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Andrius Kulikauskas
- m a t h 4 w i s d o m - g m a i l
- +370 607 27 665
- My work is in the Public Domain for all to share freely.
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- Overviews: Bott periodicity flavors, Bott periodicity models divisions, Divisions
- Expositions: Investigating Bott periodicity, Modeling Introspected Contexts With Mutually Anticommuting Linear Complex Structures, Bott periodicity for Clifford algebra maniacs, Bott periodicity for octonion maniacs, Artificial general intelligence presentation, Modeling the self
- Key topics: Hamiltonians, Quantum symmetries, Lie group embeddings, Lie algebra decomposition, Super division algebras, Clifford algebras, Symmetric spaces, Octonions, Binomial Bott, KTheory, Dynkin diagrams, Spinors, Random matrices, Krebs cycle, NSpheres, Linear complex structures
- Related topics: Topological invariants, Homotopy groups, String theory, 24 Cell
An Allegory: The Solipsistic Self as the Hamiltonian of a Noninteracting Fermion
Bott Periodicity Models Consciousness? Preliminary Exploration
博特周期性定理
Priorities
Write up my results.
- Organize my notes. Identify questions to investigate.
- Present my results with videos.
- Present my results in papers.
Answer concrete questions
- Calculate how {$iJ_2$} works for complex Bott periodicity
- Understand in what sense {$\mathbb{H}$} is the even (part?) of {$Cl_{0,4}$}
- Calculate {$J_9, J_{10}, J_{11}\dots $} and understand how they relate to {$J_1, J_2, J_3 \dots $}. Consider using the Baez free functor.
- Make sense of the operation {$-1$} which adds generators that square to {$+1$}.
Understand the three minds
Model God
Operator +2
- Geodesics
- Loopspace adjunctions
Divisions of everything
- Octonions
- Understand the divisions of everything in terms of counterquestions
- Relate the octonions and the eightfold way
Be able to explain
- Homotopy groups {$\mathbb{Z}, \mathbb{Z}_2, \mathbf{0}$}
Learn math I don't yet understand
- Symmetric spaces
- Morita equivalence and Artin-Weddeburn theorem
- Morse theory
- K-theory
Connect with related subjects
Building blocks
Matrix symmetry
- Does the formula for the sign of the square of the pseudoscalar, based on {$n(n+1)/2$}, which sums the integers from {$1$} to {$n$}, relate to the diagonal plus upper triangular entries of a matrix? and to the number of independent equations for orthogonality of vectors?
Choice frameworks
- How do the choice frameworks match up to Lie groups? and to Bott periodicity?
- Is there a Clifford algebra {$Cl_{0,k}$} for which the identity and the pseudoscalar are symmetric in every way?
Fourfold periodicity
- How might the fourfold periodicity of the sign of the pseudovector be related to the fourfold periodicity of the differentiation of sine and cosine functions?
- Where have I encountered the fourfold periodicity for the shuffle permutation?
Artin-Wedderburn theorem
Flavors of Bott periodicity
Representations of Clifford algebras
- Compare John Baez's representations over Clifford algebras (the forgetful functor and symmetric spaces) with the Clifford modules described by Attiyah, Bott, Shapiro.
Del Pezzo surfaces
Related math
anticommutativity
- What does it mean if operators are anti-commuting?
- Anticommutativity makes cross terms cancel. Nilpotents make squares cancel. What about commutativity?
homotopy
- Could twistors relate the two branches of {$O(\infty)$}? And how could the (left-handed or right-handed) chirality of spinors relate to those two branches?
- Are there two parts of {$O(\infty)$}? And is this like the unconscious and the conscious, where the conscious is a reflected version of the unconscious?
- Consider how branching into two parts (as for {$O(\infty)$}) works for each Lie group, unitary, symplectic, odd and even orthogonal groups.
transpose
- How do the transpose, conjugate transpose, quaternionic transpose simplify Cramer's rule combinatorially?
linear complex structures
- In what sense is a linear complex structure the going beyond of oneself?
- What is the meaning of products, of various lengths, of perspectives, linear complex structures?
- Is there a category where the arrows are products of linear complex structures and the objects are subgroups of the orthogonal group? Does composition work out?
Dynkin diagrams
- Is the {$E_8$} symmetry based on one half of Bott periodicity? Do the Dynkin diagrams of the exceptional Lie groups model counting backwards and forwards inside Bott periodicity?
- Is simultaneous CPT transformation the same as switching us from rotations to reflected rotations?
Operators +1, +2, +3
- In Bott periodicity, generators squaring to +1 give quaternionic structure? How does that equal to the operator +3 for consciousness with linear complex structures?
- How is {$BSp$} related to the three minds, +3? and +2?
Eightsome
- How is {$\mathbb{H}\oplus\mathbb{H}$} related to the eightsome?
