Transcript Document

Many Worlds - Many Minds
A view of our universe
Ingvar Lindgren
Einstein
”God does NOT play dice”
Bohr
”God plays dice”
Dispute about the interpretation of QM
...modern experiments and the discovery of decoherence have
shifted the prevailing quantum interpretations away from
wave function collapse towards unitary physics,....
Copenhagen school
Bohr, Heisenberg, Pauli
Measuring process acc. to Cop. interpret.
Result
Wave function
M
i
 ci i
A measurement is performed by a macroscopic apparatus
System is instantaneously and randomly transformed to an eigenstate
of the observable.
Wave function collapse
The probability for a certain result is |ci|2 ”God plays dice”
Max Born’s probalitity interpretation
EPR paradox
Einstein-Podolsky-Rosen 1935
J=0
J=0
Two-photon decay
Photons of opposite polarization. Acc. to Cop. interpret. the photons have no specific
polarization, before the pol. has been measured. Superposition of states.
The measurement of photon 1 gives it a specific polarization.
Then also the polarization of photon 2 will be given.
   ci  i
i
Hidden variables? Bell’s inequality
Schrödinger’s cat
Radiation from a radioactive material initiates a buttet that kills the cat.
Before the observation, the cat is acc. to Copenhagen interpret. in a
superposition of dead and alive.
Superposition -- entanglement
   ci  i
Mathematically a state can be expanded in any
complete basis set.
Entanglement: Coupling of physical states
(eigenstates of an observable)
   ci  i
i
Collapse of wave function: Abrupt destruction
of entanglement
Problems with the Copenhagen interpretation
• The measurement process requires an macroscopic observer.
• Artificial border between micro and macro systems.
• The collapse of the wave function does not
follow any known laws of physics.
• Born’s statistical interpretation is an additional
assumption that does not follow from the model.
Hugh Everett’s interpretation
Rev. Mod. Physics 29, 454 (1957)‫‏‬
• Dropping collapse of wf
Entire world evolves accord. to
time-dependent Schrödinger eq.
Hugh Everett
• Also measuring device treated quantum
mechanically (von Neumann)
John Wheeler
S
M
|>  ( ci |Si>) |M0>
No interaction between system and meas. device
S
M
|>   ci |SiMi>
Interaction between system and meas. device
Measuring device affected by
interaction with the system under study
S 1 M1
S
M
S2M2
S1M1O1
S
M
S2M2O1
Observer connected to ONE branch, sees only that branch
Everett termed this ”relative-state model”
DeWitt introduced around 1970 the term
”Many-worlds interpretation”
Why no interference between the branches?
The Everett original model is incomplete.
Does not explain the emergence of stable,
non-interfering brances
Does not explain the emergence of classicality
Decoherence has to be considered
Decoherens (W.H. Zurek, H.D. Zeh ~1980)
Zurek, Rev. Mod. Phys. 75, 715 (2003)
Dynamical dislocation of
quantum-mechanical entanglements,
destruction of quantum coherence
Wojciech Hubert Zurek
Purely quantum-mechanical phenomenon
Caused by interaction by the environment
Dieter Zeh
S1M1
S
M
S2M2
Left alone, strong coherences between the branches
Complete entanglement
S1M1
S
M
S2M2
Interaction with environment
S1M1
S
M
S2M2
Entanglement with environment
reduces entanglement between branches
S1M1
S
M
S2M2
Further entanglement with environment
reduces further entanglement between branches
classicality
S1M1
S
pointer states
stable, decoupled
M
S2M2
classicality
Eventually development of stable pointer states
Not further affected by environment
Branches completely decoupled
Emergence of classicality
classicality
S1M1
S
pointer states
stable, decoupled
M
S2M2
classicality
Zurek: Einselection
environment-induced superselection
Preferred states:
Independent of initial conditions
classicality
S1M1
S
pointer states
stable, decoupled
M
S2M2
classicality
This is the measurement process in MWI
No macroscopic observer
No collapse
Continuous transition to classicality – No cat!
Observer in one branch not aware of the other branches
Different “worlds” - different “minds”
classicality
S1M1
S
pointer states
stable, decoupled
M
S2M2
classicality
Compare Darwin's theory:
Origin of the spicies
Survival of the fittest
”Quantum Darvinism”
S
M
S2M2
classicality
Copenhagen interpretation:
Nature selects randomly ONE branch
”God plays dice”
Extra detektor
Extra detektor
Stern-Gerlach magnet to measure spin orientation
Extra detector will destroy interference
System (spin) – detector (magnet):
 = a | s+d+> + b | s-d->
Density matrix r = |  > <  | =
|a|2 | s+d+>< s+d+| +a*b|s+d+>< s-d-|+ba*| s-d->< s+d+| +|b|2 |s-d-> < s-d-|
Interference terms
System (spin) – detector (magnet) – environment (extra detektor)
 = a|s+d+ e+ > + b |s-d- e- >
Reduced density matrix for sd system (<ei|ej> = dij):
rr = e <e|  > <  |e> = |a|2 | s+d+> < s+d+| + |b|2 | s-d-> < s-d-|
No interference
H. D. Zeh:
The importance of decoherence was overlooked for
the first 60 years of quantum theory precisely
because entanglement was misunderstood ....
