ETCHING OF COPPER COATED MYLAR TUBES WITH CF4 GAS. Karl M. Ecklund, Keith W. Hartman, Michael J. Hebert, Stanley G. Wojcicki

Similar documents
Additives that prevent or reverse cathode aging in drift chambers with Helium-Isobutane gas *

Introduction of Vacuum Science & Technology. Diffusion pumps used on the Calutron mass spectrometers during the Manhattan Project.

Performance of a triple-gem detector for high rate charged particle triggering

The Mark III Vertex Chamber *

Plasma-Therm PECVD. Operating Characteristics. Operating Instructions. Typical Processes. I. Loading. II. Operating

Usage Policies Notebook for Xenon Difluoride (XeF 2 ) Isotropic Si Etch

Effects of materials on aging rates in wire chambers operated with DME

The Principles of Vacuum Technology

REACTIVE ION ETCHING OF SILICON DIOXIDE USING BOTH OXYGEN AND CARBON DIOXIDE AS GAS ADDITIVES. dames E. Constantino ABSTRACT

Design and Construction of a GEM-TPC Prototype for R&D Purposes

A Longterm Aging Study of the Honeycomb Drift Tubes of HERA-B Using a Circulated and Purified CF -Gas Mixture

arxiv: v1 [physics.ins-det] 16 Aug 2014

The Resistive Plate Chamber detectors at the Large Hadron Collider experiments. Danube School, September 8-13, 2014 Novi Sad

Max Planck Institute, Munich. January 10, Because of the concern about long-term silicon contamination of MDTs, we

Contact Person(s) : Isabel M. Fisenne APPLICATION

The Transition Radiation Detector of the AMS-02 Experiment

Remote Plasma Cleaning from a TEM Sample Holder with an Evactron De-Contaminator ABSTRACT

Nataliya Sharova, Truls Norby NorECs Norwegian Electro Ceramics AS

Helium Mass Spectrometric Leak Detection In Large Size Process Plants

R: The Ideal Gas Constant Pre-Lab Assignment

Characterization and Modeling of Wafer and Die Level Uniformity in Deep Reactive Ion Etching (DRIE)

5.1.3 Mechanical Hazards Drive assemblies have sufficient power to cause injury. Keep hands, fingers, clothing and tools clear of moving parts.

States of Matter. Q 7. Calculate the average of kinetic energy, in joules of the molecules in 8.0 g of methane at 27 o C. (IIT JEE Marks)

Dissolved Oxygen Guide

Plasma Sources and Feedback Control in Pretreatment Web Coating Applications

Vacuum Science Techniques and Applications Dan Dessau Adv. Lab 2007

STEAM STERILIZABLE POLAROGRAPHIC OXYGEN ELECTRODE

Gases&Technology. Measurement of Impurities in Helium Using the Dielectric Barrier Discharge Helium Ionization Detector. FEATURE.

Detecting sound wave of bubbles produced in a boiling liquid

The SPI Sputter Coater Handbook

Long term stability tests of INO RPC prototypes

Plasma Cleaner. Yamato Scientific America. Contents. Innovating Science for Over 125 Years. Gas Plasma Dry Cleaner PDC200/210/510 PDC610G.

Operating Characteristics and Handling Manual for the NAP-55A / NAP-50A Explosive/Flammable Gas Sensor NEMOTO

ARTICLE IN PRESS. Nuclear Instruments and Methods in Physics Research A

Technical Data Sheet MF010-O-LC

FAST EVAPORATION AT NORMAL PRESSURE

Dr. Rogers Chapter 5 Homework Chem 111 Fall 2003

Notes-PECVD: Chamber 1

Extension of the operational lifetime of the proportional chambers in the HERMES spectrometer

Variable Depth Bragg Peak Test Method

LUDLUM MODEL 239-1F FLOOR MONITOR. Revised December 2010

Both physical and chemical effects come into play either separately or in combination.

