on-shell methods in gauge theory david a. kosower ipht, cea–saclay taiwan summer institute,...
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![Page 1: On-Shell Methods in Gauge Theory David A. Kosower IPhT, CEA–Saclay Taiwan Summer Institute, Chi-Tou ( 溪頭 ) August 10–17, 2008 Lecture II](https://reader036.vdocuments.site/reader036/viewer/2022081506/56649ea15503460f94ba541a/html5/thumbnails/1.jpg)
On-Shell Methods in Gauge Theory
David A. KosowerDavid A. Kosower
IPhT, CEA–SaclayIPhT, CEA–Saclay
Taiwan Summer Institute, Chi-Tou (Taiwan Summer Institute, Chi-Tou ( 溪溪頭頭 ) )
August 10–17, 2008August 10–17, 2008
Lecture IILecture II
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Spinor Helicity Basis
• Spinor products
• Helicity basis
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Berends–Giele Recursion Relations
Polynomial-time approach per helicity when computing numerically
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Factorization Properties of Amplitudes
• As sums of external momenta approach poles,
• amplitudes factorize
• More generally as
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Factorization in Gauge Theories
Tree level
As butSum over helicities of intermediate legIn massless theories beyond tree level, the situation
is more complicated but at tree level it works in a standard way
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
What Happens in the Two-Particle Case?
We would get a three-gluon amplitude on the left-hand side
Butso all invariants vanish,
hence all spinor products vanish
hence the three-point amplitude vanishes
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
• In gauge theories, it holds (at tree level) for n3 but breaks down for n =2: A3 = 0 so we get 0/0
• However A3 only vanishes linearly, so the amplitude is not finite in this limit, but should ~ 1/k, that is
• This is a collinear limit
• Combine amplitude with propagator to get a non-vanishing object
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Two-Particle Case
Collinear limit: splitting amplitude
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Universal Factorization
• Amplitudes have a universal behavior in this limit
• Depend on a collinear momentum fraction z
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
• In this form, a powerful tool for checking calculations
• As expressed in on-shell recursion relations, a powerful tool for computing amplitudes
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Example: Three-Particle Factorization
Consider
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
As , it’s finite: expected because
As , pick up the first term; with
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Splitting AmplitudesCompute it from the three-point vertex
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Explicit Values
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Complex Momenta
For real momenta,
but we can choose these two spinors independently and still have k2 = 0
Recall the polarization vector: but
Now when two momenta are collinearonly one of the spinors has to be collinear but not necessarily both
Insight from Witten’s twistor string theory (2003)
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
On-Shell Recursion Relations
Britto, Cachazo, Feng & Witten (2005)
• Ingredients
Structure of factorization
Cauchy’s theorem
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Introducing Complex Momenta
• Define a shift of spinors by a complex parameter z
• which induces a shift of the external momenta
• and defines a z-dependent continuation of the amplitude
• Assume that as
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
A Contour Integral
Consider the contour integral
Determine A(0) in terms of other residues
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Using Factorization
Other poles in z come from zeros of z-shifted propagator denominators
Splits diagram into two parts with z-dependent momentum flow
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Exactly factorization limit of z-dependent amplitudepoles from zeros of
That is, a pole at
Residue
Notation
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
On-Shell Recursion Relation
==
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
• Partition P: two or more cyclicly-consecutive momenta containing j, such that complementary set contains l,
• The recursion relations are then
On shell
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Number of terms ~ |l−j| (n−3)
so best to choose l and j nearby
Complexity still exponential, because shift changes as we descend the recursion
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Applications• Very general: relies only on complex analysis +
factorization• Fermionic amplitudes• Applied to gravity
Bedford, Brandhuber, Spence, & Travaglini (2005)Cachazo & Svrček (2005)
Arkani-Hamed, Cachazo, & Kaplan (2008)• Massive amplitudes
Badger, Glover, Khoze, Svrček (2005)Forde & DAK (2005)
• Other rational functionsBern, Bjerrum-Bohr, Dunbar, & Ita (2005)
• Connection to Cachazo–Svrček–Witten constructionRisager (2005)
• CSW construction for gravityBjerrum-Bohr, Dunbar, Ita, Perkins, & Risager (2005)
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Three-Gluon Amplitude Revisted
Let’s compute it with complex momenta chosen so that
that is,
but
compute
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Choose common reference momentum q so we have to compute
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Not manifestly gauge invariant
but gauge invariant nonetheless,and exactly the n=3 case of the general Parke–
Taylor formula!
