You are in Germany, but the text in the image is Polish. Apparently this isn't an oscilloscope capture that you made yourself.
This image is doesn't look quite correct for the magnetizing current of a real transformer winding which is energized by a sine wave. Since the flux in the core is proportional to the integral of the applied voltage, the flux peak occurs at the end of each half cycle, not at the peak of the applied sine.
The exciting current consists of a sine wave of current due to the resistance of the wire, plus a peaky waveform with the peak occurring near the end of each half cycle. The image you show is too symmetrical to be representative of a small real transformer. It's what you might expect from some sort of an ideal winding with no resistance.
Very small transformers in particular tend to be designed to operate further into saturation than larger ones, because their regulation is poorer, and their surface area to volume ratio is more favorable to dissipate heat; this gives an exciting current waveform that is even more peaky than larger transformers.
I found a small (5 VA rating) transformer to make some measurements with.
Here's a scope capture of the applied voltage (blue), exciting current (orange) and the instantaneous product of the two (red):
The average of the red waveform is the true power dissipation (1.12 watts). The exciting current is much more peaky than shown in the image you posted. The third harmonic is 37% of the fundamental.
The apparent power is the product of the applied voltage (121 VAC) and the exciting current (35.3 mA), which is 4.27 VA, 3.8 times the true power. The apparent power is sufficiently larger than the true power to justify characterizing the exciting current as a mostly reactive current.
From this we get the primary inductance as 121/(2*Pi*60*.0353) = 9.09 henries. Compare this to the inductance measured on an LCR meter:
Code:
Applied Inductance
Voltage
.01 3.02H
0.1 3.29H
1.0 4.56H
10 8.30H