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Virginia Tech Update for Tracking Group, January 19, 2006

Juliette's Birthday

I'm not old enough to start counting backwards yet!




          
Beamline Design

The preliminary beamline design consists of the "right" size beamline in each region and then for regions upstream of QTOR, the maximum sheilding with a single thickness of lead in that region. Figure 1 shows the entire beamline as it is currently defined. The regions are:

          sewer pipe
          GEM
          Minitorus
          Region II
          QTOR
          downstream of QTOR

For now we have adopted the two plug solution as our favorite. We believe that it is desireable to have at least one plug to try to keep the entire region upstream of QTOR from being irradiated, but two plugs allow us to have the desired angular range for the downstream luminosity monitors. The plugs are embedded in the upstream and downstream cleanup collimators (See Figures 3 and 4).

Figure 1 - Picture of the entire beamline.

Figure 2 - Zoom in on region with the tungsten plugs.



Figure 3 - Upstream tungsten plug, embedded in the upstream cleanup collimator.

Figure 4 - Downstream tungsten plug, partially embedded
in the downstream cleanup collimator.



There are obvious flaws in this design, because there are actually openings for particles with p_z < 0 to get out of the beampipe (See Figure 1 or 2). That and other issues will eventually have to be addressed. However, there were several problems with the geometry definition, and now I am very carefully checking to make sure that the geometry and materials are defined correctly.

The elements and their lengths and inner and outer radii are listed in Table 1 below. Maybe Greg or someone could double-check the aluminum beampipe thicknesses and lengths.

When I am satisfied that the materials and geometry definitions are correct, I will calculate a baseline for the photon rates. I will then try to add and remove shielding to see if the photon rates (specifically at Region II, but also at GEM and cerenkov bar locations) can be improved. Finally, a full photon rate study will be performed to get the total rates at the 3 locations with the new collimators and beamline and sheilding in place.

Region

Component

Material

R_i (cm)

R_o (cm)

Length (cm)

target

sewer pipe

Aluminum

29.5275

30.48

49.09

upstream cleanup

Plug 1

Tungsten

1.246

4.0

7.0

GEM

BEA1

Aluminum

2.80543

3.0163

44.41

GEM

BES1

Lead

3.0163

5.2388

44.41

minitorus

BEA2

Aluminum

5.50418

5.715

171.281

minitorus

BES2

Lead

5.715

7.62

171.281

Region II

BEA3

Aluminum

10.26668

10.4775

102.1

Region II

BES3

Lead

10.4775

18.0975

102.1

dowmstream cleanup

Plug 2

Tungsten

5.95

14.55

7.0

QTOR

BEA4

Aluminum

13.0175

13.97

436.619

QTOR

BES4

Lead

13.97

wedges?

436.619

downstream of QTOR

BEA5

Aluminum

29.5275

30.48

515

downstream of QTOR

BES5

Lead

30.48

34.29

515


Table 1 - List of components and volume information.




          
Drift Chamber Update

The machine shop is 90% finished with the frames for the next Region II chamber.

Norm and Juliette have begun stretching the cathode planes and the gas windows. Figure 5 shows one of them reflecting a Virginia Tech Qweak poster.

We plan to start stringing the sense planes within the next couple of weeks. Figure 6 shows a sense plane frame with the wire scanner and camera/monitor setup that we will use to measure the wire positions. The wires will be positioned in the corners of the grooves that are magnified in the monitors view. A drawing of the card layout is taped to the frame - you can see it on the right side of the monitor view.

Figure 5 - One of the cathode planes reflecting a Qweak poster.

Figure 6 - The wire scanner setup with a sense plane.



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Last Update: 1/19/06

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