*Effects of Spin-Dependent Polariton-Polariton Interactions in
Semiconductor Microcavities: Spin Rings, Bright Spatial Solitons and
Soliton Patterns*

http://etheses.whiterose.ac.uk/3872/1/SICH_eThesis.pdf

A polariton BEC is a different animal from a matter based BEC. It involves
a process of energy flows and balances. These two types a BEC are not
comparable as explained below.

See chapter 1.2

The polaritons have a lifetime that is typically comparable to or shorter
than thermalization times, giving them an inherently non-equilibrium
nature. Nevertheless, they exhibit many of the features that would be
expected of equilibrium Bose–Einstein condensates (BECs). The
non-equilibrium nature of the system raises fundamental questions as to
what it means for a system to be a BEC, and introduces new physics beyond
that seen in other macroscopically coherent systems.

One thing I learned from this reference is that the spin of a dark
polariton is 2. That is a lot of spin. A dark poloriton is in superposition
with holes rather than electrons.

On Tue, Dec 30, 2014 at 3:09 PM, MarkI-ZeroPoint <[email protected]>
wrote:

> Hi John:
>
> To answer your two questions:
>
> - Emphatically No
>
> - Huh?  J
>
>
>
> I will go into greater detail about what temperature is when replying to
> Bob’s response…
>
> But to answer your second question, what is ‘hot’ ???  That’s an imprecise
> and relative word…
>
>
>
> Start out with any atom which is at 0K, in other words, at its lowest
> energy state.  In my model, electrons and protons are an oscillation of
> some kind.  At this lowest energy state, these oscillators will have **very
> precise** frequencies and phase relationships between them.  Here’s
> another clue as to what this state is like:
>
>
>
> ----------------
>
>
> http://newscenter.berkeley.edu/2012/06/08/theorem-unifies-superfluids-and-other-weird-materials/
>
>
>
> “In Bose-Einstein condensates, for example, “you start with a thin gas of
> atoms, cool it to incredibly low temperature — nanokelvins — and once you
> get to this temperature, atoms tend to stick with each other in strange
> ways,” Murayama said.  “They have this funny vibrational mode that gives
> you one Nambu-Goldstone boson, and this gas of atoms starts to become
> superfluid again so it  ***CAN FLOW WITHOUT VISCOSITY FOREVER.***”
>
>
>
> And this is a MOST important statement to understand what we are dealing
> with:
>
>
>
> "One characteristic of states with a low Nambu-Goldstone boson number is
> that very little energy is required to perturb the system. Fluids flow
> freely in superfluids, and
>
>      **atoms vibrate forever in Bose-Einstein condensates with just a
> slight nudge.*** "
>
> ----------------
>
>
>
> These are CLUES as to what we are really dealing with when it comes to
> atoms/electrons/protons when NOT complicated by heat…  heat is NOT the norm
> in the universe.   This is where we should have started when trying to come
> up with theories to describe atoms and the subatomic particles… however,
> living in a world bathed in heat from the sun, our theories had to deal
> with the disorder caused by a multitude of heat quanta jumping around from
> atom to atom like a hot potatoes game; each person is an atom, and the hot
> potatoes are the heat quanta…
>
>
>
> My goal with Dr. Storms, and with The Collective, is to get an accurate
> (or at least better) picture/understanding of what the ‘conditions’ are
> inside the NAE/voids/microcavities.  I would wager that it is very
> different from what most are thinking… and if I’m right, then trying to
> apply modern mainstream theories to how atoms are behaving inside the NAE
> is not going to be successful.  It’s a very different universe in there,
> with a very different set of ‘rules’…
>
>
>
> -mark iverson
>
>
>
>
>
> *From:* John Berry [mailto:[email protected]]
> *Sent:* Monday, December 29, 2014 11:04 PM
> *To:* [email protected]
> *Subject:* [Vo]:Re: [Vo]:FYI: Strong light–matter coupling in
> two-dimensional atomic crystals
>
>
>
> Can an atom have a temperature between its different parts?
>
>
>
> Is an atom that is excited and about to emit a photon not quite hot?
>
>
>
>
>
>
>
> On Tue, Dec 30, 2014 at 6:09 PM, David Roberson <[email protected]>
> wrote:
>
> I have considered what you are saying as being normal Mark.  Relative
> motion of an atom to itself is zero, so it is at zero kelvin as far as it
> knows.  When a second atom is added to the void, it becomes more
> complicated but the relative motion of the two must become zero many times
> per second as they collide and rebound within your assumed cavity.  During
> these brief intervals we have two atoms that are at zero Kelvin from their
> reference frame.  As you add more and more atoms to the mix the amount of
> time during which zero relative motion exists between them becomes smaller
> and less likely, but does occur.
>
> As long as you keep the number of atoms relatively small that are required
> to react in the process of your choice, it will have an opportunity to
