Quantum Field Theory and the Limits of Knowledge презентация

Two claims: 1. The laws of physics underlying everyday life are completely known. 2. The structure of quantum field theory provides a warrant for claim 1.

Слайд 1Sean Carroll, Caltech
Quantum Field Theory
and the
Limits of Knowledge


Слайд 2Two claims:

1. The laws of physics underlying everyday life are completely known. 2.

The structure of quantum field theory provides a warrant for claim 1.

Слайд 3“Laws of physics underlying everyday life”
= The Core Theory
Quantum field theory

in a 4-dimensional spacetime.
Matter (fermions): quarks,leptons.
Strong, weak, electromagnetic forces.
Gravitation = general relativity.
Higgs field.

Слайд 4Long history of embarrassingly premature triumphalism.
“[We are] probably nearing the limit

of all we can know
about astronomy.” – Simon Newcomb, 1888

“The more important fundamental laws and facts of physical science have all been discovered.”
– Albert Michelson, 1894

“Physics as we know it will be over in six months.”
– Max Born, 1928

There is a 50% chance that “we would find a complete unified theory of everything by the end of the century.”
– Stephen Hawking, 1980

Слайд 5Perfectly obvious but necessary caveats
We’re nowhere close to understanding the fundamental
theory

of everything.

We don’t understand the non-everyday: dark matter,
quantum gravity, the Big Bang…

We don’t fully understand macroscopic aggregations:
condensed matter, chemistry, biology, economics…

Quantum mechanics or quantum field theory could
always be wrong.


Слайд 6




Known particles/forces,
general relativity
(Core theory)
Dark matter/energy,
new particles/forces,
hidden sectors

Underlying reality
(theory of everything)
Higher-level
macro-phenomena
of everyday

life

Astrophysics,
cosmology


Слайд 7The Core Theory in more detail:
Quantum Mechanics
Think of “configurations,”
e.g. the

location x of a particle.

Assign a complex number to
every possible configuration.

That describes a quantum state: a “wave function” Ψ(x)
that lives in a very-high-dimensional Hilbert space.


Schrödinger evolution equation:

x

x


Ψ(x)



Слайд 8Measurements in Quantum Mechanics
But we don’t “see” the wave function.

Measurements return

some specific value of the
configuration (or other observable).

Probability of measurement outcome = |wave function|2.

After measurement, wave function “collapses” (becomes
suddenly concentrated on observed outcome).

Seems absurd. But – good enough to successfully
predict the outcome of every experiment ever done.

Слайд 9(Some) Observables are Quantized
Standard example: Simple Harmonic Oscillator.

Particle moving in a

potential ,

where x is the position and ω is the frequency.

Energy is quantized
into discrete levels:

Слайд 10Quantum Field Theory
QFT is not a successor/alternative to QM; it’s just
a

particular QM model, with a particular Hamiltonian.

Namely: “configurations” are “values of (relativistic)
fields throughout space.” E.g. φ(x).

The quantum state (wave function) is a complex
amplitude for each possible field configuration, Ψ[φ(x)].

Examples: electromagnetic field, electron field,
top quark field, gravitational field (metric), etc.

Слайд 11Particles from fields
Each mode acts like a simple harmonic oscillator!

Energy levels

= number of particles.
Wavelength = 1/momentum.

Indeed, relativity+QM+particles QFT.


Decompose oscillating field into a sum of “modes”
of different wavelengths (Fourier transform):

=

+

+ …

+



Слайд 12Interactions
Particle interactions are encoded in Feynman diagrams.
=
+
+
+ …


Слайд 13Adding up virtual particles
Every particle has a
momentum, and total
is conserved at
each

vertex.

Слайд 14Ken Wilson: organize QFT by energy/length scale
Remember: energy & momentum ~

1/(wavelength).

IR

UV

Λ
(“cutoff”
energy
scale)

long
wavelengths/
low energies

short
wavelengths/
high energies


Слайд 15Think of your theory as only describing energies below
the ultraviolet

cutoff scale Λ.

