Product Information Version 1.0. ZEISS Xradia 810 Ultra Nanoscale X-ray Imaging at the Speed of Science

Similar documents
Product Information Version 1.1. ZEISS Xradia 410 Versa Submicron X-ray Imaging: Bridge the Gap in Lab-based Microscopy

ZEISS Axiocam 503 color Your 3 Megapixel Microscope Camera for Fast Image Acquisition Fast, in True Color and Regular Field of View

ZEISS Axiocam 512 color Your 12 Megapixel Microscope Camera for Imaging of Large Sample Areas Fast, in True Color, and High Resolution

Low Voltage Electron Microscope

Niklas Norrby 12/17/2010

Hiding In Plain Sight. How Ultrasonics Can Help You Find the Smallest Bonded Wafer and Device Defects. A Sonix White Paper

attocfm I for Surface Quality Inspection NANOSCOPY APPLICATION NOTE M01 RELATED PRODUCTS G

v tome x m microfocus CT

S200 Course LECTURE 1 TEM

Axio Zoom.V16 The Fluorescence Zoom Microscope for Large Fields

A Laser-Based Thin-Film Growth Monitor

Agilent Cary 610/620 FTIR microscopes and imaging systems RESOLUTION FOR EVERY APPLICATION

Growing Tall Poppies: An Authentic Science Experience

Low Voltage Electron Microscope

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

Low Voltage Electron Microscope. Nanoscale from your benchtop LVEM5. Delong America

LVEM 25. Low Voltage Electron Mictoscope. fast compact powerful

Bringing Answers to the Surface

LYNXEYE XE. Innovation with Integrity. High-Resolution Energy-Dispersive Detector for 0D, 1D, and 2D Diffraction XRD

k λ NA Resolution of optical systems depends on the wavelength visible light λ = 500 nm Extreme ultra-violet and soft x-ray light λ = 1-50 nm

:... resolution is about 1.4 μm, assumed an excitation wavelength of 633 nm and a numerical aperture of 0.65 at 633 nm.

Extending Acoustic Microscopy for Comprehensive Failure Analysis Applications

Microscopic Structures

ELECTRON MICROSCOPY AN OVERVIEW

LYNXEYE XE-T. < 380 ev. Innovation with Integrity. Energy. Resolution. High-Resolution Position Sensitive Detector with Superb Energy Resolution XRD

Diffraction, Fourier Optics and Imaging

NanoSpective, Inc Progress Drive Suite 137 Orlando, Florida

EUV and Soft X-Ray Optics

VISUAL PHYSICS ONLINE DEPTH STUDY: ELECTRON MICROSCOPES

Advanced 3D Optical Profiler using Grasshopper3 USB3 Vision camera

Basics of Light Microscopy and Metallography

Discover the difference in efficiency

Katarina Logg, Kristofer Bodvard, Mikael Käll. Dept. of Applied Physics. 12 September Optical Microscopy. Supervisor s signature:...

Fast Laser Raman Microscope RAMAN

Systems Biology. Optical Train, Köhler Illumination

Leading in Desktop SEM Imaging and Analysis

Confocal Imaging Through Scattering Media with a Volume Holographic Filter

LVEM 25. Low Voltage Electron Microscope Fast Compact Powerful.... your way to electron microscopy

Scanning Electron Microscopy. EMSE-515 F. Ernst

Light Microscopy. Upon completion of this lecture, the student should be able to:

Focusing X-ray beams below 50 nm using bent multilayers. O. Hignette Optics group. European Synchrotron Radiation Facility (FRANCE) Outline

microscopy A great online resource Molecular Expressions, a Microscope Primer Partha Roy

Very short introduction to light microscopy and digital imaging

CHAPTER TWO METALLOGRAPHY & MICROSCOPY

Applications of Steady-state Multichannel Spectroscopy in the Visible and NIR Spectral Region

