NCSLI 2002 August 4-8, 2002 1 Improving Temperature Accuracy for Rapid Thermal Processing at NIST August 4-8, 2002 NCSL International Annual Workshop.

Slides:



Advertisements
Similar presentations
Yu. I. BARANOV and W. J. LAFFERTY Optical Technology Division Optical Technology Division National Institute of Standards and Technology, Gaithersburg,
Advertisements

Aim Calculate local natural convection heat-transfer coefficients for a sphere Calculate the local boundary layer Calculate experimental mean Nusselt.
Temperature measurements Maija Ojanen Licenciate course in measurement science and technology
Optical and electrical characterization of 4H-SiC detectors R. Schifano, A. Vinattieri INFM - Dipartimento di Fisica, Universita ’di Firenze ( Italy) S.
K-Space Associates, Inc. kSA BandiT: Band-edge Thermometry.
Calibration and Status of MOBY Dennis Clark, NOAA/NESDIS Carol Johnson, NIST Steve Brown, NIST Mark Yarbrough, MLML Stephanie Flora, MLML Mike Feinholz,
Fundamentals of Radio Astronomy Lyle Hoffman, Lafayette College ALFALFA Undergraduate Workshop Union College, 2005 July 06.
Modeling the imaging system Why? If a customer gives you specification of what they wish to see, in what environment the system should perform, you as.
Ch 6: Optical Sources Variety of sources Variety of sources LS considerations: LS considerations: Wavelength Wavelength  Output power Output power Modulation.
Overview of Temperature Measurement ME 115 Figures are from “Practical Guidelines for Temperature Measurement” unless otherwise notedwww.omega.com.
VTSLM images taken again at (a) 4.5  (T=84.7K), (b) 3.85  (T=85.3K), (c) 22.3  (T=85.9K), and (d) 31.6  (T=86.5K) using F-H for current and A-C for.
Investigation of Variations in the Absolute Calibration of the Laser Power Sensors for the LIGO Photon Calibrators Stephanie Erickson (Smith College) Mentor:
Scoping Study of He-cooled Porous Media for ARIES-CS Divertor Presented by John Pulsifer Major contributor: René Raffray University of California, San.
NOAA Research and Operations Marine Optical Buoy Design Review July 18-19, 2006 Plan for calibration and maintenance of AHAB Uncertainty Budget: Laboratory.
Improving Uncertainties of Non-Contact Thermometry Measurements Mark Finch Fluke Calibration.
Standards for Radiation Thermometry
Absolute Photon Calibration of Zeiss Observer Z1 Microscope Shawn Miller Department of Optical Sciences University of Arizona, Tucson, AZ Optics.
and 4181 Precision Infrared Calibrators Sales Presentation Measure With Confidence New 4180 Series IR Calibrators.
CLARREO FTS Design: Achieving Robust On-Orbit SI Traceability for IR - Principles Distilled from NIST John A. Dykema, Joe Demusz, Chris Tuozzolo, Norton.
2010 CEOS Field Reflectance Intercomparisons Lessons Learned K. Thome 1, N. Fox 2 1 NASA/GSFC, 2 National Physical Laboratory.
Sergey Mekhontsev National Institute of Standards and Technology Optical Technology Division, Gaithersburg, MD Infrared Spectral Radiance Scale.
NA62 Gigatracker Working Group Meeting 2 February 2010 Massimiliano Fiorini CERN.
Workshop on uncertainties in radiation thermometry Paris, September 7, 2001 Istituto di Metrologia G.Colonnetti The size-of-source effect (SSE) and its.
European Metrology Research Program (EMRP) MeteoMet Project (October 2011) WP3. Traceable measurements methods and protocols for ground based meteorological.
IKE University of Stuttgart Institute for Nuclear Technology and Energy Systems DIRECTORS: PROF. DR.G. LOHNERT, PROF. DR. E. LAURIEN, PROF. DR. M. SCHMIDT.
Predicting Engine Exhaust Plume Spectral Radiance & Transmittance
Real-Time Phase-Stamp Range Finder with Improved Accuracy Akira Kimachi Osaka Electro-Communication University Neyagawa, Osaka , Japan 1August.
Techniques for determination of deep level trap parameters in irradiated silicon detectors AUTHOR: Irena Dolenc ADVISOR: prof. dr. Vladimir Cindro.
Tzveta Apostolova Institute for Nuclear Research and Nuclear Energy,
Chapters Thermodynamics Introduction 1. Equilibrium of mechanical systems: the concept of temperature Three parameters were needed to describe the.
Remote Sensing Basics | August, Calibrated Landsat Digital Number (DN) to Top of Atmosphere (TOA) Reflectance Conversion Richard Irish - SSAI/GSFC.
