Ultra-High Vacuum (UHV)

for the Advanced LIGO Detector

Requirements

Materials & Components Qualification Processes

NEW _ Guidance on Qualification Material Quantity & Preparation

Approved Materials & Components List

Acceptance Testing Queue

UHV Preparation and Part QA

New Approaches to Achieve the AL UHV Requirements

Optical Contamination Exposure Cavity

Air Bake & FTIR Testing

Large, Uniform, High-Temperature, Vacuum, Bake Oven

TDMS

Extrapolating from Elevated RGA Measurements

Requirements

  • Phase Noise Limits on Partial Pressures (Outgassing Rates):

Reference: T040001-00, Vacuum Hydrocarbon Outgassing Requirements

Gas Species

LLO
Actual
(torr)

LHO
Actual
(torr)

Initial LIGO
Requirement
(torr)

Adv. LIGO
Requirement
(torr)

Goal
(torr)

H2

TBD

TBD

1 x 10-6

1 x 10-9

1 x 10-9

H2O

TBD

TBD

1 x 10-7

1 x 10-10

1 x 10-10

N2

TBD

TBD

6 x 10-8

6 x 10-11

6 x 10-11

CO

TBD

TBD

5 x 10-8

5 x 10-11

5 x 10-11

CO2

TBD

TBD

2 x 10-8

2 x 10-11

2 x 10-11

CH4

TBD

TBD

3 x 10-8

3 x 10-11

3 x 10-11

AMU 100 Hydrocarbon

TBD

TBD

7 x 10-10

2 x 10-12

7 x 10-13

AMU 300 Hydrocarbon

TBD

TBD

5 x 10-11

2.2 x 10-13

5 x 10-14

AMU 500 Hydrocarbon

TBD

TBD

1 x 10-11

9 x 10-14

1 x 10-14

 

  • Optical Loss Limits, Scatter and Absorption, Due to Deposition

Reference: TBW

Optical Loss

Initial LIGO
Requirement

(ppm/yr)

Adv. LIGO
Requirement

(ppm/yr)

Absorption

< 2  ¨

< 0.1

Scatter

< 10  ¨

< 10

¨E960022-B, section 1.1 states < 0.5 ppm/yr/optic absorption and < 10 ppm/yr/optic for initial LIGO.

Materials & Components Qualification Processes

The basic reference for the procedures by which materials and components are qualified for service in the LIGO vacuum system is:

E960022, LIGO Vacuum Compatibility, Cleaning Methods and Qualification Procedures

Pending Changes for Rev. C:

  • integrate in the cleaning/air bake/FTIR sampling and evaluating that was performed on the large parts for Initial LIGO
  • put in a qualified increase in the bake temperatures for 6061-T6 aluminum
  • deal with the issue of safety of ultrasonic cleaning with methanol
  • deal with the issues of safety of gross cleaning with acid, trichloroethane and acetone
  • switching from a callout of "Ameristat poly sheet", an obsolete term, to a generic description of an acceptable bag material
  • section 6.1.1 on material exposure tests in a high irradiance optical cavity refers to 150 kW/cm2 which is the initial LIGO test level. A note to the effect that a higher level (value?) is now employed for adv. LIGO qualification
  • add the high irradiance cavity test equipment/procedure reference, P990032

 

Guidance on Qualification Material Quantity & Preparation

For polymer materials, or other high rate outgassing elements, which are to be tested for acceptability in the LIGO vacuum system:

·        Materials must be prepared in accordance with their proposed processing, i.e. it is not just the inherent material, but also any associated surface treatment and chemical processing which must be qualified.

  • Testing composite material assemblies is much preferred over testing individual materials (e.g. best to test a kapton, adhesive, copper flexible circuit assembly than to test each material individually).
  • For RGA testing, the amount of material tested should be the larger of either:
    • ~ ½ the intended amount in the vertex vacuum volume (single IFO), or
    • ~ 2 times the intended amount in the end station vacuum volume

The above suggested amounts are based on scaling from test conditions to the LIGO in situ conditions assuming that the RGA background is limited to 2e-11 torr-liters/sec, the RGA chamber pump rate is 10 liters/sec and the target partial pressure for the hydrocarbon sum mass is 6e-14 torr. See T04001 for allocated budget for a more precise estimate.

  • For optical contamination exposure cavity testing, the surface area of the material tested should be at least 0.1 times the surface area of the amount intended in a LIGO vacuum volume, preferably 0.3 times this amount (if size and costs allow).

