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Articles Title
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Abstract
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0
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Editorial Note
Ignazio Licata
Full text: Acrobat
PDF (14 KB)
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MAJORANA
IMPACT ON CONTEMPORARY PHYSICS
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1
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The Scientific Work Of Ettore Majorana: An Introduction
Erasmo Recami
Full text: Acrobat
PDF (113 KB)
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A
Brief bibliography of the scientific work of Ettore
Majorana has been discussed.
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2
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On the Hamiltonian Form of Generalized Dirac Equation for Fermions with Two Mass States
Sergey. I. Kruglov
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PDF (126 KB)
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Dynamical
and non-dynamical components of the 20-component wave function are
separated in the generalized Dirac equation of
the first order, describing fermions with spin 1/2 and two mass states.
After the exclusion of the non-dynamical components, we obtain the
Hamiltonian Form of equations. Minimal and non-minimal electromagnetic
interactions of particles are considered here.
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3
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Majorana Equation and exotics: Higher Derivative Models, Anyons and Noncommutative
Geometry
Mikhail S. Plyushchay
Full text: Acrobat
PDF (199 KB)
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In
1932 Ettore Majorana
proposed an infinite-component relativistic wave equation for particles of
arbitrary integer and half-integer spin. In the late 80s and early 90s it
was found that the higher-derivative geometric particle models underlie the
Majorana equation, and that its (2+1)-dimensional
analogue provides with a natural basis for the description of relativistic anyons. We review these aspects and discuss the
relationship of the equation to the exotic planar Galilei
symmetry and noncommutative geometry. We also
point out the relation of some Abelian gauge
field theories with Chern-Simons terms to the
Landau problem in the noncommutative plane from
the perspective of the Majorana equation.
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4
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Wave Equations,
Renormalization and Meaning of the Planck's Mass: Some Qualitative
Considerations
Leonardo Chiatti
Full text: Acrobat
PDF (131 KB)
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The five-dimensional
version of the quantum relativistic Klein-Gordon wave equation is assumed
to be a more fundamental description for the dynamics of the single
particle without spin. The meaning of the renormalization procedure in QFT
and the Planck's mass one are briefly discussed from this point of view.
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5
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Nonlinear Field Equations and Solitons
as Particles
Attilio Maccari
Full text: Acrobat
PDF (346 KB)
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Profound
advances have recently interested nonlinear field theories and their exact
or approximate solutions. We review the last results and point out some
important unresolved questions. It is well known that quantum field
theories are based upon Fourier series and the identification of plane
waves with free particles. On the contrary, nonlinear field theories admit
the existence of coherent solutions (dromions, solitons and so on). Moreover, one can construct lower
dimensional chaotic patterns, periodic-chaotic patterns, chaotic
soliton and dromion
patterns. In a similar way, fractal dromion and
lump patterns as well as stochastic fractal excitations can appear in the
solution. We discuss in some detail a nonlinear Dirac
field and a spontaneous symmetry breaking model that are reduced by means
of the asymptotic perturbation method to a system of nonlinear evolution
equations integrable via an appropriate change of
variables. Their coherent, chaotic and fractal solutions are examined in
some detail. Finally, we consider the possible identification of some types
of coherent solutions with extended particles along the de Broglie-Bohm theory. However, the last findings suggest
an inadequacy of the particle concept that appears only as a particular
case of nonlinear field theories excitations.
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6
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The Quantum Character of Physical Fields.
Foundations of
Field Theories
Ludmila. I. Petrova
Full text: Acrobat
PDF (161 KB)
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The
existing field theories are based on the properties of closed exterior
forms, which are invariant ones and correspond to conservation laws for
physical fields. Hence, to understand the foundations of field theories and
their unity, one has to know how such closed exterior forms are obtained.
