Title: Randomness and Determination, from Physics and Computing towards Biology
1Randomness and Determination, from Physics and
Computing towards Biology
- Giuseppe Longo
- LIENS, CNRS ENS, Paris
- http//www.di.ens.fr/users/longo
2Classical dynamical determinism and
unpredictability
- A physical system/process is deterministic when
we have or we believe that it is possible to have
a set of equations or an evolution function
describing the process - i.e. the evolution of the system is fully
determined - by its current states and by a law.
- Classical/Relativistic systems are State
Determined Systems - randomness is an epistemic issue
3Classical dynamical determinism and
unpredictability
- Classical and Relativistic Physics are
deterministic randomness is deterministic
unpredictability (in chaotic systems) - Quantum Mechanics is not deterministic
- (intrinsic/objective role of probabilities in
constituting the theory the measure
entanglement, no hidden variables) - Recent survey/reflections Bailly, Longo, 2007,
Longo, Paul, 2008 - Early confusion in Computing
- A non-deterministic Turing Machine is a
classical deterministic device (ill-typed),
unless a non-classical physical process (which
one?) specifies/implements the branching
4Deterministic unpredictability
- Classical (dynamical) deterministic
unpredictability - a relation between
- a formal-mathematical system (equations,
evolution functions) - a physical process, measured by intervals (the
access). - By the mathematical system one cannot predict
(over short, long time) the evolution of the
physical process - e. g. 1. describing/modelling 2. is non
linear - Mixing (a weak chaos) decreasing correlation of
observables (Cn(fi, fj) ci,j/na for all
n 1), - b. Chaotic sensitivity, topological
transitivity, density of periodic points pure
Mathematics - (decreasing knowledge about trajectories,
increasing entropy) - ? Randomness
5Randomness as deterministic unpredictability
- Classical (epistemic) randomness
- is defined by
- deterministic unpredictability (short, long time)
- Examples dies, coin tossing, a double pendulum,
the Planetary System (Poincaré, 1890 Laskar,
1992) finite (short and long) time
unpredictability - (the dies, a SDS, know where they go along a
geodetics, determined by Hamiltons principle). - Laplace
- infinitary demon OK (over space-time continua)
- determination ? predictability (except
singularities) Wrong!
6Part I Classical Dynamical Systems and Computing
- Dynamical vs. Algorithmic Randomness
-
7Generic (point/trajectory) in Dynamics
- Objects are generic in Physics they are
experimental and theoretical invariants (chose
any falling body, gravitating planets) - A Methodological Aim
- in a deterministic dynamical system (D,T,?)
- Â Pick a generic point in D, at random
(randomize) - replaced by  pick a random (as generic)
point in D - Mathematically
- Â a probabilistic property P holds for almost all
points - replaced by  the set of random points has
measure 1 and P holds for all random pointsÂ
8Birkhoff randomness in Dynamical Systems
- Given (D, T, ?), dynamical system, a point x is
generic (or typical, in the ergodic sense) if,
for any observable f, - Limn (f(x) f(T(x)) f(Tn(x)))/n ? f d?
- That is, the average value of the observable f
along the trajectory - x, T(x), Tn(x)
- (its time average)
- is asymptotically equal to the space average of
f (i.e. ? f d?). - A generic point is a (Birkhoff) random point for
the dynamics. - It is a purely mathematical and limit notion,
within physico-mathematical dynamical systems, at
asymptotic time. - ? ML-randomness
9Algorithmic Randomness as strong undecidability
- Algorithmic randomness (Martin-Löf, 65 Chaitin,
Schnorr.) (for infinite sequences in Cantor
Space D 2?) - Def. ?, measure on D, an effective tatistical
test is - an (effective) sequence Unn, with ?(Un) ? 2n
- I.e. a statistical test is an infinite decreasing
sequence of effective open set in Cantors 2?
