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Quantum gravity and aspects of relativity Branislav Nikolic Institute for Theoretical Physics, University of Cologne Bonn-Cologne Graduate School in Physics and Astronomy

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Page 1: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

Quantum gravityand

aspects of relativity

Branislav Nikolic

Institute for Theoretical Physics,University of Cologne

Bonn-Cologne Graduate School inPhysics and Astronomy

Page 2: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

Gravitation and Relativity research groupProf. Dr. Claus Kiefer, Prof. Dr. Friedrich Hehl

who are we???

- have a look at the webpage of our group!

www.thp.uni-koeln.de/gravitation/

- Institute of Theoretical Physics, Cologne

- have a look at the webpage of our group!

www.thp.uni-koeln.de/gravitation/

- email us if you have any questions, don’t be afraid!

- join us at our seminars: Tuesdays 12h, Seminar Room 215

Page 3: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

what are we going to do today?

- tell you about what kind of interesting things we are doing in our group

- hang out with you during the coffee breaks and lunch

This talk:

A. Crash course in General Relativity

B. Crash course in Canonical Quantum Gravity

C. Overview of today’s talks

Page 4: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

A. Crash course in General Relativity

- Einstein, ~1916

geometry of non-empty (non-vacuum) 4D spacetime is not flat, but curved!

Minkowski metric general metric(encodes gravitational field)

Page 5: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

A. Crash course in General Relativity

- Einstein, ~1916

geometry of non-empty (non-vacuum) 4D spacetime is not flat, but curved!

Minkowski metric general metric(encodes gravitational field)

geometry of 4D spacetime <~> matter- Einstein’s Equations:

Page 6: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

A. Crash course in General Relativity

- Einstein, ~1916

geometry of non-empty (non-vacuum) 4D spacetime is not flat, but curved!

Minkowski metric general metric(encodes gravitational field)

geometry of 4D spacetime <~> matter- Einstein’s Equations:

curvature ( )

cosmological constant

energy-momentum tensor

given matter distribution/symmetry

find the metric

to solve EE means:

Page 7: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

A. Crash course in General Relativity

- for example:

- Friedman-Lemaitre-Robertson-Walker metric (models a homogeneous andisotropic universe)

scale factor Friedmann equations:

(rate of universe’s expansion interms of what’s inside it)

Page 8: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

A. Crash course in General Relativity

- for example:

- Friedman-Lemaitre-Robertson-Walker metric (models a homogeneous andisotropic universe)

scale factor Friedmann equations:

- Schwarzschild solution (non-rotating Black Hole!)

(rate of universe’s expansion interms of what’s inside it)

Page 9: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

A. Crash course in General Relativity

- for example:

- Friedman-Lemaitre-Robertson-Walker metric (models a homogeneous andisotropic universe)

scale factor Friedmann equations:

3. Black Holes and Naked Singularities (Alessandro)

2. Singularities in Generalized Chaplygin Gas model(Arezu)

- Schwarzschild solution (non-rotating Black Hole!)

(rate of universe’s expansion interms of what’s inside it)

Page 10: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

- unavoidable singularities in GR is a motivation to change something:

1 – quantize the theory and see if we can avoid singularities

Page 11: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

- unavoidable singularities in GR is a motivation to change something:

1 – quantize the theory and see if we can avoid singularities

2 – make a different theory of gravity

Page 12: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

- unavoidable singularities in GR is a motivation to change something:

1 – quantize the theory and see if we can avoid singularities

2 – make a different theory of gravity3 – both

Page 13: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

- unavoidable singularities in GR is a motivation to change something:

1 – quantize the theory and see if we can avoid singularities

2 – make a different theory of gravity3 – both

- other things make us think towards quantizing gravity:

- three interactions of Nature can be unified in a common framework;include gravity (“theory of everything”) ? gravitational field must also bequantized!

- three interactions of Nature can be unified in a common framework;include gravity (“theory of everything”) ? gravitational field must also bequantized!

Page 14: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

- unavoidable singularities in GR is a motivation to change something:

1 – quantize the theory and see if we can avoid singularities

2 – make a different theory of gravity3 – both

- other things make us think towards quantizing gravity:

- three interactions of Nature can be unified in a common framework;include gravity (“theory of everything”) ? gravitational field must also bequantized!

- three interactions of Nature can be unified in a common framework;include gravity (“theory of everything”) ? gravitational field must also bequantized!

- the problem of time:4D spacetime (described by metric tensor) is fixed in QFT

VSin GR, spacetime is dynamical

so how do you describe a quantum field propagating on a cruved background?

