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About LinkBacksSpace-time points are independence of each other. However, when a group of space-time points share approximately the same space domain, they form mass particles of matter. Sharing the same time domain (the same time axis), they form waves of fields and energies. When they share the same space-time domain, they form squares of energy as quantum fields or true positive and negative vacuum.
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Thread: share and share alike
- 05-12-2006 03:41 PM #1Raider of the lost time
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share and share alike
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
- 05-12-2006 04:23 PM #2Raider of the lost time
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Re: share and share alike
http://www.aip.org/history/heisenberg/p08.htm and http://en.wikipedia.org/wiki/Uncertainty_principle
When space-time points share the same space domain, it is expressed by position-momentum conjugates form of the uncertainty principle
. When they share the same time domain, it is expressed by energy-time conjugates form of the uncertainty principle 
. The product of these two forms the sharing of the same space-time domain as quantum fields of second partial time derivative of square of energy [math]\partial[/math]
. Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
- 05-12-2006 06:41 PM #3The Thinker
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Re: share and share alike
Anotnio,
What is exactly your definition of domain? Do you apply to it any mathematics? Also, is the type of domain (temporal, spatial, spatio-temporal) an indicator of the charge of the space-time points (I can't remember what name you gave to the charge though)?
- 05-14-2006 03:58 PM #4Raider of the lost time
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Re: share and share alike
A nonempty set. Particularly a set of space-time points.
Originally Posted by GUILLE Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
- 05-14-2006 05:30 PM #5The Thinker
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Re: share and share alike
But how many? Can it be from 1 to infinity? Originally Posted by AntonioLao
- 05-15-2006 12:33 PM #6Raider of the lost time
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Re: share and share alike
At least one, at most infinitely enumerable. Originally Posted by GUILLE Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
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