Fabrication of Probes for High Resolution Optical Microscopy

X-ray phase-contrast imaging

Physics 3340 Spring Fourier Optics

Characterization of Surface Structures using THz Radar Techniques with Spatial Beam Filtering and Out-of-Focus Detection

Optical Sensor Systems from Carl Zeiss CORONA PLUS. Tuned by Carl Zeiss. The next generation in the compact class

Scanning electron microscope

ANALYTICAL MICRO X-RAY FLUORESCENCE SPECTROMETER

INTRODUCTION THIN LENSES. Introduction. given by the paraxial refraction equation derived last lecture: Thin lenses (19.1) = 1. Double-lens systems

Transmission electron Microscopy

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

Add CLUE to your SEM. High-efficiency CL signal-collection. Designed for your SEM and application. Maintains original SEM functionality

The Department of Advanced Materials Engineering. Materials and Processes in Polymeric Microelectronics

Transmission Electron Microscopy 9. The Instrument. Outline

Education in Microscopy and Digital Imaging

Fastest high definition Raman imaging. Fastest Laser Raman Microscope RAMAN

Appreciating the very little things: Status and future prospects of TEM at NUANCE

Actinic Review of EUV Masks: Status and Recent Results of the AIMS TM EUV System

Indian Institute of technology Madras Presents NPTEL NATIONAL PROGRAMME ON TECHNOLOGY ENHANCED LEARNING

Development of JEM-2800 High Throughput Electron Microscope

Fast Laser Raman Microscope RAMAN

Diamond X-ray Rocking Curve and Topograph Measurements at CHESS

Application Note. The New 2D Superresolution Mode for ZEISS Airyscan 120 nm Lateral Resolution without Acquiring a Z-stack

Water-Window Microscope Based on Nitrogen Plasma Capillary Discharge Source

Sensitive measurement of partial coherence using a pinhole array

MICROSCOPE LAB. Resolving Power How well specimen detail is preserved during the magnifying process.

Chapter 4 Imaging Lecture 17

Microscope anatomy, image formation and resolution

Development of a High-speed Super-resolution Confocal Scanner

Improving the Collection Efficiency of Raman Scattering

Unit Two Part II MICROSCOPY

Module 4B7: VLSI Design, Technology, and CAD. Scanning Electron Microscopical Examination of CMOS Integrated Circuit

Chapter 16 Light Waves and Color

Optical Characterization of Compound Refractive Lenses

Bandpass Edge Dichroic Notch & More

Supporting Information. for. Visualization of Electrode-Electrolyte Interfaces in LiPF 6 /EC/DEC Electrolyte for Lithium Ion Batteries via In-Situ TEM

Observing Microorganisms through a Microscope

Introduction of New Products

Spatially Resolved Backscatter Ceilometer

Will contain image distance after raytrace Will contain image height after raytrace

M4 TORNADO PLUS. Innovation with Integrity. Super Light Element Micro-XRF Spectrometer. Micro-XRF

Instructions for the Experiment

Waveguiding in PMMA photonic crystals

3D light microscopy techniques

Resolution. Diffraction from apertures limits resolution. Rayleigh criterion θ Rayleigh = 1.22 λ/d 1 peak at 2 nd minimum. θ f D

Ion Beam Lithography next generation nanofabrication

Burton's Microbiology for the Health Sciences

An Off-Axis Hartmann Sensor for Measurement of Wavefront Distortion in Interferometric Detectors

The microscope is useful in making observations and collecting data in scientific experiments. Microscopy involves three basic concepts:

The light microscope

attosnom I: Topography and Force Images NANOSCOPY APPLICATION NOTE M06 RELATED PRODUCTS G

Εισαγωγική στην Οπτική Απεικόνιση

Application Note #548 AcuityXR Technology Significantly Enhances Lateral Resolution of White-Light Optical Profilers

Towards accurate measurements with synchrotron tomography Problems and pitfalls. Robert C. Atwood. Nghia T. Vo, Michael Drakopoulos, Thomas Connolley


Serial Block Face Imaging

Transcription:

