ORTEC 426 User manual

•
-
r-'-iv.-'a;
PRECISION
INSTRUMENTATION
FOR
RESEARCH
l»
Oak
Ridge
Technical
Enterprises
Corporation
OAK
RIDGE,
TENNESSEE
INSTRUCTION
MANUAL
MODEL
426
LINEAR
GATE

I.
f
INSTRUCTION
MANUAL
MODEL
426
LINEAR
GATE
Serial
No.
Purchaser
_
Date
Issued
OAK
RIDGE
TECHNICAL
ENTERPRISES
CORPORATION
p.
O.
BOX
C
OAK
RIDGE,
TENNESSEE
Telephone
(615)
483-8451
TWX
810-572-1078
®
Osk
Ridoe
Technlcel
Enterprises
Cerperetien
1946
Printtd
in
U.S.A.

TABLE
OF
CONTENTS
Page
WARRANTY
PHOTOGRAPH
1.
DESCRIPTION
1-1
1.1
General
Description
1
-
1
1.2
Description
of
Basic
Function
-
Linear
Gate
1
-
1
2.
SPECIFICATIONS
2-1
2.1
General
Specifications
2
-
1
2.2
Linear
Gate
Specifications
2
-
1
3.
INSTALLATION
3-1
3.1
General
Installation
Considerations
3-
1
3.2
Connection
to
Power
-
Nuclear
Standard
Bin,
ORTEC
Model
401/402
3
-
1
3.3
Input
Signal
Connection
to
Linear
Gate
3
-
1
3.4
Logic
Inputs
to
the
Enable
Input
3-2
3.5
Logic
Inputs
to
the
DC
Inhibit
Input
3-2
4.
OPERATING
INSTRUCTIONS
4-1
4.1
Front
Panel
Controls
4-
1
4.2
Initial
Testing
and
Observation
of
Pulse
Waveforms
4
-
1
4.3
Connector
Data
4-1
4.4
Typical
Operating
Considerations
4-2
5.
CIRCUIT
DESCRIPTION
5-1
5.1
Linear
Gate
-
Etched
Board
426-0201
5
-
1
6.
MAINTENANCE
6-1
6.1
Testing
Performance
of
Linear
Gate
6
-
1
6.2
Adjustment
of
Linear
Gating
Duration
6-2
6.3
Adjustment
of
Linear
Gate
Pedestal
6-2
6.4
Tabulated
Test
Point
Voltages
6-3
6.5
Suggestions
for
Troubleshooting
6-3
Continued
.
..
I

i
Table
of
Contents
Continued
Page
7.
BIN/MODULE
CONNECTOR
PIN
ASSIGNMENT
7
-
1
LIST
OF
ILLUSTRATIONS
AND
DIAGRAMS
Block
Diagram
426-0200-B2
Schematic
426-0000-S2

STANDARD
WARRANTY
FOR
ORTEC
ELECTRONIC
INSTRUMENTS
DAMAGE
IN
TRANSIT
Shipments
should
be
examined
immediately
upon
receipt
for
evidence
of
external
or
con
cealed
damage.
The
carrier
making
delivery
should
be
notified
immediately
of
any
such
damage,
since
the
carrier
is
normally
liable
for
damage
in
shipment.
Packing
materials,
v/aybills,
and
other
such
documentation
should
be
preserved
in
order
to
establish
claims.
After
such
notification
to
the
carrier,
notify
ORTEC
of
the
circumstances
so
that
we
may
assist
in
damage
claims
and
in
providing
replacement
equipment
when
necessary.
WARRANTY
ORTEC
warrants
its
electronic
products
to
be
free
from
defects
in
workmanship
and
materials,
other
than
vacuum
tubes
and
semiconductors,
for
a
period
of
twelve
months
from
date
of
ship
ment,
provided
that
the
equipment
has
been
used
in
a
proper
manner
and
not
subjected
to
abuse.
Repairs
or
replacement,
at
ORTEC
option,
will
be
made
without
charge
at
the
ORTEC
factory.
Shipping
expense
will
be
to
the
account
of
the
customer
except
in
cases
of
defects
discovered
upon
initial
operation.
Warranties
of
vacuum
tubes
and
semiconductors,
as
made
by
their
manufacturers,
will
be
extended
to
our
customers
only
to
the
extent
of
the
manufacturers'
liability
to
ORTEC.
Specially
selected
vacuum
tubes
or
semiconductors
cannot
be
warranted.
ORTEC
reserves
the
right
to
modify
the
design
of
its
products
without
incurring
responsibility
for
modification
of
previously
manufactured
units.
Since
installation
conditions
are
beyond
our
control,
ORTEC
does
not
assume
any
risks
or
liabilities
associated
with
the
methods
of
installation,
or
installation
results.
QUALITY
CONTROL
Before
being
approved
for
shipment,
each
ORTEC
instrument
must
pass
a stringent
set
of
quality
control
tests
designed
to
expose
any
flaws
in
materials
or
workmanship.
Permanent
records
of
these
tests
are
maintained
for
use
in
warranty
repair
and
as
a
source
of
statistical
information
for
design
improvements.
REPAIR
SERVICE
ORTEC
instruments
not
in
warranty
may
be
returned
to
the
factory
for
repairs
or
checkout
at
modest
expense
to
the
customer.
Standard
procedure
requires
that
returned
instruments
pass
the
same
quality
control
tests
as
those
used
for
new
production
instruments.
Please
contact
the
factory
for
instructions
before
shipping
equipment.
r

