Experiments and problems Experimenting with automata A = f A ( w ) χ k − 1 ∙ ∙ ∙ ∙ ∙ ∙ ∙ ∙ ∙ χ 1 χ 0 ξ k − 1 ∙ ∙ ∙ ∙ ∙ ∙ ∙ ∙ ∙ ξ 1 ξ 0 w = � �� � ( 0 .χ k − 1 . . . χ 1 χ 0 ; 0 .ξ k − 1 . . . ξ 1 ξ 0 ) E k ( f A ) = { ( 0 . w ; 0 . f ( w )): w runs over words of length k } Experimentally it can be observed that E k ( f A ) when k → ∞ basically exhibits behaviour of two kinds only: E k ( f ) is getting more and more dense so that at k → ∞ they fill the 1 unit square completely Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 5 / 27
Experiments and problems Experimenting with automata A = f A ( w ) χ k − 1 ∙ ∙ ∙ ∙ ∙ ∙ ∙ ∙ ∙ χ 1 χ 0 ξ k − 1 ∙ ∙ ∙ ∙ ∙ ∙ ∙ ∙ ∙ ξ 1 ξ 0 w = � �� � ( 0 .χ k − 1 . . . χ 1 χ 0 ; 0 .ξ k − 1 . . . ξ 1 ξ 0 ) E k ( f A ) = { ( 0 . w ; 0 . f ( w )): w runs over words of length k } Experimentally it can be observed that E k ( f A ) when k → ∞ basically exhibits behaviour of two kinds only: E k ( f ) is getting more and more dense 1 E k ( f ) is getting less and less dense and with pronounced straight 2 lines that constitute windings of a torus Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 5 / 27
Experiments and problems Experimenting with automata A = f A ( w ) χ k − 1 ∙ ∙ ∙ ∙ ∙ ∙ ∙ ∙ ∙ χ 1 χ 0 ξ k − 1 ∙ ∙ ∙ ∙ ∙ ∙ ∙ ∙ ∙ ξ 1 ξ 0 w = � �� � ( 0 .χ k − 1 . . . χ 1 χ 0 ; 0 .ξ k − 1 . . . ξ 1 ξ 0 ) E k ( f A ) = { ( 0 . w ; 0 . f ( w )): w runs over words of length k } Experimentally it can be observed that E k ( f A ) when k → ∞ basically exhibits behaviour of two kinds only: E k ( f ) is getting more and more dense 1 E k ( f ) is getting less and less dense and with pronounced straight 2 lines that constitute windings of a torus The goal of the talk is to explain the following: what really happens (=mathematical results), and Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 5 / 27
Experiments and problems Experimenting with automata A = f A ( w ) χ k − 1 ∙ ∙ ∙ ∙ ∙ ∙ ∙ ∙ ∙ χ 1 χ 0 ξ k − 1 ∙ ∙ ∙ ∙ ∙ ∙ ∙ ∙ ∙ ξ 1 ξ 0 w = � �� � ( 0 .χ k − 1 . . . χ 1 χ 0 ; 0 .ξ k − 1 . . . ξ 1 ξ 0 ) E k ( f A ) = { ( 0 . w ; 0 . f ( w )): w runs over words of length k } Experimentally it can be observed that E k ( f A ) when k → ∞ basically exhibits behaviour of two kinds only: E k ( f ) is getting more and more dense 1 E k ( f ) is getting less and less dense and with pronounced straight 2 lines that constitute windings of a torus The goal of the talk is to explain the following: what really happens (=mathematical results), and how the results could be related to quantum theory interpretation. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 5 / 27
Representations of automata maps in real and complex spaces The main mathematical part Experiments and problems 1 Representations of automata maps in real and complex spaces 2 General automata Finite automata Relations to quantum theory 3 Physical measurements, information, and quantum theory Torus windings and wave functions Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 6 / 27
Representations of automata maps in real and complex spaces General automata The next topic: Experiments and problems 1 Representations of automata maps in real and complex spaces 2 General automata Finite automata Relations to quantum theory 3 Physical measurements, information, and quantum theory Torus windings and wave functions Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 7 / 27
Representations of automata maps in real and complex spaces General automata The automata 0-1 law Denote via α ( f A ) Lebesgue measure of the plot of A , i.e., of the closure P ( f A ) = P ( A ) of the union of sets E k ( f A ) , k = 1 , 2 , 3 , . . . . Theorem (The automata 0-1 law; V. A., 2009) Given an automaton function f = f A , either α ( f ) = 0 , or α ( f ) = 1 . Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 8 / 27
Representations of automata maps in real and complex spaces General automata The automata 0-1 law Denote via α ( f A ) Lebesgue measure of the plot of A , i.e., of the closure P ( f A ) = P ( A ) of the union of sets E k ( f A ) , k = 1 , 2 , 3 , . . . . Theorem (The automata 0-1 law; V. A., 2009) Given an automaton function f = f A , either α ( f ) = 0 , or α ( f ) = 1 . These alternatives correspond to the cases P ( f ) is nowhere dense in I 2 and P ( f ) = I 2 , respectively. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 8 / 27
Representations of automata maps in real and complex spaces General automata The automata 0-1 law Denote via α ( f A ) Lebesgue measure of the plot of A , i.e., of the closure P ( f A ) = P ( A ) of the union of sets E k ( f A ) , k = 1 , 2 , 3 , . . . . Theorem (The automata 0-1 law; V. A., 2009) Given an automaton function f = f A , either α ( f ) = 0 , or α ( f ) = 1 . These alternatives correspond to the cases P ( f ) is nowhere dense in I 2 and P ( f ) = I 2 , respectively. We will say for short that an automaton A is of measure 1 if α ( f A ) = 1 , and of measure 0 if otherwise. Finite automata (=automata with a finite number of states) are all of measure 0 Therefore if A is a finite automaton then P ( f A ) is nowhere dense in I 2 and thus P ( f A ) cannot contain ‘figures’, but it may contain ‘lines’. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 8 / 27
Representations of automata maps in real and complex spaces Finite automata Next topic: Experiments and problems 1 Representations of automata maps in real and complex spaces 2 General automata Finite automata Relations to quantum theory 3 Physical measurements, information, and quantum theory Torus windings and wave functions Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 9 / 27
Representations of automata maps in real and complex spaces Finite automata Plots of linear finite automata Given an automaton function is f A , denote via AP ( A ) = AP ( f A ) the set of all accumulation points of the plot P ( A ) ⊂ T 2 on the torus T 2 . Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 10 / 27
