Outgassing studies DC Spark Corrected calibration Mo and Cu data with same calibration data and same experimental environment Field emission measurements.

Slides:



Advertisements
Similar presentations
Introductory Circuit Analysis Robert L. Boylestad
Advertisements

A third temperature scale has been developed, which relates the temperature changes to pressure changes for a fixed volume of gas. This scale is not based.
Unijunction Transistor
PH pH is a unit of measure which describes the degree of acidity or alkalinity (basic) of a solution. It is measured on a scale of 0 to 14. The formal.
BRAKE TEST TEC AIR BOOSTER CALL/SMS:
Atomic Emission Spectroscopy
Field Emission Measurements with CERN DC-Spark System Tomoko MURANAKA Hebrew University / CERN.
Chemical Analysis Qualitative Analysis Quantitative Analysis Determination “Analyze” a paint sample for lead “Determine” lead in a paint sample.
PMT Calibration / Greenhouses Bryan Musolf. PMT Calibration.
Experimental breakdown studies – breakdown diagnostics Linking simulation and experiment Jan W. Kovermann, CERN, RWTH Aachen SLAC workshop July 2009.
A possible new method for Neutrino mass measurement.
Pulsed Cathodic Arc Plasma Diagnostics Optical Emission Spectroscopy Results Aluminium.
1 CC analysis update New analysis of SK atm. data –Somewhat lower best-fit value of  m 2 –Implications for CC analysis – 5 year plan plots revisited Effect.
ATOMIC MASS & AVERAGE ATOMIC MASS
Gases.
Test of the high voltage strength of Pelletron’s gas insulation (18-Dec-2008) Recycler Meeting January 21, 2009 A. Shemyakin.
DC breakdown measurements Sergio Calatroni Present team: Jan Kovermann, Chiara Pasquino, Rocio Santiago Kern, Helga Timko, Mauro Taborelli, Walter Wuensch.
CLIC Breakdown Workshop – CERN, May / 13 Delay Times in Breakdown Triggering CERN, TS-MME Antoine Descoeudres, Sergio Calatroni, Mauro Taborelli.
DC breakdown measurements Sergio Calatroni Present team: Gonzalo Arnau Izquierdo, Jan Kovermann, Chiara Pasquino, Rocio Santiago Kern, Helga Timko, Mauro.
PST 2007 BNL 1 Development of High- performance Polarized e- source at Nagoya University. Nagoya University M.Yamamoto, S.Okumi, T.Konomi N.Yamamoto, A.Mano,
Spectroscopy. Spectroscopy – Getting Ready  What happens when an electron absorbs energy?  What kind of energy can cause this to happen?  Why do different.
Essential Knowledge 1.A.4: Atoms have internal structures that determine their properties. a. The number of protons in the nucleus determines the number.
Lab 12 Atomic spectra and atomic structure
Heat Flow in Welding.
Update on Channel Plate Testing B. Adams, K. Attenkofer, M. Chollet, Z. Insepov, J. McPhate, O. Siegmund, D. Walters, M. Wetstein, Z. Yusof for the LAPPD.
Progress in UCSD Chamber Simulation Experiments – Initial Results from Fast Thermometer Farrokh Najmabadi Sophia Chen, Andres Gaeris, John Pulsifer HAPL.
CLIC Workshop – CERN, October / 17 DC breakdown experiments for CLIC CERN, TS-MME Antoine Descoeudres, Trond Ramsvik, Sergio Calatroni, Mauro Taborelli.
Chapter 09Slide 1 Gases: Their Properties & Behavior 9.
PMT Calibration Bryan Musolf. Goals Transform raw data into graphs for 30 PMTs Observe how the gain and # of photoelectrons (PE) change as a LED intensity.
Composition of constituents The composition of constituent of a mixture is not fix. Air is made up of a mixture of gases. There is ___ % nitrogen gas,
Chapter 5 – Gases. In Chapter 5 we will explore the relationship between several properties of gases: Pressure: Pascals (Pa) Volume: m 3 or liters Amount:
Gases Pressure Boyle’s Law Charles’ Law Gay-Lussac’s Law
The CLIC accelerating structure development program Walter Wuensch CARE05 23 November 2005.
Matter Chemistry is the study of matter Matter takes up space and has mass Matter comes in many different forms.
K. Floettmann WSHQE, OCT. 5, 2006 WSHQE Oct. 5, 2006 Klaus Floettmann Photo cathode requirements for the European XFEL.
DC Spark Test System for CLIC
Abhilash Nair STAR Collaboration University of Illinois at Chicago 1 STAR.
Kinetic Theory of Gases. Ideal Gas Equation PV = n R T (using moles) P V = N k B T (using molecules) – P: pressure (Pa) – V: volume (m 3 ) – N: number.
THE MASS SPECTROMETER describes how a mass spectrum is produced using a mass spectrometer.
Dazhang Huang MUTAC Review LBNL, April 2008 Fermilab MTA 805 MHz RF Program.
Chemistry Chapter 5 Gases Dr. Daniel Schuerch. Gas Pressure Gas pressure is the result of simultaneous collisions of billions of rapidly moving particles.
MKDV upgrade LIU-SPS ABT meeting V. Senaj, L. Ducimetiere, P. Faure November 4 th 2014.
Ideal Gas Law To calculate the number of moles of a contained gas requires an expression that contains the variable n.
Spectroscopic Analysis of DC and RF Breakdowns
Interpretation of Hydrogen Emission Spectra
Progress report on the internal target
The GOOFIE detector as a Ternary Mixture Monitor
Properties of Pure Substances
Yeong-Shin Park and Y. S. Hwang
K. H. Lee, H. Y. Lee, Young-Gi Kim, J. Yang, S. M. Yang, K.J. Chung, Y.S. Na and Y. S. Hwang Residual Gas analysis during Glow discharge cleaning, Baking.
Date of download: 10/27/2017 Copyright © ASME. All rights reserved.
Participation IAP NAS of Ukraine in understanding of vacuum breakdown phenomena Iaroslava Profatilova, V.Baturin, O. Karpenko.
Some Common Properties of Gases
PH pH is a unit of measure which describes the degree of acidity or alkalinity (basic) of a solution. It is measured on a scale of 0 to 14. The formal.
Mass Spectronomer.
Classification of Matter
Classification of Matter
Example A 1.00-L sample of dry air at 25 ⁰C contains mol N2, mol O2, mol Ar, and mol CO2. Calculate the partial pressure.
V. Measurement pressure gauges, flow meters
5.1 Light & Energy F. Electrons & Light
Wave-Particle Duality
How do we get those numbers? Or What’s in the “Black Box”?
VIII. Production of Vacuum
Chap-19: The Kinetic Theory of Gases
Factors Affecting Solubility
SPECTROPHOTOMETRY Applied Chemistry.
Shukui Zhang, Matt Poelker, Marcy Stutzman
Pressure distribution calculations for the PETS
Ideal Gas Law To calculate the number of _______________ of a contained gas requires an _____________ that contains the variable ___.
Inductively Coupled Plasma
Presentation transcript:

