Gamma-Ray MSP Background Decomposition

Can a steady-state Bekenstein-limited computation signal be separated from OC's millisecond pulsar gamma-ray emission at Fermi-LAT and CTA sensitivity?

🔬 Established astrophysics (MSP emission) ✦ Technosignature speculation
OC's ~25 known MSPs (TRAPUM will likely find 100+) produce a collective gamma-ray luminosity that is the dominant foreground for any technosignature search. A Bekenstein-limited computation signal would need to exceed this background — or have a distinguishable spectral shape above ~10 GeV where MSP emission cuts off sharply.
MSP Population Parameters
25 MSPs
3.2×10³² erg/s
15 yr
Technosignature Signal Parameters
10³⁵ W
1.00×10⁻⁵
Flux & Sensitivity Comparison
Total MSP flux F_msp
GeV/cm²/s
Fermi-LAT sensitivity (T_obs)
GeV/cm²/s
CTA-South sensitivity (50h)
GeV/cm²/s
Predicted signal flux F_signal
GeV/cm²/s
MSP / signal flux ratio
SNR_signal (vs Fermi sens.)
SNR_separation (|F_sig−F_msp|)
Min f_leak for detection
Signal status

MSP gamma-ray background model

Each millisecond pulsar (MSP) in OC emits a characteristic gamma-ray luminosity. The representative model uses spin-down power Ė = 4π²I_NS·Ṗ/P³ with P~3 ms, Ṗ~10⁻²⁰, giving Ė~3.5×10³³ erg/s and a 10% gamma-ray efficiency η_γ~0.1, yielding L_msp~3.5×10³² erg/s per MSP. The total flux at Earth is then F_msp = N_msp × L_msp / (4π × d²) where d = 5.49 kpc.

Converting to GeV/cm²/s: F_msp [GeV/cm²/s] = N_msp × L_msp [erg/s] / (4π × d_cm²) × (1 GeV / 1.602×10⁻³ erg)

Fermi-LAT sensitivity scaling

Fermi-LAT 10-year sensitivity to a point source at 1 GeV is approximately 5×10⁻¹³ GeV cm⁻² s⁻¹. Sensitivity scales as 1/√T_obs, so at 15 years the reference sensitivity is ~4×10⁻¹³ GeV cm⁻² s⁻¹. The tool scales from this reference: F_sens(T) = 4×10⁻¹³ × √(15/T_obs) GeV/cm²/s.

CTA-South sensitivity

CTA-South 50h sensitivity for a steady source above 100 GeV is approximately 5×10⁻¹⁴ GeV/cm²/s (Cherenkov Telescope Array Observatory 2019). This is the integrated sensitivity above ~100 GeV where MSP spectral cutoffs (~2–3 GeV) leave the field clear — making CTA particularly powerful for technosignature discrimination.

Technosignature signal model

A civilization operating Bekenstein-limited computation via BZ extraction at power P_BZ would emit waste radiation. A fraction f_leak leaks as gamma-rays. The signal flux is: F_signal = f_leak × P_BZ / (4π × d²) converted to GeV/cm²/s. This represents a power-law continuum rather than the exponential MSP cutoff above ~3 GeV, which is the key spectral discriminant.

Separability and spectral discrimination

MSP gamma-ray spectra exhibit a characteristic exponential cutoff at ~2–3 GeV. Any BZ-driven emission mechanism would produce a harder spectrum. The SNR_separation metric quantifies whether the flux difference |F_signal − F_msp| exceeds the instrumental sensitivity, independent of the absolute brightness. A signal that sits below MSP emission in total flux but has a different spectral slope above 10 GeV could still be detectable — this is the CTA advantage.

The TRAPUM context

The TRAPUM (TRAnsients and PUlsars with MeerKAT) survey is expected to find ~100 MSPs in OC within a few years, compared to ~25 currently known. Each confirmed MSP contributes to the modeled background and sharpens constraints on any residual unresolved emission. A 100-MSP population raises the foreground by ~4× and makes the technosignature detection problem correspondingly harder — unless the signal has a hard spectral component above 10 GeV.

v1.0 — 2026-06-02 · Code MIT · Prose CC BY 4.0 · Abdo et al. 2013 (ApJS 208:17); Guillemot et al. 2016 (A&A 587:A109); CTA Observatory 2019

Related proposals: Fermi-LAT / CTA →