- How is {$\mathbb{H}(2)$} related to the eightsome?
Squaring to +1 or -1
- In Bott periodicity, what does it mean that adding generators which square to -1 and adding generators which square to +1 yields the same when we have four generators? Is that (unconscious) knowing and (conscious) not knowing? Are they complementing each other with regard to the eightsome?
Unconscious and conscious
- Is there (unconscious) contextualizing and (conscious) decontextualizing (deconstructing)? And does this yield contexts as the manifestation of consciousness? What has priority?
- How do the question (antilinear) and answer (linear) relate? Does the answer follow the question? Or does the question follow the answer?
Skew-symmetric matrices
- What is the relation, if any, between Sheffer polynomials and skew-symmetric matrices?
Exceptional Lie groups
- Could the exceptional Lie groups {$E_k$} be generated by Bott periodicity?
Fourier transform
- How does the Fourier transform of {$S_\infty$} relate to the Fourier transform of finite groups?
2x2matrices
- Consider the ways of constructing a 2x2 matrix by adding a generator {$a_i$} and then {$b_j$}, or alternatively, {$b_j$} and then {$a_i$}.
Loop spaces, classifying spaces, adjunctions
- What is {$BO$}? How is it related to {$O$}? and what does {$\mathbb{Z}$} mean here?
Time
- How does time arise from the symmetry of time reversal? Does unconscious switch the direction? (going from effect to cause?) and conscious switch it a second time, thus keeping it the same? (from cause to effect?)

Overviews
Homotopy groups
- John Baez. Bott periodicity. Considering how {$\pi_0(O(\infty))$} relates to {$\mathbb{R}$}, {$\pi_1(O(\infty))$} relates to {$\mathbb{C}$}, {$\pi_3(O(\infty))$} relates to {$\mathbb{H}$} and {$\pi_7(O(\infty))=\pi_{-1}(O(\infty))$} relates to {$\mathbb{O}$} and the Grassmannian.
- Caleb Ji. Various Statements of Bott Periodicity. A short overview of statements in homotopy theory and K theory.
- Jonathan Block. The Bott Periodicity Theorem. First, periodicity allows one to deloop classifying spaces and thus define cohomology theories. Second, using periodicity, “wrong way” functoriality maps can be defined and these are of integral importance in the index theorem. Siebenmann periodicity states that for M a closed manifold {$S(M)∼=S(M×I4,M×∂I4)$}. A map {$S(M)→KO[12]∗(M)$} which intertwines the two periodicities. It should be noted that {$KO[1/2]$} is four periodic with the signature operator playing the same role as the inverse of the Bott element as the Dirac operator does for complex (or real) periodicity.
Two branches
- Neil Turok Mirror universe, big bang as a mirror, CPT symmetry.
- {$O(\infty)$} has two parts and that may be reflected in the fact that the simple roots can be considered in two groups {$x_i-x_j$} and {$x_j-x_i$} where {$i<j$}.
- Idea: The threesome is what links together the two worlds of O(infinty). The threesome equates a shift in one world with a node in another world and vice versa. And this creates a circle - the three-cycle - which moves in one direction - distinguishing what is unconscious and what is conscious and defining a hole for Z.
Loop spaces and suspension (Operator +2)
- Tai-Danae Bradley. "One-Line" Proof: Fundamental Group of the Circle.
- Tai-Danae Bradley, Bryson, Terilla. Chapter 6. Paths, Loops, Cylinders, Suspensions... Suspension-loop adjunction.
- Algebraic Topology July 2016 University of Chicago
- Peter May. Introduction to Algebraic Topology 10:30 Freudenthal Suspension theorem. {$X\wedge Y=X\times Y/X\cup Y$}, {$\Sigma X = X\wedge S^1$}, {$S^n\wedge S^1=S^{n+1}$}
- Ravi Vakil slides Symmetric spaces and loop space iteration. Complex and real. Focuses on double loop space iteration, using short exact sequences to show that mapping spheres into one space is the same as mapping points into another space.
Peter May. An excellent overview of Bott periodicity. Text
- He goes through Bott's approach. Given symmetric space {$M$} and a triple {$ν = (P, Q; h)$} where {$h$} is the homotopy class of curves joining point {$P$} to {$Q$} in {$M$}. Define {$M^{\nu}$} as the set of all geodesics of minimal length which join {$P$} to {$Q$} and are in the homotopy class {$h$}. Bott shows that {$M^{\nu}$} is a symmetric space. {$\pi_k(M^{\nu})=\pi_{k+1}(M)$} for {$0<k<|\nu |-1$}. Here {$|\nu |$} is the first positive integer which occurs as the index of some geodesic from {$P$} to {$Q$} in the class {$h$}. The index is given by the Morse index theorem.
