BLR1 [ETC]
Amplifier. Other ; 功放。其他\n
| 型号： | BLR1 |
| 厂家： | 
ETC |
| 描述： | Amplifier. Other
|
| 文件： | 总2页 (文件大小：40K) |
| 中文： | 中文翻译 | 下载： | 下载PDF数据表文档文件 |
R
AMP
TEK
Amptek’s BLR1 restores the
baseline in high counting rate ap-
plications. The BLR1 is typically
used with the A275, A203, and
A225. In order to simplify test-
ing and prototype work, the PC-
275 test board is also available.
BLR1 PIN CONFIGURATION
FUNCTION
PIN
1
4
6
7
8
9
External capacitor to ground
+ Input
- Input
+6 V (At 2.5 ma)
-6 V (At 2.5 ma)
Ground & case
Output (If the unit oscillates, use Pin 1 for Output with an external 10 k, replacing the
internal 10 k.)
12
2, 3, 5, 10, 11 No connection
THEORY OF OPERATION
The BLR1 is a transconductance amplifier with transconductance of approximately 17ma/Volt and
very wide bandwidth. In operation, it amplifies both the DC baseline component and the pulse signal
component by a large factor. Typically, with the PIN 12 output connected to a low impedance, the
amplifier load is the internal 20kΩ resistor. The low frequency voltage gain at the amplifier output is
17ma/Volt x 20kΩ = 340. The amplified pulses are clipped by the pair of Schottky diodes to an
amplitude of ±0.5V and thus have little influence on the average output of the amplifier, which is
dominated by the amplified baseline. This output is then passed through a low-pass RC filter formed
by the first 10kΩ and the total capacitance (internal and external) from PIN 1 to ground. The filtered
output is fed back to the input of the shaping amplifier chain to zero the baseline at the output of the
amplifier chain.
EXAMPLE
Assume both BLR1 and the amplifier chain have zero offset voltage, so that in the absence of pulses the
BLR1 output is zero, since no correction is required. Now assume 1µs pulses are present at the output of
the amplifier chain at a rate of 105/s. At the output of the BLR1 amplifier, this will produce a 10% duty cycle
waveform with peak amplitude of 0.5V. In order that the average of this signal be near zero volts, the
baseline at this point will have to shift downward by (0.5V ÷ 9) = 56mV. Dividing by the amplifier gain of
340, we get a baseline shift at the input of the BLR1 of just minus 160µV. To generalize:
0.5V (twn)
Baseline Shift = ——————————
AV (1 - twn)
where:
tw = pulse width (near baseline)
· n = pulse rate (c.p.s.)
AV = BLR1 amplifier voltage gain (normally about 340)
Note that when the duty cycle reaches 50%, the baseline shift at the output of the BLR1 amplifier
will reach -0.5V, at which point negative clipping will occur and the baseline can no longer be
maintained. This can be considered to be BLR “saturation.”
The above example is an ideal case. In a real case, there are several complicating factors which must
be considered:
1) There is not a single pulse width, since the effective width is dependent on amplitude,
with a larger pulse appearing to be wider. Thus, the pulse height spectrum influences
the saturation count rate.
2)
3)
The statistical variation in counting rate will affect the baseline shift.
The noise is also amplified by the BLR1 amplifier and appears at the output. Normally,
this noise should be well below the clipping voltage. However, at high count rates, as the
baseline approaches the negative clipping level, negative noise peaks will be clipped,
which will cause the baseline to begin to shift sooner than in the ideal case. Using a long
low-pass time constant minimizes these effects, at the expense of slower recovery should
saturation occur.
Since saturation is dependent on duty cycle, using a shorter peaking time, or pulse width, in the
shaping amplifier will proportionally increase the saturation count rate. Too short of a peaking time
however, will increase the overall noise of the system.
AMPTEK,INC.
R
AMP
TEK
6 DE ANGELO DRIVE, BEDFORD, MA 01730-2204 USA
TEL: +1 (781) 275-2242 FAX: +1 (781) 275-3470
email: sales@amptek.com www.amptek.com
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