Page 15: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

semiclassical Einstein equations:

classical metric(classical geometry)

quantum matter

Page 16: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

semiclassical Einstein equations:

quantum matterclassical metric(classical geometry)

but Psi depends on the metric, which we cannot find without solving EE!?!very, very, very non-linear problem!

but Psi depends on the metric, which we cannot find without solving EE!?!very, very, very non-linear problem!

approximation to a more fundamental theory, which includesquantized metric, too

a quantum theory of gravity

Page 17: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

…but how…?!

Page 18: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

Many approaches to Quantum Gravity

Covariant(Path Integrals, RG, perturbations…) Canonical

String Theory

…but how…?!

Gravity fromthermodynamic

perspective

Loop quantum gravity

Quantum Geometrodynamics…

… of GR or…?

Gauge Theory

Page 19: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

Many approaches to Quantum Gravity

Canonical

…this is how we try…

Gravity fromthermodynamic

perspective

Quantum Geometrodynamics…

… of GR or…?

Gauge TheoryLoop quantum gravity

Page 20: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

-you can write down the Hamiltonian for a particle in a potential(using Hamiltonian formulation) - write

H = H (gen. coord., conj. mom.)

Page 21: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

-you can write down the Hamiltonian for a particle in a potential(Hamiltonian formulation) - write

H = H ( gen. coord., conj. mom.)

- you can even write down the Hamiltonian of General Relativity! …how?

- separate spacetime into 3D space + time, and look at geometry of 3D space only(write, hypersurfaces)

3-metric“coordinate”

Page 22: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

-you can write down the Hamiltonian for a particle in a potential(Hamiltonian formulation) - write

H = H ( gen. coord., conj. mom.)

- separate spacetime into 3D space + time, and look at geometry of 3D space only(write, hypersurfaces)

- you can even write down the Hamiltonian of General Relativity! …how?

3-metric“coordinate”

conjugate momentum

Page 23: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

-you can write down the Hamiltonian for a particle in a potential(Hamiltonian formulation) - write

H = H ( gen. coord., conj. mom.)

- separate spacetime into 3D space + time, and look at geometry of 3D space only(write, hypersurfaces)

- you can even write down the Hamiltonian of General Relativity! …how?

- Hamiltonian of GR (ADM formalism):

3-metric“coordinate”

conjugate momentum

Page 24: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

- as in ordinary quantum mechanics, Dirac quantization procedure:

Page 25: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

Wheeler-DeWitt equation

- as in ordinary quantum mechanics, Dirac quantization procedure:

Page 26: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

Wheeler-DeWitt equation

- as in ordinary quantum mechanics, Dirac quantization procedure:

…with which you can do almost no physics…

Page 27: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

Wheeler-DeWitt equation

- as in ordinary quantum mechanics, Dirac quantization procedure:

wave functional, lives in Superspace

no space, no time

…with which you can do almost no physics…

Page 28: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

Wheeler-DeWitt equation

- as in ordinary quantum mechanics, Dirac quantization procedure:

- what is Psi and defined on what kind of space?

- Hilbert space and unitarity?!

wave functional, lives in Superspace

no space, no time

…with which you can do almost no physics…

Page 29: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

…that is why you have to pick a model… (minisuperspace model)

- gravity + scalar field wave function of the Universe:

Page 30: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

…that is why you have to pick a model… (minisuperspace model)

- gravity + scalar field wave function of the Universe:

- semiclassical approximation: expansion in terms of Planck mass:- semiclassical approximation: expansion in terms of Planck mass:

- let’s see what happens order by order…

Page 31: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

…that is why you have to pick a model… (minisuperspace model)

zeroth order:

1st order: Schroedinger equation

2nd order:

quantum gravitational corrections toSchroedinger equation

Page 32: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

B. Crash course in Canonical Quantum Gravity

…that is why you have to pick a model… (minisuperspace model)

-- apply to the Cosmic Microwave Background power spectrum:

Page 33: Quantum gravity and aspects of relativity · B. Crash course in Canonical Quantum Gravity-you can write down the Hamiltonian for a particle in a potential (Hamiltonian formulation)

C. Overview of today’s talks

Canonical

Quantum Geometrodynamics…

… of GR …of ConformalGravity

Gravity fromthermodynamic

perspective

Gauge TheoryLoop quantum gravity

6. Pranjal

… of GR …of ConformalGravity

2. Arezu3. Alessandro

7. Branislav

5. Patrick 4. Jens