> happen many times per second inside each cavity.  Multiply that number by
> the number of possible active cavities within a large object and you get an
> enormous number of active sites that have the potential to react.
>
> If only 4 atoms are required at zero Kelvin in order to react as you may
> be considering, it seems obvious that this will occur so often that a large
> amount of heat will be released by a system of that type.  When you realize
> that it seems to be very difficult to achieve an LENR device that generates
> lots of heat I suspect that the number of reacting atoms confined within
> the cavity is quite a bit greater than 4.  How many do you believe are
> required in order to combine and in what form is the ash?
>
> On the other hand, if a reaction is virtually guaranteed once a modest
> number of atoms becomes confined inside the void, then the limiting factor
> might be that it becomes impossible to confine the required number under
> most conditions.  If this situation is the limiting factor, then a higher
> temperature could well allow more atoms of the reactants to enter into a
> void of the necessary type as more space become available when the cavity
> walls open with additional motion.
>
> I am not convinced that this type of reaction is the cause of LENR, but at
> least it should be given proper consideration.
>
> Dave
>
>
>
>
>
>
>
> -----Original Message-----
> From: MarkI-ZeroPoint <[email protected]>
> To: vortex-l <[email protected]>
> Sent: Mon, Dec 29, 2014 10:54 pm
> Subject: [Vo]:FYI: Strong light–matter coupling in two-dimensional atomic
> crystals
>
> FYI:
>
>
>
> Article being referenced is at the bottom, however, I wanted to toss
> something out to The Collective first…
>
>
>
> One of the things that caught my eye in the article is the ‘room
> temperature’ condition…
>
>
>
> As we all know, atoms at room temp are vibrating like crazy since they
> contain the equivalent of 273degC of energy above their lowest state.
> Thus, ‘coherent’ states in condensed matter above absolute zero is almost
> never seen.  The article’s experiment was done in material at room temp, so
> the observed behavior is a bit of a surprise.  Perhaps what they have not
> yet thought about is that the ‘microcavities’ have no temperature, as I
> will explain below.
>
>
>
> This ties in with a point I tried to explain to Dr. Storms, and although I
> think he realizes my point had merit, he glossed right over it and went off
> on a different tangent.  This was in a vortex discussion about 9 to 12
> months ago.  The point is this:
>
>
>
> The ‘temperature’ inside a ‘void’ in a crystal lattice is most likely that
> of the vacuum of space; i.e, absolute zero, or very close to it.  Because,
> temperature is nothing more than excess energy imparted to atoms from
> neighboring atoms; atoms have temperature; space/vacuum does not.  Without
> atoms (physical matter), you have no temperature.  In a lattice void, if it
> is large enough (whatever that dimension is), there is NO ‘temperature’
> inside since the void contains no atoms.  If an atom diffuses into that
> void, it enters with whatever energy it had when it entered, so it has a
> temperature.  At this time, I have not heard any discussion as to whether
> the atoms which make up the walls of the void shed IR photons which could
> get absorbed by an atom in the void and increase its temperature, however,
> would that atom want to immediately shed that photon to get back to its
> lowest energy level???  So voids in crystals likely provide an ideal
> environment for the formation of BECs.
>
>
>
> -mark iverson
>
>
>
> ARTICLE BEING REFERENCED
>
>
>
> Strong light–matter coupling in two-dimensional atomic crystals
>
> http://www.nature.com/nphoton/journal/v9/n1/full/nphoton.2014.304.html
>
>
>
> Abstract
>
> “Two-dimensional atomic crystals of graphene, as well as transition-metal
> dichalcogenides, have emerged as a class of materials that demonstrate
> strong interaction with light. This interaction can be further controlled
> by embedding such materials into optical *microcavities*. When the
> interaction rate is engineered to be faster than dissipation from the light
> and matter entities, one reaches the ‘strong coupling’ regime. This results
> in the formation of half-light, half-matter bosonic quasiparticles called 
> *microcavity
> polaritons*. Here, we report evidence of strong light–matter coupling and
> the formation of microcavity polaritons in a two-dimensional atomic crystal
> of molybdenum disulphide (MoS2) embedded inside a dielectric microcavity at 
> *room
> temperature*. A Rabi splitting of 46 ± 3 meV is observed in
> angle-resolved reflectivity and photoluminescence spectra due to coupling
> between the two-dimensional excitons and the cavity photons. Realizing
> strong coupling at room temperature in two-dimensional materials that offer
> a disorder-free potential landscape provides an attractive route for the
> development of practical polaritonic devices.”
>
>
>
>
>

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