Air Density Calculator
Calculate air density from pressure, temperature, and humidity using the ideal gas law. Includes altitude reference table and moist air corrections.
Calculate SiPM photon detection efficiency, fired microcells, saturation, signal-to-noise ratio, and dark count correction for silicon photomultiplier sensors.
| Parameter | Typical Range | Notes |
|---|---|---|
| Breakdown Voltage (Vbr) | 20−70 V | Temperature dependent (~20 mV/°C) |
| Overvoltage (Vov) | 1−5 V | Vbias − Vbr; controls gain & PDE |
| Gain | 10⁵ − 10⁷ | Gain = Cd × Vov / q |
| PDE | 15−50% | Photon detection efficiency at peak λ |
| Dark Count Rate | 10−10⁶ Hz | Thermal carriers; halves per ~8°C cooling |
| Cross Talk | 1−30% | Correlated noise; increases with Vov |
| Afterpulse Prob | 1−10% | Trapped carriers; worse at high gain |
| Recovery Time | 10−100 ns | τ = Rq × Cd per microcell |
Silicon Photomultipliers (SiPMs) are arrays of single-photon avalanche diodes (SPADs) operating in Geiger mode. Each microcell fires independently when it detects a photon, producing a standardized charge pulse. The total signal is the sum of all fired microcells.
Photon Detection Efficiency (PDE) is the probability that an incident photon triggers a microcell — it depends on overvoltage, wavelength, and fill factor. This calculator computes the expected number of photoelectrons, the saturation-corrected number of fired microcells, total output charge, dynamic range, and signal-to-noise ratio.
SiPMs have a finite number of microcells, so they saturate when many photons arrive simultaneously. The saturation model accounts for this: N_fired = N_total × (1 − exp(−Npe/N_total)). The calculator also adjusts dark count rate for temperature (DCR doubles every ~8°C).
Presets for popular SiPMs from Hamamatsu, SensL, and OnSemi let you quickly explore real device performance. This calculator is essential for designing PET scanners, LiDAR detectors, fluorescence readers, and any photon counting system using SiPMs.
SiPMs are replacing traditional PMTs in many applications, but their nonlinear saturation, temperature-dependent noise, and correlated noise require careful analysis.
It gives the essential SiPM performance metrics including saturation correction and temperature-adjusted dark count rates.
Overvoltage: Vov = Vbias − Vbr.
Photoelectrons: Npe = Nph × PDE.
Fired microcells: Nfired = Ntot × (1 − exp(−Npe/Ntot)).
Charge: Q = Nfired × Gain × q (q = 1.602×10⁻¹⁹ C).
DCR(T) = DCR(25°C) × 2^((T−25°C)/8°C).
SNR = Npe / √(Npe + DCR × t_gate).Result: Npe = 40, Nfired = 39.6, saturation = 1.1%, Q = 10.8 fC
Overvoltage = 3 V. Npe = 100 × 0.40 = 40 photoelectrons. Nfired = 3600 × (1 − exp(−40/3600)) = 39.6 (negligible saturation). Charge = 39.6 × 1.7×10⁶ × 1.6×10⁻¹⁹ = 10.8 fC.
Calculate SiPM photon detection efficiency, fired microcells, saturation, signal-to-noise ratio, and dark count correction for silicon photomultiplier sensors. Use it when you need a repeatable calculation in the physics / general category and want the setup, result, and supporting values kept together. This is especially helpful when small input changes, unit choices, or rounding decisions can change the final number.
Start by confirming that the inputs match the formula shown on the page. Then compare the main output with the worked example and any secondary values shown by the calculator. If the result will be used in another calculation, keep extra precision until the final step and record the assumptions beside the number.
Treat the result as a calculation aid rather than a substitute for context. For schoolwork, include the formula and substitution steps. For planning, technical, financial, or health-related decisions, verify important numbers against primary records, current rules, or a qualified professional before acting on them.
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Overvoltage (Vov) is the bias voltage above breakdown. Higher Vov increases gain, PDE, and detection probability but also increases dark counts, crosstalk, and afterpulsing.
Dark count rate approximately doubles every 8°C. Breakdown voltage increases ~20-50 mV/°C. Cooling a SiPM dramatically reduces noise — medical PET scanners often operate at −20°C.
The finite number of microcells. Once all microcells have fired, additional photons produce no additional signal. For linear response, keep Npe < 0.1 × Nmicrocells.
When one microcell fires, avalanche photons can trigger neighboring microcells. This "optical crosstalk" adds extra counts that inflate the apparent signal. It increases with overvoltage.
Charge carriers trapped during the avalanche are released after the microcell recharges, triggering a second avalanche. It produces delayed spurious counts on timescales of 10-100 ns.
SiPM PDE peaks at 400-450 nm (blue-green) for standard devices. UV-enhanced SiPMs peak at 350 nm. Near-infrared SiPMs use deeper junctions for sensitivity at 800-1000 nm.
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