Slide 1 Progress towards Achieving On-Orbit SI Traceability for the CLARREO IR Payload Hampton, VA, April 10, 2012 Recent results towards verification.
DECam Daily Flatfield Calibration DECam calibration workshop, TAMU April 20 th, 2009 Jean-Philippe Rheault, Texas A&M University.
DFG-NSF Astrophysics Workshop Jun 2007 G Z 1 Optics for Interferometers for Ground-based Detectors David Reitze Physics Department University.
NREL is a national laboratory of the U.S. Department of Energy, Office of Energy Efficiency and Renewable Energy, operated by the Alliance for Sustainable.
Ping Zhu, AHC5 234, Office Hours: M/W/F 10AM - 12 PM, or by appointment M/W/F,
1 Reflected Solar Calibration Demonstration System - SOLARIS K. Thome, D. Jennings, B. McAndrew, J. McCorkel, P. Thompson NASA/GSFC.
Temperature Measure of internal energy of substance Four common scales Celsius (C) Kelvin (k) Fahrenheit (F) Rankine (R)
Cielo Integrated Modeling of External Occulters for Exoplanet Missions Jet Propulsion Laboratory, Caltech Institute of Technology.
Title Light Detectors. Characteristics  Sensitivity  Accuracy  Spectral Relative Response(R( ))  Absolute Sensitivity(S( ))  Signal-to-noise ratio.
Report on CIE Division 2 CIE Session 2007 Beijing.
The affect of adding hot water to cold water on the temperature By: Sarah Fothergill Brodey Wambold.
TNO TPD TNO Science and Industry, 12 May Simulation of processing Influence of secondary electron statistics More Moore SP3WP6.4.
1 P.Rebecchi (CERN) “Monitoring of radiation damage of PbWO 4 crystals under strong Cs 137  irradiation in GIF-ECAL” “Advanced Technology and Particle.
Radiative transfer in the thermal infrared and the surface source term
On a eRHIC silicon detector: studies/ideas BNL EIC Task Force Meeting May 16 th 2013 Benedetto Di Ruzza.
Heat-Flux Measurement - Issues Convection heat transfer effects (Schmidt-Boelter & Gardon) Non-uniform temperature distribution on sensor (Gardon) Different.
Stray Light or Spectral Out-of-Band in MOS/MOBY Steve Brown & Carol Johnson (NIST) Michael Feinholz & Stephanie Flora (MLML) Jim Mueller (CHORS)
G.Villani Aug. 071 CALICE pixel Laser testing update Laser MIP equivalent calibration update Si detector coupled to low noise CA + differentiator (no shaper)
Temperature Measurements ARHAM VEERAYATAN INSTITUTE OF ENGINEERING TECHNOLOGY AND RESEARCH B. E. III, Semester – V (Chemical Branch) SUB: INSTRUMENTS &
Damian Luna Yetziel Sandoval – Alberto Gonzales – 80546
Submitted to Prof. Y. J. Morabiya Prepared by: Solanki Akshay N. Enrollment No
Digital Imaging and Remote Sensing Laboratory thermal infrared data 1 Processing of TIMS data to emissivity spectra TIMS bands for this analysis 8.407,
Calibrating DC Current Shunts: Techniques and Uncertainties Jay Klevens, Ohm-Labs, Inc. © 2011.
1 CLARREO Advances in Reflected Solar Spectra Calibration Accuracy K. Thome 1, N. Fox 2, G. Kopp 3, J. McCorkel 1, P. Pilewskie 3 1 NASA/Goddard Space.
A Study on the Effects of Bandwidth of IR Thermometry Measurements Frank Liebmann NCSLi 2009 © 2008 Fluke Corporation 1 NCSL International 2009.
Thermal Radiation Thermal Engineering Lab ME-4111 Professor: Eduardo Cabrera Damian Luna Yetziel Sandoval – Alberto Gonzales – Fernando.
NCSL-I Workshop and Symposium San Diego CA Aug 7, 2002 Alternative Paths of Traceability in Dimensional Measurements Dennis A. Swyt Chief, NIST Precision.
Temperature Sensors.
Temperature Sensors.
The “Monitor to measure the Integral TRAnsmittance” (MITRA)
Characterization,calibration and traceability for lunar observation
S. Ghosh, M. Muste, M. Marquardt, F. Stern
On Subject Instrumentation Electrical Engg 4th Sem
Detective Quantum Efficiency Preliminary Design Review
Sensor calibration.
Measurement of Flow Velocity
Consistent calibration of VIRR onboard FY-3A to FY-3C
Shanghai Institute of Technical Physics , Chinese Academy of Science
Metrological characterisation of single-photon avalanche diodes
Presentation transcript:

NCSLI 2002 August 4-8, Improving Temperature Accuracy for Rapid Thermal Processing at NIST August 4-8, 2002 NCSL International Annual Workshop and Symposium San Diego, California B.K. Tsai and D.P. DeWitt Optical Technology Division National Institute of Standards and Technology

