Optimal control of the population dynamics of the ground vibrational state of a polyatomic molecule

2011 ◽  
Author(s):  
Ludwig E. de Clercq ◽  
Lourens R. Botha ◽  
Erich G. Rohwer ◽  
Hermann Uys ◽  
Anton Du Plessis
Keyword(s):  
Optimal Control ◽  
Population Dynamics ◽  
Polyatomic Molecule ◽  
Vibrational State ◽  
Ground Vibrational State

Speed dependence of collisional relaxation in ground vibrational state of OCS: Rotational behaviour

2012 ◽  
Vol 136 (12) ◽  
pp. 124316 ◽  
Author(s):  
Maxim A. Koshelev ◽  
Mikhail Yu. Tretyakov ◽  
François Rohart ◽  
Jean-Pierre Bouanich
Keyword(s):  
Vibrational State ◽  
Rotational Behaviour ◽  
Collisional Relaxation ◽  
Ground Vibrational State ◽  
Speed Dependence

Optimal Control of Population Dynamics

1999 ◽  
Vol 102 (1) ◽  
pp. 1-14 ◽  
Author(s):  
V. Barbu ◽  
M. Iannelli
Keyword(s):  
Optimal Control ◽  
Population Dynamics

Vector Control, Optimal Control, and Vector-Borne Disease Dynamics

2020 ◽  
pp. 267-288
Author(s):  
Michael B. Bonsall
Keyword(s):  
Optimal Control ◽  
Population Genetics ◽  
Population Dynamics ◽  
Vector Control ◽  
Cost Effective ◽  
Disease Suppression ◽  
Medical Interventions ◽  
Vector Borne Disease ◽  
Vector Borne

Understanding methods of vector control is essential to vector-borne disease (VBD) management. Vaccines or standard medical interventions for many VDBs do not exist or are poorly developed so disease control is focused on managing vector numbers and dynamics. This involves understanding not only the population dynamics but also the population genetics of vectors. Using mosquitoes as a case study, in this chapter, the modern genetics-based methods of vector control (self-limiting, self-sustaining) on mosquito population and disease suppression will be reviewed. These genetics-based methods highlight the importance of understanding the interplay between genetics and ecology to develop optimal, cost-effective solutions for control. The chapter focuses on how these genetics-based methods can be integrated with other interventions, and concludes with a summary of regulatory and policy perspectives about the use of these approaches in the management of VBDs.

Millimeter Wave Rotational Transitions of 16O12C32S and 16O13C32S

1974 ◽  
Vol 29 (8) ◽  
pp. 1213-1215 ◽  
Author(s):  
N. W. Larsen ◽  
B. P. Winnewisser
Keyword(s):  
Excited States ◽  
Millimeter Wave ◽  
Vibrational Spectra ◽  
Vibrational State ◽  
Vibrational States ◽  
Ground Vibrational State ◽  
Wave Region ◽  
Rotational Transitions ◽  
Good Agreement

Rotational transitions of 16012C32S and 16013C32S in the ground vibrational state and of 16012C32S in several excited states have been accurately measured in the millimeter wave region for a minimum of four different J values. The analysis of the measured frequencies leads to rotational constants for the following vibrational states: 0 00 0 of 16O13C32S and 0 00 0, 0 1 1c 0, 0 1 1d 0, 0 20 0, 0 22c 0, 0 22d 0, 0 00 1 of 16O12C32S. Since the two components of the 0 22 0 transitions were resolved, an analysis of the l-type resonance was carried out and the interval 0 22 0 - 0 20 0 has been determined to be -4.63(10) cm-1. The result is in good agreement with the presently available determination of this level from vibrational spectra.

Optimization of Raman Cooling of 25Mg+ Ion to Ground Vibrational State in Linear Paul Trap

2019 ◽  
Vol 46 (4) ◽  
pp. 138-142
Author(s):  
P. L. Sidorov ◽  
K. Yu. Khabarova ◽  
I. V. Zalivako ◽  
A. S. Borisenko ◽  
I. A. Semerikov
Keyword(s):  
Vibrational State ◽  
Paul Trap ◽  
Linear Paul Trap ◽  
Ground Vibrational State ◽  
Raman Cooling

Elektrisches Dipolmoment von TlBr und TlJ

1971 ◽  
Vol 26 (11) ◽  
pp. 1809-1812 ◽  
Author(s):  
E. Tiemann
Keyword(s):  
Dipole Moment ◽  
Electric Dipole Moment ◽  
Electric Dipole ◽  
Vibrational State ◽  
Stark Effect ◽  
Dipole Moments ◽  
Electric Dipole Moments ◽  
Ground Vibrational State ◽  
Rotational Transitions

Stark-effect measurements on pure rotational transitions of TlBr and Til are described. The derived electric dipole moments of the most abundant isotopic molecules on the ground vibrational state are:205TL79Br : | μ0| = (4.493 ± 0.050) D , 205Tl127 I | μ 0| =(4.607 ± 0.070) D .The electric dipole moment of 205Tl19F | μ 0|=4.2282 (8) D was used as standard.

Sign in / Sign up

Export Citation Format

Share Document