I*
r
^
OHTEC®
MODEL
426
LINEAR
GATE
GATE
WIDTH
®)
PULSE
INHIBIT
I
NORM
DC
INHIBIT
[
•iFi
n
ENABLE
<©)
INPUT
O
OUTPUT
Q)
Model
426
Linear
Gate

1
-
1
MODEL
426
LINEAR
GATE
1.
DESCRIPTION
1.1
General
Description
The
Model
426
is
a
modular
linear
gate
providing
a
variable
gate
duration
whose
width
is
controlled
via
a
single-turn
front
panel
mounted
potentiometer.
The
nominal
gate
duration
range
is
from
0.3
to
4
psec.
The
operation
of
the
linear
gate
is
control
led
by
the
application
of
a
positive
enable
pulse.
The
linear
gate
is
useful
in
applications
that
require
inhibiting
a
linear
signal
according
to
chosen
coincidence
or
timing
requirements,
e.g.,
reducing
the
counting
rate
in
subsequent
linear
analysis
equipment.
The
instrument
is
designed
to
meet
the
recommended
interchangeability
stand
ards
of
USAEC
Report
TID-20893.
The
ORTEC
Model
401/402
Nuclear
Stand
ard
Bin
and
Power
Supply
provides
all
necessary
power
through
the
rear
module
power
connector.
All
signal
levels
and
impedances
are
compatible
with
other
modules
in
the
ORTEC
400
Series.
1
.2
Description
of
Basic
Function
—
Linear
Gate
The
input
to
the
linear
gate
will
accept
al
l
pulse
shapes
existing
in
the
ORTEC
400
Series
linear
function
modules.
If
the
input
signal
is
bipolar,
the
negative
portion
will
not
be
passed
through
the
linear
gate.
The
input
impedance
is
greater
than
5000
ohms,
and
the
input
is
normally
sent
from
the
factory
ac
coupled.
The
input
con
be
operated
dc
coupled
if
desired
(refer
to
Section
4.4.1).
A
dc
restoration
network
at
the
input
reduces
baseline
shift
at
high
counting
rates.
The
restoration
network
works
on
both
unipolar
and
bipolar
input
pulse
shapes.
The
linear
gate
proper
consists
of
a
series-parallel
satu
rated
transistor
switch.
This
switch
network
incorporates
an
adjustment
that
allows
the
linear
gate
to
operate
with
no
pedestal.
The
series-parallel
tran
sistor
switch
is
activated
by
a
transistor-pair
current
switch.
This
latter
switch
is
activated
by
the
gate
control
pulse
which
is
generated
with
the
application
of
on
externally
generated
enable
pulse.
The
output
of
the
linear
gate
circuit
is
fed
into
a
cascode
emitter
follower
cable
driver.
The
Model
426
has
two
operating
modes:
1)
normally
blocks
all
input
signals
not
accompanied
by
an
enable
pulse
and
2)
normally
passes
all
signals
unless
accompanied
by
an
inhibit
signal.
The
inhibit
signal
can
be
fed
into
the
front
panel
ENABLE
connector
for
PULSE
INHIBIT
operation
or
into
the
DC
INHIBIT
connector
for
dc
or
continuous
inhibit
operation.

u
2
-
1
SPECIFICATIONS
2.1
General
Specifications
The
ORTEC
Model
426
is
housed
in
a
Nuclear
Standard
Module.
The
module
is
one
standard
module
wide,
and
weighs
2.1
pounds.
The
module
contains
no
internal
power
supply
and
therefore
obtains
the
necessary
operating
power
from
the
Nuclear
Standard
Bin
and
Power
Supply,
ORTEC
Model
401/402.
Al
l
signals
in
and
out
of
the
module
are
on
front
panel
BNC
connectors,
and
the
input
power
is
via
the
standard
connector
on
the
rear
panel
.
2.2
Linear
Gate
Specifications
Linear
Input
Linear
Input
Impedance
Gain
Linearity
Gate
Width
Pulse
Feedthrough
Output
Pedestal
Output
Output
Impedance
Temperature
Stability
Operating
Temperature
Range
Enable
Input
Enable
Input
Impedance
DC
Inhibit
Input
DC
Inhibit
Input
Impedance
Unipolar
or
bipolar
with
the
positive
portion
leading.
Rated
range
0.2
to
10
volts,
12
volts
maximum.
Greater
than
5000
ohms.
Unity.
Integral
nonlinearity
less
than
0.15%
from
0.2
to
10
volts.
Continuously
variable
from
0.3
to
4psec.
Less
than
lOmV
with
a
10volt
input
pulse,
Output
pedestal
can
be
adjusted
to
less
than
1
mV.
0.2
to
10
volts
positive
rated
output
range,
12
volts
maximum.
Approximately
2
ohms,
short-circuit
protected.
Gain
shift
is
less
than
0.015%
per
°C.
0
to
50°C.
Any
positive
input
greater
than
2V,
maximum
input
20
volts.
1000
ohms,
dc
coupled.
Any
positive
dc
input
greater
than
4V,
maximum
input
20V.
650
ohms,
dc
coupled.