The suggested amount above is based on the measured uncertainty (standard deviation) in the rate of absorption change in time, after one month of testing, 0.4 ppm/yr, compared to the requirement of < 0.1 ppm/yr, accounting for the approximate test pump rate of 1/50th of the LIGO pump rate.

 

Approved Materials and Components List

The list of approved materials for advanced LIGO is given in:

E960050, LIGO Vacuum Compatible Materials List

A proposed form for documenting the results of the vacuum qualification testing:

UHV Preparation and Part QA

Every part which goes into the LIGO vacuum system must be prepared (cleaned, handled and wrapped/packaged) in an approved manner. In addition every part has some measure Quality Assurance (QA) such as process travelers which include results from a vacuum cleanliness measurement such as mass spectrometry (aka Residual Gas Assay, RGA) or Fourier Transform Infra-Red (FTIR) results. The basic reference for the procedures for part UHV preparation and QA is:

E960022, LIGO Vacuum Compatibility, Cleaning Methods and Qualification Procedures

 

New Approaches to Achieve the Adv. LIGO Vacuum Requirements

Optical Contamination Exposure Cavity

The optical contamination cavity testing appears capable of meeting Adv. LIGO requirements, with an the increase in the irradiance and a longer run time. CHECK THIS STATEMENT!

 

Filtered Air Bake and FTIR Testing for Large Components

Ideally all parts would be placed into a test vacuum chamber and their outgassing rates directly measured. However for large parts it is impractical to get large enough UHV bake chambers. In these cases we employ air baking (with filtered air) and subsequent FTIR testing of solvents which sample the surfaces of the part. However we have lost the traceability on the FTIR testing that we had in Initial LIGO for the Beam Tubes and for the Seismic Isolation System (SEI). We had established a cross-correlation between RGA results and FTIR results. The FTIR testing house has changed their equipment and a new cross-correlation factor must be established. In addition, we have learned that sample preparation and FTIR testing varies considerably between testing services. Larry Jones and Ken Mailand had embarked on a "Cleaning Pathfinder" effort to establish new methods and sources for large part cleaning in the So. California area. This was motivated by the pending SEI prototype parts, which have been delayed for other reasons.

 

Large, Uniform, High Temperature Vacuum Bake Oven

The current LIGO vacuum bake oven background levels are to high to qualify to the Adv. LIGO requirement (see T040001). In addition we have a large suspension structure, which cannot fit into the current LIGO vacuum bake ovens. Given the proximity of this structure to the optics, it seems prudent to plan for a vacuum bake and RGA measurement rather than rely upon an air bake and FTIR test. Furthermore, we know that added bake oven capacity is needed for AL. Mike Zucker and Larry Jones proposed an alternative vacuum bake oven approach where the temperatures can be higher and more uniform (no cold spots for contamination to condense; some notes from Mike are here).

Larry Jones and Oddvar Spjeld have pursued this alternative with industry to get cost and schedule information for a large vacuum bake oven. The requirements are defined in the following documents:

·        E040392-02 for the Chamber

·        E040393-02 for the Oven

·        D040502-00, Assembly

·        D040503-00, Chamber

·        D040504-00, Oven

Although the oven appears to be a close fit in the D040502 drawing, the response from the oven manufacturers is to make it larger, essentially a walk-in oven. The project has been proposed (see CR040017) to the LIGO Configuration Control Board (CCB) and the Vacuum Review Board (VRB). A decision is pending. (BTW this oven, if available, would be used for the quadruple controls prototype suspension due to be UHV prepared in ~April, 2005)

 

Thermal Desorption Mass Spectrometry (TDMS)

Rai Weiss has proposed using Thermal Desorption Mass Spectrometry (TDMS) techniques, wherein the surface is heated and the evolved gas is collected and measured by a mass spectrometer. In principal the crude (~0.1 torr) vacuum required could be generated locally and scanned across surfaces of the part. Unfortunately this method would not easily allow measurement of the outgassing from trapped holes, welded regions and complex geometries – where most of the outgassing problems likely reside. More details here …

 

Extrapolating RGA Results from Elevated Temperature Outgassing Measurements

Dennis Coyne determined the doubling temperature for outgassing from some polyimides (see T040032). If the chemical kinetics, or desorption dynamics, involved in the outgassing do not change over modest temperatures (a single rate equation applies), then one can measure the outgassing rate at a few higher temperatures and then extrapolate to room temperature conditions. This might enable current LIGO Lab vacuum bake ovens to meet the AL requirements. Thoughts?