• Sonuç bulunamadı

Investigation of polarized muon-photon shower in crystals

N/A
N/A
Protected

Academic year: 2021

Share "Investigation of polarized muon-photon shower in crystals"

Copied!
1
0
0

Yükleniyor.... (view fulltext now)

Tam metin

(1)

The Fifth Conference “ Nuclear Science and Its Application”, 14-17 October 2008

INVESTIGATION OF POLARIZED MUON-PHOTON SHOWER IN

CRYSTALS

I.M.NADZHAFOV, M.R .RADZHABO V

Baku State University, Azerbaijan, m raiabovCdmail. ru

Modem accelerator technology and existing modem electronic and muon detectors allow investigating non-elastic electromagnetic interaction of high-energy electrons, muons and y-quanta with atoms and nuclei of matter.

When high-energy charged particles (e*, p.*) and y-quanta pass trough matter, in addition to separate acts, they give birth to shower structures under certain conditions. These shower structures are continuously directed jets of various particles, such as, charged particles in solid and meters, electron (muon)-photon showers in amorphous and crystal environments, nucleon cascades in nuclear matter. Electromagnetic showers resulting from interactions of high energy particles with atom nuclei in crystal environment are main source o f electron, positron and photon beams of high energy and also are excellent tool for investigation of matter structure and electromagnetic properties of nuclei.

This article deals with theoretical investigation of polarized electron-photon showers in crystals at two different initial conditions for emergence of shower: 1) shower is created by energy (E0) initial lepton (e*,^); 2) shower may also be created by initial high-energy y-quantum (E0). We were there first who wrote down equations for the evolution of electromagnetic shower in crystals and found solutions to these equations under initial conditions indicated above. Analytical expressions that we obtained for the distribution of shower leptons and y-quanta are

Pl 2 (t,E0,E) = Fl 2 (5 ,1 ,)exp(j - 1, (s)t) r i2(t,E0, E ) ^ ® 12(s,\ ,)e x p (j - I x(s)t)

Here s - is Laplas-Mellin parameter, E0, E - are initial and current energies of shower particles,

t -- is depth of penetration, Fh2(s, I ,), <J>12(5 ,I,), I , and y - are some functions depending on s, initial energy of particles and initial conditions.

Detailed analysis o f these functions for diamond crystal indicates that initial conditions make strong impact on both distribution function o f shower particles and their polarization properties.

Referanslar

Benzer Belgeler

We change the shape of the background to be a second order polynomial function for data with p ffiffiffi s &gt; 3.7 GeV and to a shape from the inclusive MC sample for the data at p

ٕٔ لصفلا نياثلا : فيرعتلا باتكلاب ( رثوكلا يرالجا ) وتافلؤم رداصمو فلؤلدا تيلا دمتعا اهيلع في وباتك .... ٕٗ ثحبلدا لولأا : فيرعتلا ماعلا

Son sınıf biyoloji öğretmen adaylarının (N=26) modern genetik öğrenme progresyonunun yapılarından biri olan A yapısından aldıkları ortalama puanları zaman değişkenine

Antena eksopod dört segmentli, birinci segment iki, ikinci ve üçüncü segment bir, dördüncü segment üç seta taşır.. P1 eksopod ve endopod üçer

Eser elementlerin bentonitlerdeki değişimlerine bakıldığında, Yeniköy, Kargın ve Çekirdekli bentonitlerinde Cs, Rb ve U; Dereköy bentonitinde ise Cs, Rb, U ve Y

Dye adsorption and Photocatalytic degradation of RhB for the pure ZnO NR and ZnO NR-rGO nanocomposite (a) Adsorption of MB in dark, (b) degradation under visible irradiation,

Because of increasing reports of rickets [ 21 ] and the high prevalence of vitamin D deficiency in breastfeeding infants [ 6 , 8 , 21 ] and the new data in adults on the safety of up

Bu araştırmanın odağı olan televizyon program türlerindeki, do- layısıyla televizyon programlarındaki dönüşümü incelemek ve televizyonun yeni medyayla olan ilişkisini