Counting
Rate
Power
Requirements
Mechanical
Connectors
2-2
The
gain
shift
of
a
4V
reference
pulse
is
less
than
0.25%
with
the
application
of
an
additional
count
rate
of
65K
ctv^
sec
of
6.0V
random
pulses.
+24V
+
12V
-12V
-24V
30
mA
16
mA
4.9
mA
49
mA
(All
power
via
AMP
202515-3
connec
tor,
per
TID-20893.)
One
module
wide
and
designed
to
meet
the
recommended
interchangeability
standards
set
out
in
Atomic
Energy
Com
mission
report
TID-20893,
1.35
inches
wide,
8.75
inches
high,
and
9.75
inches
long.
Input
and
Output
signal
—
BNC
(UG-
1094/U).

3
-
1
3.
INSTALLATION
3.1
General
Instol
lotion
ConslderaHons
The
Model
426,
used
In
conjunction
with
a
Model
401/402
Bin
and
Power
Supply,
is
intended
for
rack
mounting
and
as
such
it
is
necessary
to
ensure
that
vacuum
tube
equipment
operating
in
the
same
rack
with
the
Model
426
have
sufficient
cooling
air
circulating
to
prevent
any
localized
heating
of
the
all
transistor
circuitry
used
throughout
the
Model
426.
The
temperature
of
equipment
mounted
in
rocks
can
easily
exceed
120°F
(50®C)
unless
pre
cautions
are
taken.
The
Model
426
should
not
be
subjected
to
temperatures
in
excess
of
120°F
(50°C).
3.2
Connection
to
Power
—
Nuclear
Standard
Bin,
ORTEC
Model
401/402
The
Model
426
contains
no
internal
power
supply
and
therefore
must
obtain
power
from
the
Nuclear
Standard
Bin
and
Power
Supply,
such
as
the
ORTEC
Model
401/402.
It
is
recommended
that
the
bin
power
supply
be
turned
off
when
inserting
or
removing
modules.
The
ORTEC
400
Series
is
designed
so
that
it
is
not
possible
to
overload
the
bin
power
supply
with
a
full
complement
of
modules
in
the
Bin.
However,
this
may
not
be
the
case
when
the
Bin
con
tains
modules
other
than
the
ORTEC
design.
Therefore,
the
power
supply
voltages
should
be
checked
after
insertion
of
modules
in
the
latter
case.
The
ORTEC
Model
401/402
has
test
points
on
the
power
supply
control
panel
to
monitor
the
dc
voltages.
When
using
the
Model
426
outside
the
Model
401/402
Bin
and
Power
Supply,
care
must
be
taken
to
ensure
that
the
power
jumper
cable
used
properly
ac
counts
for
the
power
supply
grounding
circuits
provided
in
the
recommended
standards
of
AEC
TID-20893.
Both
clean
and
dirty
ground
connections
are
provided
to
ensure
proper
reference
voltage
feedback
into
the
power
supply,
and
these
must
be
preserved
in
remote
coble
installations.
Care
must
also
be
exercised
to
avoid
ground
loops
when
the
module
is
not
physically
in
the
Bin.
3.3
Input
Signal
Connection
to
Linear
Gate
The
linear
input
to
the
Model
426
is
on
the
front
panel
BNC
connector
and
is
directly
compatible
with
the
output
of
all
linear
amplifiers,
biased
amp
lifier,
pulse
stretchers,
delay
amplifiers,
and
all
Iinear
circuitry
found
in
the
ORTEC
400
Series.
The
linear
gate
passes
only
positive
unipolar
signals
and/or
the
positive
portion
of
bipolar
signals.
This
must
be
kept
in
mind
when
putting
in
linear
signals
from
other
than
ORTEC
products.
The
linear