Product Information Version 1.0 ZEISS Nanoscale X-ray Imaging at the Speed of Science

Extending the Reach of 3D X-ray Imaging increases the throughput of nanoscale, three-dimensional X-ray imaging by up to a factor of 10. This innovative X-ray microscope (XRM) operates at 5.4 kev, a lower energy that delivers better contrast and image quality for medium to low Z samples and other materials used throughout science and industry. Better contrast enables higher-quality tomographies to be acquired an order of magnitude faster while achieving resolution down to 50 nm. 2

ZEISS : Highest resolution. Higher contrast. Faster. Non-destructive nanoscale imaging ZEISS solutions deliver the world s only nondestructive X-ray imaging with resolution down to 50 nm. Along with both absorption and Zernike phase contrast, employs advanced optics adapted from the synchrotron to deliver industry-best resolution and contrast. This innovative instrument adds a critical, nondestructive step to the traditional imaging workflow to promote breakthrough research in premier labs worldwide. Superior contrast across a wider class of materials By delivering higher contrast at 5.4 kev, Xradia 810 Ultra makes high-resolution X-ray imaging viable for a variety of difficult-to-image materials. Absorption and phase contrast optimize imaging for a diverse range of materials such as polymers, oxides, composites, fuel cells, geological samples and biological materials. Having pioneered nanoscale X-ray imaging at synchrotrons and prominent lab facilities worldwide, ZEISS solutions now optimize XRM for groundbreaking studies at the forefront of research. Extending the boundaries of science and industry By making nanoscale X-ray imaging an order of magnitude faster, optimizes the business case for XRM in both science and indus try. For central microscopy labs, a faster workflow translates into more users being able to leverage the instrument in less time, which in turn extends XRM to a broader base of subscribers. Similarly, 4D and in situ studies of internal structure can be quickly performed and repeated, making these techniques viable in many more applications. And in targeted applications such as digital rock physics used to explore feasibility oil and gas extraction, delivers measurements used to characterize critical parameters such as porosity within a matter of hours. 3

Your Insight into the Technology Behind It Unique among laboratory-based microscopes, leverages the penetration power of X-rays to deliver non-destructive 3D imaging with resolution down to 50 nm, the highest achievable by lab-based microscopes. Flexible contrast modes and unique X-ray optics provide unmatched versatility for a diverse array of applications and sample types. Researchers have long recognized the potential of short wavelength X-rays for achieving high-resolution imaging in the nanometer range. For many years, however, the development of X-ray microscopes (XRM) that could realize this potential was hindered by the limited brightness of laboratory X-ray sources and the difficulty of fabricating suitable X-ray optics. ZEISS s employs optics adapted from synchrotron research to achieve the highest reso lution of any laboratory X-ray microscope, down to 50 nm. By leveraging the non-destructive nature of X-rays, this microscope enables 3D nanoscale imaging for observing microstructural evolution over time (4D). Resolution target: 50 nm lines and spaces 4

Your Insight into the Technology Behind It Transmission X-ray Microscopy (TXM) Architecture The architecture of is conceptually equivalent to that of an optical or transmission electron microscope (TEM): A high-brightness X-ray source is focused onto the specimen by a high-efficiency capillary condenser Fresnel zone plate objectives image transmitted X-rays onto the detector An optional phase ring can be inserted into the beam path to achieve Zernike phase contrast for visualizing features in low-absorbing specimens As the specimen is rotated, images are collected over a range of projection angles that are then reconstructed into a 3D tomographic dataset X-ray Source Capillary Sample Objective Zone Plate Phase Ring (Zernike) Detector (CCD) 5