Detector Carrier Gas Comments Detector anode purge or reference gas. Electron Capture Nitrogen Maximum sensitivity Nitrogen Argon/Methane

Agilent ICP-MS Interactive Troubleshooting tool for Low sensitivity

Technical Specifications of Hydrogen Isotope Handling and Recovery System

DEVICES FOR FIELD DETERMINATION OF WATER VAPOR IN NATURAL GAS Betsy Murphy MNM Enterprises 801 N. Riverside Drive Fort Worth, Texas 76111

Introductory Lab: Vacuum Methods

APPLICATION OF A CHANNEL PLATE IN FIELD-ION MICROSCOPY

Issue: H Title: CHA E-Beam Evaporator Page 1 of 7. Table of Contents

Analysis of RPC Performance with Different Gas Mixture

Measuring Carbon Dioxide in Breath

LOW PRESSURE VOLTAGE BREAKDOWN TEST PROCEDURE FOR GSS FSU FLIGHT SPARE HVA BOARD October 28, P0938 Rev

PHENIX RPC in China. Xiaomei LI. Science and Technology on Nuclear Data Laboratory China Institute of Atomic Energy

This educational seminar discusses creating, measuring, and troubleshooting Rough Vacuum.

Unaxis PECVD. SiH4 (5% in He)

How To Use Getters and Getter Pumps

DELTI. Vac. DELTI-Vac MIL. Application. Principle. Characteristic

Victoreen B. Operators Manual. Image Intensifier Ion Chamber

CRC-EVANS SADDLE BAG WEIGHT SYSTEM

29th Monitoring Research Review: Ground-Based Nuclear Explosion Monitoring Technologies

The Experts in Vacuum Solutions

BEST KNOWN METHODS. Transpector XPR3 Gas Analysis System. 1 of 6 DESCRIPTION XPR3 APPLICATIONS PHYSICAL INSTALLATION

The Broadest Gauging Line in the Industry

Development of high pressure-high vacuum-high conductance piston valve for gas-filled radiation detectors

You should be able to: Describe Equipment Barometer Manometer. 5.1 Pressure Read and outline 5.1 Define Barometer

Gas Laws. 2 HCl(aq) + CaCO 3 (s) H 2 O(l) + CO 2 (g) + CaCl 2 (aq) HCl(aq) + NaHCO 3 (s) H 2 O(l) + CO 2 (g) + NaCl(aq)

Gas Sampling in the DST

Investigation of Thermal Effects of CO 2 on Earth-Atmosphere System

Standard Operating Manual

Experience with the ZEUS central tracking detector

Basic & Controlled Atmosphere Glove Boxes

Development of Cleaning and Processing Techniques for UHV/XHV at Daresbury Laboratory Keith Middleman

Generating Calibration Gas Standards

Columbus Instruments

Quantification of Contamination Using Quartz Crystal Thickness Monitors

Choosing a Quadrupole Gas Analyzer Application Note #9

Gas Laws. 2 HCl(aq) + CaCO 3 (s) H 2 O(l) + CO 2 (g) + CaCl 2 (aq) HCl(aq) + NaHCO 3 (s) H 2 O(l) + CO 2 (g) + NaCl(aq)

ELEVATION CORRECTION FACTORS FOR RADON MONITORS*

Arizona State University NanoFab PLASMATHERM 790 RIE. Version A

Test Facilities Experiment Review

RPC CHARACTERIZATION AND TESTING ( by S. Mathimalar, INO Student)

STS PECVD Instructions

Usage Policies Notebook for STS DRIE System

23.1 Functions, Basic Configuration, and Interfaces

EFFECTS OF LASER WINDOW DEGREDATION ON LASER POWER AND DISTRIBUTION IN LASER SINTERING. Ben Fulcher, David K. Leigh

Supplementary Operator s Manual 42/24-14 EN Rev. 3

Chemicals that will cause mutations to germ cells of humans that can be transmitted to Mutagenicity

CHM Basics of Gases (r14) Charles Taylor 1/9

MECHANICAL PROPERTIES

2 Switching off ECRIS 3. 4 Acquire Beam Spectrum 4. 6 Vent Instrument Chamber 5. 7 Pump down Chamber 5. 8 Baking out Chamber 5.