p
3-2
Input
to
the
Model
426
linear
gate
is
ac
coupled
as
normally
supplied
but
may
be
dc
coupled
if
desired.
If
the
linear
input
to
the
Model
426
is
driven
from
a
low
driving
impedance,
such
as
the
ORTEC
Model
410
output,
the
Model
426
linear
input
should
be
terminated
in
the
characteristic
impedance
of
the
connecting
coaxial
cable.
3.4
Logic
Inputs
to
the
Enable
Input
The
input
pulses
to
the
enable
input
may
come
from
any
source
of
logic
pul
ses.
The
input
impedance
of
the
enable
input
is
one
thousand
ohms,
dc
cou
pled,
and
some
care
must
be
given
to
ensure
that
reflections
do
not
occur
in
the
driving
transmission
coble.
This
probably
can
best
be
avoided
by
termi
nating
the
driving
cable
at
the
enable
input
with
the
characteristic
impedance
of
the
driving
coble.
The
amplitude
and
width
of
the
enable
input
signal
is
specified
in
Section
2.2.
The
maximum
width
of
the
enable
input
is
not
specified
in
Section
2.2
and
indeed
may
be
any
width
since
the
enable
signal
is
regenerated
to
allow
gate
width
duration
to
be
independent
of
the
pulse
shape
of
the
enable
input.
The
minimum
recommended
full-width
at
half-maximum
of
the
enable
input
is
50
nsec,
although
larger
amplitude
narrower
pulses
will
trigger
the
enable
circuitry.
3.5
Logic
Inputs
to
the
DC
Inhibit
Input
The
some
considerations
of
paragraph
one
of
this
section
apply
to
the
input
pulses
to
the
DC
INHIBIT
INPUT
connector.
This
input
provides
the
facility
to
block
the
passage
of
signals
through
the
linear
gate
by
the
application
of
a
dc
voltage
either
in
the
basic
form
of
a
battery
and
switch
contact
or
by
the
application
of
a
pulse
waveform
between
dc
voltage
levels.
The
input
is
dc
coupled
and
has
an
impedance
of
approximately
650
ohms.
A
maximum
dc
voltage
of
20
volts
is
allowed
on
this
input.
11
V
k

!•
Linear
Output
Signal
Connections
and
Terminating
Impedance
Considerations
The
source
impedance
of
the
0-10
volt
standard
linear
outputs
of
most
400
Series
modules
is
approximately
1
ohm.
Interconnection
of
linear
signals
is,
thus,
non-critical
since
the
input
impedance
of
circuits
to
be
driven
is
not
important
in
determining
the
actual
signal
span,
e.g.,
0-10
volts,
de
livered
to
the
following
circuit.
Paralleling
several
loads
on
a
single
out
put
is
therefore
permissible
while
preserving
the
0-10
volt
signal
span.
Short
lengths
of
interconnecting
coaxial
cable
(up
to
approximately
4
feet)
need
not
be
terminated.
However,
if
a
cable
longer
than
approximately
4
feet
is
necessary
on
a
linear
output,
it
should
be
terminated
in
a
resistive
load
equal
to
the
cable
impedance.
Since
the
output
impedance
is
not
purely
resistive,
and
is
slightlydifferent
for
each
individual
module,
when
a
certain
given
length
of
coaxial
cable
is
connected
and
is
not
terminated
in
the
characteristic
impedance
of
the
cable,
oscillations
will
generally
be
observed.
These
oscillations
can
be
suppressed
for
any
length
of
cable
by
properly
terminating
the
cable
either
in
series
at
the
sending
end
or
in
shunt
at
the
receiving
end
of
the
line.
To
properly
terminate
the
cable
at
the
receiving
end,
it
maybe
necessary
to
consider
the
input
impedance
of
the
driven
circuit,
choosing
an
additional
parallel
resistor
to
make
the
combination
produce
the
desired
termination
resistance.
Series
terminating
the
cable
at
the
sending
end
may
be
preferable
in
some
cases
where
re
ceiving
and
terminating
is
notdesirable
or
possible.
When
series
terminat
ing
at
the
sending
end,
full
signal
span,
i.e.,
amplitude,
isobtainedat
the
receiving
end
only
when
it
is
essentially
unloaded
or
loaded
with
an
impedance
many
times
that
of
the
cable.
This
may
be
accomplished
by
inserting
a
series
resistor
equal
to
the
characteristic
impedance
of
the
ca
ble
internally
in
the
module
between
the
actual
amplifier
output
on
the
etched
board
and
the
output
connector.
It
must
be
remembered
that
this
impedance
is
in
series
with
the
input
impedance
of
the
load
being
driven,
and
in
the
case
where
the
driven
load
is
900
ohms,
a
decrease
in
the
signal
span
of
approximately
10%
will
occur
for
a
93-ohm
transmission
line.
A
more
serious
loss
occurs
when
the
driven
load
is
93ohms
and
the
transmis
sion
system
is
93
ohms.
In
this
case,
a50%
loss
will
occur.
BNCconnec
tors
with
internal
terminators
are
available
from
a
number
of
connector
manufacturers
in
nominal
values
of
50,
100,
and
lOOOohms.
ORTEC
stocks
in
limited
quantity
both
the
50
and
100
ohm
BNC
terminators.
The
BNC
terminators
are
quite
convenient
to
use
in
conjunction
with
a
BNC
tee.

