?? F?S???S ??G????S ?O????????O? S???????O? ??? ?? S??????S???? X??S THE NATURAL ALGEBRAS OF SPACETIME SYMMETRIES AND RELATIVISTIC CHAOS - PowerPoint PPT Presentation

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?? F?S???S ??G????S ?O????????O? S???????O? ??? ?? S??????S???? X??S THE NATURAL ALGEBRAS OF SPACETIME SYMMETRIES AND RELATIVISTIC CHAOS

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Naimark M.A. Linear Representations of the Lorentz Group, Pergamon Press (1964) ... in Physics, Probability and Number Theory, Benjamin/Cummings, London (1978) ... – PowerPoint PPT presentation

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Title: ?? F?S???S ??G????S ?O????????O? S???????O? ??? ?? S??????S???? X??S THE NATURAL ALGEBRAS OF SPACETIME SYMMETRIES AND RELATIVISTIC CHAOS


1
?? F?S???S ??G????S ?O????????O? S???????O? ???
?? S??????S???? X??S THE NATURAL ALGEBRAS OF
SPACETIME SYMMETRIES AND RELATIVISTIC CHAOS
  • ??a???? ??t?????

2
????????
  • HMIEYT?? ?T???S???? ??G???O?
    LIE,S????????S ??? ???S?a Hµ?e??ea ?????sµata
    ???eß??? Lie pe????af??? t?? ??????????e?
    S?µµet??e?. ?? a?t?st???e? Ge?µet??e? p????pt???
    ?a? ta????µ???ta? ap? t?? S?µµet??e? p?? seß??ta?
    (Lie-Klein).?? ?atastase?? t?? F?s???? S?st?µat??
    p????pt??? ep?s?? ap? t?? ?atas?e?? ?a?
    ta????µ?s? t?? ??apa?astase?? t?? ???eß??? Lie
    t?? S?µµet???? t??? p?? eµpe??e???ta? st??
    ???eß?e? t?? pa?at???s?µ?? te?est?? (Wigner-Von
    Neumann). H A??eß?a t?? ?a S?et???st???? ?a?t????
    S?st?µat?? e??a? µ?a ape???d?astat? epe?tas? t??
    10-pa?aµet????? Lie ???eß?a? Poincare t?? ??d????
    S?et???t?ta? p?? s?µpe???aµßa?e? t?? ?e?est? t??
    ?????? ? ?p???? pe????afe? t?? d?ad????e?
    ?a???t?µ?e?,
  • e??e?e? ?a?a?t???st??? t?? ?a???.

3
Symmetry
  • Symmetry as wide or as narrow as you may define
    its meaning, is one idea by which man through the
    ages has tried to comprehend and create order,
    beauty and perfection
  • H. Weyl Symmetry, Princeton (1952)

4
Euclidean Symmetries
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The Structure of Euclidean Tranformations
  • The composition of Euclidean Transformations
  • S?T(x)ST(x) , x2 ?³
  • is also a Euclidean Transformation
  • The Euclidean Transformations are
  • a Semi-Direct Product Lie Group

7
Group
  • A set G with an operation GxG?G
  • (g,h) ? g h , for all g,h2 G
  • with the properties
  • Associative g (h q)(g h) q, for all
    g,h,q2 G
  • Identity 9 u 2 G u gg, for all g2 G
  • Inverse for any g2 G, 9 g¹2 G g¹ gu

8
Lie Groups
  • Lie Groups are Continuous Groups (G,) which are
    also Analytic Manifolds and
  • the group operation GxG?G is Analytic
  • (x,y)?x y
  • x?x-1

9
  • Lies motivation
  • Symmetries of Differential equations
  • Lies idea
  • Study the Group Action from
  • the local properties in the neighbourhood of
    the unit
  • Lie Algebra is the Tangent space at the unit

10
Lie Algebra
  • A vector space G over R
  • With the operation- Lie bracket ,
  • (X,Y)? X,Y X,Y, X,Y2 G
  • Bilinearity over R ?iXi,?jYj?i?j X,Y, ?i,?j
    2 R
  • Anti commutativity X,Y- Y,X
  • Jacobi identity X,Y,ZZ,X,YY,Z,X0

11
Semi-Direct Product of the Group (G,) with the
Group (X,)
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The Lie Algebra of the Semi-Direct Product of
the Lie Group (G,) with the Group (X,) isthe
Semi-Direct Sum of the corresponding Lie Algebras
  • The Semi-Direct Sum of the Lie Algebra G with the
    Lie Algebra X

14
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21
Weyl AlgebraThe Commutation Relations
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24
  • (O) A System has the Symmetry Group G?
  • The Group of Automorphisms of the Algebra
    of Observables (Functions,Operators)

