Hertzsprung-Russell Diagram: shows the evolutionary track that our sun will take as it evolves. Picture courtesy of Australia Telescope National Facility.
Stellar evolution is the life cycle that a star will take as it evolves over time. The different evolutionary stages of a star is heavily dependent on the mass of the star. For my research, I look at stars between 0.8 to 8 solar masses. These stars will start of as main sequence stars and will make their way to a white dwarf where the star will continue to cool off until it no longer emits light or heat. Within the stellar evolutionary cycle, I am specifically interested in the planetary nebula phase and the asymptotic giant branch or AGB phase.
The planetary nebula or PN phase is the last phase before the star becomes a white dwarf. In this phase, the star has ejected the majority of its mass and there isn't enough fusion reactions in the core to overcome the effects of gravity. Therefore the core will condense and increase in temperature. The core becomes hot enough to ionize the gas and dust around it, BUT the interesting thing is that there are clumps of molecular hydrogen in these ionized regions of the PNe. More defined clumps are called cometary knots, based on their comet like shape. Trivially, they shouldn't be there but somehow these molecular "clumps" are optically thick enough to survive harsh, ionized regions
Cat Eye Nebula. Picture courtesy of NASA.gov
Illustration of variable star with maser emission ranges. Picture courtesy of Wittkowski, M et al. 2008
The AGB phase is the phase right before planetary nebula. You can think of an AGB star as a specific type of red giant. Due to their stellar winds, AGB stars will lose 50 to 70 percent of their mass. These stars are also variable stars. Meaning, the star has a cycle of expansions and contractions in increments of time known as pulsations. The most interesting thing about the AGB stars are the maser emissions that are found in the atmosphere. Masers are very similar to lasers. Lasers stands for light amplification by stimulated emission of radiation. which is fundamentally a laser but in microwaves instead of visible light. SiO, H2O, and OH masers are fairly common in AGB stars and have unique characteristics.
First we should ask "where do cometary knots come from?" because that the question I'm hoping to answer. There are 2 main theories of the origins of cometary knots: 1. they are formed during the planetary nebula phase, 2. they are formed pre-planetary nebula phase. There is strong evidence that supports theory 2. I believe that the maser emissions in AGB stars are the key to solving this problem. Masers provide a perfect density enhancement for the molecular gas to be dense enough to survive ionization. Currently, I am using the astrophysics data system to gather maser emission data from papers that have investigated either variable star characteristics and/or maser emissions in variable stars. While compiling this data, I'm making plots of different parameters looking for trends in maser emission characteristics and trends in the stars themselves. The data will be used as initial conditions in a simulated AGB star. As the simulated star evolves from AGB to planetary nebula, the simulation will show whether or not it is possible for maser emissions to survive the transition to the nebula phase... if so this is great evidence to support maser emissions as the origins of cometary knots. Understanding the origins of cometary knots will help us to better understand the evolution of low to intermediate mass stars.