- He also considers the self-duality of Hopf algebras as relevant for complex Bott periodicity.
- Stable algebraic topology, 1945-1966 History of algebraic topology in the 1950s. Includes a history of the proofs of Bott periodicity.
- Raoul Bott. What Morse missed by not talking to Weyl Includes Morse theory and loop spaces.
- M.A. Aguilar, Carlos Prieto. Quasifibrations and Bott periodicity. May says this is a modern, simplest proof in terms of homotopy theory. It deals with the complex case.
Homology, cohomology
Symmetric spaces
- John Milnor. Morse Theory. (AM-51), Volume 51 Contains a helpful proof of the Bott periodicity theorem, both real and complex, in terms of Morse theory, minimal geodesics and symmetric spaces. Relates the Lie groups to the symmetric spaces and loop spaces.
Lie group embeddings
Symplectic structures
Morse theory and geodesics
Clifford algebra
- The even subalgebra of a Clifford algebra {$Cl_{0,n+1}$} is the Clifford algebra {$Cl_{0,n}$}. The unit elements of that Clifford algebra is the spin group {$Sp(n+1)$}.
Functor on Clifford algebra representations
- In John Baez's talk on the symmetric space, the functor acts on the category of representations of Clifford algebras, which is the category relevant for Morita equivalence.
Complex Clifford algebra
- In a complex Clifford algebra, the coefficient {$i$} commutes with all of the generators {$e_k$} whereas the generators anti-commute with each other. If the coefficient {$i$} anticommuted with all of the generators, then this would simply be a real Clifford algebra with one more generator. So this is a very deep fact that distinguishes complex and real Clifford algebras.
- complex Bott periodicity models the being and real Bott periodicity models their mind (and their three minds)
Clifford modules
- Dexter Chua. Clifford Algebras and Bott Periodicity.
- Yuqin Kewang. Clifford Algebras and Bott Periodicity.
- Andre Henriques. A proof of Bott periodicity via Clifford algebras
- Baez: 2) H. Blaine Lawson, Jr. and Marie-Louise Michelson, "Spin Geometry", Princeton U. Press, Princeton, 1989. or 3) Dale Husemoller, "Fibre Bundles", Springer-Verlag, Berlin, 1994. These books also describe some of the amazing consequences of this periodicity phenomenon. The topology of n-dimensional manifolds is very similar to the topology of (n+8)-dimensional manifolds in some subtle but important ways!'' Physics of fermions.
- Dale Husemoller's book is detailed and helpful.
- Roberto Rubio. Clifford algebras, spinors, and applications. Classification of Clifford algebras.
Representations
Morita equivalence
Morita equivalences as quantum Hamiltonian reductions
Vector bundles on unit spheres
Symmetry
- The fact that, for orthogonal matrices, {$O^T=O^{-1}$} and thus the inverse can be understood as reversing arrows (similarly for the unitary and compact symplectic cases) is an expression of the symmetry in math. Bott periodicity organizes these symmetries in math itself.
- Knowledge is the marking of a state in a symmetry. You have two views (two levels). Different states (known) and their symmetric transformation (no visible change, thus unknown).
Eigenvector
- In the orthogonal group, commuting means that we have some eigenvector.
- the foursome relates {$V_+$} and {$V_-$} as two twosomes. And then divide further into two. A perspective becomes a twosome. Until it all collapses.
Threefold way
- Freeman J. Dyson. The Threefold Way. Algebraic Structure of Symmetry Groups and Ensembles in Quantum Mechanics. J. Math. Phys. 3, 1199–1215 (1962)
Building block
- {$A_1$} is the building block for Lie theory and its Lie algebra serves both {$SU(2)$} and {$SO(3)$}, thus relates vectors and spinors, and seems relevant for Bott periodicity.
Permutations
- {$S_\infty$} = colimit of symmetric groups = permutations with finite support
- Consider all permutations of all lengths. (In considering the moments.) This is similar to {$O(\infty)$} or {$U(\infty)$} which considers all rotations. There is a theorem that relates them. And consider how to take the Fourier transform of all of that.
24-cell?
Extensions
Ideas
- Max Karoubi mentioned in his video that loop equations for rings with R,C,H,H' and {$\epsilon = +/-1$} yields 10 homotopy equivalences.
- Bott periodicity exhibits self-folding. Note the duality of 1 with the pseudoscalar.
Outreach
People who may care
Raoul Bott
- Raoul Bott mirė Carslbad, Kalifornijoje. Attiyah apie Bott gyvenimą. Nekrologas New York Times Dukra Jocelyn Scott gyveno Rancho Santa Fe, dirbo C.B.S. Scientific. Jisai gyveno: assisted living - Sunrise at La Costa, 7020 Manzanita St, Carlsbad, CA 92011-5123 Studied geodesics on {$SU(2)$}.
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