Your Insight into the Technology Behind It Contrast for diverse sample types offers both absorption and phase contrast to optimize visualization of features of interest in a wide range of samples. Absorption contrast imaging, essentially shadow or projection imaging, utilizes the varying attenuation power of different materials to generate contrast. It is best suited to specimens containing materials of varying density for example, material and pore space. Phase contrast imaging utilizes the refraction of X-rays rather than absorption. It is very sensitive to interfaces between materials of similar density or low absorption (edge enhancement). The Xradia Ultra family employs the Zernike method for phase contrast, whereby the sample is illuminated by an annular beam and a phase ring is inserted in the beam path after the objective. The phase ring shifts the phase of the background light relative to the light scattered by the specimen. The interference of the two beams in the detector plane turns phase shifts into intensity variations. 25 μm 3D view of a bee antennae imaged using phase contrast. Sample courtesy of University of Bristol Imaging Zone Pate Phase Ring 20 μm 3D nanoscale view of a polyamide sample imaged using absorption contrast, exhibiting silica platelets. University of Wroclaw Phase Ring 6

Your Insight into the Technology Behind It Choose X-ray energy to optimize contrast: 5.4 kev or 8.0 kev In XRM, contrast depends on the material being imaged and the X-ray energy used. The Xradia Ultra family comprises Xradia 800 Ultra, operating at 8 kev photon energy, and, operating at 5.4 kev. In general, lower energy X-rays are absorbed more strongly and therefore provide higher contrast. Thus, as long as transmission remains sufficient, the resulting image quality and/or throughput are greatly improved with. For materials of higher density, or thick specimens, the higher X-ray energy of Xradia 800 Ultra may be needed to provide sufficient transmission. Segment Application 5.4 kev Xradia 800 Ultra 8.0 kev Materials Science Polymers preferred Ceramics* Metals* Composites* SOFC Batteries* Natural Resources Carbonate preferred Shale preferred Life Sciences Soft tissue preferred Calcified tissue preferred Bio scaffolds preferred Semiconductor TSV preferred Preferred = optimal choice for higher throughput and contrast *Dependent on the exact material within these materials classes, either 5.4 or 8 may be preferred 7

Your Insight into the Technology Behind It Choose X-ray energy to optimize contrast: 5.4 kev or 8.0 kev 10 μm 10 μm Dentin imaged at 5.4 kev, left, and 8.0 kev, right. At 5.4 kev, image quality is equivalent while acquisition is 10 times faster due to optimized contrast Greater intensity drop at 5.4 kev leads to higher contrast Example where the greater penetration at 8 kev is beneficial. In the highlighted region, transmission of 5.4 kev X-rays is too low to detect variations in local density. Transmission at 5.4 kev is insufficient to discern small variations 8

Your Insight into the Technology Behind It Unique X-ray Optics For X-rays, traditional light or electron optics schemes are not suitable because refraction is extremely weak and X-rays do not get deflected in magnetic fields. Instead, employs proprietary X-ray optics originally developed at synchrotron facilities and optimized by ZEISS for a wide variety of lab-based applications. Highlights include: Reflective capillary condensers, precision-fabricated to match source properties and imaging optics at maximum flux density; Fresnel zone plates, circular diffraction gratings used as objective lenses. Maintaining high resolution and high efficiency requires both very narrow and tall ring structures, leading to a high-aspect ratio construction, a significant challenge in nanofabrication technology. This is addressed by multiple ZEISS patents and years of experience aligning and integrating high-quality optics; Schematic of a Fresnel zone plate Phase rings for Zernike phase contrast; Scanning Electron Micrograph of a Fresnel Zone Plate High contrast and efficiency detectors based on scintillators, optically coupled to a CCD detector. Capillary condenser 9

Tailored Precisely to Your Applications Typical Applications Task offers Oil & Gas Virtual core analysis Nanoscale pore structure measurements for geological samples can now be conducted in a few hours Material Science Study and predict material properties and evolution Measure and identify porosity, cracks, phase distribution etc. Non-destructive, high resolution 4D and in situ studies can now be performed in hours as opposed to more than 1 day Life Sciences Examine both hard and soft tissue Superior contrast, nanoscale 3D X-ray imaging of a variety of bio materials such as polymers for drug delivery, tissue samples, and scaffolds for tissue engineering Semiconductor Process optimization and defect characterization for wafer-level packaging Through-silicon via (TSV), MEMS, and failure analysis of interconnects 10