Representations of automata maps in real and complex spaces Finite automata Plots of linear finite automata Given an automaton function is f A , denote via AP ( A ) = AP ( f A ) the set of all accumulation points of the plot P ( A ) ⊂ T 2 on the torus T 2 . Important example: linear automata Let A be a finite automaton, and let f A ( z ) = f ( z ) = az + b ( a , b ∈ Z p ∩ Q then). Considering I 2 as a surface of the torus T 2 , we have that � ( x mod 1 ; ( ax + b ) mod 1 ) ∈ T 2 : x ∈ R � AP ( f ) = is a link of N f torus knots either of which is a cable (= winding ) with slope a of the unit torus T 2 : If a = q / k , b = r / s are irreducible fractions, d = gcd ( k , s ) then N f is multiplicative order of p modulo s / d . Each cable winds q times around the interior of T 2 and k times around Z -axis. Given a , b ∈ Z p , the mapping z �→ az + b is an automaton function of a suitable finite automaton if and only if a , b ∈ Z p ∩ Q . set of all rational p -adic integers is denoted via Z p ∩ Q . Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 10 / 27
Representations of automata maps in real and complex spaces Finite automata Plots of linear finite automata Important example: linear automata Let A be a finite automaton, and let f A ( z ) = f ( z ) = az + b ( a , b ∈ Z p ∩ Q then). Considering I 2 as a surface of the torus T 2 , we have that � ( x mod 1 ; ( ax + b ) mod 1 ) ∈ T 2 : x ∈ R � AP ( f ) = is a link of N f torus knots either of which is a cable (= winding ) with slope a of the unit torus T 2 : If a = q / k , b = r / s are irreducible fractions, d = gcd ( k , s ) then N f is multiplicative order of p modulo s / d . By using cylindrical coordinates ( T 2 : ( r 0 − R ) 2 + z 2 = A 2 ; R = A = 1 for unit torus) we get: � ax − 2 π b ∙ p ℓ � r 0 R + A ∙ cos = , x ∈ R , ℓ = 0 , 1 , 2 , . . . θ x � ax − 2 π b ∙ p ℓ � A ∙ sin z Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 10 / 27
Representations of automata maps in real and complex spaces Finite automata Plots of linear finite automata Important example: linear automata Let A be a finite automaton, and let f A ( z ) = f ( z ) = az + b ( a , b ∈ Z p ∩ Q then). Considering I 2 as a surface of the torus T 2 , we have that � ( x mod 1 ; ( ax + b ) mod 1 ) ∈ T 2 : x ∈ R � AP ( f ) = is a link of N f torus knots either of which is a cable (= winding ) with slope a of the unit torus T 2 : If a = q / k , b = r / s are irreducible fractions, d = gcd ( k , s ) then N f is multiplicative order of p modulo s / d . Therefore the plot of f (=of the automaton A ) can be described by N f complex-valued functions: → e i ( ax − 2 π b ∙ p ℓ ) ; ( x ∈ R , ℓ ∈ N 0 ) AP ( A ) = AP ( az + b ) ← Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 10 / 27
Representations of automata maps in real and complex spaces Finite automata The affinity of smooth finitely computable functions Q: What smooth curves are finitely computable; i.e. what smooth curves may lie in the plot P ( A ) of a finite automaton A ? Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 11 / 27
Representations of automata maps in real and complex spaces Finite automata The affinity of smooth finitely computable functions Q: What smooth curves are finitely computable; i.e. what smooth curves may lie in the plot P ( A ) of a finite automaton A ? A: Only straight lines (=cables of torus with rational p -adic slopes and rational p -adic constant terms). Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 11 / 27
Representations of automata maps in real and complex spaces Finite automata The affinity of smooth finitely computable functions Q: What smooth curves are finitely computable; i.e. what smooth curves may lie in the plot P ( A ) of a finite automaton A ? A: Only straight lines (=cables of torus with rational p -adic slopes and rational p -adic constant terms). Theorem (V.A., in pNUAA, 2015, vol. 7, No 3, pp. 169–227) Let g be a two times differentiable function (w.r.t. the metric in R ) defined on [ α, β ] ⊂ [ 0 , 1 ) and valuated in [ 0 , 1 ) ; let g ′′ be continuous on [ α, β ] . If ( x ; g ( x )) ∈ P ( A ) for all x ∈ [ α, β ] then there exist a , b ∈ Z p ∩ Q such that g ( x ) = ax + b for all x ∈ [ α, β ] and AP ( az + b ) ⊂ P ( A ) . Given a finite automaton A , there are no more than a finite number of a , b ∈ Z p ∩ Q such that AP ( az + b ) ⊂ P ( A ) . Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 11 / 27
Representations of automata maps in real and complex spaces Finite automata The affinity of smooth finitely computable functions Theorem (V.A., in pNUAA, 2015, vol. 7, No 3, pp. 169–227) Let g be a two times differentiable function (w.r.t. the metric in R ) defined on [ α, β ] ⊂ [ 0 , 1 ) and valuated in [ 0 , 1 ) ; let g ′′ be continuous on [ α, β ] . If ( x ; g ( x )) ∈ P ( A ) for all x ∈ [ α, β ] then there exist a , b ∈ Z p ∩ Q such that g ( x ) = ax + b for all x ∈ [ α, β ] and AP ( az + b ) ⊂ P ( A ) . Given a finite automaton A , there are no more than a finite number of a , b ∈ Z p ∩ Q such that AP ( az + b ) ⊂ P ( A ) . Actually this means that smooth curves in the plot of a finite automaton constitute a finite union of torus links, and every link consists of a finite number of torus knots with the same slope. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 11 / 27
