Status and future measurements on Micron detectors Outline: Irradiation and measurement in dry...

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Status and future measurements on Micron detectors Outline: Irradiation and measurement in dry atmosphere Measurements in vacuum

Transcript of Status and future measurements on Micron detectors Outline: Irradiation and measurement in dry...

Page 1: Status and future measurements on Micron detectors Outline: Irradiation and measurement in dry atmosphere Measurements in vacuum.

Status and future measurements on Micron detectors

Outline:

Irradiation and measurement in dry atmosphere

Measurements in vacuum

Page 2: Status and future measurements on Micron detectors Outline: Irradiation and measurement in dry atmosphere Measurements in vacuum.

Irradiation and measurement in dry atmosphere

Motivation: test of the oxide charge as possibly shorting the read-out strips after heavy irradiation. Oxide charge build-up favoured by irradiation under bias. Test ability to stand high voltage in dry air.

Is there a saturation oxide charge concentration? Our p-spray: 1.1 1012 ± 0.3 B cm-2

Possible scenario: strips could be shorted if oxide charge > p-spray.

But: evidences from other works (MPI) that after irradiation strips are insulated also with p-spray doses < p-spray. Tentative explanation is that insulation is given by interface states.

Page 3: Status and future measurements on Micron detectors Outline: Irradiation and measurement in dry atmosphere Measurements in vacuum.
Page 4: Status and future measurements on Micron detectors Outline: Irradiation and measurement in dry atmosphere Measurements in vacuum.
Page 5: Status and future measurements on Micron detectors Outline: Irradiation and measurement in dry atmosphere Measurements in vacuum.

Monitoring the irradiation

Irradiation was performed in the ATLAS cool box, in nitrogen atmosphere.

Page 6: Status and future measurements on Micron detectors Outline: Irradiation and measurement in dry atmosphere Measurements in vacuum.

Detector was vertical in the beam. The irradiated area is ~ 2x2 cm2, maximum fluence > 2 1015 p cm-2.

Typical Irrad 7 fluence horizontal profile

(to be rescaled to max ~2.2 1015 cm-2).

0

10

20

30

40

50

60

70

80

20 30 40 50 60 70 80

Position from Ref [mm]

Me

as

ure

d f

lue

nc

e [

x1

013

cm

-2]

Page 7: Status and future measurements on Micron detectors Outline: Irradiation and measurement in dry atmosphere Measurements in vacuum.

Reverse bias current during irradiation

0.0E+00

2.0E-05

4.0E-05

6.0E-05

8.0E-05

1.0E-04

1.2E-04

1.4E-04

1.6E-04

1.8E-04

2.0E-04

3.1509E+09 3.1510E+09 3.1511E+09 3.1512E+09 3.1513E+09 3.1514E+09

Time (s)

Cu

rre

nt

(A)

0.0E+00

5.0E-05

1.0E-04

1.5E-04

2.0E-04

0.0E+00 2.0E+07 4.0E+07 6.0E+07 8.0E+07 1.0E+08

SEC counts

Cu

rre

nt

(A)

Bias changed from 100V to 200V.

Page 8: Status and future measurements on Micron detectors Outline: Irradiation and measurement in dry atmosphere Measurements in vacuum.

Measurements foreseen with the irradiated device:

•CCE(V) measurement of the irradiated area (to determine, if possible, the irradiation profile).

•Measurement of strip insulation (charge spread over multiple strips) with laser light injection next to a strip as a function of the fluence.

•Possible estimation of the maximum survival limit (fluence on the detector varies from 0 to > 2 1015 cm-2)

Page 9: Status and future measurements on Micron detectors Outline: Irradiation and measurement in dry atmosphere Measurements in vacuum.

Measurements in vacuum

A LHCb VELO phi measuring detector, PR02 version has been put in vacuum (~10-2 mb) and left under 250V for 6 days (it’s still running at present). The reverse current (initially 0.8 µA) didn’t vary significantly over this period (small variations due to temperature variation where in the order of ± 2%.