ZEISS at Work 40 μm Al-Cu eutectic alloy: determine dendritic structure at ROI 50 μm Shale: rapidly determine internal porosity at nanoscale resolution 30 μm 30 µm Dentin: 4D study of tubule occlusion Carbonate: pore network characterization 11

Your Flexible Imaging Solution 2 5 3 6 1 4 5 Workstation and Software Powerful workstation with GPU-based reconstruction XMController for data acquisition XMReconstructor for tomographic reconstruction XM3DViewer for 3D visualization Compatible with a wide range of 3D viewers and analysis programs 6 Microscope architecture for stability, flexibility and ease of use Vibration isolation and thermal control Ability to integrate in situ stages Integrated visible light microscope for sample inspection and alignment 1 X-ray Microscope ZEISS 50 nm spatial resolution for synchrotronquality imaging in the laboratory 2 X-ray Source Options High brightness x-ray source 5.4 kev x-ray energy 3 X-ray Optics High efficiency condenser High resolution, high efficiency zone plate objectives Phase contrast optics (optional) 4 Detector System Optically coupled scintillator with high resolution and sensitivity 12

Technical Specifications Imaging High Resolution Mode (HRES) Large Field of View Mode (LFOV) Spatial resolution 50 nm 150 nm Field of View 16 µm 65 µm Voxel size 16 nm 64 nm Magnification 800x 200x Contrast Modes Absorption Contrast Standard Phase contrast Optional X-ray Source Xradia 800 Ultra Source type Rotating Anode Rotating Anode Target Material Chromium Copper X-ray Photon Energy 5.4 kev 8.0 kev Voltage 35 kev 40 kev Power 0.9 kw 1.2 kw Sample Stage Travel (x, y, z) 12, 8, 12 mm Rotation 280 Load capacity 1 kg Features Xradia 800 Ultra Automated image alignment for tomographic reconstruction* HRES and LFOV modes LFOV mode Integrated visible light microscope GPU based tomographic reconstruction Comprehensive software suite for data acquisition, reconstruction and visualization * Sufficient room temperature and sample stability required 13

Count on Service in the True Sense of the Word Because the ZEISS microscope system is one of your most important tools, we make sure it is always ready to perform. What s more, we ll see to it that you are employing all the options that get the best from your microscope. You can choose from a range of service products, each delivered by highly qualified ZEISS specialists who will support you long beyond the purchase of your system. Our aim is to enable you to experience those special moments that inspire your work. Repair. Maintain. Optimize. Attain maximum uptime with your microscope. A ZEISS maintenance contract lets you budget for operating costs, all the while avoiding costly downtime and achieving the best results through the improved performance of your system. Choose from service contracts designed to give you a range of options and control levels. We ll work with you to select the service program that addresses your system needs and usage requirements, in line with your organization s standard practices. Our standard preventative maintenance and repair on demand contracts also bring you distinct advantages. ZEISS service staff will analyze any problem at hand and resolve it whether using remote maintenance software or working on site. Enhance Your Microscope System Your ZEISS microscope system is designed for a variety of updates. As a result you ll work more efficiently now, while extending the productive lifetime of your microscope as new update possibilities come on stream. Please note that our service products are always being adjusted to meet market needs and may be subject to change. Profit from the optimized performance of your microscope system with a Carl Zeiss service contract now and for years to come. >> www.zeiss.com/microservice 14

The moment "I think" becomes "I know". This is the moment we work for. // TECHNOLOGY MADE BY CARL ZEISS 15

Carl Zeiss Microscopy GmbH 07745 Jena, Germany BioSciences and Materials microscopy@zeiss.com www.zeiss.com/xrm EN_42_011_080 CZ 08-2013 Design, scope of delivery and technical progress subject to change without notice. Carl Zeiss Microscopy GmbH