(thus, it is given in Recursion Theory) -
- Def. x is random if, for any statistical test
Unn, x is not in ?nUn, - (x passes all tests)
- Random not being contained in any effective
intersection - to stay eventually outside any test (it
passes all tests)
10Algorithmic randomness and undecidability
- Algorithmic randomness a purely computational
notion (a lot of work by Chaitin, Calude Gacs,
Vyugin, Galatolo). - An (infinite) algorithmic-random sequence
contains no infinite effectively generated (r.e.,
semidecidable) subsequence. - Thus Algorithmic randomness is (strictly)
stronger than undecidability (non r.e.,
Gödel-Turings sense) - there exist non rec. enum. sequences which are
not algorithmically random - (e.g. x1 e1 x2 e2 x3 x algo-random, e
effective) - Note there is no randomness in finite time
sequential computing! - At most uncompressibility (finite Kolmogoroff
complexity)
11Dynamical random algorithmic random (Hoyrup,
Rojas Theses)
12Dynamical random algorithmic random (Hoyrup,
Rojas Theses)
- Given a mixing (weakly chaotic) dynamics (D, T,
?), with good computability properties (the
metric, the measure are effective), then - Main Theorem
- A point x in D is generic (Birkhoff random) for
the dynamics iff it is (Schnorr) algorithmically
random. - Note at infinite time
- Dynamical randomness (a la Birkhoff) derives from
Poincarés Theorem (deterministic
unpredictability) - Algorithmic randomness is a strong form of
(Gödels) undecidability Q.E.D.
13Towards Biology
- The Physical Singularity of Life Phenomenain
terms of Dualities
14The Physical Singularity of Life Phenomenain
terms of Dualities
- Physics generic objects and specific
trajectoires (geodetics) - Biology generic trajectories (compatible/possibl
e) and specific objects (individuation)
Bailly, Longo, 2006
15The Physical Singularity of Life Phenomenain
terms of Dualities
- Physics generic objects and specific
trajectoires (geodetics) - Biology generic trajectories (compatible/possibl
e) and specific objects (individuation)
Bailly, Longo, 2006 - Physics energy as operator Hf, time as
parameter f(t, x) - Biology time as operator, energy as parameter
- Time given by (speed of) entropy production by
all irreversile processes it acts as an operator
on a state function (bio-mass density) - Applications both in phylogenesis (long-time
Goulds curb) and ontogenesis (short-time
scalling factors in allometry) - F. Bailly, G. Longo. Biological Organization and
Anti-Entropy, - in J. of Biological Systems, Vol. 17, n.1, 2009.
16Randomness in Life Phenomena
- Recall in Computing and Physics
- 1. For infinite sequences
- (Birkhof) dynamical randomness algorithmic
randomness - 2. In finite time
- determistic unpredictability ? (quantum)
indetermination and randomness - (epistemic vs. intrinsic Bell inequalities)
- Yet, in infinite time, they merge (semi-classical
limit)! - T. Paul, 2008.
17Randomness in Life Phenomena
- Physics all within a given phase (reference)
space (the possible states and observables). - Biology intrinsic indetermination due to change
of the phase space, in phylogenesis
(ontogenesis?) - A proper notion of biological randomness, at
finite short/long time? - Due to the entanglement of the two physical
notions? - Randomness Physics/Computing/Biology
- Physics 2 forms of randomness (different
probability measures) - In Concurrency? In Computers Neworks? A lot of
work - Biology the sum of all forms? What can we learn
from the different forms of randomness and
(in-)determination?
