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dawn of power LASER
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dawn of power LASER - 03-15-2008, 12:49 PM

Yesterday was Einstein’s 129 birthdays. It was the middle of 1916*, after his monumental achievement of special relativity and before the experimental proof of general relativity by Sir Arthur Eddington, Einstein first introduced the concept of stimulated emission of radiation now known as the working principle of LASER (light amplification by stimulated emission of radiation). The power of LASER is its concentration of thermal energy obeying the principle of superposition for all bosons. Its converse is the Pauli Exclusion Principle for all fermions. Ordinary light at best can provide thermal energy of 10000 kelvins but with LASER 1 000 000 000 000 000 000 000 000 000 000 kelvins is feasible. Note that the corona of the sun is only about 2000000 kelvins, a fraction of 24 powers of 10 cooler and water boils merely at about 400 kelvins.

In spite of this tremendous power, LASER still could not sustain inertial fusion. This brings back the questions whether controlled thermonuclear fusion processes are truly temperature dependence and that which also allows the rethinking of cold fusion at room temperature. However, if a working principle of proximity can be allowed to prove a proximity theorem for virtual reality then it is possible to find a power source for amplifying virtual photons and to make them oscillate inside a resonating cavity. This possibility is tantamount to scratching the tip of the iceberg of vacuum energy by making virtual imaginary photons into real powerful photons that exceed the thermal output of a quadrillion suns, all put together at a space-time point.

*For a complete English translation, see Doc. 34, The Collected Papers of Albert Einstein, Volume 6, The Berlin years: Writings, 1914-1917.


Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²
  
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Re: dawn of power LASER
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Re: dawn of power LASER - 03-15-2008, 01:01 PM

Isn't pressure tied into temperature. Maybe that's what is missing.

Best,

Pat
  
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Re: dawn of power LASER - 03-15-2008, 01:16 PM

Quote:
Originally Posted by Profpat
Isn't pressure tied into temperature
Pressure seems to apply exclusively for fermions when they try to violate the principle of exclusion while for bosons when they try to get away from each other faster than lightspeed.


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Smile Re: dawn of power LASER - 03-15-2008, 01:20 PM

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Pressure seems to apply exclusively for fermions when they try to violate the principle of exclusion while for bosons when they try to get away from each other faster than lightspeed.

Those dam bosons,too quick for me,don't trust em!




regards michael.


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Re: dawn of power LASER - 03-15-2008, 01:21 PM

I guess I didn't know that Antonio. I was thinking about the fussion power of our sun and other stars which make the heavier elements due to pressure and temperature.
  
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Re: dawn of power LASER - 03-15-2008, 01:23 PM

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Those dam bosons,too quick for me,don't trust em!




regards michael.
LOL. I only trust God Michael. I don't even trust myself.
  
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Re: dawn of power LASER - 03-15-2008, 01:33 PM

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don't trust em
This seems to imply that the only trusting person is a blind person since photon bosons are the ones that are responsible for the faculty of sight not sound, taste, touch, or smell and some people trust their noses. Still for many to see is to believe.


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Re: dawn of power LASER - 03-15-2008, 01:37 PM

Well maybe New York will have a governor they can trust.
  
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Smile Re: dawn of power LASER - 03-15-2008, 01:42 PM

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This seems to imply that the only trusting person is a blind person since photon bosons are the ones that are responsible for the faculty of sight not sound, taste, touch, or smell and some people trust their noses. Still for many to see is to believe.

Maybe thats why that boson winked at me,prehaps it was a nervous tic?


regards michael


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Re: dawn of power LASER - 03-15-2008, 01:44 PM

Quote:
Originally Posted by Profpat
a governor they can trust
Unless they are blinded by lust for sensual pleasures.


Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²
  
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