4
-
1
4.
OPERATING
INSTRUCTIONS
4.1
Froni-
Panel
Controls
GATE
WIDTH
—
A
single-turn
potentiometer
is
provided
to
adjust
the
gate
width
to
the
desired
value
within
the
nominal range
of
0.3
to
4
psec.
This
control
is
recess
mounted
and
as
such
is
a
screwdriver
adjustment,
but
it
may
be
panel
mounted
so
that
a
knob
may
be
added
to
the
potentiometer
shaft
to
allow
finger-thumb
adjustment
if
this
seems
desirable.
MODE
SWITCH
—
A
three-position
switch
is
used
to
set
the
linear
gate
into
the
desired
operation
mode.
The
three
modes
are
described
below.
Normal
—
In
this
mode
the
linear
gate
normally
blocks
al
l
input
signals
unless
an
enable
signal
sets
the
linear
gate
to
pass
signals
for
a
selected
duration
(as
set
by
the
Pulse
Width
control)
after
receiving
an
enable
pulse.
Pulse
Inhibit
—
The
reciprocal
of
the
Normal
mode
is
available
with
the
switch
in
this
position,
i.e.,
the
linear
gate
passes
all
signals
except
when
a
pulse
is
applied
to
the
Enable
input.
The
pulse
on
the
Enable
input
causes
the
gate
to
block
the
passage
of
signals
through
the
linear
gate
for
a
duration
set
by
the
Pulse
Width
adjustment.
DC
Inhibit
—
This
mode
is
identical
to
the
Pulse
Inhibit
mode
except
the
application
of
an
inhibit
or
block
input
must
be
mode
on
the
rear
panel
BNC
connector
and
the
linear
gate
will
remain
blocked
for
the
duration
that
the
dc
signal
is
applied
to
the
DC
Inhibit
connector.
For
applications
where
the
linear
gate
is
desired
to
be
switched
for
Normal,
i.e.,
selectively
passing,
to
a
condition
of
passing
all
signals,
the
switch
should
be
operated
between
Normal
and
DC
Inhibit
position
and
there
should
be
no
connection
on
the
DC
Inhibit
rear
panel
connector.
4.2
Initial
Testing
and
Observation
of
Pulse
Waveforms
See
Sections
6.1
and
6.2
for
test
performance
data.
4.3
Connector
Data
CNl
Input
BNC
connector
—
ac
coupled
linear
gate
input.
Input
imped
ance
greater
than
5000
ohms.
Input
rated
voltage
range
0.2
to
lOvolts.
Maximum
input
12
volts.
To
minimize
reflections
when
driving
from
low
impedance
sources
into
this
connector,
a
terminator
equal
to
the
charac
teristic
impedance
of
the
driving
cable
sould
be
shunted
from
this
connec
tor
to
ground.

4-2
CN2
Linear
Gate
output
—
BNC
connector
—
dc
coupled
output.
Output
impedance
less
than
2
ohms.
Positive
ouput
signals
only
with
rated
range
of
0.2
to
10
volts.
Maximum
output
12
volts.
TP2
Linear
Gate
Output
Test
Point
—
Oscilloscope
test
point
for
moni
toring
signal
on
linear
gate
output
BNC
connector
CN2.
This
test
point
has
470
ohm
series
resistor
connecting
it
to
CN2.
CN3
Enable
input
—
BNC
connector
—
dc
coupled.
Input
impedance
1000
ohms.
Requires
a
positive
2V
pulse.
Maximum
input
20
volts.
CN4
DC
Inhibit
Input
—
BNC
connector
—
dc
coupled.
Input
impedance
650
ohms.
Requires
a
positive
4-volt
pulse
or
dc
level.
Maximum
input
20
volts.
Power
Connector
—
Nuclear
Standard
Module
Power
Connector.
AMP
#202515-3.
4.4
Typical
Operating
Considerations
In
the
Normal
mode
the
Linear
Gate
is
opened,
i.e.
passes
input
signals,
with
the
application
of
a
positive
pulse
on
the
Enable
input.
The
duration
that
the
linear
gate
will
remain
open
is
normally
continuously
variable
from
0.3
to
4
psec
via
the
front
panel
control,
for
other
pulse
widths
refer
to
Section
6.2.
Figure
4.1
illustrates
the
gating
action
of
the
Linear
Gate.
Notice
that
only
the
positive
portion
of
the
input
signal
is
passed
through
the
Linear
Gate.
The
Linear
Gate
has
an
internal
pedestal
adjustment
that
al
lows
the
pedestal
to
be
reduced
to
a
negligible
value
(refer
to
Section
6.2
for
adjustment
pro
cedure).
Figure
4.2
shows
the
output
of
the
Linear
Gate
with
the
pedestal
a)
properly
adjusted
and
b)
improperly
adjusted.
4.4.1
The
Linear
Gate
is
normally
operated
in
the
normally
closed
mode
of
operation
with
both
input
and
output
ac
coupled.
Two
variants
from
this
mode
are
possible
1)
gate
operating
normally
open,
i.e.
normally
passes
all
input
signals
except
when
accompanied
by
an
enable
or
inhibit
pulse,
and
2)
gate
dc
coupled
operating
either
normally
closed
or
normally
open.
Operation
in
mode
2
requires
modification
to
the
actual
etched
circuit
board.
For
dc
operation
the
input
and
output
capacitors
C1
and
C6
must
be
replaced
with

