• In a Geiger-Muller (GM) radiation detection tube, the primary fill gas is an inert noble gas, most commonly Argon (at approx. 0.1 atm pressure).
• Incident ionizing radiation ionizes argon gas atoms, producing primary electron-ion pairs that accelerate toward the central anode wire to trigger a Townsend avalanche.
• small amount of a quench gas (such as ethyl alcohol vapor or halogens like chlorine/bromine) is admixed to prevent continuous secondary discharges.
• Argon is universally selected due to its chemically inert behavior, low ionization potential, and stable Townsend cascade generation.

Thermalized (slow) neutrons reach thermal equilibrium with soil hydrogen atoms at ambient temperatures, traveling at an approximate velocity of 2.7 km/s.

• 7 km/s: Below the thermal equilibrium velocity corresponding to thermal neutron energies at room temperature.
• 1600 km/s: Corresponds to intermediate epithermal neutron velocities.
• 7 km/s: At thermal equilibrium (energy ~0.025 to 0.04 eV at 20-25 °C), slowed neutrons attain a mean velocity of roughly 2.2 to 2.7 km/s.
• 500 m/s: Far below the kinetic velocity of thermalized neutrons.

• The Liquid Scintillation Counter (LSC) is an analytical instrument designed to detect and quantify radioactive decay by converting beta particle kinetic energy into light pulses using a scintillation fluor.
• LSC is universally recognized as the gold standard for counting low-energy beta emitters, notably Tritium (3H, E_max = 0.0186 MeV), Carbon-14 (14C, E_max = 0.156 MeV), and Sulfur-35 (35S, E_max = 0.167 MeV).
• High-energy beta emitters like Phosphorus-32 (32P, E_max = 1.71 MeV) produce substantial Cherenkov radiation and can also be counted on LSC or Geiger-Muller counters.
• RPSC officially designated Option 1 (Phosphorus-32 / beta radiation) as the keyed answer.