Representations of automata maps in real and complex spaces Finite automata The affinity of smooth finitely computable functions Theorem (V.A., in pNUAA, 2015, vol. 7, No 3, pp. 169–227) Let g be a two times differentiable function (w.r.t. the metric in R ) defined on [ α, β ] ⊂ [ 0 , 1 ) and valuated in [ 0 , 1 ) ; let g ′′ be continuous on [ α, β ] . If ( x ; g ( x )) ∈ P ( A ) for all x ∈ [ α, β ] then there exist a , b ∈ Z p ∩ Q such that g ( x ) = ax + b for all x ∈ [ α, β ] and AP ( az + b ) ⊂ P ( A ) . Given a finite automaton A , there are no more than a finite number of a , b ∈ Z p ∩ Q such that AP ( az + b ) ⊂ P ( A ) . The theorem can be considered as a contribution to the theory of com- putable functions since the main result means that a finite automaton can compute only a very restricted class of smooth functions; namely, only affine ones. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 11 / 27
Representations of automata maps in real and complex spaces Finite automata The affinity of smooth finitely computable functions Theorem (V.A., in pNUAA, 2015, vol. 7, No 3, pp. 169–227) Let g be a two times differentiable function (w.r.t. the metric in R ) defined on [ α, β ] ⊂ [ 0 , 1 ) and valuated in [ 0 , 1 ) ; let g ′′ be continuous on [ α, β ] . If ( x ; g ( x )) ∈ P ( A ) for all x ∈ [ α, β ] then there exist a , b ∈ Z p ∩ Q such that g ( x ) = ax + b for all x ∈ [ α, β ] and AP ( az + b ) ⊂ P ( A ) . Given a finite automaton A , there are no more than a finite number of a , b ∈ Z p ∩ Q such that AP ( az + b ) ⊂ P ( A ) . The theorem holds for automata with m inputs and n outputs: Smooth surfaces in the plot (in multidimensional torus) constitute a finite number of families of multidimensional torus windings, and each family is a finite collection of windings with the same matrix A . → e i ( x A − 2 π b ∙ p ℓ ) ; ( x ∈ R m ; b ∈ R n ; ℓ ∈ N 0 ) AP ( z A + b ) ← Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 11 / 27
Representations of automata maps in real and complex spaces Finite automata The affinity of smooth finitely computable functions Theorem (V.A., in pNUAA, 2015, vol. 7, No 3, pp. 169–227) Let g be a two times differentiable function (w.r.t. the metric in R ) defined on [ α, β ] ⊂ [ 0 , 1 ) and valuated in [ 0 , 1 ) ; let g ′′ be continuous on [ α, β ] . If ( x ; g ( x )) ∈ P ( A ) for all x ∈ [ α, β ] then there exist a , b ∈ Z p ∩ Q such that g ( x ) = ax + b for all x ∈ [ α, β ] and AP ( az + b ) ⊂ P ( A ) . Given a finite automaton A , there are no more than a finite number of a , b ∈ Z p ∩ Q such that AP ( az + b ) ⊂ P ( A ) . The theorem holds for automata with m inputs and n outputs: Smooth surfaces in the plot (in multidimensional torus) constitute a finite number of families of multidimensional torus windings, and each family is a finite collection of windings with the same matrix A . Thus the theorem can be applied to study hash functions since they all are automata functions of finite automata with multiple inputs/outputs. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 11 / 27
Relations to quantum theory Final part Experiments and problems 1 Representations of automata maps in real and complex spaces 2 General automata Finite automata Relations to quantum theory 3 Physical measurements, information, and quantum theory Torus windings and wave functions Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 12 / 27
Relations to quantum theory Physical measurements, information, and quantum theory The next topic: Experiments and problems 1 Representations of automata maps in real and complex spaces 2 General automata Finite automata Relations to quantum theory 3 Physical measurements, information, and quantum theory Torus windings and wave functions Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 13 / 27
Relations to quantum theory Physical measurements, information, and quantum theory On physical measurements A physical law is a mathematical correspondence between quantities of impacts a physical system is exposed to and quantities of responses the system exhibits. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 14 / 27
Relations to quantum theory Physical measurements, information, and quantum theory On physical measurements A physical law is a mathematical correspondence between quantities of impacts a physical system is exposed to and quantities of responses the system exhibits. The measured experimental values of physical quantities lie in Q . Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 14 / 27
Relations to quantum theory Physical measurements, information, and quantum theory On physical measurements A physical law is a mathematical correspondence between quantities of impacts a physical system is exposed to and quantities of responses the system exhibits. The measured experimental values of physical quantities lie in Q . People usually are trying to find a physical law as a correspondence between accumulation points (w.r.t. the metrics in R ) of experimental values. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 14 / 27
Relations to quantum theory Physical measurements, information, and quantum theory On physical measurements A physical law is a mathematical correspondence between quantities of impacts a physical system is exposed to and quantities of responses the system exhibits. The measured experimental values of physical quantities lie in Q . People usually are trying to find a physical law as a correspondence between accumulation points (w.r.t. the metrics in R ) of experimental values. An experimental curve is a smooth curve (the C 2 -smoothness is common) which is the best approximation of the set of the experimental points. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 14 / 27