Quantum-mechanical
decoherence has been verified
experimentally
Haroche et al, PRL 77, 4887 (1996)
Zeilinger et al., Nature 401, 680 (1999)
Serge Haroche
Anton Zeilinger
Advantages with Everett-DeWitt model
(with decoherence)
Schrödinger equation strictly valid.
No collapse of wave function.
No classical observer needed.
No artificial border between micro
and macro systems.
Decoherence leads to emergence of
classicality – No cat states
Born’s statistical interpretation
follows from the model (Zurek 2005)
Many experts consider this to be the most –
or even the only -- consistent interpretation of
mechanics quantum presented so far.
Dieter Zeh 2000:
The multi-universe interpretation (which should rather be called
multi-consciousness interpretation) seems to be the only
interpretation of a universal quantum theory (with an exact
Schrödinger equation) that is compatible with the way the world
is perceived. However, because of quantum non-locality it
requires an appropriate modification of the traditional
epistemological postulate of psycho-physical parallelism.
In this interpretation, the physical world is completely described
by Everett's wave function that evolves deterministically
(Laplacean). This global quantum state then defines an indeterministic (hence "branching") succession of states for all
observers. Therefore, the world itself appears indeterministic
subjective in principle, but largely objective through quantum
correlations (entanglement).
Dieter Zeh 2000:
... the Heisenberg-Bohr picture of quantum mechanics is dead.
Neither classical concepts, nor any uncertainty relations,
complementarity, observables, quantum logic, quantum
statistics, or quantum jumps have to be introduced on a
fundamental level.
Personal view
The decoherence leads to disentanglement of entangled
states. The branches still exist but are not aware of each
other.
Universe – a bifurcations tree
Universe – a bifurcations tree
Universe – a bifurcations tree
Universe – a bifurcations tree
Universe – a bifurcations tree
Universe – a bifurcations tree
Life
.......
Universe – a bifurcations tree
Homo
sapiens
Life
.......
.......
Universe – a bifurcations tree
Homo
sapiens
Life
.......
.......
. . . . . . I.L.
Universe – a bifurcations tree
Homo
sapiens
Life
.......
.......
Probability for Life  Hom.sap.  I.L extremely small.
. . . . . . I.L.
Tage Danielssons statistik
”Jag menar, före Harrisburg så var det ju ytterst osannolikt att det som
hände i Harrisburg skulle hända, men så fort det hade hänt, rakade ju
sannolikheten upp till inte mindre än 100 procent, så det var nästan sant
att det hade hänt.”
Universe – a bifurcations tree
Homo
sapiens
Life
.......
.......
Probability for Life  Hom.sap.  I.L extremely small.
”Men när det väl har hänt, är sannolikheten 100 %,
och det är nästan sant att det har hänt.”
. . . . . . I.L.
Universe – a bifurcations tree
Homo
sapiens
Life
.......
.......
All branches remain – no collapse of wave function
. . . . . . I.L.
My universe
Homo
sapiens
Life
.......
.......
All branches remain – no collapse of wave function
But each observer can see only one branch –
”Many minds”
. . . . . . I.L.
My universe
Homo
sapiens
Life
.......
.......
. . . . . . I.L.
All branches remain – no collapse of wave function
But each observer can see only one branch –
”Many minds”
Looks like a collapse of wave function for each observer
”Anthropic principle”
Anthropic principle
Anthropic principle
(Dicke 1961, Brandon Carter, 1973)
No coincidence that the universe has the
properties it has
Brandon Carter
Acc. to anthropic principle universe must
have exactly these properties
in order for humans to be created
and to develop
If not, we would not exist and could not
worry about it.
B a r r o w a n d F r a n k , O x fo r d 1 9 8 8
Stephen Hawking
A Brief History of Time
(1988)9(
mill. copies)
Universe in a nutshell
(2001)
Hugh Ross: Fingerprint of God
Creator and the Cosmos
Martin Rees:
Before the beginning
Barrow-Silk:
The left hand of creation
H. Dieter Zeh
The direction of time
(5.ed.)
Knowledge and the world
Max Tegmark
Commentary
Nature 448, 23-24 (5 July 2007)
Many lives in many worlds
Max Tegmark1
1.
Abstract
In this Universe, Max Tegmark is a physicist at the Massa chusetts Institute of Technology, Cambridge,
Massachusetts, USA.
Top of page
Accepting quantum physics to be universally true, argues Max
Tegmark, means that you should also believe in parallel universes.
MIRAGE ENTERPRISES/RGA
Is it only in fiction that we can experience parallel lives? If atoms can be
in two places at once, so can you.
Further reading
Zurek, Rev. Mod. Phys. 75, 715 (2003)
Zurek, Physics Today 44, 36 (1991)
Stanford Encyclopedia of Philosophy
D. H. Zeh, arXiv:quant-ph
Peter Byrne: The Many Worlds of Hugh Everett, Sci. Amer. Nov. 2007
Tegmark and Wheeler: 100 years of the Quantum,
arXiv:quant-ph/0101077v1
I.L. Interpretation of Quantum Mechanics, http://fy.chalmers.se/~f3ail/