18Physical time vs. RandomnessGeneral tentative
approach to time as an irreversible parameter (in
Physical Theories)
19Physical time vs. RandomnessPreliminary Remarks
- 1. There is no irreversible time in the
mathematics of classical mechanics
(Euler-Lagrange, Newton-Laplace... equations are
time-reversible also a linear field has reverse
determination). - 2. Classically, irreversible time appears in
- 2.1 Deterministic chaos, where randomness is
unpredictability (an action at finite time -
short/long decreasing knowledge) - 2.2 Thermodynamics increasing entropy
(dispersion of trajectories, diffusion of a gas,
of heath along random paths) - Notes underlying a diffusion (e.g. energy
degradation) there is always a random path - 2.1 and 2.2 dispersion of trajectories (entropy
increases in both)
20Thesis Irreversible Time is Randomness(in
Physical Theories)
21Thesis 1 Irreversible Time implies
Randomness(in Physical Theories)
- By the previous argument
- Classical Physics the arrow of time is related
(implies) randomness (by deterministic
unpredictability and random walks in
thermodynamics), in finite (not asymptotic) time. - But also, in Quantum Physics
- t and -t may be interchanged in Schrödinger
equation, as -i is equivalent to i (time may be
reversed) - Irreversible time appears at the (irreversible)
act of measure, which gives probability values
(intrinsic randomness, to the theory) - Thus, if one wants (irreversible) time, one has
randomness.
22Conversely Randomness implies Irreversible Time
- Classical Physics Randomness is (deterministic)
unpredictability - But, unpredictability concerns predicting, thus
the future, in time (decreasing knowledge or no
inverse map). - An epistemic issue, both in Dynamics and
Thermodynamics (increasing entropy) - Similarly, the intrinsic randomness in Quantum
Physics, concern the irreversible act of measure,
irreversible in time - measure produces irreversible time, by a
before and an after. - In conclusion, in Physics, by the structure of
determination - (irreversible) time and randomness are related
(equivalent?)
23What about Biology?
- Life phenomena include
- 1 - Irreversible thermodynamic processes (with
their irreversible time) - But also
- 2.1 Darwinian Evolution (increasing phenotypic
complexity, Gould number of tissue
differentiations, of connections in networks) - 2.2 Morphogenesis (embryogenesis and its
opposite disorganization - death) - Evolution and Morphogenesis are setting-up of
organization (the opposite of entropy and its
internal random processes) - Death is tissue disorganization and includes the
randomness in thermodynamic processes (entropy
increase)
24The double irreversibility of Biological Time
- Evolution, morphogenesis and death are strictly
irreversible, but their irreversibility is
proper, it adds on top of the physical
irreversibility of time (thermo-dynamical) - It is due to a proper observable biological
organization (integration/regulation between
different levels of organization in an organism) - This observable anti-entropy
- F. Bailly, G. Longo. Biological Organization and
Anti-Entropy, in J. of Biological Systems, Vol.
17, n.1, 2009. - One reason for an intrinsic, proper Biological
Randomness...
25Some references (more on http//www.di.ens.fr/user
s/longo )
- Bailly F., Longo G. Mathématiques et sciences de
la nature. La singularité physique du vivant.
Hermann, Visions des Sciences, Paris, 2006. - M. Hoyrup, C. Rojas, Theses, June, 2008 (see
http//www.di.ens.fr/users/longo ) - Bailly F., Longo G., Randomness and Determination
in the interplay between the Continuum and the
Discrete, Mathematical Structures in Computer
Science, 17(2), pp. 289-307, 2007. - Bailly F., Longo G. Extended Critical
Situations, in J. of Biological Systems, Vol.
16, No. 2, 1-28, 2007. - F. Bailly, G. Longo. Biological Organization and
Anti-Entropy, in J. of Biological Systems, Vol.
17, n.1, 2009. - G. Longo. From exact sciences to life phenomena
following Schrödinger on Programs, Life and
Causality, lecture at "From Type Theory to
Morphological Complexity A Colloquium in Honour
of Giuseppe Longo," to appear in Information
and Computation, special issue, 2008. - G. Longo, T. Paul. The Mathematics of Computing
between Logic and Physics. Invited paper,
Computability in Context Computation and Logic
in the Real World, (Cooper, Sorbi eds) Imperial
College Press/World Scientific, 2008.