Relations to quantum theory Physical measurements, information, and quantum theory On physical measurements A physical law is a mathematical correspondence between quantities of impacts a physical system is exposed to and quantities of responses the system exhibits. The measured experimental values of physical quantities lie in Q . People usually are trying to find a physical law as a correspondence between accumulation points (w.r.t. the metrics in R ) of experimental values. An experimental curve is a smooth curve (the C 2 -smoothness is common) which is the best approximation of the set of the experimental points. A physical law is a curve which can be approximated by the experimental curves with the highest achievable accuracy. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 14 / 27
Relations to quantum theory Physical measurements, information, and quantum theory On physical measurements Let physical quantities which correspond to impacts and reactions are quantized; i.e, take only values, say, 0 , 1 , . . . , p − 1 . Then, once the sys- tem is exposed to a sequence of k of impacts, it outputs corresponding sequence of k reactions. Considering these sequences as base- p ex- pansions of natural numbers z = α k − 1 p r − 1 + ∙ ∙ ∙ + α 0 , after the normal- ization z p k we obtain experimental points in a unit square of R 2 . Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 14 / 27
Relations to quantum theory Physical measurements, information, and quantum theory On physical measurements Let physical quantities which correspond to impacts and reactions are quantized; i.e, take only values, say, 0 , 1 , . . . , p − 1 . Then, once the sys- tem is exposed to a sequence of k of impacts, it outputs corresponding sequence of k reactions. Considering these sequences as base- p ex- pansions of natural numbers z = α k − 1 p r − 1 + ∙ ∙ ∙ + α 0 , after the normal- ization z p k we obtain experimental points in a unit square of R 2 . Our main theorem shows that if the number of states of automaton which corresponds to a physical system is much less than the length of input sequence of impacts then experimental curves necessarily tend to straight lines (or torus windings, under a natural map of the unit square onto a torus). This implies the linearity of a physical law. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 14 / 27
Relations to quantum theory Physical measurements, information, and quantum theory On physical measurements Let physical quantities which correspond to impacts and reactions are quantized; i.e, take only values, say, 0 , 1 , . . . , p − 1 . Then, once the sys- tem is exposed to a sequence of k of impacts, it outputs corresponding sequence of k reactions. Considering these sequences as base- p ex- pansions of natural numbers z = α k − 1 p r − 1 + ∙ ∙ ∙ + α 0 , after the normal- ization z p k we obtain experimental points in a unit square of R 2 . Our main theorem shows that if the number of states of automaton which corresponds to a physical system is much less than the length of input sequence of impacts then experimental curves necessarily tend to straight lines (or torus windings, under a natural map of the unit square onto a torus). This implies the linearity of a physical law. Q: Once Prof. A. Yu. Khrennikov asked a question: “ Why mathemati- cal formalism of quantum theory is linear? ” Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 14 / 27
Relations to quantum theory Physical measurements, information, and quantum theory On physical measurements Let physical quantities which correspond to impacts and reactions are quantized; i.e, take only values, say, 0 , 1 , . . . , p − 1 . Then, once the sys- tem is exposed to a sequence of k of impacts, it outputs corresponding sequence of k reactions. Considering these sequences as base- p ex- pansions of natural numbers z = α k − 1 p r − 1 + ∙ ∙ ∙ + α 0 , after the normal- ization z p k we obtain experimental points in a unit square of R 2 . Our main theorem shows that if the number of states of automaton which corresponds to a physical system is much less than the length of input sequence of impacts then experimental curves necessarily tend to straight lines (or torus windings, under a natural map of the unit square onto a torus). This implies the linearity of a physical law. Q: Once Prof. A. Yu. Khrennikov asked a question: “ Why mathemati- cal formalism of quantum theory is linear? ” A: Quantization + Small set of states ⇒ Linearity Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 14 / 27
Relations to quantum theory Physical measurements, information, and quantum theory Information in physics: Wheeler’s ‘it from bit’ doctrine John Archibald Wheeler (July 9, 1911 – April 13, 2008) was a promi- nent American physicist known for his contribution to general relativity and quantum theory. In 1990, Wheeler suggested that information is fundamental to the physics of the universe and started developing the informational interpretation of physics. He wrote: Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 15 / 27
Relations to quantum theory Physical measurements, information, and quantum theory Information in physics: Wheeler’s ‘it from bit’ doctrine John Archibald Wheeler (July 9, 1911 – April 13, 2008) was a promi- nent American physicist known for his contribution to general relativity and quantum theory. In 1990, Wheeler suggested that information is fundamental to the physics of the universe and started developing the informational interpretation of physics. He wrote: ‘It from bit’ symbolizes the idea that every item of the physical world has at bottom — a very deep bottom, in most instances — an immaterial source and explanation; that which we call re- ality arises in the last analysis from the posing of yes-no ques- tions and the registering of equipment-evoked responses; in short, that all things physical are information-theoretic in origin and that this is a participatory universe. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 15 / 27