4-3
jumper
wires
for
a
dc
connection.
With
this
arrangement
a
small
dc
offset
voltage
from
input
to
output
will
be
observed,
approximately
160
mV,
and
must
be
considered
in
the
connection
of
the
gate
to
the
input
and
output
equipment.
For
operation
in
the
Inhibit
mode,
all
input
signals
will
be
passed
except
when
an
inhibit
signal
is
applied
to
either
the
Enable
input
or
to
the
DC
Inhibit
input.
The
particular
input
depends
on
the
po
sition
of
the
mode
switch.
Enable
input
for
Pulse
Inhibit
position
and
DC
Inhibit
Input
for
the
DC
Inhibit
position
(refer
to
Section
4.1).
With
the
mode
switch
set
to
DC
Inhibit
and
no
input
to
the
DC
Inhibit
connector,
the
linear
gate
will
pass
all
input
signals.
This
can
be
a
very
useful
mode
for
setting
up
experiments
since
the
proper
timing
of
the
input
signal
to
the
Enable
input
is
not
necessary
to
get
an
out
put
signal
.
A
slight
difference
in
the
pedestal
magnitude
may
be
noticed
when
changing
operating
modes
from
Normal
to
DC
Inhibit.
The
pedestal
is
normally
adjusted
for
minimum
in
the
Normal
mode,
but
may
be
adjusted
to
suit
the
experiment
in
any
mode
desired.
Notice
that
as
supplied
C6
is
shorted
with
a
jumper
wire
and
therefore,
the
output
is
dc
coupled.
There
will
be
a
small
dc
offset
voltage
that
is
dependent
on
the
saturation
properties
of
the
gate
transistors
that
will
have
to
be
considered
when
going
into
an
ADC
or
other
units
that
are
dc
coupled.
Capacitor
C6
is
provided
to
allow
ac
coupling
in
these
cases,
but
polarity
of
the
offset
must
be
determined
to
properly
connect
the
solid
tantalum
electrolytic
capacitor,
C6.

5
-
1
CIRCUIT
DESCRIPTION
5.1
Linear
Gate
—
Etched
Board
426-0201
The
input
to
the
linear
gate
can
be
either
ac
or
dc
coupled.
Refer
to
Draw
ings
426-0201-51,
and
426-0201-Bl
.
The
ac-coupled
signal
is
fed
in
on
the
etched
board
and
then
into
the
baseline
recovery
network
consisting
of
diodes
D1
through
D4
and
resistors
R1
and
R40.
The
dc
restoration
network
works
as
follows:
With
the
application
of
a
positive
input
signal
it
is
coupled
through
capacitor
C1
to
the
junction
of
D2
and
R1
.
As
the
junction
of
D2-R1
increases
in
the
positive
direction,
the
current
through
D1
increases
while
the
current
through
D2
decreases
due
to
the
current
flow
out
of
capacitor
C1
through
R1.
The
current
flow
out
of
C1
and
through
R1
is
that
current
necessary
to
main
tain
the
amplitude
of
the
input
voltage
at
the
junction
of
D2
and
R1.
With
the
removal
of
the
input
pulse,
the
quiescent
current
flow
through
D1
is
avail
able
to
recharge
capacitor
C1
back
to
its
steady-state
value,
since
the
current
through
D1
con
be
reduced
to
zero
and
the
current
through
D2
can
increase
in
magnitude
to
a
value
of
21.
Therefore,
the
potential
at
the
junction
of
D2
and
R1
will
be
restored
to
its
steady-state
value
in
a
period
of
time
approximately
equal
to
the
pulse
width
of
the
incoming
pulse.
The
linear
gate
will
gate
through
positive
signals
or
the
positive
part
of
bi
polar
signals.
The
input
signals
are
coupled
through
emitter-follower
Q1
to
the
collector
of
Q2,
the
series
section
of
a
series-shunt
linear
gate.
The
positive
part
of
the
input
signal
back
biases
diode
D6,
while
the
negative
parts
of
bipolar
signals
are
blocked
by
D5.
In
the
steady-state
condition
Q2
is
normally
Off,
since
the
current
switch,
Q4
and
Q5,
is
requiring
a
current
through
R9
of
approximately
4
milliamperes.
Q4
of
the
current
switch
is
nor
mally
On,
and
the
current
required
in
the
emitter
circuit
of
the
current
switch
is
drawn
from
diode
D7
and
resistor
R5.
With
the
heavy
conduction
of
04,
the
base
current
for
Q2
is
zero;
therefore,
the
series
resistance
of
the
collec
tor
to
the
emitter
of
02
is
very
high.
Conversely,
transistor
03
has
a
constant-
current
base
drive
through
R6
of
approximately
1
milliampere,
and
diode
D8
is
back
biased,
causing
shunt
transistor
04
to
be
heavily
saturated.
With
the
application
of
a
positive
signal
to
the
collector
of
02,
and
with
the
absence
of
a
signal
to
the
current
switch,
transistors
04
and
05,
the
series-
shunt
gate
is
closed
for
input
signals
to
C1
.
The
linear
gate
is
opened
by
the
application
of
a
positive
signal
to
the
base
of
05,
which
causes
the
current
switch
to
switch
its
emitter
current
from
04
to
05.
When
05
conducts
the
emitter
current
of
the
current
switch,
the
base
drive
to
02
is
available
via
R5,
and
concurrently,
base
current
for
03
become
negligible,
since
the
col
lector
of
05
requires
approximately
4
mil
I
iamperes.
With
the
current
switch

