kta1 · 2014. 1. 26. · bhabha (e+) positron annihilation 10 100 e (mev) 0.20 0.15 0.10 0.05 1000...
TRANSCRIPT
![Page 1: KTA1 · 2014. 1. 26. · Bhabha (e+) Positron annihilation 10 100 E (MeV) 0.20 0.15 0.10 0.05 1000 1.0 0.5 Figure 30.11: Fractional energy loss per radiation length in lead as a function](https://reader036.vdocuments.pub/reader036/viewer/2022071401/60ec2794e750794ef87813e4/html5/thumbnails/1.jpg)
KTA 1
Folien zur Vorlesung vom 27.11.2013
![Page 2: KTA1 · 2014. 1. 26. · Bhabha (e+) Positron annihilation 10 100 E (MeV) 0.20 0.15 0.10 0.05 1000 1.0 0.5 Figure 30.11: Fractional energy loss per radiation length in lead as a function](https://reader036.vdocuments.pub/reader036/viewer/2022071401/60ec2794e750794ef87813e4/html5/thumbnails/2.jpg)
Energieverlust von Elektronen
![Page 3: KTA1 · 2014. 1. 26. · Bhabha (e+) Positron annihilation 10 100 E (MeV) 0.20 0.15 0.10 0.05 1000 1.0 0.5 Figure 30.11: Fractional energy loss per radiation length in lead as a function](https://reader036.vdocuments.pub/reader036/viewer/2022071401/60ec2794e750794ef87813e4/html5/thumbnails/3.jpg)
Gewichtsfaktoren für Äquivalentdosis
Aus W.R. Leo: Techniques for Nuclear and ParLcle Physics Experiments
![Page 4: KTA1 · 2014. 1. 26. · Bhabha (e+) Positron annihilation 10 100 E (MeV) 0.20 0.15 0.10 0.05 1000 1.0 0.5 Figure 30.11: Fractional energy loss per radiation length in lead as a function](https://reader036.vdocuments.pub/reader036/viewer/2022071401/60ec2794e750794ef87813e4/html5/thumbnails/4.jpg)
MiQlere Strahlungsdosis von verbreiteten Quellen
Aus W.R. Leo: Techniques for Nuclear and ParLcle Physics Experiments
![Page 5: KTA1 · 2014. 1. 26. · Bhabha (e+) Positron annihilation 10 100 E (MeV) 0.20 0.15 0.10 0.05 1000 1.0 0.5 Figure 30.11: Fractional energy loss per radiation length in lead as a function](https://reader036.vdocuments.pub/reader036/viewer/2022071401/60ec2794e750794ef87813e4/html5/thumbnails/5.jpg)
Aus W.R. Leo: Techniques for Nuclear and ParLcle Physics Experiments