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Dive into the hybrid scheme of simulations to estimate energy in giant air showers, including transport equations, photon interactions, and results from the Yakutsk array. Understand the energy balance in electron-photon cascades and the detailed cascade equations. Explore the energy scales, space scales, and source functions involved in this complex atmospheric phenomenon. Learn about the Monte Carlo method for particles in real atmospheres and how scintillator detectors respond to these massive showers.
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First energy estimates of giant air showerswith help of the hybrid scheme of simulations L.G. DedenkoM.V. Lomonosov Moscow State University,119992 Moscow, Russia
CONTENT • Introduction • 5-level scheme - Monte-Carlo for leading particles - Transport equations for hadrons - Transport equations for electrons and gamma quanta - The LPM showers - The primary photons - Monte-Carlo for low energy particles in the real atmosphere - Responses of scintillator detectors • The basic formula for estimation of energy • The relativistic equation for a group of muons • Results for the giant inclined shower detected at the Yakutsk array • Conclusion
Transport equations for hadrons: here k=1,2,....m – number of hadron types; - number of hadrons k in bin E÷E+dE and depth bin x÷x+dx; λk(E) – interaction length; Bk – decay constant; Wik(E′,E) – energy spectra of hadrons of type k produced by hadrons of type i.
The integral form: here E0 – energy of the primary particle; Pb (E,xb) – boundary condition; xb– point of interaction of the primary particle.
The decay products of neutral pions are regarded as a source function Sγ(E,x) of gamma quanta which give origins of electron-photon cascades in the atmosphere: Here – a number of neutral pions decayed at depth x+ dx with energies E΄+dE΄
The basic cascade equations for electrons and photons can be written as follows: where Г(E,t), P(E,t) – the energy spectra of photons and electrons at the depth t; β – the ionization losses; μe, μγ – the absorption coefficients; Wb, Wp – the bremsstrahlung and the pair production cross-sections; Se, Sγ– the source terms for electrons and photons.
The integral form: where At last the solution of equations can be found by the method of subsequent approximations. It is possible to take into account the Compton effect and other physical processes.
Source functions for low energy electrons and gamma quanta x=min(E0;E/ε)
Balance of energyby 1 - the primary photon; 2 - electrons; 3 - photons and 4 - under threshold in e-ph shower; 5 - sum of 1,2,3; 6 - total sum
Balance of energyby 1 - the primary photon; 2 - electrons; 3 - photons and 4 - under threshold in e-ph shower; 5 - sum of 1,2,3; 6 - total sum
Balance of energyby 1 - the primary photon; 2 - electrons; 3 - photons and 4 - under threshold in e-ph shower; 5 - sum of 1,2,3; 6 - total sum
Balance of energyby 1 - the primary photon; 2 - electrons; 3 - photons and 4 - under threshold in e-ph shower; 5 - sum of 1,2,3; 6 - total sum
Balance of energyby 1 - the primary photon; 2 - electrons; 3 - photons and 4 - under threshold in e-ph shower; 5 - sum of 1,2,3; 6 - total sum
Balance of energyby 1 - the primary photon; 2 - electrons; 3 - photons and 4 - under threshold in e-ph shower; 5 - sum of 1,2,3; 6 - total sum
Balance of energyby 1 - the primary photon; 2 - electrons; 3 - photons and 4 - under threshold in e-ph shower; 5 - sum of 1,2,3; 6 - total sum
Balance of energyby 1 - the primary photon; 2 - electrons; 3 - photons and 4 - under threshold in e-ph shower; 5 - sum of 1,2,3; 6 - total sum
Balance of energyby 1 - the primary photon; 2 - electrons; 3 - photons and 4 - under threshold in e-ph shower; 5 - sum of 1,2,3; 6 - total sum
Balance of energyby 1 - the primary photon; 2 - electrons; 3 - photons and 4 - under threshold in e-ph shower; 5 - sum of 1,2,3; 6 - total sum
Balance of energyby 1 - the primary photon; 2 - electrons; 3 - photons and 4 - under threshold in e-ph shower; 5 - sum of 1,2,3; 6 - total sum
Balance of energyby 1 - the primary photon; 2 - electrons; 3 - photons and 4 - under threshold in e-ph shower; 5 - sum of 1,2,3; 6 - total sum
Balance of energyby 1 - the primary photon; 2 - electrons; 3 - photons and 4 - under threshold in e-ph shower; 5 - sum of 1,2,3; 6 - total sum
Balance of energyby 1 - the primary photon; 2 - electrons; 3 - photons and 4 - under threshold in e-ph shower; 5 - sum of 1,2,3; 6 - total sum
Balance of energyby 1 - the primary photon; 2 - electrons; 3 - photons and 4 - under threshold in e-ph shower; 5 - sum of 1,2,3; 6 - total sum
Energyby under threshold: 1 - by electrons; 2 - by photons; 3 - by pair; 4 - sum of 1, 2, 3
Energyby under threshold: 1 - by electrons; 2 - by photons; 3 - by pair; 4 - sum of 1, 2, 3
Energyby under threshold: 1 - by electrons; 2 - by photons; 3 - by pair; 4 - sum of 1, 2, 3
Energyby under threshold: 1 - by electrons; 2 - by photons; 3 - by pair; 4 - sum of 1, 2, 3
Energyby under threshold: 1 - by electrons; 2 - by photons; 3 - by pair; 4 - sum of 1, 2, 3
Energyby under threshold: 1 - by electrons; 2 - by photons; 3 - by pair; 4 - sum of 1, 2, 3
Energyby under threshold: 1 - by electrons; 2 - by photons; 3 - by pair; 4 - sum of 1, 2, 3
Energyby under threshold: 1 - by electrons; 2 - by photons; 3 - by pair; 4 - sum of 1, 2, 3
Energyby under threshold: 1 - by electrons; 2 - by photons; 3 - by pair; 4 - sum of 1, 2, 3
Energyby under threshold: 1 - by electrons; 2 - by photons; 3 - by pair; 4 - sum of 1, 2, 3
Energyby under threshold: 1 - by electrons; 2 - by photons; 3 - by pair; 4 - sum of 1, 2, 3
Energyby under threshold: 1 - by electrons; 2 - by photons; 3 - by pair; 4 - sum of 1, 2, 3
Energyby under threshold: 1 - by electrons; 2 - by photons; 3 - by pair; 4 - sum of 1, 2, 3
Energyby under threshold: 1 - by electrons; 2 - by photons; 3 - by pair; 4 - sum of 1, 2, 3
Cascade curves: - NKG; - LPM; lines - individualLPM curves
Cascade curves: - NKG; - LPM; lines - individualLPM curves
Muon density in gamma-induced showers:______ - BH; ______ - LPM; ■ – Plyasheshnikov, Aharonian; - our individual points
Muon density in gamma-induced showers:1 - AGASA; 2 - Homola et al.; 3 - BH; 4 - Plyasheshnikov, Aharonian; 5, 6 - our calculations; 7 - LPM
For the grid of energies Emin≤ Ei ≤ Eth (Emin=1 MeV, Eth=10 GeV) and starting points of cascades 0≤Xk≤X0 (X0=1020 g∙cm-2) simulations of ~ 2·108 cascades in the atmosphere with help of CORSIKA code and responses (signals) of the scintillator detectors using GEANT 4 code SIGNγ(Rj,Ei,Xk) SIGNγ(Rj,Ei,Xk) 10m≤Rj≤2000m have been calculated