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Barak Kol
Hebrew University - Jerusalem
Jun 2011, Milos
Outline
• set-up
• puzzles and previous work Based on arXiv: 1103.5741 BK
• The new effective theory W. Goldberger – early collaboration
• Results w/ M. Smolkin - related work
Set-up
Ultra relativistic (massless)
weak scattering
The parameters
Generalizations: Possible interactions, dimensions, masses
Planckian scattering
• Intuitive condition for
black hole creation
• Quantum black holes
The perturbative regime
• The small parameter
• Objective:
– trajectories and especially
– scattering angle
Background
puzzles
• „t Hooft – natural probe
for quantum gravity
- 4d Gravity simplifies for light-
like
- reminiscent of 3d branch cuts
• w. Dray (1985) jump at shock
wave
• (1987) Classical dominance
including sub-planckian b!
• Relation with Veneziano
amplitude
Background
puzzles
• Amati, Ciafaloni, Veneziano
(1987,…,2008)
string theory as quant. Grav.
Eikonal approx, effective theory
“H” correction diagram, dealing
with IR div
• Verlinde2 (1992) –
“topological field theory”
• Giddings
• Computer simulations
Choptuik-Pretorius 2009
Sperhake et al (2010)
Post-Newtonian approximation
• Definition: relativistic correction to slow motion in
flat space-time Damour, Blanchet, Schäfer
i.e. Mercury around the sun, binary system in
adiabatic inspiral
• Small parameter v2/c2 ~GM/R <<1
• The EFT approach r0=2GM<<R Goldberger, Rothstein
(2004)
• The instantaneous
spatial propagator
Grav Field Re-definition
Stationary (t-independent) Physical interpretation
problem of fields
• Technically – KK
• Φ – Newtonian
reduction over time
potential
• “Non-Relativistic
Gravitation” - NRG fields • A – Gravito-magnetic
Non-linear definition vector potential,
similar poles attract
0712.4116
BK, Smolkin
Recovering time dependence
1009.4116
BK, Smolkin
Non-orthonormal frame
1PN: 0712 Kol Smolkin
2PN: 0809 Gilmore Ross
3PN: 1104 Sturani-Foffa
Difficulty in importing PN ideas
Each particle unperturbed motion is
invariant under a different light-cone
coordinate z+, z-.
Relation to other work presented at
this meeting
• Holographic renormalization (Papadimitriou)
• Hydrodynamics and gravity (Y. Oz, A.
Strominger, K. Skenderis)
Related concepts
Vought_V-173 “flying pancake”
experimental aircraft tested 1942-7
Related concepts
Beat 1 Beat 2 Beat 3
Mahler symphony no. 2, 3rd movement
Conducted by L. Bernstein
“St. Anthony Preaches to the Fishes”
The effective theory
Recall the set-up..
The action
Field lines
• Imagine the field lines emanating from a point
charge
• At rest – spherical
• When ultra relativistic
– Lorentz contracted longitudinally
– pancake-shaped transversely
– Aichelburg-Sexl
• “The particle carries
a pancake on its nose”
“flying pancake”
Sudden interaction
• The moment of passing – when the pancakes
coincide
• Interaction localized in z,t
• Eq of motion are sudden,
algebraic recursion
rather than differential
Mahler‟s 2nd
The propagator
2 k+ k- is a quadratic perturbation
The momentum transfer
Field decomposition
• Dimensional reduction onto transverse space BK 2010
à la Kaluza-Klein
• Gab are (transverse) scalars. Analogous to the
Newtonian potential.
G++ couples to R, G-- couples to L.
• Aai are two (transverse) vectors.
couple to mass current in the transverse plane.
• Spin is dipole charge for vectors.
Whole action
BK (2011)
Yoon (1996,99)
Extrinsic curvature
deWitt metric
Results
1st order and momentum transfer
Ultra-relativistic dynamics
• “Light-cone”/ “infinite momentum frame”
• A particle has a total of 3 degrees of Dirac
Weinberg
freedom Susskind
• 2 transverse (ordinary) degrees of
freedom
• p+ plays the role of mass, z+ is time
• z- is a 1st order ODE – constraint – half dof
• e the world-line metric, or equiv z+ is the
other half
2-body effective action
Scalar interaction
For scalar→gravitational change e factors, add non-linear blik vertices
2nd order
Mass shall
Energy unchanged in CM frame
Improved “renormalization”
• “Ordinary” initial conditions for scattering
at t=-∞
• Specify initial conditions at nearest
approach “t=0”
pretending to know them.
Higher symmetry: parity in the pert theory
Evolve both forward and backward in time to
eliminate the t=0 conditions
Interaction duration – 3rd order
• Obtain a term of type
• ε2 c3/c1 estimates τ2, where τ is the (finite)
duration
• We find τ≈ε b BK2011 At d=4 there is a pole in dim. Reg.
• This is consistent with the arc‟s radius of
curvature being b,
namely the center of force being at the other
particle
Discussion
• We defined a classical effective field theory
(CLEFT) - different from PN.
• Result: interaction duration resolved
• Relation with eikonal approximation
Late 1960s, QFT context,
concept borrowed from optics –
an approximation of wave optics calculated on the
basis of rays
Eikon=image in greek
Open questions
Non-conservation due to radiation:
Energy, momentum, angular momentum
Cylon raider from Battlestar Galactica
ΕΦΧΑΡΙΣΤΟ! Thank you!
Darkness and Light in our region
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