In the present paper it is shown that closed exterior forms corresponding
to field theories are obtained from the equations modeling conservation
(balance) laws for material media. It has been developed the evolutionary
method that enables one to describe the process of obtaining closed
exterior forms. The process of obtaining closed exterior forms discloses
the mechanism of evolutionary processes in material media and shows that
material media generate, discretely, the physical structures, from which
the physical fields are formed. This justifies the quantum character of
field theories. On the other hand, this process demonstrates the connection
between field theories and the equations for material media and points to
the fact that the foundations of field theories must be conditioned by the
properties of material media. It is shown that the external and internal
symmetries of field theories are conditioned by the degrees of freedom of
material media. The classification parameter of physical fields and
interactions, that is, the parameter of the unified field theory, is
connected with the number of noncommutative
balance conservation laws for material media.
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7
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Relativistic
Causality and
Quasi -Orthomodular
Algebras
Renato.Nobili
Full text: Acrobat
PDF (218 KB)
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The concept of fractionability or decomposability in parts of a
physical system has its mathematical counterpart in the lattice--theoretic
concept of orthomodularity. Systems with a finite
number of degrees of freedom can be decomposed in different ways,
corresponding to different groupings of the degrees of freedom. The orthomodular structure of these simple systems is
trivially manifest. The problem then arises as to whether the same property
is shared by physical systems with an infinite number of degrees of
freedom, in particular by the quantum relativistic ones. The latter case
was approached several years ago by Haag and Schroer
(1962; Haag, 1992) who started from noting that the causally complete sets
of Minkowski spacetime
form an orthomodular lattice and posed the
question of whether the subalgebras of local
observables, with topological supports on such subsets, form themselves a
corresponding orthomodular lattice. Were it so,
the way would be paved to interpreting spacetime
as an intrinsic property of a local quantum field
algebra. Surprisingly enough, however, the hoped property does not hold for
local algebras of free fields with superselection
rules. The possibility seems to be instead open if the local currents that
govern the superselection rules are driven by
gauge fields. Thus, in the framework of local quantum physics, the request
for algebraic orthomodularity seems to imply
physical interactions! Despite its charm, however, such a request appears
plagued by ambiguities and criticities that make
of it an ill--posed problem. The proposers
themselves, indeed, concluded that the orthomodular
correspondence hypothesis is too strong for having a chance of being
practicable. Thus, neither the idea was taken seriously by the proposers nor further investigated by others up to a
reasonable degree of clarification. This paper is an attempt to
re--formulate and well--pose the problem. It will be shown that the idea is
viable provided that the algebra of local observables: (1) is considered
all over the whole range of its irreducible representations; (2) is widened
with the addition of the elements of a suitable intertwining group of automorphisms; (3) the orthomodular
correspondence requirement is modified to an extent sufficient to impart a
natural topological structure to the intertwined algebra of observables so
obtained. A novel scenario then emerges in which local quantum physics
appears to provide a general framework for non--perturbative
quantum field dynamics.
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8
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Lorentz Invariant Majorana
Formulation of Electrodynamics in
the Clifford Algebra Formalism
Tomislav Ivezic
Full text: Acrobat
PDF (143 KB)
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In this paper we present a new geometric
formulation (Clifford algebra formalism) of the field equations, which is
independent of the reference frame and of the chosen system of coordinates
in it. This formulation deals with the complex 1-vector \Psi =E-icB (i is the unit imaginary), which is four-dimensional
(4D) geometric generalization of Majorana's
complex 3D quantity \Psi }=E-icB. When the sources are
absent the field equations with the complex \Psi become Dirac-like
relativistic wave equations for the free photon. In the frame of ``fiducial'' observers (the observers who measure fields
are at rest) and in the standard basis the component form of the field
equations with 4D \Psi reproduces the component form of Majorana-Maxwell equations with 3D field \Psi . The important differences between the approach
with the 4D \Psi and that one
with the 3D \Psi are discussed.
