Unitarity and the Mandelstam Representation. II. Large-Angular-Momentum Partial-Wave Amplitudes

1968 ◽  
Vol 173 (5) ◽  
pp. 1439-1451 ◽  
Author(s):  
Arthur W. Martin
Keyword(s):  
Angular Momentum ◽  
Partial Wave ◽  
Mandelstam Representation ◽  
Large Angular Momentum

Deuteron elastic scattering in the large angular momentum limit

1981 ◽  
Vol 371 (3) ◽  
pp. 381-392 ◽  
Author(s):  
R.C. Johnson ◽  
E.J. Stephenson
Keyword(s):  
Angular Momentum ◽  
Elastic Scattering ◽  
Large Angular Momentum

Magnetic Resonance with Large Angular Momentum

1964 ◽  
Vol 135 (1A) ◽  
pp. A39-A43 ◽  
Author(s):  
J. W. Cederberg ◽  
N. F. Ramsey
Keyword(s):  
Angular Momentum ◽  
Magnetic Resonance ◽  
Large Angular Momentum

General Properties of Higher-Spin Fermion Interaction Currents and Their Test in πN-Scattering

2021 ◽  
Vol 57 (11) ◽  
pp. 1179
Author(s):  
Yu.V. Kulish ◽  
E.V. Rybachuk
Keyword(s):  
Angular Momentum ◽  
Partial Wave ◽  
Total Angular Momentum ◽  
Mass Shell ◽  
Present Approach ◽  
Partial Wave Analysis ◽  
Wave Analysis ◽  
Fermion Propagator ◽  
Higher Spin ◽  
Spin Tensors

The currents of higher-spin fermion interactions with zero- and half-spin particles are derived. They can be used for the N*(J) ↔ Nπ-transitions (N*(J) is thenucleon resonance with the J spin). In accordance with the theorem on currents and fields, the spin-tensors of these currents are traceless, and their products with the γ-matrices and the higher-spin fermion momentum vanish, similarly to the field spin-tensors. Such currents are derived explicitly for J=3/2and 5/2. It is shown that, in the present approach, the scale dimension of a higher spin fermion propagator equals to –1 for any J ≥ 1/2. The calculations indicate that the off-mass-shell N* contributions to the s-channel amplitudes correspond to J = JπN only ( JπN is the total angular momentum of the πN-system). As contrast, in the usually exploited approaches, such non-zero amplitudes correspond to 1/2 ≤  JπN ≤ J. In particular, the usually exploited approaches give non-zero off-mass-shell contributions of the ∆(1232)-resonance to the amplitudes S31, P31( JπN = 1/2) and P33, D33(JπN = 3/2), but our approach – to P33 and D33 only. The comparison of these results with the data of the partial wave analysis on the S31-amplitude in the ∆(1232)-region shows the better agreement for the present approach.

Three-particle partial wave amplitudes and unitarity conditions at complex values of angular momentum

1966 ◽  
Vol 37 (2) ◽  
pp. 227-263 ◽  
Author(s):  
A.A. Anselm ◽  
Ya.I. Azimov ◽  
G.S. Danilov ◽  
I.T. Dyatlov ◽  
V.N. Gribov
Keyword(s):  
Angular Momentum ◽  
Partial Wave

scholarly journals Study of rotating high energy systems with the differential HBT method

2014 ◽  
Vol 23 (09) ◽  
pp. 1450043 ◽  
Author(s):  
L. P. Csernai ◽  
S. Velle
Keyword(s):  
Angular Momentum ◽  
Energy Systems ◽  
Heavy Ion ◽  
High Energy ◽  
Heavy Ion Reactions ◽  
Particle Correlations ◽  
Large Angular Momentum

Peripheral heavy-ion reactions at ultra relativistic energies have large angular momentum that can be studied via two particle correlations using the Differential Hanbury Brown and Twiss method. In the present work, we analyze the possibilities and sensitivity of the method in rotating, few source systems. Analytic results provide insight in the advantages of this method.

Evidence for large angular momentum window associated with incomplete fusion reactions

1986 ◽  
Vol 323 (2) ◽  
pp. 163-171 ◽  
Author(s):  
H. Tricoire ◽  
C. Gerschel ◽  
A. Gillibert ◽  
N. Perrin
Keyword(s):  
Angular Momentum ◽  
Incomplete Fusion ◽  
Fusion Reactions ◽  
Large Angular Momentum
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