  • or the state space
  • contains a Representation of G as a
    Subgroup
  • Pythagoras, Plato,, Lie, Klein, Weyl
  • Beings are manifestations of Symmetries
  • Representations of the
    relevant Symmetry Group G
  • Classifications of Beings ? Classifications of
    the Representations of G
  • Composite Beings correspond to Reducible
    Representations of G
  • Elementary Beings correspond to Irreducible
    Representations of G

25
  • Aristotle Mechanics - Euclidean Group
  • Newton Mechanics - Galilei Group
  • Relativistic Mechanics - Poincare Group
  • Construction , Classification and Significance of
  • the Representations of the Symmetry Groups
  • Barut A.O. and Raczka R., The Theory of Group
    Representations and Applications, Polish Sci.
    Publishers, Warsaw (1977).
  • Wigner E.P., Unitary representations of the
    Inhomogenous Lorenz group, Ann. Math. 40, 149-204
    (1939).
  • Naimark M.A. Linear Representations of the
    Lorentz Group, Pergamon Press (1964).
  • Wigner E.P. Group Theory and its Application to
    the Quantum Mechanics of Atomic Spectra, Academic
    Press, New York (1959).
  • Wigner E.P., Houtappel R. and Van Dam H., The
    conceptual basis and use of the geometric
    invariance principles, Rev. Mod. Phys. 37,
    595-632 (1965).
  • Mackey G.W. Unitary Group Representations in
    Physics, Probability and Number Theory,
    Benjamin/Cummings, London (1978).
  • Mackey G.W. Harmonic Analysis as the Exploitation
    of Symmetry-A Historical Survey, Bull. Am. Math.
    Soc. 3, 543-698 (1980).
  • Wigner E., The unreasonable effectiveness of
    mathematics in the natural sciences, Comm. Pure
    Appl. Math. 13, 1-14 (1960).

26
  • What is the Algebra of Observables of
    Relativistic Chaotic Systems?
  • It should include the Poincare Algebra
  • qualifying Relativistic Symmetry
  • and the Internal Time qualifying Chaos

27
  • (T)Innovation Process?
  • Time Operator formula for Age ?
  • Time Operator defined in terms of
  • the Canonical Commutation Relation
  • in the Weyl or Heisenberg form

28
  • Innovation Process

29
  • Time Operator formula for Age

30
  • Weyl CCR for the Time Operator

31
  • Weyl CCR

32
  • Stone-Von Neuman-Mackey Theorem
  • Representations of CCR
  • Translation Representation
  • Spectral Representation

33
  • Construction of a Time Operator for Relativistic
    Systems
  • Work within the Rational envelopping Algebra of
    the Relativistic System

34
  • Relativistic Chaos
  • Representation of the Lie Algebra generated by

35
  • The simplest ExampleWave Equation

36
  • Wave Equation

37
  • Time Operator

38
  • Spectral Representation

39
  • The RIT Algebra

40
  • RIT

41
  • RIT

42
  • RIT Structure

43
  • Antoniou I. and Misra B., The relativistic
    internal time algebra, Nuclear Physics, Proceed.
    Suppl. Sect. 6, 240-242 (1989).
  • Antoniou I. and Misra B., Relativistic Internal
    Time Operator, Int. J. Theor.Phys. 31, 119-136
    (1992).
  • RIT is not in the known / classified Infinite
    Dimensional Lie Algebras
  • Kac V.G., Infinite Dimensional Lie
    Algebras, Cambridge University Press (1985).
  • How to characterise RIT
  • So that we can compare RIT with other known
    Infinite Dimensional Lie Algebras ?
  • ex. The Bondi-Metzner-Sachs Algebra of
    Asymptotic SpaceTime

44
  • Antoniou I. and and Misra B., Characterization of
    semidirect sum Lie algebras,
  • J. Math. Phys. 32, 864-868 (1991).
  • If we know the Representations of the Lie Algebra
    G
  • then we may characterise the semi-direct sum of G
    with X
  • by characterising the representation of G
    provided by X

45
  • The Representations of the Lorentz Algebra are
    known
  • Naimark M.A. Linear Representations of the
    Lorentz Group, Pergamon Press (1964).

46
  • Antoniou I., Iyudu N. Poincare-Hilbert Series,pi
    and Noetherianity of the Enveloping of the
    Relativistic Internal Time Algebra, Comm. in
    Algebra 29, 4183-4196 (2001).
  • Study of the Envelopping Algebra of RIT,
    Groebner basis technique
  • Antoniou I., Iyudu N. Wisbauer R., On Serre's
    Problem for the RIT Algebra, Comm. in Algebra 31,
    6037-6050 (2003).
  • RIT provides a counterexample to the
    Serres Problem
  • Any finitely generated projective module
    over the ring of commutative polynomials over a
    field is free
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