Partial Wave Analysis and Amplitude Analysis PhenomenologyTheory of

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Partial Wave Analysis and Amplitude Analysis Phenomenology/Theory of amplitude parameterization and analysis (2 meson

Partial Wave Analysis and Amplitude Analysis Phenomenology/Theory of amplitude parameterization and analysis (2 meson and 3 mesons production) How to factorize amplitudes

A Physics Goal : three step process Identify old (a 2) and new (

A Physics Goal : three step process Identify old (a 2) and new ( 1) states Use data (“physical sheet”) as input to constrain theoretical amplitudes Resonances appear as a result of amplitude analysis and are identified as poles on the “un-physical sheet” 3. Interpretation: composite or fundamental, structure, relation to QCD, lattice, etc

Example of factorization s/t >> 1 T(s, t) several partial wave in s- channel

Example of factorization s/t >> 1 T(s, t) several partial wave in s- channel s ~ mx 2 single partial wave in s- channel

Two meson production Single Regge limit Double Regge limit Derive corresponding amplitudes and establish

Two meson production Single Regge limit Double Regge limit Derive corresponding amplitudes and establish singularity structure in sub-channel variables Add normal singularities (resonances) Use FESR to constrain parameters Resonance production

Resonance shape modification ZEUS W=70 Ge. V Szczurek et. al

Resonance shape modification ZEUS W=70 Ge. V Szczurek et. al

Establishing a P-wave in the , ’ M s>>t, M Regge Low energy EFT

Establishing a P-wave in the , ’ M s>>t, M Regge Low energy EFT t Complicated analytical structure Single resonance pole

 O(p 2 /f 2 ) = Low order expansion + Higher order expansion

O(p 2 /f 2 ) = Low order expansion + Higher order expansion + unitarization Interplay between “elementary” (CDD) and “dynamical” resonances

Lesniak et al. (98)

Lesniak et al. (98)

No FSI With FSI

No FSI With FSI

Amplitudes in three particle (meson) production a 2 -(1320) - (1) (J) CJLS L

Amplitudes in three particle (meson) production a 2 -(1320) - (1) (J) CJLS L Breit-Wigner S 0 - (2) + M s 1 (3) A(s 1, s 2, M) = CJLS (M) / D 1(s 1) 1 2 F(s 1, s 2, M) = N 1(M)/D 1(s 1) + N 2(M)/D 2(s 2) Independent on 2 -particle sub-channel energy : violates unitarity !

Has to depend on 2 -particle energy

Has to depend on 2 -particle energy

F 1(s 1, M)i = H(s 1, M)ij Cj(M) i, j= ,

F 1(s 1, M)i = H(s 1, M)ij Cj(M) i, j= ,

Some comments on the isobar model 7 kinematical variables + polarization +(1) -(3) isobar

Some comments on the isobar model 7 kinematical variables + polarization +(1) -(3) isobar +(2) s 13>>s 23 otherwise channels overlap : need disp. relations (FMSR) isobar model violates unitarity K-matrix “improvements” violate analyticity

Ambiguities in the 3 system

Ambiguities in the 3 system

Methods for constructing amplitudes (amplitude analysis) Analyticity: Data (in principle) allows to determine full

Methods for constructing amplitudes (amplitude analysis) Analyticity: Data (in principle) allows to determine full (including “unphysical” parts) Amplitudes. Bad news : need data for the entire universe Approximations: Crossing relates “unphysical regions” of a channel with a physical region of another Unitarity relates cuts to physical data Other symmetries (kinematical, dynamical: chiral, U(1), …) constrain low-energy parts of amplitudes (partial wave expansion, fix subtraction constant)

It is important to have a statement from a significant and respected representation of

It is important to have a statement from a significant and respected representation of the subatomic community to the effect that the scientific goals of the CLEO-c and Glue. X programs w. r. t. gluonic excitations are fundamental and important and that there is general agreement among theoretical and experimental components of the community as to what defines clear results.

A plan for theory (v. r. t amplitude analysis) Develop amplitude parameterization for selected

A plan for theory (v. r. t amplitude analysis) Develop amplitude parameterization for selected 2 and 3 meson production amplitudes Interplay between s and t channel physics constrained by analyticity and duality Prepare a review (manual ? ) describing amplitude analysis

Finite energy sum rules is an analytical function Continue out of physical region to

Finite energy sum rules is an analytical function Continue out of physical region to look for resonances