Flow in a shock tube

MASSIVE TITANIUM SUBLIMATION PUMPING IN THE CESR INTERACTION REGION *

School of Chemistry SOP For Operation Of Glove Boxes

EUROPEAN LABORATORY FOR PARTICLE PHYSICS STUDY OF AGEING AND GAIN LIMITS OF MICROSTRIP GAS CHAMBERS AT HIGH RATES

Chemistry Chapter 11 Test Review

A Journal of Practical and Useful Vacuum Technology. By Phil Danielson

JANIS OPERATING INSTRUCTIONS FOR SUPERCONDUCTING MAGNET CRYOSTATS

Study of the IBF of Double/Triple THGEM

FLOWMETER UNITS FLOWMETER DEVICES, BY-PASS SYSTEMS

Application Note. ASTRON Remote Plasma Source Ignition Best Practices PROBLEM

Transcription:

SLAC-PUB-16219 ICFA INSTRUMENTATION B ULLETIN ETCHING OF COPPER COATED MYLAR TUBES WITH CF4 GAS Karl M. Ecklund, Keith W. Hartman, Michael J. Hebert, Stanley G. Wojcicki Department of Physics, Stanford University Stanford, California 94309 ABSTRACT Using 5 mm diameter copper coated mylar straw tubes at a potential of 2.30 KV relative to a concentric 20 pm diameter gold-plated tungsten anode, it has been observed that with very low flow rates of CF4-based gases the conductive copper cathode material may be removed entirely from the mylar surface. 1 Introduction Experiment E871 in the B5 line of the Alternating Gradient Synchrotron at Brookhaven National Laboratory, is designed to search for very rare KL decays with a single event sensitivity below 10-12. For this search, the 24 GeV AGS proton beam producing w 2 x 108 Kg per spill from a watercooled platinum target is used. Expecting chamber rates of w 200 MHz/m2 for this experiment, we selected 5 mm straw tubes with CF4 based gases as a starting point for initial prototype studies. Our interest in CFL based gases lies primarily in their high drift velocities [1] and in their good aging characteristics [2 4]. 2 Hardware Configuration Our small test chamber is constructed of two 60 cm long, 5.0 mm diameter tubes each with a concentric 20 pm diameter gold-plated tungsten wire stretched to a tension of ~40 gm. The tubes This material is based upon work supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-76SF00515.

are made of 2-ply 0.5 mil mylar, the inner layer of which has a 1000 ~ layer of copper vapordeposited onto its inside surface. Cylindrical brass sleeves provide the mechanical support for and electrical contact between the straws and the endplates. Feedthroughs passing through the endplates and into the sleeves position the wire. Details of the endplate and feedthrough assembly will be provided upon request. 3 Copper Etching Using two thin pieces of scintillator connected to phototubes, a trigger was defined with which the operating voltage of each gas was determined using a 5 source. No difference in the operating voltage was observed between the two straw tubes with gases used in this study: Ar-CzHG (50:50) and CF4-CH4 (30:70). The operating voltages for Ar-CzHG and CFL-CHl are 1.65 KV and 2.30 KV, respectively. Typically, the gas flow was about one volume change per minute. The copper etching effect was first noticed accidentally: for a period of about ten hours, the gas (CF4-CH4) flow was off while for one of the two straws, the HV was on. Visually, the difference between the two straws was striking: one was mostly transparent and the other appeared normal. A white powder was observed on the bottom of the etched tube. There are apparently no known volatile copper compounds. Under more controlled circumstances, the etching effect was repeated with the undamaged straw. The basic procedure was simple: flow gas through the chamber, apply high volt age and note the current flowing between anode and cathode. At this point the gas flow was turned off and subsequent current measurements were made at regular time intervals. With CFA-CH4 flowing at ~20 ml/min, no measurable current was flowing (with 10 na sensitivity) at 2.30 KV. Approximately 90 minutes after turning the gas flow off, the chamber began drawing ~10 na; after 2 hours it was drawing 5pA. This was repeated many times. When the chamber was drawing 5pA of current, a small amount of fresh gas (~2 ml) was introduced at which point the current dropped to less than 10 na. About twenty minutes later, it was drawing measurable current again and after ~40 minutes, it was drawing 2 pa. This also was very repeatable. Changing the gas to the Ar-CzHG mixture and correspondingly reducing the operating voltage to 1.65 KV, the current at normal gas flow was less than 10 na. Stopping gas flow, no measurable current was observed for 7 hours. At this point we changed to pure CF4 operating at the same voltage, namely 2.30 KV. Pure CF4 began to draw current within a few minutes of turning off the gas flow and after about ten minutes the chamber was drawing ~60 pa; see Figure la. About an hour later, the current reached a maximum of ~180 pa and after about 90 minutes, it leveled off at around 140 PA. The straw -48-

