VbvNeuE-001

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Chapter 12 About muonic neutrino The reactions of antineutrino and neutrino with nucleons have muonic and electronic modes: µ + + n ↗ ˜ν + p (12.1) ↘ e + + n ν + n µ − + p ↗ ↘ e − + p (12.2) The Lederman’s experiment has shown that those neutrinos that were born in the transformation pion→muon can participate only in muonic modes of reactions in the future. While electronic modes are not implemented at all. This result is surprising. All neutrinos - muonic and electronic - are born with the abrupt appearance of magnetic moments. The Heaviside’s functions describing this process have only one variable. The stair has two meanings only - up or down. This is in according with existence of neutrinos or antineutrinos (Fig.(11.2)). Heaviside’s stairs can not have any other parameters. It is impossible to put any label for them. Magnetic gamma-quanta can not bear any specific muonic and electronic ”charges”. This seems quite unnecessary to assume that the birth of a free electron in the ground state and the birth of it in the excited state (as muon) must be described in different Heaviside’s stairs. Differences may be in the magnitude of these stairs. But because of a wide range of energies characteristic for neutrinos at β-decay, this parameter can not distinguish the types of neutrinos. 57
58 CHAPTER 12. ABOUT MUONIC NEUTRINO 12.1 The Lederman’s experiment The primary beam of protons with energy of 15 GeV was used in the L.Lederman’s experiment [14]. As a result of their interaction with the target, a beam of highly energetic charged π-mesons was formed. In turn at their decay, highly energetic charged µ-mesons and neutrinos were created. In future, the muonic reaction mode was observed only and e-mode reaction was not registered. On this basis, it was concluded on the existence of specific muon-type neutrinos. This conclusion would be true if these reactions would be equally probable. However, this is not the case, since products of these reactions have different phase volumes. For example, let’s turn our attention on the reaction of the charged π-meson decay. This decay has two modes: π ± µ ± + ν ≃ ↗ (12.3) ↘ e ± + ν ≃ Measurements show that the muonic mode of this reaction is more probable for 10 4 times. The reason of the electronic channel suppression is that these reactions generate relativistic electrons. Because of the kinetic energy of electrons in this decay much more of their mass and their helicity is preserved with good accuracy, this mode of decay must be suppressed relatively to the muon mode on the factor [15] R π = m 2 µ m 2 e ( 1 − mµ m π ) ≈ 1.3 · 10 −4 . (12.4) In the reaction of interaction of neutrinos with nucleons Eq.(12.1) - Eq.(12.2), we should expect the same phenomenon, because there are muonic and electronic modes of reaction also, and electronic mode must be suppressed because of its relativism. At time when L.Lederman with his colleagues made their measurements, this was not known and this factor can not be taken into account. For this reason we can assume, that L.Lederman and his colleagues found no electrons and positrons not because neutrinos had a specific muon ”charge” but due to the strong suppression of the electron channel of reaction. 12.2 How to clarify the Lederman’s experiment? The primary proton beam used Lederman had very high energy. This helped him to form a large beam of neutrinos flying forward. However, this advantage led to the suppression of the electronic mode of reaction.
Page 2 and 3:
About Quantum-Mechanical Nature of
Page 4 and 5:
Contents I Introduction 5 1 The mai
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Part I Introduction 5
Page 9 and 10: 8 CHAPTER 1. THE MAIN PRINCIPLE OF
Page 11 and 12: 10 CHAPTER 1. THE MAIN PRINCIPLE OF
Page 13 and 14: 12CHAPTER 2. IS IT POSSIBLE TO CONS
Page 15 and 16: 14CHAPTER 2. IS IT POSSIBLE TO CONS
Page 18 and 19: Basic properties of proton and neut
Page 20 and 21: Chapter 3 Is neutron an elementary
Page 22 and 23: 3.1. EQUILIBRIUM IN THE SYSTEM OF R
Page 24 and 25: 3.2. MAIN PROPERTIES OF NEUTRON 23
Page 26 and 27: 3.2. MAIN PROPERTIES OF NEUTRON 25
Page 28 and 29: Chapter 4 Discussion The consent of
Page 30: Part III Nature of nuclear forces 2
Page 33 and 34: 32CHAPTER 5. THE ONE-ELECTRON BOND
Page 35 and 36: 34CHAPTER 5. THE ONE-ELECTRON BOND
Page 37 and 38: 36 CHAPTER 6. THE MOLECULAR HYDROGE
Page 39 and 40: 38 CHAPTER 7. DEUTRON AND OTHER LIG
Page 41 and 42: 40 CHAPTER 7. DEUTRON AND OTHER LIG
Page 43 and 44: 42 CHAPTER 8. DISCUSSION
Page 46 and 47: Chapter 9 Introduction W.Pauli was
Page 48 and 49: Chapter 10 Electromagnetic radiatio
Page 50 and 51: 10.3. THE MAGNETIC FIELD GENERATED
Page 52 and 53: Chapter 11 Photons and Neutrinos At
Page 54 and 55: 11.2. NEUTRINOS AND ANTINEUTRINOS 5
Page 56 and 57: 11.3. MESONS AS EXCITED STATES OF E
Page 60 and 61: 12.2. HOW TO CLARIFY THE LEDERMAN
Page 62: Part V Conclusion 61
Page 65 and 66: 64 nuclear shells. β-decay does no
Page 67: 66 BIBLIOGRAPHY [10] Heitler W., Lo
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