Caltech Tests of HAWC/SHARC JFET Modules

Darren Dowell -- (626)395-6675 (office), -2600 (lab), 796-8806 (FAX)
Last modified Monday, 10-September-2001 14:41 PDT
cdd@submm.caltech.edu

Information on this page

This page is meant to contain information regarding the properties of the JFET modules designed by Goddard for HAWC/SHARC -- thermal characteristics, assembly status, performance summaries. To find out more details regarding electrical tests of JFET dies, go to a separate page .

Warm Board Measurements Complete -- September 2001

The assembly and testing of seven warm boards were completed in August 2001. A Microsoft Word document summarizing the measurements is available.

Warm Board Performance Qualification -- October 2000

The detailed qualification plan is given here.

(**Put a circuit diagram here in the future.**)

The median amplifier noise is 4.4, 3.9, and 3.7 nV Hz^-1/2 at 3, 10, and 30 Hz, and has been subtracted from the noise spectra.

Warm Board #1 -- October 2000

We have tested all of substrate 1 with two cooldowns and some JFET replacement in between. The 6 heaters and 2 diodes passed the qualification on the first try. The 120 K resistances of the heaters were 1977 to 1997 ohms. The 120 K diode voltages for a 10 microamp excitation were 0.951 and 0.952 V.

During the first cooldown, 127 of 128 JFETs were functional; the drain wirebond on the nonfunctional device was accidentally omitted. The noise performance was marginal. In group A, 5 JFETs had noise in excess of the tight cutoff (allowance of 4), and 2 had noise in excess of the looser cutoff (allowance of 1). In group B, the number of noisy JFETs was 5 and 3 for the two cutoffs; C: 2 and 0, D: 3 and 1. Only groups C and D passed. We replaced the following JFETs: 101, 106, 206, 207, 215, 220, 221, 223, 231, 316, 329, 407, 423, and 427.

During the second cooldown, all 128 JFETs were functional. We remeasured the replaced devices, and the noise performance was well within specifications, with a median of 8.8, 4.9, and 4.0 nV Hz^-1/2 at 3, 10, and 30 Hz. There is only one device (404) which does not fall under the tight noise cutoff.

At 120 K, the JFET gain was 0.996+-0.001, and the source voltages were 0.543 to 0.587 V. These parameters are dependent on the operating current, which for our measurements is 18 microamps.

The noise data are available on-line:

A caveat about the time records: due to the quirks of the spectrum analyzer, a true 'oscilloscope' mode is not available. Only the absolute value of the voltage as a function of time is available.


Assembly of JFET substrate 1 -- October 2000

container
Figure. JFET substrate #1 with JFETs, heaters, and diodes glued down. The warm board is sitting in a storage/shipping container.

wire bonding D diode, heater JFET closeup D drain C-D heater B-C heaters A diode, heater
Figures. Photographs of components on assembled/wire bonded substrate #1. For the diodes, conductive epoxy is used to make the electrical connection from the collector to the gold traces.

interface
Figure. JFET substrate #1, post wire bonding, installed in test fixture. The test fixture has wire bond interfaces to the warm board, and connectors on the underside to interface with the amplifier electronics.

interface closeup
Figure. Closeup view of interface fixture.

PLAN: Substrate #1 will be electronically characterized at Caltech at ~120 K. Assuming no unanticipated problems, we will then send the warm board to Goddard for evaluation and integration with the JFET drawer.


Thermal tests of warm board -- May 2000

Ceramic warm boards were provided by Sachi Babu for JFET population and thermal tests. Sachi also provided G10 tubes with approximate dimensions 0.43" diameter x 0.28" length x 0.005" wall; we assume that this is the tube intended to provide thermal isolation of the warm boards in the final assembly. Three diodes and one heater were glued to the warm board for diagnostic purposes. One tube was glued to the warm board and to an aluminum block. We used StyCast 2850FT.

Warm board Warm board
Figure. Three diodes were glued to the warm board -- 'C' at the end near the G10 tube, 'A' at the far end, and 'B' in the middle. The heater resistor was located at the far end near diode 'A'. This setup provides a worst case for the warm board, with all of the heating at one end and all of the cooling at the other.

Heat required to bring warm board to JFET operating temperature

The assembly was initially cooled to 4 K. We applied 50 mW to the heater to warm the board. In retrospect, this was a reasonable choice, but the time required to heat the board to 120 K would have been somewhat less if the thermal conductance of the G10 tube had not been so large.
temperature   time A    time B    time C
-----------  --------  --------  --------
    77 K      4.1 min   4.4 min   4.6 min
   120 K     21        25        25
The integrated heat capacity of the assembly from 4 K to 77 K is 13 Joules, and the integrated heat capacity from 4 K to 120 K is 75 Joules.

The waiting time of 25 minutes at the reasonable power level of 50 mW is acceptable in our opinion.


Equilibrium for 12 mW applied power

Diode  Temperature
-----  -----------
  A       78.1 K
  B       77.7 K
  C       77.9 K
base       4.8 K
The temperature gradient across the board is less than 0.5 K.

Equilibrium for 31 mW applied power

Diode  Temperature
-----  -----------
  A      120   K
  B      117   K
  C      117   K
base       5.5 K
The temperature gradient across the board is no greater than 3 K. However, this is a large amount of power.

For a G10 thermal conductivity of 0.3 W/m/K, and two 0.05" glue lines, we would expect a power of ~35 mW to be required to warm the board to 120 K. This is consistent with the measurement.

Summary

  1. The thermal conductance across the warm board is good. In our worst case scenario, the temperature gradient across the board is no more than 3 K. For distributed heating, the gradient will be less.
  2. The thermal conductance of the G10 tube was much too large. In the full assembly, 6 tubes will operate in parallel to isolate the 120 K JFETs from the 4 K package. This will require a power of 180 mW, much greater than the target of 50 mW total dissipation through the G10 and silicon microbridges. Detrimental effects include increased helium consumption and the increased difficulty of sinking the JFET power into the cold bath without leakage to the detectors.

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