5-2
conducting
current
In
Q5,
It
Is
seen
that
Q2,
the
series
element.
Is
In
heavy
saturation,
with
the
base
drive
current
supplied
from
R5
flowing
Into
the
base
through
the
emitter
and
back
through
diode
Dll
to
the
emitter-follower,
Q1
.
Also,
Q3,
the
shunt
element
In
the
linear
gate.
Is
now
back
biased
and
pre
sents
a
high
shunt
Impedance
to
signals
flowing
through the
series
element,
Q2.
With
the
series-shunt
linear
gate
In
the
open
position.
I.e.,
Q2
saturated
and
Q4
back
biased,
the
output
signals
of
emitter-follower
Q1
are
presented
to
emitter-follower
Q6
and
then
to
the
cascode
emitter
follower
consisting
of
Q7
and
Q8.
The
output
of
the
cascode
emitter-follower
Is
taken
from
the
emitter
of
Q7
through
C6
to
the
output
of
the
linear
gate,
CN2.
The
current
switch
Q4
and
Q5
Is
controlled
by
the
enable
circuitry,
consisting
of
transistors
Q9
through
Q13.
With
the
application
of
a
positive
enable
sig
nal
at
CN3
greater
than
2
volts
the
Input
trigger
circuit
generates
a
standard
ized
output
pulse
which
Is
fed
to
the
"gate
width"
trigger
pair,
Q12
and
Q13.
Q9
and
QIO
constitute
a
Schmitt
trigger
circuit
which
will
change
from
Its
quiescent
current
carrying
state
when
the
Input
signal
at
the
base
of
Q9
exceeds
the
base
voltage
of
QIO.
In
the
quiescent
state,
09
Is
Off
and
OlO
Is
On
and
conducting
approximately
4
mA
through
R27.
This
trigger
circuit
Is
Independent
of
the
Input
pulse
shape
since
It
Is
dc
coupled.
When
the
quiescent
current
Is
transferred
from
OlO
to
09,
a
positive
voltage
spike
Is
generated
at
the
collec
tor
of
010
due
to
LI
and
R24.
This
signal
causes
Oil,
which
Is
normally
Off,
to
conduct
current
through
R31
which
generates
a
negative
voltage
spike
at
the
collector
of
O
11
.
This
signal
Is
coupled
to
the
base
of
013
via
C8.
013
Is
normally
On
and
012
Is
normally
Off
due
to
the
forward
bias
on
the
base
of
013
from
D9.
With
the
negative
signal
from
the
collector
of
011,
013
turns
off
and
012
conducts
the
quiescent
current
through
R33,
the
com
mon
emitter
resistor.
The
current
through
012
will
flow
until
capacitor
C8
charges
enough
to
cause
the
base
of
013
to
equal
the
base
voltage
of
012.
At
this
time
013
wil
l
return
to
Its
stable
state
conducting
the
quiescent
cur
rent
through
R33.
The
duration
012
conducts
Is
controlled
by
the
time
constant
of
R34
and
R35
and
C8.
The
gate
width
Is
then
seen
to
be
control
led
by
the
setting
of
R35.
The
positive
pulse
generated
at
the
collector
of
013
Is
fed
to
the
current
switch
04
and
05
to
switch
the
current
flowing
In
R9
through
05
during
the
gating
period.
The
above
circuit
description
assumes
the
mode
switch
to
be
In
the
Normal
position.
With
the
switch
In
Pulse
Inhibit
position,
the
base
of
05
Is
held
at
ground
while
the
base
of
04
Is
held
at
-0.6V.
Therefore,
the
current
switch
will
have
the
current
through
R9
flowing
In
05
and
04
will
be
cut

5-3
off.
With
the
current
switch
in
this
condition
Q2
is
saturated
and
Q3
is
cut
off,
thereby
passing
all
input
signals
to
the
base
of
Q6.
With
the
application
of
an
enable
input
pulse,
a
positive
signal
is
applied
to
Q4
base
via
capacitor
C2
and
the
transistors
Q2
and
Q3
change
state
and
thereby
block
passage
of
signals
from
the
input
to
the
base
of
Q6
and
con
sequently
there
is
no
output
from
the
linear
gate.
In
the
DC
Inhibit
position,
the
same
conditions
apply
to
the
current
switch
Q4
and
Q5
and
the
current
switch
can
change
state
only
with
the
application
of
a
positive
input
on
the
DC
Inhibit
input
CN4.
Notice
that
in
the
DC
In
hibit
position
the
current
switch
is
dc
coupled
to
the
connector
CN4
and
therefore,
absolute
control
of
the
linear
gate
is
available
on
connector
CN4.