Relations to quantum theory Physical measurements, information, and quantum theory Information in physics: Wheeler’s ‘it from bit’ doctrine John Archibald Wheeler (July 9, 1911 – April 13, 2008) was a promi- nent American physicist known for his contribution to general relativity and quantum theory. In 1990, Wheeler suggested that information is fundamental to the physics of the universe and started developing the informational interpretation of physics. He wrote: ‘It from bit’ symbolizes the idea that every item of the physical world has at bottom — a very deep bottom, in most instances — an immaterial source and explanation; that which we call re- ality arises in the last analysis from the posing of yes-no ques- tions and the registering of equipment-evoked responses; in short, that all things physical are information-theoretic in origin and that this is a participatory universe. ...it is not unreasonable to imagine that information sits at the core of physics, just as it sits at the core of a computer. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 15 / 27
Relations to quantum theory Physical measurements, information, and quantum theory Information in physics: Wheeler’s ‘it from bit’ doctrine John Archibald Wheeler (July 9, 1911 – April 13, 2008) was a promi- nent American physicist known for his contribution to general relativity and quantum theory. In 1990, Wheeler suggested that information is fundamental to the physics of the universe and started developing the informational interpretation of physics. He wrote: ‘It from bit’ symbolizes the idea that every item of the physical world has at bottom — a very deep bottom, in most instances — an immaterial source and explanation; that which we call re- ality arises in the last analysis from the posing of yes-no ques- tions and the registering of equipment-evoked responses; in short, that all things physical are information-theoretic in origin and that this is a participatory universe. ...it is not unreasonable to imagine that information sits at the core of physics, just as it sits at the core of a computer. Let’s give some mathematical reasoning why ‘it’ is indeed ‘from bit’. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 15 / 27
Relations to quantum theory Torus windings and wave functions The next topic: Experiments and problems 1 Representations of automata maps in real and complex spaces 2 General automata Finite automata Relations to quantum theory 3 Physical measurements, information, and quantum theory Torus windings and wave functions Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 16 / 27
Relations to quantum theory Torus windings and wave functions Speculation: Automata as models of quantum systems Accumulation points of a plot of a finite linear automaton (whose au- tomaton function is then f : z �→ az + b for suitable a , b ∈ Z p ∩ Q ) look like a finite collection of waves with the same wavenumber a (up to a normalization s.t. � = 1 ), where x stands for position, 2 π b for angular frequency ω and p ℓ for time t . → e i ( ax − 2 π b ∙ p ℓ ) ; ( x ∈ R , ℓ ∈ N 0 ) AP ( A ) = AP ( az + b ) ← Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 17 / 27
Relations to quantum theory Torus windings and wave functions Speculation: Automata as models of quantum systems Accumulation points of a plot of a finite linear automaton (whose au- tomaton function is then f : z �→ az + b for suitable a , b ∈ Z p ∩ Q ) look like a finite collection of waves with the same wavenumber a (up to a normalization s.t. � = 1 ), where x stands for position, 2 π b for angular frequency ω and p ℓ for time t . Consider a special case when a ∈ Z and b = 0 : → e i ( ax ) ; ( x ∈ R , ℓ ∈ N 0 ) AP ( A ) = AP ( az ) ← Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 17 / 27
Relations to quantum theory Torus windings and wave functions Speculation: Automata as models of quantum systems → e i ( ax ) ; ( x ∈ R , ℓ ∈ N 0 ) AP ( A ) = AP ( az ) ← It is reasonable to suggest that indeed a is the wavenumber (cf. 1 left and right pictures); thus wavelength λ = a . Moreover, then ω = λ − 1 = a ; and note that AP ( az + at ) = AP ( az ) for every t ∈ Z . Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 17 / 27
Relations to quantum theory Torus windings and wave functions Speculation: Automata as models of quantum systems → e i ( ax − 2 π b ∙ p ℓ ) ; ( x ∈ R , ℓ ∈ N 0 ) AP ( A ) = AP ( az + b ) ← The “time-looking” multiplier p ℓ is a proper time of the automaton. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 17 / 27
Relations to quantum theory Torus windings and wave functions Speculation: Automata as models of quantum systems → e i ( ax − 2 π b ∙ p ℓ ) ; ( x ∈ R , ℓ ∈ N 0 ) AP ( A ) = AP ( az + b ) ← The “time-looking” multiplier p ℓ is a proper time of the automaton. Namely, multiplying by p corresponds to on step of the automaton: ( p ℓ x ) mod 1 is an ℓ -step shift of base- p expansion of x ∈ R . Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 17 / 27
Relations to quantum theory Torus windings and wave functions Speculation: Automata as models of quantum systems → e i ( ax − 2 π b ∙ p ℓ ) ; ( x ∈ R , ℓ ∈ N 0 ) AP ( A ) = AP ( az + b ) ← The “time-looking” multiplier p ℓ is a proper time of the automaton. Can p ℓ be treated a physical time ? Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 17 / 27
Relations to quantum theory Torus windings and wave functions Speculation: Automata as models of quantum systems → e i ( ax − 2 π b ∙ p ℓ ) ; ( x ∈ R , ℓ ∈ N 0 ) AP ( A ) = AP ( az + b ) ← The “time-looking” multiplier p ℓ is a proper time of the automaton. Can p ℓ be treated a physical time ? Yes! Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 17 / 27
