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  1. #1
    Raider of the lost time AntonioLao is a splendid one to behold AntonioLao is a splendid one to behold AntonioLao is a splendid one to behold AntonioLao is a splendid one to behold
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    introduction to Hadamard space

    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(tr(t)=c²

  2. #2
    The Thinker Guille is a glorious beacon of light Guille is a glorious beacon of light
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    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.

  3. #3
    Raider of the lost time AntonioLao is a splendid one to behold AntonioLao is a splendid one to behold AntonioLao is a splendid one to behold AntonioLao is a splendid one to behold
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    Quote Originally Posted by GUILLE
    Can you give me the equation for that?
    It is in the introduction to the paper on Hadamard matrices dated October 11, 2005.
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²

  4. #4
    The Thinker Guille is a glorious beacon of light Guille is a glorious beacon of light
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    Quote Originally Posted by AntonioLao
    It is in the introduction to the paper on Hadamard matrices dated October 11, 2005.
    What page?

  5. #5
    Raider of the lost time AntonioLao is a splendid one to behold AntonioLao is a splendid one to behold AntonioLao is a splendid one to behold AntonioLao is a splendid one to behold
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    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(tr(t)=c²

  6. #6
    The Thinker Guille is a glorious beacon of light Guille is a glorious beacon of light
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    Quote 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]
    Can't see the latex equation in your post. But I did find it in the paper. Thanks.

  7. #7
    Raider of the lost time AntonioLao is a splendid one to behold AntonioLao is a splendid one to behold AntonioLao is a splendid one to behold AntonioLao is a splendid one to behold
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    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(tr(t)=c²

  8. #8
    Master neutralino is a jewel in the rough neutralino is a jewel in the rough
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    Re: introduction to Hadamard space

    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.

  9. #9
    Raider of the lost time AntonioLao is a splendid one to behold AntonioLao is a splendid one to behold AntonioLao is a splendid one to behold AntonioLao is a splendid one to behold
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    Re: introduction to Hadamard space

    Quote Originally Posted by neutralino
    provide a link to the paper that you mention here
    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!
    Time independence: [∂E(g)]²=[∂F(a)×∂r(a)]·[∂F(b)×∂r(b)] and Mass independence: a(tr(t)=c²


 

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