NCSLI 2002 August 4-8, Objectives Goal: Improve LP calibration accuracy and understand LP performance. Review NIST LP calibration facility and procedures Outline methods of LP characterization Evaluate optical inspection techniques for LPs Make recommendations for accurate LP calibrations

NCSLI 2002 August 4-8, RTP Technology Moore’s Law

NCSLI 2002 August 4-8, RTP Technology Importance 1995 total semiconductor equipment sales was about 15 billion dollars 1995 RTP equipment sales was less than 1% of total sales but is steadily increasing

NCSLI 2002 August 4-8, RTP Technology Types of Processing Batch Multiple wafer processing RTP (Rapid Thermal Processing) Single wafer processing

NCSLI 2002 August 4-8, RTP Technology Comparison of batch vs. RTP processing

NCSLI 2002 August 4-8, RTP Technology Temperature Measurement Challenges Stray light Temperature variations with time Emissivity and reflectivity changes Nonuniform wafer temperature distributions

NCSLI 2002 August 4-8, RTP Test Bed and Lightpipes

NCSLI 2002 August 4-8, ITRS Requirements (International Technology Roadmap for Semiconductors) Goal: To measure RTP temperatures and temperature differences of ±2 °C and ±0.25 °C at 1000 °C. Don Lindholm, SEMATECH, RTP ‘97 Conference SIA Roadmap 1999 goal for 0.18 µm line widths requires that temperature accuracy and repeatability in the RTP environment is better than ±2 °C and ±0.25 °C at 1000 °C

NCSLI 2002 August 4-8, NIST RTP Project Tasks Radiation thermometer in situ calibration using thin-film thermocouples Characterization of new generation radiation thermometers Characterization of wafer radiation environment Collaboration with industry

NCSLI 2002 August 4-8, Temperature Measurement Equation  eff = effective emissivity T = corrected temperature T = spectral radiance temperature = spectral radiance c 2 = second radiation constant

NCSLI 2002 August 4-8, Sodium Heat Pipe Blackbody

NCSLI 2002 August 4-8, Na-HPBB Calibration Uncertainty Factor Uncertainty, k=2 [°C] Na-HPBB radial uniformity0.57 Na-HPBB length uniformity0.10 LPRT noise0.02 LPRT short-term drift0.05 Total0.60

NCSLI 2002 August 4-8, NIST LP Calibration Procedures Inspection visually Clean with ethyl alcohol Set Na-HPBB to temperature Surround LP with water-cooled sleeve Take three cold measurements

NCSLI 2002 August 4-8, NIST LP Calibrations (4 LPs over 1 y)

NCSLI 2002 August 4-8, Other Calibration Procedures Reset sensor factor using Na-HPBB Calibrate before and after use Clean with flame if necessary Keep LP attached to LPRT

NCSLI 2002 August 4-8, LP Spatial Response

NCSLI 2002 August 4-8, LP Spectral Response

NCSLI 2002 August 4-8, LP Temporal Response

NCSLI 2002 August 4-8, Visualization Techniques Sapphire light pipe He/Ne laser (0.95 mW) Quartz-fiber cable Camera Microscope

NCSLI 2002 August 4-8, Photograph of LPRT2-LP2 under microscope using HeNe laser

NCSLI 2002 August 4-8, Photograph of LPRT2-LP2 under microscope without HeNe laser

NCSLI 2002 August 4-8, Laser Illumination LPRT2-LP2 LPRT1-LP2

NCSLI 2002 August 4-8, Integrating Sphere Technique He/Ne laser (0.95 mW) Integrating sphere Current amplifier Digital voltmeter Computer Quartz-fiber cable Silicon detector Sapphire LP

NCSLI 2002 August 4-8, Integrating Sphere Setup HeNe laser (0.95 mW) Integrating sphere A B LP

NCSLI 2002 August 4-8, Integrating Sphere Results (1: LPRT1-LP2, 2: LPRT2-LP2) Before or After Cleaning LP Make LocationDifference ApertureInside[%] Before V V0.43 Before V V0.88 After V V0.11 After V V0.27

NCSLI 2002 August 4-8, Vendor Calibrations Large variability within single vendor Large variability among vendors Differences are a slight function of temperature Need to understand vendor calibrations

NCSLI 2002 August 4-8, Hot versus Cold Calibrations General trend is initial constant period, slight decrease, and increase to final stable period Other patterns observed Correlation of patterns with visualization results

NCSLI 2002 August 4-8, Issues from Hot Calibrations Particle contamination Disturbance of radiation environment Importance of uncertainty analysis Frequency of recalibration Stray radiation

NCSLI 2002 August 4-8, Recommendations 1.Visually inspect the LP first 2.Understand the factory calibration 3.Characterize the LPRT 4.Minimize lateral scattering 5.Calibrate the LPRT as it will be used 6.Calibrate the LPRT using blackbodies that are traceable to a National Measurement Institute, such as NIST 7.Calibrate before and after use