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9
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"
Anticoherent " Spin States via the Majorana
Representation
Jason Zimba
Full text: Acrobat
PDF (400 KB)
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In
this article we define and exhibit '' anticoherent"
spin states, which are in a sense '' the opposite" of the familiar coherent spin states. Since the familiar coherent states are as
"classical" as spin states can be, the anticoherent
states may turn out to be better candidates for applications involving
non-classical behaviors such as quantum entanglement. Thanks to the Majorana representation of spinors
as 2s-tuples of points on the Riemann sphere, classes of anticoherent states are easy to find; the development
of such examples also leads us into some curious geometry involving the
perfect solids.
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10
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Stretching the
Electron as Far as it Will Go
G. W. Semenoff and P. Sodano
Full text: Acrobat
PDF (287 KB)
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Effects associated with the existence of
isolated zero modes of Majorana fermions are
discussed. It is argued that the quantization of this system necessarily
contains highly extended quantum states and that populating and
depopulating such states by interacting with the quantum system leads to
long-ranged teleportation-like processes. Also leads to spontaneous
violation of fermion parity symmetry. A
quasi-realistic model consisting of a quantum wire embedded in a p-wave
superconductor is discussed as an explicit example of a physical system
with an isolated Majorana zero mode.
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11
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Why do Majorana Neutrinos Run Faster than Dirac
Neutrinos?
Zhi-zhong Xing and He Zhang
Full text: Acrobat
PDF (380 KB)
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The
\tau-lepton dominance in the one-loop
renormalization-group equations (RGEs) of
neutrinos sets a cute criterion to parametrize
the 3x3 lepton flavor mixing matrix U: its elements U_{3i} (for i=1,2,3) should be as simple as possible. Such a novel parametrization is different from the ``standard"
one used in the literature and can lead to greatly simplified RGEs for three mixing angles and the physical
CP-violating phase(s), no matter whether neutrinos are Dirac
or Majorana particles. We show that the RGEs of Dirac neutrinos are
not identical with those of Majorana neutrinos
even if two Majorana CP-violating phases vanish.
As the latter can keep vanishing from the electroweak scale to the typical
seesaw scale, it makes sense to explore the similarities and differences
between the RGE running effects of Dirac and Majorana neutrinos. We conclude that Majorana neutrinos are in general expected to run
faster (i.e., more significantly) than Dirac
neutrinos.
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12
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Universe Without Singularities
A Group Approach to De Sitter Cosmology
Ignazio Licata
Full text: Acrobat
PDF (162 KB)
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In
the last years the traditional scenario of ``Big Bang'' has been deeply
modified by the study of the quantum features of the Universe evolution,
proposing again the problem of using ``local'' physical laws on cosmic
scale, with particular regard to the cosmological constant role. The
``group extention'' method shows that the De
Sitter group univocally generalizes the Poincaré
group, formally justifies the cosmological constant use and suggests a new
interpretation for Hartle-Hawking boundary
conditions in Quantum Cosmology.
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13
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Majorana and the Investigation of Infrared Spectra of Ammonia
Elisabetta. Di Grezia
Full text: Acrobat
PDF (169 KB)
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An
account is given on the first studies on the physics of ammonia, focusing
on the infrared spectra of that molecule. Relevant contributions from
several authors, in the years until 1932, are pointed out, discussing also
an unknown study by E.Majorana on this topic.
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14
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Exact Solution of Majorana Equation via Heaviside
Operational Ansatz
Valentino A. Simpao
Full text: Acrobat
PDF (215 KB)
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In
context of a transformation between Majorana and Dirac wavefunctions, it
suffices to solve the related interactive Dirac
problem and then apply the transformation of variables on the Dirac wavefunction in order
to obtain the Majorana wavefunction
of the given Majorana equation. Clearly, this
connection between solutions continues to hold if the free Majorana and Dirac equations
are each coupled to an external gauge field [e.g., Electromagnetism] via
the minimum coupling prescription. Applying the formal solution scheme Heaviside Operational Ansatz[heretofore, HOA]
put forward in [ EJTP 1 (2004), 10-16], provides an exact quadrature solution for the massive minimum-coupled Majorana equation in terms of the solution of the
corresponding massive minimum-coupled Dirac
equation.