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Four-Point Example
Pick a shift, giving one diagram
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
shift
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Choosing Shift Momenta
• What are legitimate choices?• Need to ensure that as• At tree level, legitimate choices
• Power counting argument in Feynman diagrams for
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Three-point vertices with z-dependent momentum flow ~ z
Four-point vertices with z-dependent momentum flow ~ 1
Propagators with z-dependent momentum flow ~ 1/z
Leading contributions from diagrams with only three-point vertices and propagators connecting j to l: ~ 1/z
(one more vertex than propagators & two εs)
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Factorization in Complex Momenta
• Factorization theorems derived for real momenta• For multiparticle poles, hold for complex
momenta as well
• At tree level, collinear factorization holds for complex momenta as well, because splitting amplitudes only involve 1/spinor product, so we only get pure single poles
• Double poles cannot arise because each propagator can only give rise to a single invariant in the denominator
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
MHV Amplitudes
Compute the (1−,j−) amplitude: choose shift
Other diagrams vanish becauseor
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
• Prove Parke–Taylor equation by induction
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Singularity Structure
• On-shell recursion relations lead to compact analytic expressions
• Different form than Feynman-diagram computation
• Appearance of spurious singularities
physical singularitiesunphysical singularity — cancels between terms
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Loop Calculations: Textbook Approach
• Sew together vertices and propagators into loop diagrams
• Obtain a sum over [2,n]-point [0,n]-tensor integrals, multiplied by coefficients which are functions of k and
• Reduce tensor integrals using Brown-Feynman & Passarino-Veltman brute-force reduction, or perhaps Vermaseren-van Neerven method
• Reduce higher-point integrals to bubbles, triangles, and boxes
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
• Can apply this to color-ordered amplitudes, using color-ordered Feynman rules
• Can use spinor-helicity method at the end to obtain helicity amplitudes
BUT• This fails to take advantage of gauge
cancellations early in the calculation, so a lot of calculational effort is just wasted.
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Can We Take Advantage?
• Of tree-level techniques for reducing computational effort?
• Of any other property of the amplitude?
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Unitarity
• Basic property of any quantum field theory: conservation of probability. In terms of the scattering matrix,
In terms of the transfer matrix we get,
or
with the Feynman i
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
This has a direct translation into Feynman diagrams, using the Cutkosky rules. If we have a Feynman integral,
and we want the discontinuity in the K2 channel, we should replace
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
• When we do this, we obtain a phase-space integral
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
In the Bad Old Days of Dispersion Relations
• To recover the full integral, we could perform a dispersion integral
in which so long as when • If this condition isn’t satisfied, there are
‘subtraction’ ambiguities corresponding to terms in the full amplitude which have no discontinuities
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
• But it’s better to obtain the full integral by identifying which Feynman integral(s) the cut came from.
• Allows us to take advantage of sophisticated techniques for evaluating Feynman integrals: identities, modern reduction techniques, differential equations, reduction to master integrals, etc.
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Computing Amplitudes Not Diagrams
• The cutting relation can also be applied to sums of diagrams, in addition to single diagrams
• Looking at the cut in a given channel s of the sum of all diagrams for a given process throws away diagrams with no cut — that is diagrams with one or both of the required propagators missing — and yields the sum of all diagrams on each side of the cut.
• Each of those sums is an on-shell tree amplitude, so we can take advantage of all the advanced techniques we’ve seen for computing them.
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Original Unitarity-Based Method at One Loop
• Compute cuts in a set of channels• Compute required tree amplitudes• Form the phase-space integrals• Reconstruct corresponding Feynman integrals• Perform integral reductions to a set of master
integrals• Assemble the answer
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Unitarity-Based Calculations
Bern, Dixon, Dunbar, & DAK (1994)
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Unitarity-Based Calculations
• In general, work in D=4-2 full answervan Neerven (1986): dispersion relations converge
• At one loop in D=4 for SUSY full answer
• Merge channels rather than blindly summing: find function w/given cuts in all channels
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
The Three Roles of Dimensional Regularization
• Ultraviolet regulator;• Infrared regulator;• Handle on rational terms.• Dimensional regularization effectively removes the
ultraviolet divergence, rendering integrals convergent, and so removing the need for a subtraction in the dispersion relation
• Pedestrian viewpoint: dimensionally, there is always a factor of (–s)–, so at higher order in , even rational terms will have a factor of ln(–s), which has a discontinuity
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Integral Reductions
• At one loop, all n5-point amplitudes in a massless theory can be written in terms of nine different types of scalar integrals:
• boxes (one-mass, ‘easy’ two-mass, ‘hard’ two-mass, three-mass, and four-mass);
• triangles (one-mass, two-mass, and three-mass);
• bubbles
• In an N =4 supersymmetric theory, only boxes are needed.
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
The Easy Two-Mass Box
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On-Shell Methods in Gauge Theory, Taiwan Summer Institute ( 溪頭 ), Aug 10–17, 2008
Infrared Singularities
Loop momentum nearly on shelland softor collinear with massless external legor both
Coefficients of infrared poles anddouble poles must be proportionalto the tree amplitude for cancellationsto happen