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Grant: Discovery Grants Program - Individual

University of Northern British Columbia

$13,084.00

Tunnelling of molecules and quantum decay

EF 2009-10

Résumé
In our everyday experience, particles trapped inside energy wells can escape only if they have more energy than the energy barrier; a marble trapped in a bowl stays inside unless it has enough energy to rise to the top of the bowl and get out. For microscopic particles it is possible for a particle to escape even if its energy is less than the barrier. This phenomenon is call "tunnelling." Tunnelling has been investigated almost solely for single particles. Investigations into the tunnelling of molecules began relatively recently. The simplest molecule consists of two atoms and thus has an elongated structure: this is what makes the study of tunnelling of molecules interesting and challenging. In order to escape confinement inside an energy barrier, both atoms need to tunnel out, and there are several ways this can happen. For example: the molecule breaks up into two atoms. In the proposed research we investigate how the possible breaking up of the molecule affects the probability of tunnelling. In previous work we found that for special values of the molecule's total energy, the probability is 100%, and is called "resonant tunnelling." In the case of molecular tunnelling, we want to find out how the possibility of molecular break-up will affect these resonances, i.e. we know that the probability will go down, but the question is by how much and why that amount? We will first consider a molecule moving along a straight line. We will extend our work to the more realistic case where the molecule moves in three dimensions. Our goal is to understand why the probabilities of tunnelling and reflection have the values they do and why they change with the energy of the molecule as they do, and not some other way. We will also study the special case where the molecule is very weakly bound, i.e. it will certainly break apart in attempting to tunnel. This will also be done for one and three dimensions. Our ultimate objective is to extend our study so that it can be compared with real molecules and other pairs of particles. We will also do two other investigations in the behaviour of quantum mechanical systems. This work will eventually have practical applications; the specific details are not known at this time.
Programme
Discovery Grants Program - Individual
Emplacement
British Columbia, Canada
Type de bénéficiaire
Academia
Type
Grant
Source
NSERC's Awards Data

Tel que publié

Application id
180572-2008
Name nom
Shegelski, Mark
Department département
Physics
Organization id
3
Institution établissement
University of Northern British Columbia
Province en
British Columbia
Province fr
Colombie-Britannique
Country en
CANADA
Country fr
CANADA
Fiscal year exercice financier
2009
Competition year année de concours
2008
Award amount
13084
Program id
RGPIN
Program nane en
Discovery Grants Program - Individual
Program name fr
Programme de subventions à la découverte - individuelles
Group en
Discovery grants programs
Group fr
Programmes de subventions à la découverte
Committee code
28
Committee name en
Condensed Matter Physics
Committee name fr
Phys. de la matière condensée
Area of application code
405
Area of application group en
Environment
Area of application group fr
Environnement
Area of application en
Modelling and mathematical simulation of natural processes
Area of application fr
Modélisation et simulation mathématique des processus naturels
Research subject code
3150
Research subject group en
Theoretical physics and chemistry
Research subject group fr
Physique et chimie théoriques
Research subject en
Theoretical physics and chemistry
Research subject fr
Physique et chimie théoriques
Partie
2
Nb partie
3
Application title
Tunnelling of molecules and quantum decay
Keyword
NA
Application summary
In our everyday experience, particles trapped inside energy wells can escape only if they have more energy than the energy barrier; a marble trapped in a bowl stays inside unless it has enough energy to rise to the top of the bowl and get out. For microscopic particles it is possible for a particle to escape even if its energy is less than the barrier. This phenomenon is call "tunnelling." Tunnelling has been investigated almost solely for single particles. Investigations into the tunnelling of molecules began relatively recently. The simplest molecule consists of two atoms and thus has an elongated structure: this is what makes the study of tunnelling of molecules interesting and challenging. In order to escape confinement inside an energy barrier, both atoms need to tunnel out, and there are several ways this can happen. For example: the molecule breaks up into two atoms. In the proposed research we investigate how the possible breaking up of the molecule affects the probability of tunnelling. In previous work we found that for special values of the molecule's total energy, the probability is 100%, and is called "resonant tunnelling." In the case of molecular tunnelling, we want to find out how the possibility of molecular break-up will affect these resonances, i.e. we know that the probability will go down, but the question is by how much and why that amount? We will first consider a molecule moving along a straight line. We will extend our work to the more realistic case where the molecule moves in three dimensions. Our goal is to understand why the probabilities of tunnelling and reflection have the values they do and why they change with the energy of the molecule as they do, and not some other way. We will also study the special case where the molecule is very weakly bound, i.e. it will certainly break apart in attempting to tunnel. This will also be done for one and three dimensions. Our ultimate objective is to extend our study so that it can be compared with real molecules and other pairs of particles. We will also do two other investigations in the behaviour of quantum mechanical systems. This work will eventually have practical applications; the specific details are not known at this time.