Figure 1: a) Short-term time dependence of current in straw #2 at 2.30 KV in pure CF4 gas; b) Long-term time dependence; the copper began to thin visibly from the tube wall somewhere between 410-470 minutes on this plot. These data were taken over two days and the second set begins at t=160 minutes. -49-

ICFA INSTRUMENTATION BULLETIN was turned off, flushed with fresh gas and the measurements started again at t=160 minutes in Figure 1b. About 310 minutes after beginning the second set of measurements, it became visibly apparent that the copper was being removed from the straw surface. 4 Suspected Mechanism Under normal conditions CF4 is considered a very inert gas; nonetheless, it is used[5,6] in the microelectronic fabrication industry as a component in the plasma etching of pure silicon and SiOz. In one application of this process, CF4 and either O2 or H2 are introduced into an evacuated chamber which is pumped with RF producing a plasma. In addition to ionizing the gas, the RF liberates fluorine radicals which react with the silicon to produce SiF4. One may vary the etching rate of either the silicon or its oxide by introducing either O2 or H2. Suspecting that O2 was leaking into the chamber and reacting with the CF4 in the high-field region near the anode wire, we built another small two-straw chamber for subsequent studies. This chamber was subjected to the same conditions as previously mentioned: pure CF4 with HV at 2.30 KV and no gas flow. This chamber gave no indications of etching after 30 hours under these conditions. While introducing water vapor through a bubbler at room temperature did not induce etching, a pin hole in the straw tube wall did: the straw was drawing ~20 pa after about 20 minutes. Repeating the exercise in a volume of N2, the chamber drew no current. Returning the chamber again to an atmosphere of air and raising the voltage to 2.30 KV with a fresh supply of CF4 and zero flow rate, the copper began to visibly etch after about 4 hours in the region near the hole. It was suggested[7] that the copper was being removed through a reaction resulting in CUF2 as a final product. A possible reaction is: The flourine is then free to react with the copper. As mentioned, a white powder was observed in the straw after the copper was removed and CUF2 is known to be white in its crystalline form [8]. 5 Summary In the presence of O2 in the high-field region of a straw drift chamber, CF4-based gases will undergo a chemical reaction with the conducting copper coating of the straws. While it is, in general, not a good idea to introduce Oz into a drift chamber, under certain conditions complete destruction of the chamber may result. A number of points may be made: -50-

CF4 plus air in a straw chamber under high voltage removes the copper cathode material from the straw; ionizing radiation does not appear to be a factor; water vapor in the gas does not appear to be a factor; N2 does not appear to be a factor. For other reasons, the seven of eight straw chambers in experiment E871 at BNL were rebuilt for the 1996 run and to avoid problems arising from this effect two precautionary measures were taken: 1) the copper layer was increased from 1000 ~ to 2000 ~; 2) all straws were individually pressure checked for leaks before installation. In addition to this, two operational changes were implemented: 1) gas flow rate was increased from 3 volume exchanges per day to 10 per day; 2) chamber voltage was ramped down between beam spills. The final chamber gas used in E871 was CF4-C2H6 (50:50) with an operating voltage of 1950V (measured with an 55Fe source, the gas gain is 8 x 10 4 ). Due to chamber capacitance, we were unable to ramp more than 100V down in the ~ 2 seconds available between the end of one AGS spill and the beginning of the next. As of this time, there is no indication of copper etching. References [1] Fisher, J., et. al., NIM, A238 (1987) 249. [2] Henderson, R., et. al., IEEE Trans. Nucl. Sci. NS-35 (1988) 477. [3] Openshaw, R. S., et. al., IEEE Trans. Nucl. Sci. NS-36 (1989) 567. [4] Kadyk, J., et. al., IEEE Trans. Nucl. Sci. NS-37 (1990) 478. [5] A Guide to Reactive Ion Etching (1991) March Instruments, Inc., 125-J Mason Circle, Concord, CA 94520. [6] Poulsen, R. G., J. Vat. Sci. Technol., Vol. 14, No. 1, (1977) 266. [7] Va Vra, J., private communication. [8] CRC Handbook of Chemistry and Physics 76th ed. (CRC Press, Inc.) 4-55. -51-