6-
1
6.
MAINTENANCE
6.1
Testing
Performance
of
Linear
Gate
The
following
paragraphs
are
intended
as
an
aid
in
the
instal
lation
and
checkout
of
the
Model
426.
These
instructions
present
information
on
front
panel
controls,
waveforms
at
test
points
and
output
connectors.
6.1.1
Test
Equipment
The
following,
or
equivalent,
test
equipment
is
needed:
1.
ORTEC
Model
419
Pulse
Generator
2.
Tektronix
Model
580
Series
Oscilloscope
3.
100
Ohm
BNC
Terminators
4.
Vacuum
Tube
Voltmeter
5.
ORTEC
Model
410
Linear
Amplifier
6.
ORTEC
Model
415
Sum-Delay
Amplifier
7.
ORTEC
Model
407
Crossover
Pickoff
8.
Schematic
and
Block
Diagrams
for
Model
426
Linear
Gate
6.1.2
Preliminary
Procedures
1.
Visually
check
module
for
possible
damage
due
to
shipment.
2.
Connect
ac
power
to
Nuclear
Standard
Bin,
ORTEC
Model
401/402.
3.
Plug
module
into
Bin
and
check
for
proper
mechanical
alignment.
4.
Switch
ac
power
on
and
check
the
dc
power
supply
voltages
at
the
test
points
on
the
401
Power
Supply
control
panel.
6.1.3
Linear
Gate
A.
1
.
Feed
the
Model
419
into
a
Model
410.
Feed
the
Bipolar
Output
of
the
Model
410
into
a
Model
407.
Feed
the
Output
from
the
Model
407
into
the
Enable
input
of
the
Model
426.
Set
the
Model
410
pulse
shaping
mode
to
Double
RC
(DRC),
i.e..
Integrator,
First
and
Second
Differentiator
to
0.2
psec.
2.
Also
feed
the
Bipolar
Output
of
the
Model
410
into
the
Delaying
input
of
a
Model
415
Sum-Delay
Amplifier.
The
output
of
the
Model
415
should
be
approximately
0.5
volts.

p
6-2
B.
1.
Observe
the
output
of
the
Model
426
Linear
Gate.
Adjust
the
trimpot
at
the
topof
the
board
for
a
minimum
pedestal
.
2.
The
amplitude
of
both
the
initial
and
final
transient
negative
spikes
should
not
exceed
300
mV.
3.
Feed
the
Output
of
the
Model
415
into
the
linear
Input
of
the
Model
426.
Measure
the
input
and
output
of
the
Model
426.
The
input
should
not
differ
from
the
output
by
more
than
80mV.
4.
Adjust
the
Model
410
Linear
Amplifier
gain
controls
to
give
a
-h8V
pulse
into
the
linear
Input
of
the
Model
426.
The
linear
gate
Output
should
be
8
±0.4V.
Load
the
Model
426
Output
with
100
ohms.
The
output
pulse
amplitude
should
not
decrease
more
than
0.15V.
5.
Adjust
the
Model
410
Linear
Amplifier
gain
controls
to
give
a
+1IV
pulse
into
the
Input
of
the
linear
gate.
The
linear
gate
Output
should
saturate
at
greater
than
lOV.
6.
Remove
the
Model
415
Output
from
the
linear
Input
on
the
Model
426.
Rotate
the
Gate
Width
control
over
its
entire
range
and
measure
the
resultant
gating
period.
The
minimum
should
be
0.3
psec
or
less
and
the
maximum
should
be
4
psec
or
greater.
6.2
Adjustment
of
Linear
Gating
Duration
The
linear
gating
period
is
continuously
variable
from
approximately
0.3
psec
to
4
psec.
The
pulse
width
is
controlled
by
capacitor
C8
and
resistors
R34
and
R35.
To
change
the
gating
duration
simply
adjust
the
control
R35
which
is
recess
mounted
on
the
front
panel.
In
the
event
that
gating
durations
different
from
0.3
to
4
psec
are
desirable,
the
capacitor
C8
may
be
replaced
with
a
capacitor
of
different
value
to
change
the
range
of
gating
duration.
R35
wil
l
stjil
provide
continuously
adjustable
pulse
wdith
within
the
new
range.
6.3
Adjustment
of
Linear
Gate
Pedestal
The
Linear
Gate
has
a
trimpot,
Rll,
to
allow
the
pedestal
on
the
Linear
Gate
Output
to
be
reduced
to
a
negligible
value,
typically
1
mV.
The
trimpot
is
located
near
the
top
of
the
etched
circuit
board.
To
adjust
the
pedestal
it
is
necessary
to
open
the
linear
gate,
with
no
input
signal
feeding
into
the
linear
gate
input
CNl
while
observing
with
an
oscilloscope
the
out
put
of
the
linear
gate.
Observing
the
linear
gate
output,
adjust
the
pedestal
trimpot
until
the
pedestal
is
reduced
to
a
negligible
amount.
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