URL: https://www.desy.de/school/school_lab/zeuthen_site/cosmic_particles/glossar/@@siteview

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## Breadcrumb Navigation

# Glossar

# A

## Atmospheric Pressure Correction

As they pass through the Earth's atmosphere, cosmic particles interact with particles in the air. Therefore, the distance between the air particles and thus the air pressure has an influence on the number of cosmic particles that can be measured on the Earth's surface. Back in the 1920s, physicists were able to prove experimentally that the rate of cosmic particles is lower at high atmospheric pressure and higher at low atmospheric pressure. However, this effect could only really be explained many years later after the discovery of muons and pions. When primary particles of cosmic radiation interact with air molecules, charged pions are created along with other particles. Pions decay after an extremely short average lifetime into a muon and a neutrino. At low atmospheric pressure, the density of the air is lower and it is more likely that pions decay before they can interact with other nuclei. This leads to a higher rate of muons reaching the earth's surface.

In order to investigate the correlation, the data is fitted. This means that we seek a function that describes the data distribution best. The deviation (the error) between the true measured value and the value of the function should be as small as possible. Computer programs can automatically find the best fit with the smallest error. Therefore, it varies the variables of the mathematical formula in a way that it results in the best description of the experimental data. This is also possible by manual means, but it is very time-consuming.

The figure on the right shows the muon rate versus the atmospheric pressure measured by the Neumayer Station III in 2013. The dark blue line is a least squares fitting of the data distribution. It shows an exponential dependence which can be described mathematically with this formula:

with $R$ the muon rate, $p$ the atmospheric pressure and $a$ and $b$ factors depending on the measurement.

Every investigation of cosmic particle rates has to consider variations of the atmospheric pressure. To correct this effect, one has to estimate the dependence of the particle rate on the atmospheric pressure and then apply a correction function. The procedure to estimate this correction function can be simplified by fitting a linear function. The necessary linear relation can be obtained by applying the logarithm of the particle rate versus atmospheric pressure as shown in the second figure.

Now, the experimental distribution can be described by a linear function:

In order to get to the needed correction function, which can be applied to the experimental data, the slope $m$ must be determined. For this, the adjacent figure is used:

From this relation the correction function can be derived:

with $m$ the barometric coefficient, $\mathrm{Rg}$ the measured muon rate, $\mathrm{Rk}$ the corrected muon rate, $\mathrm{pg}$ the measured atmospheric pressure and $\mathrm{pM}$ the mean value of the atmospheric pressure.

The right part of the equation can now be used as a correction function for the particle rates provided in Cosmic@Web. But how can the individual parameters and variables be determined?

Step 1: The value $\mathrm{pM}$ is the average atmospheric pressure of the investigated period of time. It is displayed as "mean" in the legend of a 1D histogram.

Step 2: In Cosmic@Web the linear fit function and the start parameters have to be defined. Then the slope $m$ is fitted automatically and the result is shown in the legend of the log(muon rate) vs air pressure diagram.

Step 3: The corrected particle rate is obtained by setting the correction function into the field “Correction Function for y-Variable” of Cosmic@Web.

## Avalanche Photo Diode

When light hits the diode, it triggers electrons in the intrinsically conductive i-layer, resulting in electron-hole pairs (photoelectric effect). The defect electrons ("imaginary" positive movable charge carriers) then move to the p-layer, the electrons move to the p-n junction. There they are strongly accelerated due to the high field strength and trigger further electrons by impact ionization. In this way, an avalanche of electrons is created, as in a PMT, which multiplies the signal strength.