Outgassing studies DC Spark Corrected calibration Mo and Cu data with same calibration data and same experimental environment Field emission measurements on the damaged SLAC sample

Motivation Results used for vacuum quality simulations Material differences? Connect outgassing properties to breakdown resistance?

Calibration Extrapolation from nitrogen calibration was expected to be OK for order of magnitude studies In the particular system used, a separate algorithm is used to give hydrogen current, hence a separate calibration is absolutely needed Sorry!

Cu results revisited Pumping speed ~0.02 l/s of nitrogen No argon or water found (differing from measurements by T. Ramsvik on molybdenum)

Cu results revisited Fixed energy 0.8 J Integration time 4 min Amount of released hydrogen and CO gas about the same

Mo results Fixed energy 0.95 J Ratios are the same Same gases Slight overall increase Result is within range of what T. Ramsvik measured No significant material difference observed!

Mo conditioning Virgin spot on cathode No change in outgassing rates Seems there is some energy dependence

SLAC sample Virgin spot in damaged area Difficult to know if the high peaks are probed Fowler—Nordheim plot, so steeper curve means lower field enhancement (beta) I do not trust this value to be real

SLAC sample A re-run of field emission measurement at same spot Beta change from 2 -> 40 Spot not been subjected to more than 1µA

SLAC sample Voltage increased in steps of 2 V (usually 50 V) Observe some discrete current jumps Lower trigger limit for field emission?