
4
Fig. 4.2. Semiconductor Detector Bias and Current
Measuring Circuit Using a Nonfloating Meter.
4.6. UNDESIRABLE LEAKAGE
CURRENTS
Teflon-insulated current monitoring jacks and SHV
connectors are used in an effort to reduce leakage
currents to a minimum in the 428. Insulation
resistance of 1 x 1013 Ùor greater is desirable to
measure a detector leakage current of 1 nA at 1000
V. In order to maintain insulation resistances of this
magnitude, the insulators will have to be cleaned
frequently. Either Freon or methyl alcohol is a good
cleaning agent.
It may not be practical to reduce the leakage in
external cables and connections to a negligible
magnitude. In such cases it may suffice to note the
residual leakage current with all wiring in place
except the detector itself, and then subtract this
residual current from the indicated current to obtain
the actual detector current. If the leakage
phenomenon is essentially a resistance, then its
value may be computed from Ohm's law for use in
determining the residual current at various voltages,
without the necessity of actual measurements.
4.7. DETERMINATION OF ACTUAL
DETECTOR BIAS
In addition to its use as an indicator of physical
condition of the detector, the detector current allows
accurate determination of the actual bias voltage
across the detector, This actual voltage differs from
that indicated by the bias selector dials by the
amount of drop in voltage across the detector load
and filter resistors due to the detector current.
Accurate determination of actual detector voltage is
important, since it is an important parameter in both
the depleted (sensitive) depth of the detector and
the collecting field strength.
To obtain the actual detector voltage, one must
know the sum of all series resistances in the circuit
between voltage source and detector. The
resistance of the internal circuit of the 428 may be
approximated by 1.3 MÙ, unless this has been
reduced by a current monitor (Section 4.5). Detector
load resistors may vary from 10 MÙto 200 MÙin
ordinary applications, and may be several thousand
megohms in special applications involving cooled
detectors. In addition, there is usually a filter resistor
of 1 MÙor more near and in series with the load
resistor. The values of these resistors can usually be
ascertained from the schematic diagram of the
preamplifier used. Once having determined the total
series resistance, the loss of bias in that resistance
can be calculated by Ohm's law.
4.8. GUARD-RING VOLTAGE SUPPLY
When detectors that require a separate bias
connection to a guard ring are used, the 428 will
prove convenient in that the signal electrode bias
can be taken from one bias output connector and
the guard-ring potential taken from the other. In this
way the two potentials can be varied independently
of each other to determine the optimum biasing
condition. The usual optimum is obtained when both
are nearly the same, but a small difference is
sometimes beneficial. In general, that setting which
minimizes the signal electrode current will be near
optimum.