I.e., only include wavelengths longer than 1/Λ.







Result is an effective field theory below Λ.

Effective Field Theory


Слайд 16All diagrams with N legs contribute to an interaction
term (in Lagrangian)

between N particles.

There are an infinite number of terms in
EFT equations of motion…




φ4

φ8

φ6


Слайд 17Both the field φ and the cutoff Λ have units of

energy,
and the Lagrangian governing interactions is (energy)4.

So schematically we have:






Higher-order terms are negligible at low energy (<< Λ).

Only a finite number of relevant/marginal interactions.

… but only a finite number of terms matter

“relevant”

“marginal”

“irrelevant”


Слайд 18At energies below Λ, an EFT can be a complete theory.
Above

Λ, new phenomena can kick in.

E.g. Fermi theory of weak interactions Standard Model.

Effective field theories tell us their regime of applicability:
below the ultraviolet cutoff Λ.


Fermi coupling


Слайд 19“We haven’t quantized gravity,” but I’m treating
gravity like a perfectly ordinary

effective field theory.

Because it is – as long as gravity is weak (far from
black holes, Big Bang, etc.).

In terms of curvature parameter R, interactions look like




Here on Earth, 1st term is 1050 times bigger than 2nd.

Quantum Gravity?


Слайд 20A given effective field theory with cutoff Λ could have
many “ultraviolet

completions” at higher energies.

That’s why it’s hard to do experiments relevant to
quantum gravity: we expect Λ ~ Eplanck ~ 1015 ELHC.

Multiple realizability

loop quantum gravity string theory dynamical triangulations


Слайд 21




Known particles/forces,
general relativity
(Core theory)
Dark matter/energy,
new particles/forces,
hidden sectors

Underlying reality
(theory of everything)
Higher-level
emergent phenomena
of

everyday life

Astrophysics,
cosmology



Underlying physics only influences us via Core Theory.


Слайд 22What about new particles/forces?



strongly
interacting
light/
long range/
low energy
heavy/
short range/
high energy
weakly
interacting
Unknown unknowns = violations

of QFT itself.

Слайд 23QFT puts very tight
constraints on new phenomena.


Слайд 24Constraints on new particles
As-yet-undiscovered
particles must be either:

very weakly interacting,
too heavy

to create, or
too short-lived to detect.

In any of those cases, the new particle would
be irrelevant to our everyday lives.


Слайд 25To be relevant to everyday physics, any new forces
must interact with

protons, neutrons, electrons,
and/or photons.

Experiments are ongoing (torsion balances) to
search for new, weak, long-range forces.

Two ways to hide:

weak interactions, or
very short ranges.

Constraints on new forces


Слайд 26Strength (relative to gravity)
Range
[Long et al. 2003; Antoniadis 2003]
Experimental limits on

new forces

new
gravitational-
strength
force
(10-36 E&M)


Слайд 27




Known particles/forces,
general relativity
(Core theory)
Dark matter/energy,
new particles/forces,
hidden sectors

Underlying reality
(theory of everything)
Higher-level
emergent phenomena
of

everyday life

Astrophysics,
cosmology


New particles/forces are too heavy/weak to influence us.


Слайд 28Punchline:
the laws of physics underlying everyday experience.
Other phenomena are too massive

or weakly-coupled to
have any impact on the particles of which we are made.

Слайд 29Astrology is not correct.
Implications of the Core Theory
You can’t bend spoons

with your mind.

The soul does not survive the body.


Слайд 303. Accessible deviations from textbook QM.
(Hidden variables, spontaneous/induced

collapse.)

Loopholes?

2. Breakdown of QFT itself. E.g. non-local constraints/
interactions from quantum gravity (holography).

1. New forces with environment-dependent couplings.

4. Divine intervention.


Слайд 31




Known particles/forces,
general relativity
(Core theory)
Dark matter/energy,
new particles/forces,
hidden sectors

Underlying reality
(theory of everything)
Higher-level
emergent phenomena
of

everyday life

Astrophysics,
cosmology


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