Relations to quantum theory Torus windings and wave functions Speculation: Automata as models of quantum systems → e i ( ax − 2 π b ∙ p ℓ ) ; ( x ∈ R , ℓ ∈ N 0 ) AP ( A ) = AP ( az + b ) ← The “time-looking” multiplier p ℓ is a proper time of the automaton. Can p ℓ be treated a physical time ? Yes! Just take p close to 1 (forgetting for a moment that p is a base of a radix system); i.e., p = 1 + τ where τ is small. For instance, assume that τ is a Planck time (=a quant of time) or other time interval which is less then the accuracy of measurements and thus can not be measured. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 17 / 27
Relations to quantum theory Torus windings and wave functions Speculation: Automata as models of quantum systems → e i ( ax − 2 π b ∙ p ℓ ) ; ( x ∈ R , ℓ ∈ N 0 ) AP ( A ) = AP ( az + b ) ← The “time-looking” multiplier p ℓ is a proper time of the automaton. Can p ℓ be treated a physical time ? Yes! Just take p close to 1 (forgetting for a moment that p is a base of a radix system); i.e., p = 1 + τ where τ is small. Then p ℓ ≈ 1 + ℓτ and therefore for large ℓ we see that ℓτ = t is just a time. And here we are: e i ( ax − 2 π b ∙ p ℓ ) ≈ e i ( ax − 2 π b ∙ ( 1 + t )) = c ∙ e i ( ax − 2 π b ∙ t ) ← the wave!!! Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 17 / 27
Relations to quantum theory Torus windings and wave functions Speculation: Automata as models of quantum systems → e i ( ax − 2 π b ∙ p ℓ ) ; ( x ∈ R , ℓ ∈ N 0 ) AP ( A ) = AP ( az + b ) ← The “time-looking” multiplier p ℓ is a proper time of the automaton. Can p ℓ be treated a physical time ? Yes! Just take p close to 1 (forgetting for a moment that p is a base of a radix system); i.e., p = 1 + τ where τ is small. Then p ℓ ≈ 1 + ℓτ and therefore for large ℓ we see that ℓτ = t is just a time. And here we are: e i ( ax − 2 π b ∙ p ℓ ) ≈ e i ( ax − 2 π b ∙ ( 1 + t )) = c ∙ e i ( ax − 2 π b ∙ t ) ← the wave!!! Is it mathematically correct to put p = 1 + τ where 0 < τ ≪ 1 ? Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 17 / 27
Relations to quantum theory Torus windings and wave functions Speculation: Automata as models of quantum systems → e i ( ax − 2 π b ∙ p ℓ ) ; ( x ∈ R , ℓ ∈ N 0 ) AP ( A ) = AP ( az + b ) ← The “time-looking” multiplier p ℓ is a proper time of the automaton. Can p ℓ be treated a physical time ? Yes! Just take p close to 1 (forgetting for a moment that p is a base of a radix system); i.e., p = 1 + τ where τ is small. Then p ℓ ≈ 1 + ℓτ and therefore for large ℓ we see that ℓτ = t is just a time. And here we are: e i ( ax − 2 π b ∙ p ℓ ) ≈ e i ( ax − 2 π b ∙ ( 1 + t )) = c ∙ e i ( ax − 2 π b ∙ t ) ← the wave!!! Is it mathematically correct to put p = 1 + τ where 0 < τ ≪ 1 ? Yes , if one uses β -expansions (introduced by R´ enyi—Parry in 1957– 1960) rather than base p -expansions. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 17 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers To construct a plot of an automaton over a p -letter alphabet we use base- p expansions of numbers: To every pair of input/output words input word χ k − 1 . . . χ 1 χ 0 − → output word ξ k − 1 . . . ξ 1 ξ 0 we put into the correspondence the point on the torus ( χ k − 1 p − 1 + ∙ ∙ ∙ χ 1 p − k + 1 + χ 0 p − k ; ξ k − 1 p − 1 ∙ ∙ ∙ + ξ 1 p − k + 1 + ξ 0 p − k ) Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers To construct a plot of an automaton over a p -letter alphabet we use base- p expansions of numbers: To every pair of input/output words input word χ k − 1 . . . χ 1 χ 0 − → output word ξ k − 1 . . . ξ 1 ξ 0 we put into the correspondence the point on the torus ( χ k − 1 p − 1 + ∙ ∙ ∙ χ 1 p − k + 1 + χ 0 p − k ; ξ k − 1 p − 1 ∙ ∙ ∙ + ξ 1 p − k + 1 + ξ 0 p − k ) We may take β ∈ R + such that ⌊ β ⌋ = p − 1 and use β -expansions rather than base- p expansions; that is, we put into the correspondence to the pair of input/output words the following point on the torus: ( χ k − 1 β − 1 + ∙ ∙ ∙ χ 1 β − k + 1 + χ 0 β − k ; ξ k − 1 β − 1 ∙ ∙ ∙ + ξ 1 β − k + 1 + ξ 0 β − k ) Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers To construct a plot of an automaton over a p -letter alphabet we use base- p expansions of numbers: To every pair of input/output words input word χ k − 1 . . . χ 1 χ 0 − → output word ξ k − 1 . . . ξ 1 ξ 0 we put into the correspondence the point on the torus ( χ k − 1 p − 1 + ∙ ∙ ∙ χ 1 p − k + 1 + χ 0 p − k ; ξ k − 1 p − 1 ∙ ∙ ∙ + ξ 1 p − k + 1 + ξ 0 p − k ) We may take β ∈ R + such that ⌊ β ⌋ = p − 1 and use β -expansions rather than base- p expansions; that is, we put into the correspondence to the pair of input/output words the following point on the torus: ( χ k − 1 β − 1 + ∙ ∙ ∙ χ 1 β − k + 1 + χ 0 β − k ; ξ k − 1 β − 1 ∙ ∙ ∙ + ξ 1 β − k + 1 + ξ 0 β − k ) We must take β s.t. arithmetics of numbers represented by β - expansions can be performed by a finite automaton. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers To construct a plot of an automaton over a p -letter alphabet we use base- p expansions of numbers: To every pair of input/output words input word χ k − 1 . . . χ 1 χ 0 − → output word ξ k − 1 . . . ξ 1 ξ 0 we put into the correspondence the point on the torus ( χ k − 1 p − 1 + ∙ ∙ ∙ χ 1 p − k + 1 + χ 0 p − k ; ξ k − 1 p − 1 ∙ ∙ ∙ + ξ 1 p − k + 1 + ξ 0 p − k ) We may take β ∈ R + such that ⌊ β ⌋ = p − 1 and use β -expansions rather than base- p expansions; that is, we put into the correspondence to the pair of input/output words the following point on the torus: ( χ k − 1 β − 1 + ∙ ∙ ∙ χ 1 β − k + 1 + χ 0 β − k ; ξ k − 1 β − 1 ∙ ∙ ∙ + ξ 1 β − k + 1 + ξ 0 β − k ) We must take β s.t. arithmetics of numbers represented by β - expansions can be performed by a finite automaton. √ N Such β do exist; e.g., we may for instance take β = 2 . Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers We may take β ∈ R + such that ⌊ β ⌋ = p − 1 and use β -expansions rather than base- p expansions; that is, we put into the correspondence to the pair of input/output words the following point on the torus: ( χ k − 1 β − 1 + ∙ ∙ ∙ χ 1 β − k + 1 + χ 0 β − k ; ξ k − 1 β − 1 ∙ ∙ ∙ + ξ 1 β − k + 1 + ξ 0 β − k ) We must take β s.t. arithmetics of numbers represented by β - expansions can be performed by a finite automaton. √ N Such β do exist; e.g., we may for instance take β = 2 . In general to ensure the finiteness, if β = 1 + τ with 0 < τ ≪ 1 , then β must satisfy equation 2 = u ( β ) where u is a polynomial with coefficients 0 , 1 √ N (for instance, we may take β = 2 with N large enough). Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers We may take β ∈ R + such that ⌊ β ⌋ = p − 1 and use β -expansions rather than base- p expansions; that is, we put into the correspondence to the pair of input/output words the following point on the torus: ( χ k − 1 β − 1 + ∙ ∙ ∙ χ 1 β − k + 1 + χ 0 β − k ; ξ k − 1 β − 1 ∙ ∙ ∙ + ξ 1 β − k + 1 + ξ 0 β − k ) We must take β s.t. arithmetics of numbers represented by β - expansions can be performed by a finite automaton. √ N Such β do exist; e.g., we may for instance take β = 2 . In general to ensure the finiteness, if β = 1 + τ with 0 < τ ≪ 1 , then β must satisfy equation 2 = u ( β ) where u is a polynomial with coefficients 0 , 1 √ N (for instance, we may take β = 2 with N large enough). Then necessarily the input/output alphabets are binary, and Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers We may take β ∈ R + such that ⌊ β ⌋ = p − 1 and use β -expansions rather than base- p expansions; that is, we put into the correspondence to the pair of input/output words the following point on the torus: ( χ k − 1 β − 1 + ∙ ∙ ∙ χ 1 β − k + 1 + χ 0 β − k ; ξ k − 1 β − 1 ∙ ∙ ∙ + ξ 1 β − k + 1 + ξ 0 β − k ) We must take β s.t. arithmetics of numbers represented by β - expansions can be performed by a finite automaton. √ N Such β do exist; e.g., we may for instance take β = 2 . In general to ensure the finiteness, if β = 1 + τ with 0 < τ ≪ 1 , then β must satisfy equation 2 = u ( β ) where u is a polynomial with coefficients 0 , 1 √ N (for instance, we may take β = 2 with N large enough). Then necessarily the input/output alphabets are binary, and any torus link will be dense and can be ascribed to a matter wave ce i ( ax − 2 π bt ) where x , t are space and time coordinates accordingly. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers We may take β ∈ R + such that ⌊ β ⌋ = p − 1 and use β -expansions rather than base- p expansions; that is, we put into the correspondence to the pair of input/output words the following point on the torus: ( χ k − 1 β − 1 + ∙ ∙ ∙ χ 1 β − k + 1 + χ 0 β − k ; ξ k − 1 β − 1 ∙ ∙ ∙ + ξ 1 β − k + 1 + ξ 0 β − k ) Then (as β = 1 + τ with τ small) necessarily the input/output alphabets are binary, and any torus link can be ascribed to a matter wave ce i ( ax − 2 π bt ) where x , t are space and time coordinates accordingly. Therefore our main theorem can serve a mathematical reasoning why a specific ‘it’ — the matter wave, which is a core of quantum theory — is indeed ‘from bit’; that is, from sufficiently long binary inputs of an automaton with a relatively small number of states. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers We may take β ∈ R + such that ⌊ β ⌋ = p − 1 and use β -expansions rather than base- p expansions; Then (as β = 1 + τ with τ small) necessarily the input/output alphabets are binary, and any torus link can be ascribed to a matter wave ce i ( ax − 2 π bt ) where x , t are space and time coordinates accordingly. The approach seemingly reveals more correspondences between phys- ical entities and mathematical properties of automata, for instance: helicity corresponds to the sign of a ; Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers We may take β ∈ R + such that ⌊ β ⌋ = p − 1 and use β -expansions rather than base- p expansions; Then (as β = 1 + τ with τ small) necessarily the input/output alphabets are binary, and any torus link can be ascribed to a matter wave ce i ( ax − 2 π bt ) where x , t are space and time coordinates accordingly. The approach seemingly reveals more correspondences between phys- ical entities and mathematical properties of automata, for instance: helicity corresponds to the sign of a ; probability of finding a particle at a certain point of space corresponds to the average amplitude when t ∈ [ 0 , ∞ ) ; Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers We may take β ∈ R + such that ⌊ β ⌋ = p − 1 and use β -expansions rather than base- p expansions; Then (as β = 1 + τ with τ small) necessarily the input/output alphabets are binary, and any torus link can be ascribed to a matter wave ce i ( ax − 2 π bt ) where x , t are space and time coordinates accordingly. The approach seemingly reveals more correspondences between phys- ical entities and mathematical properties of automata, for instance: helicity corresponds to the sign of a ; probability of finding a particle at a certain point of space corresponds to the average amplitude when t ∈ [ 0 , ∞ ) ; automata with multiple inputs/outputs correspond to finite-dimensional Hilbert spaces (to include into the consideration infinite-dimensional Hilbert spaces one needs to consider automata of measure 0 rather then just finite ones); Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers We may take β ∈ R + such that ⌊ β ⌋ = p − 1 and use β -expansions rather than base- p expansions; Then (as β = 1 + τ with τ small) necessarily the input/output alphabets are binary, and any torus link can be ascribed to a matter wave ce i ( ax − 2 π bt ) where x , t are space and time coordinates accordingly. helicity corresponds to the sign of a ; probability of finding a particle at a certain point of space corresponds to the average amplitude when t ∈ [ 0 , ∞ ) ; automata with multiple inputs/outputs correspond to Hilbert spaces ; pure states correspond to ergodic linear subautomata, mixed states correspond to automata states leading to more than 1 ergodic subautomata; entagled states correspond to states from ergodic subautomata of automata with multiple inputs/outputs. