Calculator for our levers
Components
Diode
- Reverse biased diode forms a depletion region as charges migrate
- Electron moves faster - induces curent
- Great for gamma ray detection
- Charged particles (gammas from Bremsstrahlung radiation) deposit energy onto depletion region of photodiode.
- Produces an electron-hole pair due to:
- Thermal excitation of photodiode material induces a dark current
- Source of our baseline
- When this baseline is too large, lose range in our channel
Op-Amp
- Standard non-inverting config
- 0-3.3V range
- Gain will amplify our baseline and any noise!
- Gain provided by ratio of lower resistor network
Capacitor
- Q = C * V
- Q is the charge from induced current from photodiode - constant
- V is the pulse we see that gets read by ADC (after amplification)
- Voltage pulse is inversely proportional to capacitance
- Basically, capacitance inversely proportional to sensitivity
- smaller capacitance = more sensitive
- low C → high V → bigger pulse to be read → more sensitive
- larger capacitance = less sensitive
- high C → low V → smaller pulse to be read → less sensitive
- smaller capacitance = more sensitive
Resistor
- V = I * R
- I is the current from diode
- V is the pulse we see that gets read by ADC
- Resistance proportional to baseline voltage
- If R too high, baseline is too high, and our usable range is smaller
- Less sensitive sensor!
Time Constant
- R * C
- Higher time constant
- Slower decay
- Can sample slower!
- lower data volume
- Can sample slower!
- Only possible by:
- Increasing baseline (bad)
- Decreasing sensitivity
- Not suitable for more sensitive channels
- Slower decay
- Lower time constant
- Faster decay
- Must sample faster!
- higher data volume
- Must sample faster!
- Only possible by:
- Lowering baseline (good)
- Increasing sensitivity
- Not suitable for less sensitive channels
- Faster decay