Abstract:Using CORSIKA simulations of the highest energy extensive air showers we show that all showers are similar when described by the shower age parameter: the angular and energy spectra of electrons at a given level in the atmosphere depend only on the shower age at this level. Moreover, electrons with a given energy have the same angular distributions at any level (age) of the shower. We have calculated these distributions and found analytical functions describing them quite well. The total number of particles ca… Show more
“…on the age parameter s [8]; it does not depend on primary particle mass or energy (the same conclusion was obtained by Nerling et al [10]), -the angular distribution of electrons with a fixed energy depends on this energy only -it is the same anywhere in the shower [9]; from the two statements above it follows that the angular distribution of all electrons (with any energy) depends on the shower age only, -the lateral distribution of electrons, if distances are expressed in the Molière unit r M at the level in consideration, depends on the shower age only [14] (the same holds for electrons with a fixed energy [19]). …”
Section: The General Ideasupporting
confidence: 67%
“…We show here that due to the similarity of high energy showers [8,9,14] it is possible to calculate the lateral distribution of ChL (LDCh) without time-consuming shower simulations, but in an analytical way (with numerical calculations of integrals), using the various earlier determined electron distributions which are universal.…”
Section: The Methods Of Calculation Of the Lateral Distribution Of Chlmentioning
confidence: 99%
“…The angular distribution G e θ (θ; s, h) (per unit angle θ) can be calculated from the known angular distributions of electrons with fixed energies, g θ (θ; E) (per unit solid angle) [9], and the energy spectrum of all electrons at level s, f (E; s) [8,10],…”
Section: Angular Distribution Of Ch Electrons G E θ (θ; S H)mentioning
confidence: 99%
“…This effect has been first aknowledged and allowed for by the Fly's Eye Collaboration [4]. Later some other methods to take it into account have been proposed [9][10][11]. In these papers, however, it was only the total number of Ch photons emitted from consecutive shower track elements that were taken into consideration.…”
We calculate the lateral distribution of Cherenkov light at different levels of shower development. The calculations use the universal characteristics of large showers. We derive that the angular and lateral distributions of Cherenkov photons emitted by a shower path element depend only on the shower age and height in the atmosphere of this element. The width of a shower image in the Cherenkov scattered light also depends, however, on the zenith angle and X max . We also show that below shower maximum it is considerably wider than the width in the fluorescence light.
“…on the age parameter s [8]; it does not depend on primary particle mass or energy (the same conclusion was obtained by Nerling et al [10]), -the angular distribution of electrons with a fixed energy depends on this energy only -it is the same anywhere in the shower [9]; from the two statements above it follows that the angular distribution of all electrons (with any energy) depends on the shower age only, -the lateral distribution of electrons, if distances are expressed in the Molière unit r M at the level in consideration, depends on the shower age only [14] (the same holds for electrons with a fixed energy [19]). …”
Section: The General Ideasupporting
confidence: 67%
“…We show here that due to the similarity of high energy showers [8,9,14] it is possible to calculate the lateral distribution of ChL (LDCh) without time-consuming shower simulations, but in an analytical way (with numerical calculations of integrals), using the various earlier determined electron distributions which are universal.…”
Section: The Methods Of Calculation Of the Lateral Distribution Of Chlmentioning
confidence: 99%
“…The angular distribution G e θ (θ; s, h) (per unit angle θ) can be calculated from the known angular distributions of electrons with fixed energies, g θ (θ; E) (per unit solid angle) [9], and the energy spectrum of all electrons at level s, f (E; s) [8,10],…”
Section: Angular Distribution Of Ch Electrons G E θ (θ; S H)mentioning
confidence: 99%
“…This effect has been first aknowledged and allowed for by the Fly's Eye Collaboration [4]. Later some other methods to take it into account have been proposed [9][10][11]. In these papers, however, it was only the total number of Ch photons emitted from consecutive shower track elements that were taken into consideration.…”
We calculate the lateral distribution of Cherenkov light at different levels of shower development. The calculations use the universal characteristics of large showers. We derive that the angular and lateral distributions of Cherenkov photons emitted by a shower path element depend only on the shower age and height in the atmosphere of this element. The width of a shower image in the Cherenkov scattered light also depends, however, on the zenith angle and X max . We also show that below shower maximum it is considerably wider than the width in the fluorescence light.
“…Studies have shown that two extra parameters are needed for the full description of the general profiles, but there can be strong correlations between them [6,7]. A widely use, successful parametrization is the GaisserHillas profile [8], which can be written in terms of the new variables, X , N , as follows:…”
The longitudinal development of extreme energy cosmic ray showers has a characteristic "Universal Shower Profile" when normalized and translated to the shower maximum. Experimentally accessible observables can be defined to parametrize the average shape and characterize each event. By describing the full shape of the profile, information related to the first hadronic interactions and primary particle type can be extracted. A shape variable which measures the distance from the first interaction to the depth of maximum can lead to a cosmic ray composition analysis with independent extraction of the primary cross-sections.
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