation and high throughput for TEM analysis must be consistent and efficient. 3. Requirements for sample thickness uniformity have grown more stringent. As a result, thickness discrepancies due to curtaining effects caused by the material distribution at the sample surface or the interior structure must be resolved. In this regard, FIB-SEM systems are playing an increasingly important role. At Hitachi High-Tech, we are developing technologies responding to the above issues. Multiple methods for resolving the above challenges are presented in this article by using the Triplebeam NX2000 FIB-SEM system (Figure 1). Fig. 1 NX2000 instrument Hitachi High-Technologies Corporation All rights reserved. 2017[36]

2. Triplebeam The strategy typically adopted for addressing challenge 1-1 above by reducing damage due to FIB processing is to apply low-energy argon ion beam at the final processing stage. With Hitachi High-Tech's system, the exposed cross section can be observed by SEM simultaneously during FIB etching process without sacrificing SEM resolution. This enables precise end-point detection at the user defined location. The trend toward miniaturization of structures and the need for higher-precision analysis have increased the demand for higher-quality samples with less surface damage. As shown in Fig. 2, the Triplebeam system a unique instrument configuration developed by Hitachi High-Tech consists of a Focused Ion Beam (FIB), an Electron Beam (EB), and an argon ion beam (Ar) focusing at one coincidence point; 1) the damage layer resulting from FIB processing can be removed by etching with the low-energy Ar ion beam. The key advantages of the Triplebeam system include the following: Ar ion-beam processing can be performed within the same instrument, reducing the time required for the overall sample preparation process. Since the majority of processing steps required for sample preparation are carried out by the FIB, the use of the Ar ion beam can be minimized. This allows curtaining effects sometimes a problematic consequence of Ar ion-beam etching to be minimized. During the preparation of thin samples, bending or curling can occur. It is practically impossible to continue FIB processing which is based on raster scanning for additional processing on bent or curled samples. However, with Ar ion-beam etching in the Triplebeam system, the relatively large diameter beam allows thin samples to be exposed to Ar ion etching entirely, so that additional processing can be performed independent of the sample shape. The status of the Ar ion-beam processing can be monitored by SEM. This makes it possible for operators of the instrument even those with relatively little experience to avoid errors due to over- or under-etching, a frequent problem with dedicated Ar ion beam milling systems. The design advantages of the Triplebeam system s approach to address the challenges described in 1-1 and 1-2 can effectively yield superior high quality results. Key specifications (1) FIB Accelerating voltage: 0.5-30 kv Maximum beam current: 100 na Resolution: 4 nm @ 30 kv, 60 nm @ 2 kv (2) SEM Accelerating voltage: 0.5-30 kv (or 0.7-30 kv when a voltage is applied to the cap electrode) Resolution: 2.8 nm@ 5 kv, 3.5 nm @ 1 kv (3) Ar Accelerating voltage: 0.5-2 kv Maximum beam current: 20 na or more @ 1 kv Si etching rate: 10 nm / min @ 1 kv Fig. 2 Key specifications of NX2000 and basic configuration of the Triplebeam system Hitachi High-Technologies Corporation All rights reserved. 2017[37]

3. High-quality TEM sample preparation using low-energy xenon (Xe) ion beam processing The NX2000 system also includes a new option; a Xe ion beam, which has approximately 3.2 times the mass of Ar ions. Similarly to the Ar ion-beam system, the accelerating voltage of the Xe ion beam can be varied over the range of 0.5-2.0 kv. The added flexibility of the low energy ion system allows for the same system to supply either a Xe ion beam or an Ar ion beam simply by switching the supply gas for the ion source. Fig. 3 shows TEM images of a GaN sample with final-stage processing conducted with an Ar ion beam and a Xe ion beam 2). As is the case for the Ar ion beam, the underlying lattice is clearly visible in the TEM image for the sample using final-stage processing with the Xe ion beam. (a) Sample processed with Ar ion beam (1 kv) (b) Sample processed with Xe ion beam (1 kv) Fig.3 TEM images with two final-stage processing methods. Sample: Single-crystal GaN Instrument: HF-3300 Accelerating voltage: 300 kv Hitachi High-Technologies Corporation All rights reserved. 2017[38]

4. ACE (Anti-Curtaining Effect) Technology To mitigate curtaining effects, Hitachi High-Tech has been involved in the development of Anti-Curtaining Effect (ACE) technology. One component of this technology is a sample-orientation control using microsampling with an axis of rotation, this technique has been widely accepted 3). However, in recent years such conventional methods are becoming insufficient for most advanced devices with increasing complexity of three-dimensional structures. To address this difficulty, we have developed the double-tilt system as a new component for addressing curtaining effects in samples with complex structures typically found in today s cutting-edge high-performance devices. 4) This section describes this new technique. The double-tilt system consists of a standard 5-axis motorized sample stage which is mounted on a 2-axis tilting mechanism. This results in a motorized sample stage with a total of 7 axes of motion. Although each axis can be controlled independently, we have created a user-friendly software control environment to assist operators when carrying out procedures with the instrument. In addition, the double-tilt system can be mounted or unmounted by operators without breaking the vacuum in the sample chamber. Thus, the instrument can also be used as a conventional 5-axis motorized sample-stage instrument. The adoption of the double-tilt system allows the change of direction and incidence angle of the incoming ion beam during TEM sample preparation while monitoring by SEM on a real time basis. Fig. 4 shows a comparison of the preparation results for a 3D NAND flash-memory sample with and without the double-tilt system employed. In 3D NAND flash memory arrays, there are complex structures consisting of multiple differing materials across a wide area of the cross section. For this reason, there are significant curtaining effects under conventional conditions, as shown in Fig. 4(a). In contrast, the double-tilt system realizes multiple incidence angles during the etching process. This results in a drastic reduction of curtaining effects during sample preparation, as shown in Fig. 4(b). (a) Without double-tilt system (b) With double-tilt system Fig.4 Reduction of curtaining effects using the double-tilt system. Sample: 3D NAND flash memory Hitachi High-Technologies Corporation All rights reserved. 2017[39]

5. Conclusions In this article we introduced the Triplebeam system a proprietary technology developed by Hitachi High-Tech as well as two new features of the NX2000: the low-energy Xe ion-beam system and the double-tilt system. On the Triplebeam system, ACE technology, such as the double-tilt system and low-energy Xe ion-beam processing, enables high-quality sample preparation with higher throughput. Hitachi High-Tech is committed to meeting the R&D and quality-control needs of researchers and engineers by reducing the burdens associated with sample preparation and building higher-precision analytical technologies. Notes Triplebeam is a registered trademark of Hitachi High-Tech Science Corporation in Japan. (Registered trademark #5136729) References 1)H. Takahashi et al, The 63rd Annual Meeting of The Japanese Society of Microscopy 2)T. Sato et al, The 72nd Annual Meeting of The Japanese Society of Microscopy 3)K. Kondo et al. The 28th Annual LSI Testing Symposium 4)S. Torikawa et al. The 34th Annual NANO Testing Symposium Authors *1 Masahiro Kiyohara, Shota Torikawa Beam Technology System Design Department Design Division Hitachi High-Tech Science Corporation *2 Takahiro Sato Scientific & Medical Systems Business Group Scientific Systems Product Div, Application Development Dept Hitachi High Technologies Corporation THE HITACHI SCIENTIFIC INSTRUMENT NEWS ー 2017 Vol.8 Hitachi High-Technologies Corporation All rights reserved. 2017[40]