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers pure states correspond to ergodic linear subautomata, mixed states correspond to automata states leading to more than 1 ergodic subautomata; entagled states correspond to states from ergodic subautomata of automata with multiple inputs/outputs. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers Interpretation of the case β = 1 + τ where 0 < τ ≪ 1 In our model, β j may be interpreted as a time which is needed to acquire the next j -th bit; so the time T k needed to acquire a k -bit τ ( β k − 1 ) . information is exponential in k , namely T k = 1 Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers Interpretation of the case β = 1 + τ where 0 < τ ≪ 1 In our model, β j may be interpreted as a time which is needed to acquire the next j -th bit; so the time T k needed to acquire a k -bit τ ( β k − 1 ) . information is exponential in k , namely T k = 1 Note that then T k ≈ k for large k . Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers Interpretation of the case β = 1 + τ where 0 < τ ≪ 1 In our model, β j may be interpreted as a time which is needed to acquire the next j -th bit; so the time T k needed to acquire a k -bit τ ( β k − 1 ) . information is exponential in k , namely T k = 1 Note that then T k ≈ k for large k . The case T k ∼ k implies that the time needed to acquire the next j -th bit does not depend on j . Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers Interpretation of the case β = 1 + τ where 0 < τ ≪ 1 In our model, β j may be interpreted as a time which is needed to acquire the next j -th bit; so the time T k needed to acquire a k -bit τ ( β k − 1 ) . information is exponential in k , namely T k = 1 Note that then T k ≈ k for large k . The case T k ∼ k implies that the time needed to acquire the next j -th bit does not depend on j . But E. Lerner recently has shown that in the latter case the plot will be a polygon (=”body”) rather than a torus winding (=”wave”). Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers Interpretation of the case β = 1 + τ where 0 < τ ≪ 1 In our model, β j may be interpreted as a time which is needed to acquire the next j -th bit; so the time T k needed to acquire a k -bit τ ( β k − 1 ) . information is exponential in k , namely T k = 1 Note that then T k ≈ k for large k . The case T k ∼ k implies that the time needed to acquire the next j -th bit does not depend on j . But E. Lerner recently has shown that in the latter case the plot will be a polygon (=”body”) rather than a torus winding (=”wave”). So in QT acquiring of information actually is exponential in time, in a contrast to classical case when this is linear. In our model, classical case appears as a limit case at τ → 0 ; i.e., as it should be: In a contrast to QT, there are arbitrarily small time intervals in classical case. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers In our model, classical case appears as a limit case at τ → 0 ; i.e., as it should be: In a contrast to QT, there are arbitrarily small time intervals in classical case. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers In our model, classical case appears as a limit case at τ → 0 ; i.e., as it should be: In a contrast to QT, there are arbitrarily small time intervals in classical case. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers In our model, classical case appears as a limit case at τ → 0 ; i.e., as it should be: In a contrast to QT, there are arbitrarily small time intervals in classical case. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers In our model, classical case appears as a limit case at τ → 0 ; i.e., as it should be: In a contrast to QT, there are arbitrarily small time intervals in classical case. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers In our model, classical case appears as a limit case at τ → 0 ; i.e., as it should be: In a contrast to QT, there are arbitrarily small time intervals in classical case. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Relations to quantum theory Torus windings and wave functions Using β -expansions of numbers In our model, classical case appears as a limit case at τ → 0 ; i.e., as it should be: In a contrast to QT, there are arbitrarily small time intervals in classical case. Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 18 / 27
Messages of the talk Discreteness+Causality+Finiteness ⇒ Waves Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 19 / 27
Messages of the talk Discreteness+Causality+Finiteness ⇒ Waves Waves, the its , are indeed from bits Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 19 / 27
Messages of the talk Discreteness+Causality+Finiteness ⇒ Waves Waves, the its , are indeed from bits Acquisition of information in QT during a measurement is exponential in time (though base is close to 1) Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 19 / 27
Thank you! Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 20 / 27
Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 21 / 27
p = 2 : f ( x ) = 1 + x + 4 x 2 ; α ( f ) = 1 . Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 22 / 27
f ( z ) = 11 15 z + 1 21 , p = 2 . (Therefore N f = mult 7 2 = 3 ) Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 23 / 27
f 1 ( z ) = − 2 z + 1 3 ; f 2 ( z ) = 3 5 z + 2 7 , ( p = 2 ). Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 24 / 27
Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 25 / 27
Vladimir Anashin (MSU-RAS) Quantization causes waves September 8, 2015, Belgrade 26 / 27
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