'Buffer gas' presentation slideshows

Introduction to PhD research

Introduction to PhD research. Edward Gash 30 June 2004. Introduction to PhD research. Investigation into the role of naphthalene cations in the interstellar medium. Edward Gash 30 June 2004. Absorption lines observed when light from a distant star passes through an interstellar cloud.

543 views • 44 slides

Search for physics beyond the Standard Electroweak model with the WITCH experiment

Search for physics beyond the Standard Electroweak model with the WITCH experiment. Simon Van Gorp PhD defense 28 th of February, Leuven. Promotor: Prof. Dr. Nathal Severijns. Outline. The WITCH experiment Motivation Status Overview Simbuca , a Penning trap simulation package

506 views • 38 slides

Laser Spectroscopy for Nuclear Structure Charge Radii and Moments

Laser Spectroscopy for Nuclear Structure Charge Radii and Moments. Peter Mueller. Laser Spectroscopy of Radioactive Isotopes. Nuclear charge radii + nuclear moments. New opportunities with CARIBU & ATLAS upgrade.

383 views • 38 slides

WITCH status + Simbuca, a Penning trap simulation program

WITCH status + Simbuca, a Penning trap simulation program. S. Van Gorp, M. Breitenfeldt , V. De Leebeeck,T. Porobic, G. Soti, M. Tandecki, F. Wauters, N. Severijns (K.U.Leuven, Belgium) , M. Beck, P. Friedag, C. Weinheimer (Univ. Munster, Germany) , M. Beck (Univ. Mainz, Germany) ,

511 views • 37 slides

Laser Laboratory (-ies)

315 views • 31 slides

Inventory of consumables

Inventory of consumables. Food Water Oxygen Per day and for entire length of stay Factor in back up in case of emergency?. Food. Men 2500 calories per day 1260000 for entire duration Woman 2000 calories per day 1008000 for entire duration For a crew of 10 (5 men & 5 woman)

327 views • 21 slides

Unusual Time-Dependant Absorption of Naphthalene-Gas mixtures, after

UV. Unusual Time-Dependant Absorption of Naphthalene-Gas mixtures, after UV flash photolysis, measured with Cavity Ring-Down Spectroscopy. Kieran Lynch Supervisors: Andy Ruth Michael Mansfield 27/03/02. Outline. Motivation Cavity Ring-Down Spectroscopy

362 views • 21 slides

Practical design of h elical cooling channel

Practical design of h elical cooling channel. Katsuya Yonehara APC, Fermilab. Outline. Show result of 200 MHz base HCC simulation by using analytical electromagnetic field To demonstrate cooling efficiency and compare with other cooling channels Show beam & lattice parameter list

326 views • 20 slides

WELCOME TO

2014 - MRO Dry Gas Seal Reliability Improvement. WELCOME TO. Presenter. Presenter: Ali Shallwani Career Summary: Rotating Equipment Specialist at Nova Chemicals (2014-onwards) Rotating Equipment Engineer at Saudi based petrochemical company (2011-2014)

125 views • 12 slides

Dry Wall Response to the HIB (close-coupled) IFE target

Dry Wall Response to the HIB (close-coupled) IFE target. Presented by D. A. Haynes, Jr. for the staff of the Fusion Technology Institute University of Wisconsin. Summary/Outline.

182 views • 9 slides

Dry Wall Response to the HIB (close-coupled) IFE target

Dry Wall Response to the HIB (close-coupled) IFE target. Presented by D. A. Haynes, Jr. for the staff of the Fusion Technology Institute University of Wisconsin. Summary/Outline.

99 views • 9 slides

217 views • 6 slides

REXTRAP plans for 2005 And future developments

135 views • 5 slides

Components of the Rubidium Apparatus

Components of the Rubidium Apparatus Magnet: Confines the electron beam to go through the aperture separating the source and target chambers. Probe Laser: Allows us to determine the rubidium density and polarization through a Faraday rotation.

88 views • 5 slides

Ion Motion Through an RFQ Varying the q-value Varying the Buffer Gas Pressure The q-value

Ion Motion Through an RFQ Varying the q-value Varying the Buffer Gas Pressure The q-value We define the q-value for an ion inside an RFQ device to be:. Where: e = the charge on the ion V pp = the peak-to-peak voltage applied to the RFQ m = the mass of the ion

208 views • 4 slides

Ion Motion Through an RFQ Varying the q-value Varying the Buffer Gas Pressure The q-value

Ion Motion Through an RFQ Varying the q-value Varying the Buffer Gas Pressure The q-value We define the q-value for an ion inside an RFQ device to be:. Where: e = the charge on the ion V pp = the peak-to-peak voltage applied to the RFQ m = the mass of the ion

42 views • 4 slides