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15
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A Logical Analysis
of Majorana’s Papers on Theoretical Physics
A. Drago and S. Esposito
Full text: Acrobat
PDF (161 KB)
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We study two celebrated Majorana's papers through a method of investigation
which relies upon the recently recognized distinction between classical
logic and several kinds of non-classical logics, i.e. the failure of the
double negation law. This law fails when a double negated sentence is not
equivalent to the corresponding positive sentence, owing to the lack of scientific
evidence of the latter one. All recognized double negated sentences inside
the text of each paper are listed; the mere sequence of such sentences
giving the logical thread of Majorana's arguing.
This one is recognized to be of the Lagrangian
kind, which mixes logical arguing and mathematical calculation; i.e. the
author puts a fundamental problem which is solved by anticipating the
mathematical hypothesis able to solve it, and then by drawing from this
hypothesis the mathematical consequences in order to reach to desired
result. Furthermore the rethoric of presentation used by Majorana
results to be a juridical one, owing to his style of presenting the laws to
which an ideal theoretical physicist has to conform his mind in order to
solve the problem at issue.
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16
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Four Variations on
Theoretical Physics by Ettore Majorana
Salvatore.
Esposito
Full text: Acrobat
PDF (219 KB)
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An
account is given of some topical unpublished work by Ettore
Majorana, revealing his very deep intuitions and
skillfulness in Theoretical Physics. The relevance of the quite unknown
results obtained by him is pointed out as well.
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17
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The Majorana Oscillator
Eliano Pessa
Full text: Acrobat
PDF (124 KB)
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At
present the expression ‘Majorana oscillator’ does
not appear to be in use in theoretical physics. However, the author of this
paper heard it in the Seventies, during private conversations with the late
Prof. B.Touschek. This little contribution tries
to explore the possible meanings of this expression and introduces a new
field equation, generalizing the one already introduced by Majorana himself, which could describe a hypothetical ‘Majorana oscillator’.
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18
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Scattering of an
\alpha Particle by a Radioactive Nucleus
Unpublished 1928
Ettore Majorana
Full text: Acrobat
PDF (166 KB)
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In the following we reproduce, translated
into English, a section of Volumetto II, a
notebook written by Majorana in 1928 when he was
still a Physics student at the University of Rome (see S. Esposito, E. Majorana jr, A. van der Merwe and E. Recami (eds.) Ettore Majorana: Notes on
Theoretical Physics, Kluwer, New York, 2003).
This study was performed by the author when he was preparing his Thesis
work on ``The Quantum Theory of Radioactive Nuclei'' (unpublished), whose supervisor was E. Fermi.
S.
Esposito
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19
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Comments on a Paper
by Majorana Concerning Elementary Particles
David. M. Fradkin
Full text: Acrobat
PDF (145 KB)
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An
early paper (1932) by Majorana, that has received but scant attention, is reexamined
in light of later developments. This pioneering paper constructs a relativistically invariant theory of arbitrary spin
particles, develops and utilizes infinite dimensional representations of
the homogeneous Lorentz group, and provides a
mass spectrum for elementary particles. The relevance of Majorana’s approach and results to later and current
research is explained.
Reprinted with permission from the
AMERICAN JOURNAL OF PHYSICS, Volume 34, Issue 4,
pp. 314-318. Copyright 1966, American Association of Physics Teachers
We
reproduce here the historical D. M. Fradkin 1966
paper whose role among the physicists of high energy was decisive; since
then espressions like "Majorana
mass", "Majorana spinors"
and "Majorana neutrino" have become usual. The paper is based upon the work Teoria di Particelle
con Momento Intrinseco Arbitrario, translated by Italiam
from Edoardo Amaldi.
Ignazio
Licata
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