scholarly journals Numerical and exact kinetic energy operator using Eckart conditions with one or several reference geometries: Application to HONO

2016 ◽  
Vol 144 (8) ◽  
pp. 084116 ◽  
Author(s):  
David Lauvergnat ◽  
Josep M. Luis ◽  
Bernard Kirtman ◽  
Heribert Reis ◽  
André Nauts
Keyword(s):  
Kinetic Energy ◽  
Energy Operator ◽  
Kinetic Energy Operator

Kinetic-energy operator in the effective shell-model interaction

1992 ◽  
Vol 46 (6) ◽  
pp. 2333-2339 ◽  
Author(s):  
L. Jaqua ◽  
M. A. Hasan ◽  
J. P. Vary ◽  
B. R. Barrett
Keyword(s):  
Kinetic Energy ◽  
Shell Model ◽  
Energy Operator ◽  
Kinetic Energy Operator ◽  
Model Interaction

An exact kinetic energy operator for (HF)3 in terms of local polar and azimuthal angles

2001 ◽  
Vol 79 (2-3) ◽  
pp. 623-639 ◽  
Author(s):  
X -G Wang ◽  
T Carrington Jr.
Keyword(s):  
Kinetic Energy ◽  
Energy Operator ◽  
Kinetic Energy Operator

To facilitate exploiting the symmetry of (HF)3 we propose using local polar and azimuthal angles to specify the orientation of the HF units with respect to the frame of the trimer. We present and discuss the derivation of a kinetic energy operator in local polar and azimuthal angles and Pekeris–Jacobi coordinates. PACS No.: 31.15-P

scholarly journals HEAVY QUARK KINETIC ENERGY IN B MESONS BY A QCD RELATIVISTIC POTENTIAL MODEL

1996 ◽  
Vol 11 (34) ◽  
pp. 2693-2702 ◽  
Author(s):  
FULVIA DE FAZIO
Keyword(s):  
Kinetic Energy ◽  
B Mesons ◽  
Potential Model ◽  
B Meson ◽  
Energy Operator ◽  
Kinetic Energy Operator ◽  
Theoretical Approaches ◽  
The Matrix ◽  
Relativistic Potential ◽  
Meson States

The matrix element of the kinetic energy operator between B meson states is computed by means of a QCD relativistic potential model, with the result: [Formula: see text]. A comparison with the outcome of other theoretical approaches and a discussion of the phenomenological implications of this result are carried out.

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