Similar to the Hilbert space of quantum mehanics, Hadamard space is a vector space of two outer products or cross products or vector products then the inner product of these products give square of energy.
Similar to the Hilbert space of quantum mehanics, Hadamard space is a vector space of two outer products or cross products or vector products then the inner product of these products give square of energy.
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
Can you give me the equation for that?
It's that I find it much easier in equations, the thing is that in language it looks like a lot of words saying nothing.
It is in the introduction to the paper on Hadamard matrices dated October 11, 2005.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
What page?Originally Posted by AntonioLao
If you cant find it on page 1 then I'm going to write the latex equation here
[Unparseable Latex Formula]
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
Can't see the latex equation in your post. But I did find it in the paper. Thanks.Originally Posted by AntonioLao
As the classifications of several known algebraic structures, the special Hadamard matrices used for spacetime quantization are all classifiable as semigroups with only the property of associativity for both operations of addition and multiplication. Although these special types of Hadamard matrices are not invertible (zero determinants), there still exist unique zero matrices as the identities of addition. The advantage of these special Hadamard matrices over other algebraic structures is their commutative property under the operations of both addition and multiplication.
Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: ¶a(t)·¶r(t)=c²
Antonio;
Could you please provide a link to the paper that you mention here. I notice you talk of these Hadamard matrices quite often, so I'd like to get more of a feel for them.
~neutralino
If you haven't found something strange during the day, it hasn't been much of a day - John A. Wheeler.
I'll try to recover the file I made about Hadamard matrices which was lost from the url site. Merry Christmas and a Happy New Year!Originally Posted by neutralino
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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